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Polymers, Volume 8, Issue 3 (March 2016) – 41 articles

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1775 KiB  
Article
Application of Chitinous Materials in Production and Purification of a Poly(l-lactic acid) Depolymerase from Pseudomonas tamsuii TKU015
by Tzu-Wen Liang, Shan-Ni Jen, Anh Dzung Nguyen and San-Lang Wang
Polymers 2016, 8(3), 98; https://doi.org/10.3390/polym8030098 - 22 Mar 2016
Cited by 30 | Viewed by 6621
Abstract
The management of fishery residues and plastics is considered to be a vital strategy for conserving resources and maintaining the quality of the environment. Poly(l-lactic acid) (PLA) is a commercially promising, renewable, and biodegradable plastic. In this study, a PLA depolymerase [...] Read more.
The management of fishery residues and plastics is considered to be a vital strategy for conserving resources and maintaining the quality of the environment. Poly(l-lactic acid) (PLA) is a commercially promising, renewable, and biodegradable plastic. In this study, a PLA depolymerase was produced in a squid pen powder (SPP) and recycled plastic waste (PLA powder)-containing medium by Pseudomonas tamsuii TKU015, a bacterial strain isolated from Taiwanese soil. This PLA depolymerase had a molecular weight of 58 kDa and was purified to homogeneity from the supernatant of a TKU015 culture. The optimum pH of TKU015 PLA depolymerase is 10, and the optimal temperature of the enzyme is 60 °C. In addition to PLA, TKU015 PLA depolymerase degraded fibrinogen and tributyrin, but did not hydrolyze casein, triolein, and poly(?-hydroxybutyrate). Taken together, these data demonstrate that P. tamsuii TKU015 produces a PLA depolymerase to utilize SPP and polylactide as carbon/nitrogen sources. Full article
(This article belongs to the Special Issue Biodegradable Polymers)
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Graphical abstract
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<p>Effects of MPS concentration (<b>a</b>) and culture temperature (<b>b</b>) on cell growth (dashed line) and PLA depolymerase activity (solid line) of <span class="html-italic">P. tamsuii</span> TKU015. All data points are means ± S.D. (standard deviation) of three different experiments performed on different days (each experiment was conducted in triplicate).</p>
Full article ">Figure 2
<p>Elution profile of TKU015 PLA depolymerase from DEAE-Sepharose CL-6B.</p>
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<p>Sodium dodecyl sulphate polyacrylamide gel electrophoresis (SDS–PAGE) analysis of PLA depolymerase produced by <span class="html-italic">P. tamsuii</span> TKU015. Lanes: M, molecular markers (170, 130, 95, 72, 55, 43, 34, and 26 kDa); (1) crude enzyme; (2) adsorbed PLA depolymerase fractions after DEAE-Sepharose CL-6B chromatography; (3) adsorbed PLA depolymerase fractions after Macro-prep DEAE chromatography; (4) PLA depolymerase fractions after Sephacryl S-100.</p>
Full article ">Figure 4
<p>Effects of pH and temperature on the activity and stability of the PLA depolymerase from <span class="html-italic">P. tamsuii</span> TKU015. (<b>a</b>) Optimum pH; (<b>b</b>) pH stability; (<b>c</b>) optimum temperature; (<b>d</b>) thermal stability. All data points are means ± S.D. of three different experiments performed on different days (each experiment was conducted in triplicate). Means with different letters are significantly different at <span class="html-italic">p</span> &lt; 0.05.</p>
Full article ">Figure 4 Cont.
<p>Effects of pH and temperature on the activity and stability of the PLA depolymerase from <span class="html-italic">P. tamsuii</span> TKU015. (<b>a</b>) Optimum pH; (<b>b</b>) pH stability; (<b>c</b>) optimum temperature; (<b>d</b>) thermal stability. All data points are means ± S.D. of three different experiments performed on different days (each experiment was conducted in triplicate). Means with different letters are significantly different at <span class="html-italic">p</span> &lt; 0.05.</p>
Full article ">
5235 KiB  
Article
Influence of Electrospinning Parameters on Fiber Diameter and Mechanical Properties of Poly(3-Hydroxybutyrate) (PHB) and Polyanilines (PANI) Blends
by Ahmed M. El-hadi and Fatma Y. Al-Jabri
Polymers 2016, 8(3), 97; https://doi.org/10.3390/polym8030097 - 22 Mar 2016
Cited by 43 | Viewed by 8071
Abstract
Random and oriented fibers of poly (3-hydroxybutyrate) (PHB) and their blends were manufactured using electrospinning using a co-solvent. The kind and the concentration of the co-solvent affected the diameter of electrospun fibers. The morphology, thermal analysis, and crystalline structure of electrospun fibers was [...] Read more.
Random and oriented fibers of poly (3-hydroxybutyrate) (PHB) and their blends were manufactured using electrospinning using a co-solvent. The kind and the concentration of the co-solvent affected the diameter of electrospun fibers. The morphology, thermal analysis, and crystalline structure of electrospun fibers was studied using polarized optical microscop (POM), Differential scanning colametry (DSC), Scanning Electron Microscopy (SEM), Wide angle X-ray diffraction (WAXD), and FT-IR analysis. The diameter of the electrospun fibers decreases with increasing collector speed for the blends compared to pure PHB, which are about 6 µm in diameter. The fibers obtained from blends reduce to 2 µm. The aligned electrospun fiber mats obtained from pure PHB showed no signs of necking at different take-up speeds, but the blends show multiple necking. It was found by FT-IR that the peak intensity at 1379 cm?1 was lower by take up speed than in casting films; this peak is sensitive to crystallinity of PHB. The addition of polyanilines (PANIs) to (PHB) with a plasticizer decreases the diameter of the electrospun fiber. Full article
(This article belongs to the Special Issue Biodegradable Polymers)
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Graphical abstract
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<p>The samples of pure PHB and blend 1 were collected on the aluminum foil with the following die diameter, applied voltages, CF/DCM ratios, flow rate, and the distance between needle and target: 20 wt %, 1.3 mm, 20 kV, 75:25, 0.185 µm·h<sup>−1</sup>, and 20 cm, respectively; (<b>a</b>,<b>a'</b>) pure PHB at a fixed target (random) and rotating drum with a speed of 1100 rpm with polymer concentrations of 20%; (<b>b</b>,<b>b'</b>) blend 1 at a fixed target (random) and at a rotating drum with a speed 1100 rpm with polymer concentrations of 25%.</p>
Full article ">Figure 2
<p>The samples of pure PHB at different scales were collected on the aluminum foil with the following polymer concentrations, die diameter, applied voltages, CF/DMF ratios, flow rate, and distance between the needle and target: 20 wt %, 1.3 mm, 20 kV, 90:10, 0.185 µm·h<sup>−1</sup>, and 20 cm, respectively. (<b>a</b>,<b>c</b>) at a fixed target (random) with different scales, and (<b>b</b>,<b>d</b>) at a rotating drum with a speed of 1100 rpm.</p>
Full article ">Figure 3
<p>The samples of blend 1 at different scales and speeds were collected on the aluminum foil with the following polymer concentrations, die diameter, applied voltages, CF/DMF ratios, flow rate, and distance between the needle and target: 25 wt %, 1.3 mm, 20 kV, 90:10, 0.185 µm·h<sup>−1</sup> and 20 cm, (<b>a</b>,<b>c</b>) at fixed target (random); (<b>b</b>,<b>d</b>) at a rotating drum with a speed of 1100 rpm, respectively.</p>
Full article ">Figure 4
<p>The samples of blend 2 were collected on the aluminum foil with the following polymer concentrations, die diameter, applied voltages, CF/DMF ratios, flow rate, and distance between the needle and target: 25 wt %, 1.3 mm, 20 kV, 90:10, 0.185 µm·h<sup>−1</sup>, and 20 cm. (<b>a</b>) at a fixed target (random); (<b>b</b>) at a rotating drum with a speed of 380 rpm; (<b>c</b>) at a rotating drum with a speed of 490 rpm; (<b>d</b>) at a rotating drum with a speed of 610 rpm; (<b>e</b>) at a rotating drum with a speed of 740 rpm, and (<b>f</b>) at a rotating drum with speed 850 rpm.</p>
Full article ">Figure 5
<p>Stress-strain curves of nanofibers: (<b>a</b>) pure PHB with a speed of 610 rpm; (<b>b</b>) blend 2 with a speed of 610 rpm; (<b>c</b>) blend 2 (random); and (<b>d</b>) blend 1 (random).</p>
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<p>SEM micrographs of fractured surfaces of multiple neck formations in electrospun fibers of blend 2 (<b>a</b>, <b>b</b>, and <b>c</b>) and blend 1 (<b>d</b>) after cold drawing, at different magnifications.</p>
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<p>DSC curves for pure PHB and its blends (<b>a</b>) first heating; (<b>b</b>) cooling; (<b>c</b>) second heating; and (<b>d</b>) second heating to determine the glass transition temperature region.</p>
Full article ">Figure 8
<p>WAXD of electrospun fibers of (<b>a</b>) pure PHB with different take-up speeds (v), (<b>b</b>) blend 1 with different take-up speeds, and (<b>c</b>) pure PHB, blends 1, 2, and blend 2 with different take-up speed (v).</p>
Full article ">Figure 9
<p>FT-IR spectrum of electrospun PHB and their blends in the infrared spectrum regions at different take-up speeds (<b>a</b>) from 400 to 1600 cm<sup>−1</sup> of PHB and (<b>a'</b>) from 1600 to 4000 cm<sup>−1</sup> of PHB; (<b>b</b>) from 400 to 1600 cm<sup>−1</sup> of blend 10; and (<b>b'</b>) from 1600 to 4000 cm<sup>−1</sup> of blend 10; (<b>c</b>) from 400 to 1600 cm<sup>−1</sup> of blends 10, 14, 16, 17, and (<b>c'</b>) from 1600 to 4000 cm<sup>−1</sup> of pure PHB and blends 1 and 2, at constant take-up speeds of 490 rpm, but blends 3 and 4 as a casting film.</p>
Full article ">
4895 KiB  
Article
Water-Dispersible Silica-Polyelectrolyte Nanocomposites Prepared via Acid-Triggered Polycondensation of Silicic Acid and Directed by Polycations
by Philip Overton, Elena Danilovtseva, Erno Karjalainen, Mikko Karesoja, Vadim Annenkov, Heikki Tenhu and Vladimir Aseyev
Polymers 2016, 8(3), 96; https://doi.org/10.3390/polym8030096 - 22 Mar 2016
Cited by 7 | Viewed by 11918
Abstract
The present work describes the acid-triggered condensation of silicic acid, Si(OH)4, as directed by selected polycations in aqueous solution in the pH range of 6.5–8.0 at room temperature, without the use of additional solvents or surfactants. This process results in the [...] Read more.
The present work describes the acid-triggered condensation of silicic acid, Si(OH)4, as directed by selected polycations in aqueous solution in the pH range of 6.5–8.0 at room temperature, without the use of additional solvents or surfactants. This process results in the formation of silica-polyelectrolyte (S-PE) nanocomposites in the form of precipitate or water-dispersible particles. The mean hydrodynamic diameter (dh) of size distributions of the prepared water-dispersible S-PE composites is presented as a function of the solution pH at which the composite formation was achieved. Poly(2-(dimethylamino)ethyl methacrylate) (PDMAEMA) and block copolymers of DMAEMA and oligo(ethylene glycol) methyl ether methacrylate (OEGMA) were used as weak polyelectrolytes in S-PE composite formation. The activity of the strong polyelectrolytes poly(methacryloxyethyl trimethylammonium iodide) (PMOTAI) and PMOTAI-b-POEGMA in S-PE formation is also examined. The effect of polyelectrolyte strength and the OEGMA block on the formation of the S-PE composites is assessed with respect to the S-PE composites prepared using the PDMAEMA homopolymer. In the presence of the PDMAEMA60 homopolymer (Mw = 9400 g/mol), the size of the dispersible S-PE composites increases with solution pH in the range pH 6.6–8.1, from dh = 30 nm to dh = 800 nm. S-PDMAEMA60 prepared at pH 7.8 contained 66% silica by mass (TGA). The increase in dispersible S-PE particle size is diminished when directed by PDMAEMA300 (Mw = 47,000 g/mol), reaching a maximum of dh = 75 nm. S-PE composites formed using PDMAEMA-b-POEGMA remain in the range dh = 20–30 nm across this same pH regime. Precipitated S-PE composites were obtained as spheres of up to 200 nm in diameter (SEM) and up to 65% mass content of silica (TGA). The conditions of pH for the preparation of dispersible and precipitate S-PE nanocomposites, as directed by the five selected polyelectrolytes PDMAEMA60, PDMAEMA300, PMOTAI60, PDMAEMA60-b-POEGMA38 and PMOTAI60-b-POEGMA38 is summarized. Full article
(This article belongs to the Special Issue Polymers for Aqueous Media)
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Graphical abstract
Full article ">Figure 1
<p>Quaternization of the DMAEMA repeating units of the homopolymer or PDMAEMA<sub>n</sub>-<span class="html-italic">b</span>-POEGMA<sub>m</sub> block copolymers <span class="html-italic">via</span> reaction with excess iodomethane in acetone.</p>
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<p>Representative DLS data of S-PDMAEMA<sub>60</sub> particles prepared at pH 8.0 (blue diamonds <math display="inline"> <semantics> <mrow> <mo mathcolor="#5B9BD5">♦</mo> </mrow> </semantics> </math>), pH 7.4 (green triangles <math display="inline"> <semantics> <mrow> <mo mathcolor="#92D050">▲</mo> </mrow> </semantics> </math>) and pH 6.9 (red squares <math display="inline"> <semantics> <mrow> <mo mathcolor="#C00000">■</mo> </mrow> </semantics> </math>) using a 1:1 feed ratio of SS/PDMAEMA, corresponding to a 10 mM concentration of DMAEMA repeating units, a 1.57 g/L polymer concentration: (<b>a</b>) The total intensity of scattered light and (<b>b</b>) Mean hydrodynamic diameter of corresponding size distributions (<span class="html-italic">d</span><sub>h</sub>) are shown, as observed over 12 h following acid-triggered initiation of particle growth. Data obtained at a 173° scattering angle using the Zetasizer instrument.</p>
Full article ">Figure 3
<p>Comparison of stable aqueous colloid dispersions of S-PDMAEMA<sub>60</sub> particles prepared using 10 mM SS/PDMAEMA (1:1) feed ratio. The initial polymer mass concentration is 1.57 g/L. Particle size shows dependence on the pH at the time of the initiation of particle growth. Particle size by mean hydrodynamic diameter is shown for S-PDMAEMA<sub>60</sub> particles prepared at pH 5.9 (red squares <math display="inline"> <semantics> <mrow> <mo mathcolor="#C00000">■</mo> </mrow> </semantics> </math>), pH 6.8 (green open squares <math display="inline"> <semantics> <mrow> <mo mathcolor="#92D050">□</mo> </mrow> </semantics> </math>), pH 6.9 (green triangles <math display="inline"> <semantics> <mrow> <mo mathcolor="#92D050">▲</mo> </mrow> </semantics> </math>), pH 7.3 (purple circles <math display="inline"> <semantics> <mrow> <mo mathcolor="#7030A0">●</mo> </mrow> </semantics> </math>) and pH 8.0 (blue diamonds <math display="inline"> <semantics> <mrow> <mo mathcolor="#4F81BD">♦</mo> </mrow> </semantics> </math>).</p>
Full article ">Figure 4
<p>Time-dependent change in the mean hydrodynamic diameter (<span class="html-italic">d</span><sub>h</sub>, nm) of S-PDMAEMA<sub>60</sub> particles prepared at pH 6.8 using feed ratio of 1:1 SS/PDMAEMA (10 mM SS, filled blue circles <math display="inline"> <semantics> <mrow> <mo mathcolor="#0033CC">●</mo> </mrow> </semantics> </math>) and of 2:1 SS/PDMAEMA (20 mM SS, filled blue squares <math display="inline"> <semantics> <mrow> <mo mathcolor="#0033CC">■</mo> </mrow> </semantics> </math>) presented as a function of time (h). Here the concentration of DMAEMA repeating units is 10 mM and the polymer concentration is 1.57 g/L. Light scattering intensity (I, kcps) is shown as open red symbols of corresponding shape (<math display="inline"> <semantics> <mrow> <mo mathcolor="#C00000">○</mo> </mrow> </semantics> </math> and <math display="inline"> <semantics> <mrow> <mo mathcolor="#C00000">□</mo> </mrow> </semantics> </math>). Data obtained at a 173° scattering angle using the Zetasizer instrument.</p>
Full article ">Figure 5
<p>Colloidal dispersions of (1:1) S-PMOTAI particles prepared at pH 6.0 (red circles <math display="inline"> <semantics> <mrow> <mo mathcolor="red">○</mo> </mrow> </semantics> </math>), pH 6.7 (dark red squares <math display="inline"> <semantics> <mrow> <mo mathcolor="#C00000">■</mo> </mrow> </semantics> </math>), pH 7.8 (green triangles <math display="inline"> <semantics> <mrow> <mo mathcolor="#92D050">▲</mo> </mrow> </semantics> </math>), pH 7.9 (purple circles <math display="inline"> <semantics> <mrow> <mo mathcolor="#7030A0">●</mo> </mrow> </semantics> </math>) and pH 8.6 (blue diamonds <math display="inline"> <semantics> <mrow> <mo mathcolor="#4F81BD">♦</mo> </mrow> </semantics> </math>). A constant 10 mM concentration of MOTAI repeating units is used (2.99 g/L). The mean hydrodynamic diameter (<span class="html-italic">d</span><sub>h</sub>, nm) is shown as a function of time (h). Lines are drawn only as a guide for the eye.</p>
Full article ">Figure 6
<p>The mean hydrodynamic diameter (<span class="html-italic">d</span><sub>h</sub>, nm) of stable S-PE particles 72 h after particle growth initiation by addition of the appropriate volume of (0.1 M) HCL (see Experimental <a href="#sec2dot2dot3-polymers-08-00096" class="html-sec">Section 2.2.3</a>). Each data point is obtained using exponential fit of individual DLS data sets (<span class="html-italic">i.e.</span>, <span class="html-italic">d</span><sub>h</sub> <span class="html-italic">vs.</span> time curves) gathered at the corresponding pH: S-PDMAEMA<sub>60</sub> (blue diamonds <math display="inline"> <semantics> <mrow> <mo mathcolor="#5B9BD5">♦</mo> </mrow> </semantics> </math>), S-PMOTAI (red squares <math display="inline"> <semantics> <mrow> <mo mathcolor="#C00000">■</mo> </mrow> </semantics> </math>), S-PDMAEMA<sub>60</sub>-<span class="html-italic">b</span>-POEGMA<sub>38</sub> (green triangles <math display="inline"> <semantics> <mrow> <mo mathcolor="#538135">▲</mo> </mrow> </semantics> </math>), S-PMOTAI<sub>60</sub>-<span class="html-italic">b</span>-POEGMA<sub>38</sub> (purple circles <math display="inline"> <semantics> <mrow> <mo mathcolor="#7030A0">●</mo> </mrow> </semantics> </math>) and PDMAEMA<sub>300</sub> (orange circles <math display="inline"> <semantics> <mrow> <mo mathcolor="#F79646">○</mo> </mrow> </semantics> </math>). All S-PE composites were prepared using a 1:1 (10 mM) SS/DMAEMA or SS/MOTAI ratio with respect to the concentration of amine-functional repeating units.</p>
Full article ">Figure 7
<p>SEM images of S-PDMAEMA<sub>60</sub> precipitates prepared using a 5:1 feed ratio of SS/PDMAEMA at (<b>a</b>) pH 7.8; (<b>b</b>) pH 8.5; (<b>c</b>) pH 8.8 and (<b>d</b>) pH 10.0. Polymer concentration was fixed at 10 mM of repeating units. Frames (<b>a</b>)–(<b>c</b>) are at 60,000× magnification; frame (<b>d</b>) is 70,000× magnification. A 500 nm scale bar is provided within each frame.</p>
Full article ">Figure 8
<p>SEM images of water-stable and precipitated composites (60,000× magnification). (<b>a</b>) S-PDMAEMA water-stable particles prepared at pH 7.8 using a 1:1 feed ratio of SS and PDMAEMA and extracted by ultrafiltration; (<b>b</b>) precipitated S-PDMAEMA particles prepared at the same pH using a 5:1 feed ratio and collected by centrifuge. Both samples were washed with deionized water, isolated by freeze-drying and adhered to electrically conductive carbon tape for SEM imaging.</p>
Full article ">Figure 9
<p>Degree of protonation (α) of PDMAEMA (10 mM of repeating units, 1.57 g/L, black diamonds ♦) and silicate (initially SiO<sub>3</sub><sup>2−</sup> from a 10 mM solution of SS, which undergoes hydrolysis to yield SA, red squares <math display="inline"> <semantics> <mrow> <mo mathcolor="#C00000">■</mo> </mrow> </semantics> </math>) solutions as a function of pH, as determined by titration. The pKa (PDMAEMA) = 6.1 and pKa (SA) = 9.9.</p>
Full article ">Figure 10
<p>Acid-triggered hydrolysis of sodium silicate (Na<sub>2</sub>SiO<sub>3</sub>) and subsequent polycondensation of silicic acid (Si(OH)<sub>4</sub>) is directed by polycation bearing DMAEMA repeating units. The resultant silica-polyelectrolyte (S-PE) nanocomposites either precipitate or form water-stable (dispersible) particles, depending on the initial concentration of the sodium silicate precursor with respect to the (10 mM) concentration of DMAEMA repeating units.</p>
Full article ">
10462 KiB  
Article
Multilayer Graphene/Carbon Black/Chlorine Isobutyl Isoprene Rubber Nanocomposites
by Daniele Frasca, Dietmar Schulze, Volker Wachtendorf, Bernd Krafft, Thomas Rybak and Bernhard Schartel
Polymers 2016, 8(3), 95; https://doi.org/10.3390/polym8030095 - 22 Mar 2016
Cited by 30 | Viewed by 8798
Abstract
High loadings of carbon black (CB) are usually used to achieve the properties demanded of rubber compounds. In recent years, distinct nanoparticles have been investigated to replace CB in whole or in part, in order to reduce the necessary filler content or to [...] Read more.
High loadings of carbon black (CB) are usually used to achieve the properties demanded of rubber compounds. In recent years, distinct nanoparticles have been investigated to replace CB in whole or in part, in order to reduce the necessary filler content or to improve performance. Multilayer graphene (MLG) is a nanoparticle made of just 10 graphene sheets and has recently become commercially available for mass-product nanocomposites. Three phr (part for hundred rubbers) of MLG are added to chlorine isobutyl isoprene rubber (CIIR)/CB composites in order to replace part of the CB. The incorporation of just 3 phr MLG triples the Young’s modulus of CIIR; the same effect is obtained with 20 phr CB. The simultaneous presence of three MLG and CB also delivers remarkable properties, e.g. adding three MLG and 20 phr CB increased the hardness as much as adding 40 phr CB. A comprehensive study is presented, showing the influence on a variety of mechanical properties. The potential of the MLG/CB combination is illustrated to reduce the filler content or to boost performance, respectively. Apart from the remarkable mechanical properties, the CIIR/CB/MLG nanocomposites showed an increase in weathering resistance. Full article
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Graphical abstract
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<p>SEM micrographs of (<b>a</b>–<b>c</b>) MLG and (<b>d</b>–<b>f</b>) CB.</p>
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<p>UV-Vis absorption of water dispersions of CB, MLG and their mixture.</p>
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<p>Change in pressure during the cumene oxidation with and without MLG or CB.</p>
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<p>(<b>a</b>) Dynamic viscosity as a function of the frequency of CIIR and its composites; and (<b>b</b>) dynamic viscosity at 0.25 Hz as a function of the filler content; the line is a visual guide.</p>
Full article ">Figure 5
<p>(<b>a</b>) Storage modulus as a function of the strain amplitude of CIIR and its composites; and (<b>b</b>) difference between initial and final storage modulus as a function of the filler content; the line is a visual guide.</p>
Full article ">Figure 6
<p>(<b>a</b>) Curing curves of CIIR (chlorine isobutyl isoprene rubber) and its composites; (<b>b</b>) maximum of the torque; (<b>c</b>) minimum of the torque; and (<b>d</b>) difference between maximum and minimum of the torque as a function of the filler content; the lines are visual guides.</p>
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<p>(<b>a</b>)–(<b>g</b>) SEM micrographs of CIIR and its composites.</p>
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<p>(<b>a</b>) and (<b>b</b>) TEM micrographs of CIIR/MLG3.</p>
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<p>(<b>a</b>) Tensile stress <span class="html-italic">vs.</span> strain curves and of CIIR and its composites; (<b>b</b>) tensile strength; (<b>c</b>) elongation at break; (<b>d</b>) stress at 100% of elongation; (<b>e</b>) stress at 200% of elongation; and (<b>f</b>) stress at 300% of elongation as functions of the filler content. The lines are visual guides.</p>
Full article ">Figure 10
<p>(<b>a</b>) Stress <span class="html-italic">vs.</span> strain curves to determine Young’s modulus of CIIR and its composites; and (<b>b</b>) Young’s modulus as a function of the filler content. The line is a visual guide.</p>
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<p>Hardness of CIIR and its composites as a function of the filler content; the line is a visual guide.</p>
Full article ">Figure 12
<p>(<b>a</b>) Storage modulus of CIIR and its composites as a function of the temperature; (<b>b</b>) storage modulus at 25 °C as a function of the filler content—the line is a visual guide; (<b>c</b>) tan δ of CIIR and its composites as a function of temperature; and (<b>d</b>) maximum of tan η as a function of the filler content—the line is a visual guide.</p>
Full article ">Figure 13
<p>Tensile strength of CIIR and its composites as a function of the weathering/exposure duration time. The lines are visual guides.</p>
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3893 KiB  
Article
Mussel-Inspired Anisotropic Nanocellulose and Silver Nanoparticle Composite with Improved Mechanical Properties, Electrical Conductivity and Antibacterial Activity
by Hoang-Linh Nguyen, Yun Kee Jo, Minkyu Cha, Yun Jeong Cha, Dong Ki Yoon, Naresh D. Sanandiya, Ekavianty Prajatelistia, Dongyeop X. Oh and Dong Soo Hwang
Polymers 2016, 8(3), 102; https://doi.org/10.3390/polym8030102 - 22 Mar 2016
Cited by 61 | Viewed by 14394
Abstract
Materials for wearable devices, tissue engineering and bio-sensing applications require both antibacterial activity to prevent bacterial infection and biofilm formation, and electrical conductivity to electric signals inside and outside of the human body. Recently, cellulose nanofibers have been utilized for various applications but [...] Read more.
Materials for wearable devices, tissue engineering and bio-sensing applications require both antibacterial activity to prevent bacterial infection and biofilm formation, and electrical conductivity to electric signals inside and outside of the human body. Recently, cellulose nanofibers have been utilized for various applications but cellulose itself has neither antibacterial activity nor conductivity. Here, an antibacterial and electrically conductive composite was formed by generating catechol mediated silver nanoparticles (AgNPs) on the surface of cellulose nanofibers. The chemically immobilized catechol moiety on the nanofibrous cellulose network reduced Ag+ to form AgNPs on the cellulose nanofiber. The AgNPs cellulose composite showed excellent antibacterial efficacy against both Gram-positive and Gram-negative bacteria. In addition, the catechol conjugation and the addition of AgNP induced anisotropic self-alignment of the cellulose nanofibers which enhances electrical and mechanical properties of the composite. Therefore, the composite containing AgNPs and anisotropic aligned the cellulose nanofiber may be useful for biomedical applications. Full article
(This article belongs to the Special Issue Renewable Polymeric Adhesives)
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Graphical abstract
Full article ">Figure 1
<p>Schematic figures of (<b>A</b>) the anisotropic carboxylated cellulose nanofibers (CCNF)-dopamine (DA)/silver nanoparticles (AgNPs) composite formation process; and (<b>B</b>) the antibacterial activity of CCNF-DA/AgNPs composite.</p>
Full article ">Figure 1 Cont.
<p>Schematic figures of (<b>A</b>) the anisotropic carboxylated cellulose nanofibers (CCNF)-dopamine (DA)/silver nanoparticles (AgNPs) composite formation process; and (<b>B</b>) the antibacterial activity of CCNF-DA/AgNPs composite.</p>
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<p>Morphological change of carboxylated cellulose nanofibers (CCNF) by conjugating catechol and silver nanoparticles. (<b>A</b>) TEM images of CCNF and (<b>B</b>) CCNF-DA/AgNPs; (<b>C</b>) polarized optical microscopy (POM) image of CCNF-DA with retardation (λ) plate; magenta and blue (or yellow) show disordered and anisotropic domains, respectively. The insect in (<b>C</b>) indicates the polarization directions of the polarizer (P) and analyzer (A); (<b>D</b>) SEM image of CCNF-DA.</p>
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<p>(<b>A</b>) UV–Vis spectroscopy of supernatant from CCNF, CCNF-DA and CCNF films. The insect in (<b>A</b>) shows the supernatant from the CCNF-DA/AgNPs film; (<b>B</b>) high-resolution transmission electron microscopy (HRTEM) image of extracted AgNPs. The inset black box in (<b>B</b>) indicates the area where the enlarged HRTEM image (bottom-right panel) was taken; (<b>C</b>) selected area electron diffraction (SAED) pattern of silver crystal of CCNF-DA/AgNP.</p>
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<p>(<b>A</b>) Stress-strain curve; (<b>B</b>) tensile strength; (<b>C</b>) toughness; and (<b>D</b>) Young’s modulus of CCNF, CCNF-DA, and CCNF-DA/AgNPs films. The data of quadruplicate samples represent mean ± standard deviation with statistical significance (<b>*</b> <span class="html-italic">p</span> &lt; 0.05, <b>**</b> <span class="html-italic">p</span> &lt; 0.01, <b>***</b> <span class="html-italic">p</span> &lt; 0.005; unpaired <span class="html-italic">t</span>-test).</p>
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<p>Antibacterial test on CCNF-DA/AgNPs membrane. (<b>A</b>) Disk diffusion test; (<b>B</b>) bacterial growth profiles; and (<b>C</b>) bactericidal profiles of the CCNF-DA/AgNPs membrane against <span class="html-italic">E. coli</span>; (<b>D</b>) Growth-inhibiting (<b>left</b>) and bactericidal (<b>right</b>) efficacies of CCNF-DA/AgNPs membrane for a long period. White arrows indicate the inhibition zone. The data represent mean ± standard deviation with statistical significance (<b>*</b> <span class="html-italic">p</span> &lt; 0.05, ** <span class="html-italic">p</span> &lt; 0.01, <b>***</b> <span class="html-italic">p</span> &lt; 0.005; unpaired <span class="html-italic">t</span>-test).</p>
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4541 KiB  
Article
Amphiphilic Fluorinated Block Copolymer Synthesized by RAFT Polymerization for Graphene Dispersions
by Hyang Moo Lee, Suguna Perumal and In Woo Cheong
Polymers 2016, 8(3), 101; https://doi.org/10.3390/polym8030101 - 22 Mar 2016
Cited by 16 | Viewed by 8680
Abstract
Despite the superior properties of graphene, the strong ?–? interactions among pristine graphenes yielding massive aggregation impede industrial applications. For non-covalent functionalization of highly-ordered pyrolytic graphite (HOPG), poly(2,2,2-trifluoroethyl methacrylate)-block-poly(4-vinyl pyridine) (PTFEMA-b-PVP) block copolymers were prepared by reversible addition-fragmentation chain [...] Read more.
Despite the superior properties of graphene, the strong ?–? interactions among pristine graphenes yielding massive aggregation impede industrial applications. For non-covalent functionalization of highly-ordered pyrolytic graphite (HOPG), poly(2,2,2-trifluoroethyl methacrylate)-block-poly(4-vinyl pyridine) (PTFEMA-b-PVP) block copolymers were prepared by reversible addition-fragmentation chain transfer (RAFT) polymerization and used as polymeric dispersants in liquid phase exfoliation assisted by ultrasonication. The HOPG graphene concentrations were found to be 0.260–0.385 mg/mL in methanolic graphene dispersions stabilized with 10 wt % (relative to HOPG) PTFEMA-b-PVP block copolymers after one week. Raman and atomic force microscopy (AFM) analyses revealed that HOPG could not be completely exfoliated during the sonication. However, on-line turbidity results confirmed that the dispersion stability of HOPG in the presence of the block copolymer lasted for one week and that longer PTFEMA and PVP blocks led to better graphene dispersibility. Force–distance (F–d) analyses of AFM showed that PVP block is a good graphene-philic block while PTFEMA is methanol-philic. Full article
(This article belongs to the Special Issue Selected Papers from ASEPFPM2015)
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<p>Schematic drawing of the mechanism for syntheses of (<b>a</b>) PTFEMA macro-RAFT agent (PTFEMA<sub>n</sub>-CTP) and (<b>b</b>) PTFEMA<sub>n</sub>-<span class="html-italic">b</span>-PVP<sub>m</sub> block copolymer. CTP: 4-Cyano-4-(phenylcarbonothioylthio)pentanoic acid; TFEMA: 2,2,2-Trifluoroethyl methacrylate; AIBN: 2,2′-Azobisisobutyronitrile; VP: 4-Vinyl pyridine; PTFEMA-b-PVP: Poly(2,2,2-trifluoroethyl methacrylate)-<span class="html-italic">block</span>-poly(4-vinyl pyridine). RAFT: Reversible addition-fragmentation chain transfer.</p>
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<p>SEC elution curves for two different macro-RAFT agents: PTFEMA<sub>66</sub>-CTP (blue) and PTFEMA<sub>136</sub>-CTP (red).</p>
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<p>Representative <sup>1</sup>H-NMR spectra for (<b>a</b>) PTFEMA<sub>66</sub>-CTP and (<b>b</b>) PTFEMA<sub>66</sub>-<span class="html-italic">b</span>-PVP<sub>41</sub> block copolymer.</p>
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<p>Representative FT-IR spectra for (<b>a</b>) PTFEMA<sub>66</sub>-CTP homopolymer and (<b>b</b>) PTFEMA<sub>66</sub>-<span class="html-italic">b</span>-PVP<sub>41</sub> block copolymer.</p>
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<p>Time-evolution turbiscan stability index (TSI) curves for pristine HOPG (<b>raw</b>) and pristine HOPG with PTFEMA<sub>66</sub>-<span class="html-italic">b</span>-PVP<sub>41</sub> (<b>1</b>), PTFEMA<sub>66</sub>-<span class="html-italic">b</span>-PVP<sub>205</sub> (<b>2</b>), PTFEMA<sub>136</sub>-<span class="html-italic">b</span>-PVP<sub>31</sub> (<b>3</b>), and PTFEMA<sub>136</sub>-<span class="html-italic">b</span>-PVP<sub>194</sub> (<b>4</b>). The TSI values are calculated for the middle parts of the sample vials shown in <a href="#polymers-08-00101-f006" class="html-fig">Figure 6</a>. The inset shows magnified TSI curves for samples <b>1</b>–<b>4</b>.</p>
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<p>Photographic images for HOPG dispersions <span class="html-italic">versus</span> time obtained for pristine HOPG (M-25, <b>raw</b>), HOPG with PTFEMA<sub>66</sub>-<span class="html-italic">b</span>-PVP<sub>41</sub> (<b>1</b>), PTFEMA<sub>66</sub>-<span class="html-italic">b</span>-PVP<sub>205</sub> (<b>2</b>), PTFEMA<sub>136</sub>-<span class="html-italic">b</span>-PVP<sub>31</sub> (<b>3</b>), and PTFEMA<sub>136</sub>-<span class="html-italic">b</span>-PVP<sub>194</sub> (<b>4</b>).</p>
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<p>Raman spectra for supernatant solution of HOPG dispersions obtained from pristine HOPG (M-25, <b>raw</b>), HOPG with PTFEMA<sub>66</sub>-<span class="html-italic">b</span>-PVP<sub>41</sub> (<b>1</b>), PTFEMA<sub>66</sub>-<span class="html-italic">b</span>-PVP<sub>205</sub> (<b>2</b>), PTFEMA<sub>136</sub>-<span class="html-italic">b</span>-PVP<sub>31</sub> (<b>3</b>), and PTFEMA<sub>136</sub>-<span class="html-italic">b</span>-PVP<sub>194</sub> (<b>4</b>).</p>
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<p>Atomic Force Microscopy (AFM) topographic images of the supernatant solution from HOPG dispersions with (<b>a</b>) PTFEMA<sub>66</sub>-<span class="html-italic">b</span>-PVP<sub>41</sub>, (<b>b</b>) PTFEMA<sub>66</sub>-<span class="html-italic">b</span>-PVP<sub>205</sub>, (<b>c</b>) PTFEMA<sub>136</sub>-<span class="html-italic">b</span>-PVP<sub>31</sub>, and (<b>d</b>) PTFEMA<sub>136</sub>-<span class="html-italic">b</span>-PVP<sub>194</sub>. Height profiles from the red line on topographic images are depicted below their corresponding images (<b>a</b>–<b>d</b>), and the Δh in height profile reveals the height diffrences between red triangles.</p>
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4563 KiB  
Article
Rheological and Mechanical Behavior of Silk Fibroin Reinforced Waterborne Polyurethane
by Yongzhen Tao, Anwarul Hasan, George Deeb, Changkai Hu and Huipeng Han
Polymers 2016, 8(3), 94; https://doi.org/10.3390/polym8030094 - 21 Mar 2016
Cited by 23 | Viewed by 8008
Abstract
Waterborne polyurethane (WPU) is a versatile and environment-friendly material with growing applications in both industry and academia. Silk fibroin (SF) is an attractive material known for its structural, biological and hemocompatible properties. The SF reinforced waterborne polyurethane (WPU) is a promising scaffold material [...] Read more.
Waterborne polyurethane (WPU) is a versatile and environment-friendly material with growing applications in both industry and academia. Silk fibroin (SF) is an attractive material known for its structural, biological and hemocompatible properties. The SF reinforced waterborne polyurethane (WPU) is a promising scaffold material for tissue engineering applications. In this work, we report synthesis and characterization of a novel nanocomposite using SF reinforced WPU. The rheological behaviors of WPU and WPU-SF dispersions with different solid contents were investigated with steady shear and dynamic oscillatory tests to evaluate the formation of the cross-linked gel structure. The average particle size and the zeta potential of WPU-SF dispersions with different SF content were examined at 25 °C to investigate the interaction between SF and WPU. FTIR, SEM, TEM and tensile testing were performed to study the effects of SF content on the structural morphology and mechanical properties of the resultant composite films. Experimental results revealed formation of gel network in the WPU dispersions at solid contents more than 17 wt %. The conjugate reaction between the WPU and SF as well as the hydrogen bond between them helped in dispersing the SF powder into the WPU matrix as small aggregates. Addition of SF to the WPU also improved the Young’s modulus from 0.30 to 3.91 MPa, tensile strength from 0.56 to 8.94 MPa, and elongation at break from 1067% to 2480%, as SF was increased up to 5 wt %. Thus, significant strengthening and toughening can be achieved by introducing SF powder into the WPU formulations. Full article
(This article belongs to the Special Issue Polymers Applied in Tissue Engineering)
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<p>Schematic representation of the preparation of: (<b>a</b>) WPU Prepolymer and (<b>b</b>) the WPU-SF dispersions in Water/Acetone.</p>
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<p>Schematic representation of the preparation of: (<b>a</b>) WPU Prepolymer and (<b>b</b>) the WPU-SF dispersions in Water/Acetone.</p>
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<p>Steady-shear flow behavior of WPU dispersions: dependence of the shear stress σ on the shear rate γ (<b>a</b>,<b>b</b>); flow behavior index, <span class="html-italic">n</span>, as a function of log <span class="html-italic">k</span> (<b>c</b>); and dependence of the steady shear viscosity on the shear rate for WPU dispersions with different solid contents (<b>d</b>); for WPU-SF3 dispersions (<b>e</b>); and for WPU17-SF (<b>f</b>) at <span class="html-italic">T</span> = 25 °C, respectively.</p>
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<p>Dynamic rheological behavior of WPU and WPU-SF dispersions under oscillatory shear: (<b>a</b>,<b>b</b>) <span class="html-italic">G′</span> and <span class="html-italic">G</span>′′, and η* as a function of <span class="html-italic">ω</span> for WPU dispersions with different solid contents at <span class="html-italic">T</span> = 25 °C; (<b>c</b>,<b>d</b>) Temperature and time dependence of <span class="html-italic">G</span>′, <span class="html-italic">G</span>′′, and <span class="html-italic">η</span>* for the WPU17-SF5 dispersion; (<b>e</b>,<b>f</b>) Dynamic shear moduli, <span class="html-italic">G′</span>, and <span class="html-italic">G</span>′′, and loss tangent, tan <span class="html-italic">δ</span> as a function of ω for WPU17-SF dispersions with different silk fibroin contents at <span class="html-italic">T</span> = 37 °C. The x-axis of (<b>a</b>,<b>e</b>) is extended by a factors a = 1~10<sup>9</sup> to obtain a valid comparison.</p>
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<p>FTIR spectra of the WPU17, WPU17-SF and WPU17-SF5a films: (<b>a</b>) FTIR spectra of the WPU17 and WPU17-SF films in the wavenumber range of 1800–1200 cm<sup>−1</sup>; and (<b>b</b>) FTIR spectra of the WPU17, WPU17-SF5a, and WPU17-SF5 films in the wavenumber range of 3750–1400 cm<sup>−1</sup>.</p>
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<p>SEM and TEM images of the cross-sections of WPU and WPU-SF films: (<b>a</b>–<b>f</b>) SEM images of the WPU17, WPU17-SF1, WPU17-SF2, WPU17-SF3, WPU17-SF4, and WPU17-SF5 films in sequence; (<b>g</b>–<b>j</b>) TEM images of the WPU17-SF3 film.</p>
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<p>Uniaxial tensile mechanical properties of WPU17 and WPU17-SF films: (<b>a</b>) stress-strain curves; (<b>b</b>) elastic modulus; (<b>c</b>) tensile strength; and (<b>d</b>) elongation at break. WPU17-SF5a is the blended film with 5 wt % SF, which is prepared by blending SF into WPU17 dispersion, and is plotted for comparison. The bars represent mean ± standard deviation (<span class="html-italic">n</span> = 3; *<span class="html-italic">p</span> &lt; 0.05).</p>
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<p>Schematic Illustration of Phase Separation in the: (<b>a</b>) WPU17 and (<b>b</b>) WPU17-SF films. The black and thin line, the blue and thick line, and the green ellipsoid represent soft segments of polyurethane, hard segments of polyurethane, and silk fibroin, respectively.</p>
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2805 KiB  
Article
Studies on Preparation of Poly(3,4-Dihydroxyphenylalanine)-Polylactide Copolymers and the Effect of the Structure of the Copolymers on Their Properties
by Dongjian Shi, Jiali Shen, Zenghui Zhao, Chang Shi and Mingqing Chen
Polymers 2016, 8(3), 92; https://doi.org/10.3390/polym8030092 - 18 Mar 2016
Cited by 9 | Viewed by 6450
Abstract
Properties of copolymers are generally influenced by the structure of the monomers and polymers. For the purpose of understanding the effect of polymer structure on the properties, two kinds of copolymers, poly(3,4-dihydroxyphenylalanine)-g-polylactide and poly(3,4-dihydroxyphenylalanine)-b-polylactide (PDOPA-g-PLA and PDOPA- [...] Read more.
Properties of copolymers are generally influenced by the structure of the monomers and polymers. For the purpose of understanding the effect of polymer structure on the properties, two kinds of copolymers, poly(3,4-dihydroxyphenylalanine)-g-polylactide and poly(3,4-dihydroxyphenylalanine)-b-polylactide (PDOPA-g-PLA and PDOPA-b-PLA) were designed and prepared by ring-opening polymerization of lactide with pre-prepared PDOPA as the initiator and the amidation of the functional PLA and PDOPA oligomer, respectively. The molecular weight and composition of the copolymers could be adjusted by changing the molar ratio of LA and DOPA and were confirmed by gel permeation chromatography (GPC) and proton nuclear magnetic resonance (1H NMR) spectra. The obtained copolymers with graft and block structures showed high solubility even in common organic solvents. The effects of the graft and block structures on the thermal and degradation properties were also detected. The PDOPA-g-PLA copolymers showed higher thermal stability than the PDOPA-b-PLA copolymers, due to the PDOPA-g-PLA copolymers with regular structure and strong ?-? stacking interactions among the intermolecular and intramolecular chains. In addition, the degradation results showed that the PDOPA-g-PLA copolymers and the copolymers with higher DOPA composition had quicker degradation speeds. Interestingly, both two kinds of copolymers, after degradation, became undissolved in the organic solvents because of the oxidation and crosslinking formation of the catechol groups in the DOPA units during degradation in alkaline solution. Moreover, fluorescent microscopy results showed good biocompatibility of the PDOPA-g-PLA and PDOPA-b-PLA copolymers. The PDOPA and PLA copolymers have the potential applications to the biomedical and industrial fields. Full article
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<p><sup>1</sup>H NMR spectra of DOPA(TBDMS)<sub>2</sub> (<b>a</b>); PDOPA(TBDMS)<sub>2</sub> (<b>b</b>); PDOPA (<b>c</b>); and PDOPA-<span class="html-italic">g</span>-PLA<sub>20</sub> (<b>d</b>).</p>
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<p><sup>1</sup>H NMR spectra of H<sub>2</sub>N–PLA–COOH (<b>a</b>); PDOPA(TBDMS)<sub>2</sub>-<span class="html-italic">b</span>-PLA<sub>20</sub> (<b>b</b>); and PDOPA-<span class="html-italic">b</span>-PLA<sub>20</sub> (<b>c</b>).</p>
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<p>TGA curves of the PDOPA-<span class="html-italic">g</span>-PLA (<b>a</b>), and PDOPA-<span class="html-italic">b</span>-PLA (<b>b</b>) copolymers with various compositions under N<sub>2</sub>.</p>
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<p>Remaining weights of PDOPA-<span class="html-italic">g</span>-PLA (<b>a</b>) and PDOPA-<span class="html-italic">b</span>-PLA (<b>b</b>) with degradation time in buffer solution at pH 10.2.</p>
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<p>SEM and photo images of the PDOPA-<span class="html-italic">g</span>-PLA<sub>20</sub> copolymer films before (<b>a</b>) and after (<b>b</b>) degradation.</p>
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<p>Fluorescence microscopy images of NIH/3T3 cells grown on the PDOPA-<span class="html-italic">g</span>-PLA<sub>5</sub> (<b>a</b>) and PDOPA-<span class="html-italic">b</span>-PLA<sub>5</sub> (<b>b</b>) copolymers.</p>
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<p>Synthesis of the PDOPA-<span class="html-italic">g</span>-PLA copolymer.</p>
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<p>Synthesis of the PDOPA-<span class="html-italic">b</span>-PLA copolymer.</p>
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<p>Representative schemes of the PDOPA-<span class="html-italic">g</span>-PLA (<b>a</b>), and PDOPA-<span class="html-italic">b</span>-PLA (<b>b</b>) copolymers.</p>
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7699 KiB  
Article
Preparation of Uniform-Sized and Dual Stimuli-Responsive Microspheres of Poly(N-Isopropylacrylamide)/Poly(Acrylic acid) with Semi-IPN Structure by One-Step Method
by En-Ping Lai, Yu-Xia Wang, Yi Wei and Guang Li
Polymers 2016, 8(3), 90; https://doi.org/10.3390/polym8030090 - 17 Mar 2016
Cited by 29 | Viewed by 8966
Abstract
A novel strategy was developed to synthesize uniform semi-interpenetrating polymer network (semi-IPN) microspheres by premix membrane emulsification combined with one-step polymerization. Synthesized poly(acrylic acid) (PAAc) polymer chains were added prior to the inner water phase, which contained N-isopropylacrylamide (NIPAM) monomer, N, [...] Read more.
A novel strategy was developed to synthesize uniform semi-interpenetrating polymer network (semi-IPN) microspheres by premix membrane emulsification combined with one-step polymerization. Synthesized poly(acrylic acid) (PAAc) polymer chains were added prior to the inner water phase, which contained N-isopropylacrylamide (NIPAM) monomer, N,N?-methylene bisacrylamide (MBA) cross-linker, and ammonium persulfate (APS) initiator. The mixtures were pressed through a microporous membrane to form a uniform water-in-oil emulsion. By crosslinking the NIPAM in a PAAc-containing solution, microspheres with temperature- and pH-responsive properties were fabricated. The semi-IPN structure and morphology of the microspheres were confirmed by Fourier transform infrared spectroscopy (FTIR), scanning electron microscopy (SEM), and transmission electron microscopy (TEM). The average diameter of the obtained microspheres was approximately 6.5 ?m, with Span values of less than 1. Stimuli-responsive behaviors of the microspheres were studied by the cloud-point method. The results demonstrated that semi-IPN microspheres could respond independently to both pH and temperature changes. After storing in a PBS solution (pH 7.0) at 4 °C for 6 months, the semi-IPN microspheres remained stable without a change in morphology or particle size. This study demonstrated a promising method for controlling the synthesis of semi-IPN structure microspheres with a uniform size and multiple functionalities. Full article
(This article belongs to the Special Issue Selected Papers from ASEPFPM2015)
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<p>Process for the preparation of PNIPAM/PAAc semi-IPN microspheres.</p>
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<p>Size distributions of the semi-IPN3 microspheres prepared under different trans-membrane pressures.</p>
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<p>Size distributions of the semi-IPN3 microspheres prepared under different number of trans-membrane passes.</p>
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<p>FT-IR spectra for the PAAc, PNIPAM, and semi-IPN3 microspheres.</p>
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<p>SEM images of semi-IPN and PNIPAM microspheres.</p>
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<p>Particle size distribution of the semi-IPN and PNIPAM microspheres (10 mM, pH 7.0 PBS, 25 °C).</p>
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<p>TEM images of semi-IPN with different initiator amounts (samples were labeled with uranyl acetate).</p>
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<p>DSC curves of the PAAc, PNIPAM, and semi-IPN3 microspheres.</p>
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<p>Transmittance of the PNIPAM and semi-IPN microsphere suspensions in different temperatures at pH 7.0.</p>
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<p>Transmittance of the PNIPAM and semi-IPN microsphere suspensions in different pH conditions at 25 °C.</p>
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<p>CLSM images of the semi-IPN microspheres at different storage times (4 °C, 10 mM pH 7.0 PBS solution; the samples were labeled with Rh 123).</p>
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<p>Size distribution of the PNIPAM (<b>a</b>) and semi-IPN3 (<b>b</b>) microspheres at different storage times (4 °C, 10 mM pH 7.0 PBS solution).</p>
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41203 KiB  
Review
Decorating Nanoparticle Surface for Targeted Drug Delivery: Opportunities and Challenges
by Zhiqiang Shen, Mu-Ping Nieh and Ying Li
Polymers 2016, 8(3), 83; https://doi.org/10.3390/polym8030083 - 17 Mar 2016
Cited by 87 | Viewed by 16463
Abstract
The size, shape, stiffness (composition) and surface properties of nanoparticles (NPs) have been recognized as key design parameters for NP-mediated drug delivery platforms. Among them, the surface functionalization of NPs is of great significance for targeted drug delivery. For instance, targeting moieties are [...] Read more.
The size, shape, stiffness (composition) and surface properties of nanoparticles (NPs) have been recognized as key design parameters for NP-mediated drug delivery platforms. Among them, the surface functionalization of NPs is of great significance for targeted drug delivery. For instance, targeting moieties are covalently coated on the surface of NPs to improve their selectively and affinity to cancer cells. However, due to a broad range of possible choices of surface decorating molecules, it is difficult to choose the proper one for targeted functions. In this work, we will review several representative experimental and computational studies in selecting the proper surface functional groups. Experimental studies reveal that: (1) the NPs with surface decorated amphiphilic polymers can enter the cell interior through penetrating pathway; (2) the NPs with tunable stiffness and identical surface chemistry can be selectively accepted by the diseased cells according to their stiffness; and (3) the NPs grafted with pH-responsive polymers can be accepted or rejected by the cells due to the local pH environment. In addition, we show that computer simulations could be useful to understand the detailed physical mechanisms behind these phenomena and guide the design of next-generation NP-based drug carriers with high selectivity, affinity, and low toxicity. For example, the detailed free energy analysis and molecular dynamics simulation reveals that amphiphilic polymer-decorated NPs can penetrate into the cell membrane through the “snorkeling” mechanism, by maximizing the interaction energy between the hydrophobic ligands and lipid tails. We anticipate that this work will inspire future studies in the design of environment-responsive NPs for targeted drug delivery. Full article
(This article belongs to the Special Issue Computational Modeling and Simulation in Polymer)
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<p>Design of nanoparticle (NP)-based drug delivery platform, according to the size, shape, stiffness (composition), and surface properties of NPs. The figure is adapted from Reference [<a href="#B11-polymers-08-00083" class="html-bibr">11</a>] with permission.</p>
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<p>Penetration of the amphiphilic polymer decorated NPs and its dependence on NP diameter and surface composition. (<b>A</b>) Schematic description of the interaction between amphiphilic polymer-decorated NPs and the cell membrane; (<b>B</b>) Transmission electron microscopy (TEM) image of the giant multilayer vesicle interacting with 1:1 MUS:OT NPs. The red arrows point out that the Au NPs were inserted into the lipid bilayer. The average diameter of the NPs is 2.2 nm; (<b>C</b>) Filled-in squares represent experimental particles that successfully inserted, while empty squares specify those that did not; (<b>D</b>) HeLa cellular uptake in 37 <math display="inline"> <msup> <mrow/> <mo>∘</mo> </msup> </math>C for all MUS NPs with different diameters, a (<math display="inline"> <mrow> <mn>2</mn> <mo>.</mo> <mn>4</mn> <mo>±</mo> <mn>0</mn> <mo>.</mo> <mn>2</mn> </mrow> </math> nm), b (<math display="inline"> <mrow> <mn>2</mn> <mo>.</mo> <mn>9</mn> <mo>±</mo> <mn>0</mn> <mo>.</mo> <mn>5</mn> </mrow> </math> nm), c (<math display="inline"> <mrow> <mn>3</mn> <mo>.</mo> <mn>4</mn> <mo>±</mo> <mn>0</mn> <mo>.</mo> <mn>8</mn> </mrow> </math> nm), d (<math display="inline"> <mrow> <mn>4</mn> <mo>.</mo> <mn>9</mn> <mo>±</mo> <mn>1</mn> <mo>.</mo> <mn>1</mn> </mrow> </math> nm), e (<math display="inline"> <mrow> <mn>5</mn> <mo>.</mo> <mn>8</mn> <mo>±</mo> <mn>1</mn> <mo>.</mo> <mn>4</mn> </mrow> </math> nm). The cellular uptake was measured by the median fluorescence intensity. The figures are adapted from References [<a href="#B52-polymers-08-00083" class="html-bibr">52</a>,<a href="#B54-polymers-08-00083" class="html-bibr">54</a>] with permission.</p>
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<p>Structure difference in lipid molecule-decorated NPs and its effect on endocytosis. (<b>A</b>) Schematic of the two-stage-microfluidic platform; (<b>B</b>) Cryo-TEM images of monolayer shell lipid-polymer hybrid nanoparticles (MP P-L NPs) and bilayer shell lipid-polymer hybrid NPs (BP P-W-L NPs), the electron density showed that the BPs had a lipid bilayer. While the MPs have only one layer of lipids; (<b>C</b>) Plot of the fluorescence emission spectrum of BPs and MPs. It suggests that the BPs contain more water; (<b>D</b>) Plot of the Young’s moduli for MPs and BPs. MPs had higher Young’s modulus than the BPs with same size of 40 nm in diameter; <b>E</b>: The HeLa cells had a higher uptake of MPs than BPs. Chlorpromazine (CPZ), Ethylisopropyl amiloride (EIPA), and Genistein are used for inhibiting clathrin-mediated endocytosis, macropinocytosis, and caveolae-mediated endocytosis, respectively. The figures are adapted from References [<a href="#B50-polymers-08-00083" class="html-bibr">50</a>,<a href="#B51-polymers-08-00083" class="html-bibr">51</a>] with permission.</p>
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<p>Properties of pH-responsive polymer-decorated NPs and their influence on cellular uptake efficiency. (<b>A</b>) Schematic of ligand exchange reaction between dodecylamine (DDA) NPs and mercaptoundecanoic acid (MUA), <span class="html-italic">N</span>,<span class="html-italic">N</span>,<span class="html-italic">N</span>-trimethyl(11-mercaptoun decyl)ammonium (TMA) ; (<b>B</b>) Images of solution under various pH values, containing 8.0 nm mixed-charged (MC) NPs with <math display="inline"> <mrow> <msub> <mi>α</mi> <mtext>surf</mtext> </msub> <mo>=</mo> <mn>2</mn> <mo>.</mo> <mn>5</mn> </mrow> </math>. The MC NPs would be stable except at pH value 6.6. The scheme in the lower part illustrates the corresponding surface charge of the MC NPs, and it became zero net charge at pH value 6.6; (<b>C</b>) Plot of the changes of the <span class="html-italic">ζ</span> potential on the MC NP’s surface, relating to the solvent pH value and the ligand composition <math display="inline"> <msub> <mi>α</mi> <mtext>surf</mtext> </msub> </math>. The diameter of the NP core was 8 nm; (<b>D</b>) Optical images of Rat 2 cellular uptake, indicated by the arrows. The cellular uptake increases with increasing net surface charge. The figures are adapted from Reference [<a href="#B55-polymers-08-00083" class="html-bibr">55</a>] with permission.</p>
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<p>Free energy and kinetic barrier analysis for penetration of amphiphilic polymer-decorated NPs. (<b>A</b>) (<b>Upper</b> part) Schematic of the solvent-accessible surface area (SASA), a parameter of the hydrophobic free energy, and electrostatic interactions; (<b>Lower</b> part) comparison between the initial and final stable states of the amphiphilic polymer-decorated NPs. The hydrophilic ligands are squeezed out of the bilayer’s hydrophobic region, forming a so-called “snorkeling” phenomenon; (<b>B</b>) Decomposition of the free energy during the NP penetration process. <math display="inline"> <mrow> <mo>Δ</mo> <msub> <mi>G</mi> <mtext>total</mtext> </msub> </mrow> </math> is the total free energy change. <math display="inline"> <mrow> <mo>Δ</mo> <msub> <mi>G</mi> <mtext>phobic</mtext> </msub> </mrow> </math> is the change of hydrophobic energy, determined through the SASA. <math display="inline"> <mrow> <mo>Δ</mo> <msub> <mi>E</mi> <mtext>elec</mtext> </msub> </mrow> </math> is the electrostatic energy change. <math display="inline"> <mrow> <mo>Δ</mo> <msub> <mi>E</mi> <mtext>thick</mtext> </msub> </mrow> </math> is the free energy change corresponding to deformation of the lipid bilayer. <math display="inline"> <mrow> <mo>Δ</mo> <msub> <mi>S</mi> <mtext>conf</mtext> </msub> </mrow> </math> is the conformation entropy change of the decorated amphiphilic polymers; (<b>C</b>) Total free energy change <math display="inline"> <mrow> <mo>Δ</mo> <msub> <mi>G</mi> <mtext>total</mtext> </msub> </mrow> </math> as a function of NP diameter and monolayer composition. The ligand density on the Au NPs is kept constant; (<b>D</b>) Snapshots of the initial and final states of the NPs interacting with a lipid bilayer. For the case of 1:1 MUS:OT NP on the top of the bilayer, it cannot penetrate into the bilayer (<b>Upper</b> part); while it can penetrate in the bilayer through the edge (<b>Lower</b> part); (<b>E</b>) Snapshots of the transition states during NP penetration through the edge of a bilayer. At the transition time (<span class="html-italic">t</span> = 17.66 ns), the protruding lipids were in contact with the amphiphilic NP. The figures are adapted from References [<a href="#B52-polymers-08-00083" class="html-bibr">52</a>,<a href="#B54-polymers-08-00083" class="html-bibr">54</a>,<a href="#B57-polymers-08-00083" class="html-bibr">57</a>,<a href="#B63-polymers-08-00083" class="html-bibr">63</a>] with permission.</p>
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<p>Self-assembly and subsequent endocytosis of lipid molecule-decorated NPs (MPs and BPs). (<b>A</b>) Computational modeling on the self-assembly process of the modes A and B given in <a href="#polymers-08-00083-f003" class="html-fig">Figure 3</a>A. In mode A (<b>Upper</b> part), the NP core could interact with the random lipids and form the MPs. While in mode B (<b>Lower</b> Part), the NP core will interact with the pre-assembled liposome and form the BPs; (<b>B</b>) Snapshots of the MPs and BPs interacting with a vesicle. Upper and lower parts are corresponding to the MPs and BPs, respectively; (<b>C</b>) Schematic of different states of the endocytosis of soft NP; (<b>D</b>) Phase diagram for the endocytosis of NPs with different stiffness. <math display="inline"> <msub> <mi>κ</mi> <mn>1</mn> </msub> </math> and <math display="inline"> <msub> <mi>κ</mi> <mn>2</mn> </msub> </math> are the bending rigidities of the NP and membrane, respectively. The solid lines represent the phase boundaries between the fully wrapping and partial wrapping regimes. The horizontal axis represents the adhesion energy <math display="inline"> <mover accent="true"> <mi>γ</mi> <mo>¯</mo> </mover> </math> and the vertical one denotes the membrane tension <math display="inline"> <mover accent="true"> <mi>σ</mi> <mo>¯</mo> </mover> </math>. These figures are adapted from References [<a href="#B51-polymers-08-00083" class="html-bibr">51</a>,<a href="#B64-polymers-08-00083" class="html-bibr">64</a>] with permission.</p>
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<p>Internalization process of PEGylated NPs and related free energy change. (<b>A</b>) Snapshots of PEGylated NPs used in the dissipative particle dynamics (DPD) simulations with two grafting densities: 0.2 and 1.6 chains/nm<math display="inline"> <msup> <mrow/> <mn>2</mn> </msup> </math>. The diameter of the NP core is about 8 nm. The polymerization degree of tethered chains is 18, corresponding to the molecular weight 838 Da; (<b>B</b>) Endocytosis of PEGylated NPs with different grafting densities. When the grafting density is low, <span class="html-italic">i.e.</span>, 0.2 chains/nm<math display="inline"> <msup> <mrow/> <mn>2</mn> </msup> </math>, the NP will be trapped on the surface of membrane. While for high grafting density, 1.6 chains/nm<math display="inline"> <msup> <mrow/> <mn>2</mn> </msup> </math>, the NP will be fully wrapped by the membrane; (<b>C</b>) Wrapping ratio versus time for PEGylated NPs with different grafting densities; (<b>D</b>) Free energy change of the tethered polymers during endocytosis. The dashed line represents the bending energy of the membrane.</p>
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<p>Design of NP superstructure by using the DNA linkers for self-assembly. (<b>A</b>) Individual NPs (<b>red</b> and <b>yellow</b> spheres) were coated with thiolated and single-stranded DNA and then self-assembled together due to the complementary DNA sequence. The surface of the assembled NP can be further decorated by PEG polymers (blue clouds) to control interactions with cells and tissues; (<b>B</b>) Cross-sectional view of the self-assembled NP superstructure of a core-satellite. The insert shows that the payloads could be encapsulated either via hybridizing (<b>green</b> circle) or intercalating (<b>orange</b> hexagon) to the DNA linkers; (<b>C</b>) TEM images of the NP superstructure of two-layer core satellites as a function of the satellite-to-core ratio (<span class="html-italic">r</span> = 2, 8, 16, and 24); (<b>D</b>) TEM images on the NP superstructure of two-layer core satellites as a function of the satellite PEG length (molecular weight <math display="inline"> <msub> <mi>M</mi> <mi>w</mi> </msub> </math> = bare, 1, 5, and 10 kDa); (<b>E</b>) TEM images of the NP superstructure of three-layer core satellites by introducing the third DNA sequence. The scale bars for TEM images are 50 nm. The figure is adapted from Reference [<a href="#B83-polymers-08-00083" class="html-bibr">83</a>] with permission.</p>
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2899 KiB  
Article
A Heterobimetallic Anionic 3,6-Connected 2D Coordination Polymer Based on Nitranilate as Ligand
by Samia Benmansour and Carlos J. Gómez-García
Polymers 2016, 8(3), 89; https://doi.org/10.3390/polym8030089 - 16 Mar 2016
Cited by 25 | Viewed by 6921
Abstract
In order to synthesize new coordination polymers with original architectures and interesting magnetic properties, we used the nitranilate ligand (C6O4(NO2)22? = C6N2O82?), derived from the dianionic ligand dhbq [...] Read more.
In order to synthesize new coordination polymers with original architectures and interesting magnetic properties, we used the nitranilate ligand (C6O4(NO2)22? = C6N2O82?), derived from the dianionic ligand dhbq2? (2,5-dihydroxy-1,4-benzoquinone = H2C6O42?). The use of this bis-bidentate bridging ligand led to [(DAMS)2{FeNa(C6N2O8)3}·CH3CN]n (1) (DAMS+ = C16H17N2+ = 4-[4-(dimethylamino)-?-styryl]-1-methylpyridinium), a 2D heterometallic coordination polymer presenting an unprecedented structure for any anilato-based compound. This structural type is a 3,6-connected 2D coordination polymer derived from the well-known honeycomb hexagonal structure, where Fe(III) ions alternate with Na+ dimers (as Na2O12 units) in the vertices of the hexagons and with an additional [Fe(C6N2O8)3]3? anion located in the center of the hexagons connecting the three Na+ dimers. The magnetic properties of compound 1 show the presence of paramagnetic isolated high spin Fe(III) complexes with a zero field splitting, |D| = 8.5 cm?1. Full article
(This article belongs to the Special Issue Coordination Polymers: New Materials for Multiple Applications)
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<p>Ortep views of the fragments of the structure of compound <b>1</b> with the labeling scheme: (<b>a</b>) structure of the [Fe(C<sub>6</sub>N<sub>2</sub>O<sub>8</sub>)<sub>3</sub>]<sup>3−</sup> unit; (<b>b</b>) structure of the Na<sub>2</sub>O<sub>12</sub> dimer; (<b>c</b>) structure of the DAMS<sup>+</sup> cation.</p>
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<p>(<b>a</b>) View of the alternating cationic and anionic layers in compound <b>1</b>. H atoms have been omitted for clarity; (<b>b</b>) View along the <span class="html-italic">c</span> direction of two consecutive cationic layers showing the different orientation of the DAMS<sup>+</sup> molecules in each layer (yellow and red). The anionic intermediate layer is only represented by the Fe(III) and Na<sup>+</sup> ions (orange and purple, respectively).</p>
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<p>View of the 3,6-connected anionic layer [NaFe(C<sub>6</sub>N<sub>2</sub>O<sub>8</sub>)<sub>3</sub>]<sup>2−</sup> generated with Fe(III) and pairs of Na<sup>+</sup> cations (the oxygen atoms of the NO<sub>2</sub> groups have been omitted for clarity). Color code: Fe = orange, Na = purple, O = red, N = blue and C = grey.</p>
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<p>Thermal variation of the χ<sub>m</sub><span class="html-italic">T</span> product per Fe(III) ion for compound <b>1</b>. Solid line is the best fit to the model (see text).</p>
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<p>Structures of (<b>a</b>) nitranilate ligand and (<b>b</b>) DAMS<sup>+</sup> cation.</p>
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2865 KiB  
Article
Stability Study of Flexible 6,13-Bis(triisopropylsilylethynyl)pentacene Thin-Film Transistors with a Cross-Linked Poly(4-vinylphenol)/Yttrium Oxide Nanocomposite Gate Insulator
by Jin-Hyuk Kwon, Xue Zhang, Shang Hao Piao, Hyoung Jin Choi, Jin-Hyuk Bae and Jaehoon Park
Polymers 2016, 8(3), 88; https://doi.org/10.3390/polym8030088 - 16 Mar 2016
Cited by 14 | Viewed by 7638
Abstract
We investigated the electrical and mechanical stability of flexible 6,13-bis(triisopropylsilylehtynyl)pentacene (TIPS-pentacene) thin-film transistors (TFTs) that were fabricated on polyimide (PI) substrates using cross-linked poly(4-vinylphenol) (c-PVP) and c-PVP/yttrium oxide (Y2O3) nanocomposite films as gate insulators. Compared with the electrical characteristics [...] Read more.
We investigated the electrical and mechanical stability of flexible 6,13-bis(triisopropylsilylehtynyl)pentacene (TIPS-pentacene) thin-film transistors (TFTs) that were fabricated on polyimide (PI) substrates using cross-linked poly(4-vinylphenol) (c-PVP) and c-PVP/yttrium oxide (Y2O3) nanocomposite films as gate insulators. Compared with the electrical characteristics of TIPS-pentacene TFTs with c-PVP insulators, the TFTs with c-PVP/Y2O3 nanocomposite insulators exhibited enhancements in the drain current and the threshold voltage due to an increase in the dielectric capacitance. In electrical stability experiments, a gradual decrease in the drain current and a negative shift in the threshold voltage occurred during prolonged bias stress tests, but these characteristic variations were comparable for both types of TFT. On the other hand, the results of mechanical bending tests showed that the characteristic degradation of the TIPS-pentacene TFTs with c-PVP/Y2O3 nanocomposite insulators was more critical than that of the TFTs with c-PVP insulators. In this study, the detrimental effect of the nanocomposite insulator on the mechanical stability of flexible TIPS-pentacene TFTs was found to be caused by physical adhesion of TIPS-pentacene molecules onto the rough surfaces of the c-PVP/Y2O3 nanocomposite insulator. These results indicate that the dielectric and morphological properties of polymeric nanocomposite insulators are significant when considering practical applications of flexible electronics operated at low voltages. Full article
(This article belongs to the Collection Silicon-Containing Polymeric Materials)
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<p>(<b>a</b>) TEM images of Y<sub>2</sub>O<sub>3</sub> particles; (<b>b</b>) Schematic of the fabricated flexible TIPS-pentacene TFT.</p>
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<p>Output characteristics of the flexible TIPS-pentacene TFTs with the (<b>a</b>) c-PVP/Y<sub>2</sub>O<sub>3</sub> composite and (<b>b</b>) c-PVP gate insulators |<span class="html-italic">I</span><sub>D</sub>| <span class="html-italic">vs. V</span><sub>G</sub> and |<span class="html-italic">I</span><sub>D</sub>|<sup>1/2</sup> <span class="html-italic">vs. V</span><sub>G</sub> plots of TIPS-pentacene TFTs with the (<b>c</b>) c-PVP/Y<sub>2</sub>O<sub>3</sub> composite and (<b>d</b>) c-PVP gate insulators.</p>
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<p>AFM images of the (<b>a</b>) c-PVP and (<b>b</b>) c-PVP/Y<sub>2</sub>O<sub>3</sub> composite films. The insets show the contact angles on both films. AFM images of the TIPS-pentacene films deposited on the (<b>c</b>) c-PVP and (<b>d</b>) c-PVP/Y<sub>2</sub>O<sub>3</sub> composite films.</p>
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<p>Time-dependent decay behaviors of the (<b>a</b>) drain and (<b>b</b>) gate currents of the flexible TIPS-pentacene TFTs, during a prolonged bias stress test.</p>
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<p>Leakage current paths through the (<b>a</b>) c-PVP/Y<sub>2</sub>O<sub>3</sub> composite and (<b>b</b>) c-PVP gate insulators. (<b>c</b>) Possible interaction between the holes and the Y<sub>2</sub>O<sub>3</sub> nanoparticles in the c-PVP/Y<sub>2</sub>O<sub>3</sub> composite insulator.</p>
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<p>Variations in the threshold voltages of the flexible TIPS-pentacene TFTs with the c-PVP/Y<sub>2</sub>O<sub>3</sub> composite and c-PVP gate insulators, during a prolonged bias stress test.</p>
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<p>(<b>a</b>) Variations in the drain current of the fabricated TFTs, induced by cyclic bending stresses. Transfer characteristics of the flexible TIPS-pentacene TFTs with the (<b>b</b>) c-PVP/Y<sub>2</sub>O<sub>3</sub> composite and (<b>c</b>) c-PVP gate insulators, measured during cyclic bending stress tests.</p>
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6132 KiB  
Article
Charge Transport in LDPE Nanocomposites Part I—Experimental Approach
by Anh T. Hoang, Love Pallon, Dongming Liu, Yuriy V. Serdyuk, Stanislaw M. Gubanski and Ulf W. Gedde
Polymers 2016, 8(3), 87; https://doi.org/10.3390/polym8030087 - 16 Mar 2016
Cited by 62 | Viewed by 7587
Abstract
This work presents results of bulk conductivity and surface potential decay measurements on low-density polyethylene and its nanocomposites filled with uncoated MgO and Al2O3, with the aim to highlight the effect of the nanofillers on charge transport processes. Material [...] Read more.
This work presents results of bulk conductivity and surface potential decay measurements on low-density polyethylene and its nanocomposites filled with uncoated MgO and Al2O3, with the aim to highlight the effect of the nanofillers on charge transport processes. Material samples at various filler contents, up to 9 wt %, were prepared in the form of thin films. The performed measurements show a significant impact of the nanofillers on reduction of material’s direct current (dc) conductivity. The investigations thus focused on the nanocomposites having the lowest dc conductivity. Various mechanisms of charge generation and transport in solids, including space charge limited current, Poole-Frenkel effect and Schottky injection, were utilized for examining the experimental results. The mobilities of charge carriers were deduced from the measured surface potential decay characteristics and were found to be at least two times lower for the nanocomposites. The temperature dependencies of the mobilities were compared for different materials. Full article
(This article belongs to the Special Issue Nano- and Microcomposites for Electrical Engineering Applications)
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<p>Schematic illustration of the test setup for conductivity measurements. DAQ, denotes data acquisition card and pA, picoammeter.</p>
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<p>Schematic illustration of the setup for corona charging (<b>a</b>); and surface potential decay measurements (<b>b</b>).</p>
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<p>Multilayered sample structures used in SPD measurements: (<b>a</b>) NC/NC; (<b>b</b>) Ref/NC(G); and (<b>c</b>) NC/Ref(G). Ref and NC denote respectively the reference LDPE and LDPE/Al<sub>2</sub>O<sub>3</sub> 3 wt % nanocomposite whereas index (G) indicates the layer in contact with the grounded copper plate during the test.</p>
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<p>Densities of charging currents as functions of time measured at 60 °C for reference LDPE and both nanocomposites (Al<sub>2</sub>O<sub>3</sub> (<b>a</b>) and MgO (<b>b</b>)).</p>
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<p>Dependence of dc conductivity (at 60 °C) of the studied nanocomposites on filler content.</p>
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<p>Densities of charging currents as functions of time measured at room temperature (RT) ~20–22 °C, 40 °C, and 60 °C for the reference LDPE (Ref) and 3 wt % LDPE/Al<sub>2</sub>O<sub>3</sub> nanocomposite (NC).</p>
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<p>Temperature dependences of current densities at 4 × 10<sup>4</sup> s of LDPE and its nanocomposites. The calculated activation energies are indicated.</p>
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<p>Distribution of surface potential during potential decay measurement on LDPE/Al<sub>2</sub>O<sub>3</sub> 3 wt % nanocomposite at 60 °C.</p>
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<p>Measured surface potentials (<b>a</b>); and calculated decay rates (<b>b</b>) for reference LDPE (Ref) and LDPE/Al<sub>2</sub>O<sub>3</sub> 3 wt % nanocomposite (NC) at different temperatures.</p>
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<p>Surface potential decay on multilayered samples. Decay curves (a)–(c) are respectively obtained on samples (a)–(c) illustrated in <a href="#polymers-08-00087-f003" class="html-fig">Figure 3</a>. Curve (1) is a difference in surface potential measured on samples (a) and (b), whereas curve (2)—is the difference for samples (a) and (c).</p>
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<p>Return voltages measured after short-circuiting multilayered samples for 10 s at the end of SPD measurement. The inset shows the measured potential before and after removal of the top layer of sample Ref/NC(G).</p>
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<p>Schematic illustration of charge distribution and electric field (<b>a</b>) prior to; and (<b>b</b>) immediately after short-circuiting the Ref/NC(G) sample.</p>
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<p>Decay rate of surface potential on reference LDPE and Ref/NC(G).</p>
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<p>Temperature dependences of charge carrier (hole) mobility derived based on Sonnonstine and Perlman model.</p>
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<p>Plots −<span class="html-italic">t</span>d<span class="html-italic">V</span>/d<span class="html-italic">t</span> <span class="html-italic">vs</span>. log(<span class="html-italic">t</span>) (<b>a</b>); and −<span class="html-italic">t</span>d<span class="html-italic">V</span>/d<span class="html-italic">t</span> <span class="html-italic">vs.</span> <span class="html-italic">E<sub>t</sub></span> (<b>b</b>) obtained at different temperatures for reference LDPE.</p>
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<p>Trap energy distributions in reference LDPE and its nanocomposite.</p>
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<p>Log-log plot of <span class="html-italic">J</span> <span class="html-italic">vs.</span> <span class="html-italic">E</span> for reference LDPE (<b>a</b>); and LDPE/Al<sub>2</sub>O<sub>3</sub> 3wt % nanocomposite (<b>b</b>) at various temperatures. Regions 1 and 2 in figure (<b>b</b>) are featured by different slopes of the dependencies.</p>
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<p>Schottky plot for reference LDPE (<b>a</b>); and LDPE/Al<sub>2</sub>O<sub>3</sub> 3 wt % nanocomposite (<b>b</b>) at various temperatures. Regions 1 and 2 in figure (<b>b</b>) are featured by different slopes of the dependencies.</p>
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<p>Poole-Frenkel plot for reference LDPE (<b>a</b>); and LDPE/Al<sub>2</sub>O<sub>3</sub> 3 wt % nanocomposite (<b>b</b>) at various temperatures. Regions 1 and 2 in figure (<b>b</b>) are featured by different slopes of the dependencies.</p>
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4890 KiB  
Article
Synthesis, Structures and Luminescence Properties of Metal-Organic Frameworks Based on Lithium-Lanthanide and Terephthalate
by Mohammed S. M. Abdelbaky, Zakariae Amghouz, Santiago García-Granda and José R. García
Polymers 2016, 8(3), 86; https://doi.org/10.3390/polym8030086 - 16 Mar 2016
Cited by 14 | Viewed by 8928
Abstract
Metal-organic frameworks assembled from Ln(III), Li(I) and rigid dicarboxylate ligand, formulated as [LiLn(BDC)2(H2O)·2(H2O)] (MS1-6,7a) and [LiTb(BDC)2] (MS7b) (Ln = Tb, Dy, Ho, Er, Yb, Y0.96Eu0.04, Y0.93Tb0.07, and [...] Read more.
Metal-organic frameworks assembled from Ln(III), Li(I) and rigid dicarboxylate ligand, formulated as [LiLn(BDC)2(H2O)·2(H2O)] (MS1-6,7a) and [LiTb(BDC)2] (MS7b) (Ln = Tb, Dy, Ho, Er, Yb, Y0.96Eu0.04, Y0.93Tb0.07, and H2BDC = terephthalic acid), were obtained under hydrothermal conditions. The isostructural MS1-6 crystallize in monoclinic P21/c space group. While, in the case of Tb3+ a mixture of at least two phases was obtained, the former one (MS7a) and a new monoclinic C2/c phase (MS7b). All compounds have been studied by single-crystal and powder X-ray diffraction, thermal analyses (TGA), vibrational spectroscopy (FTIR), and scanning electron microscopy (SEM-EDX). The structures of MS1-6 and MS7a are built up of inorganic-organic hybrid chains. These chains constructed from unusual four-membered rings, are formed by edge- and vertex-shared {LnO8} and {LiO4} polyhedra through oxygen atoms O3 (vertex) and O6-O7 (edge). Each chain is cross-linked to six neighboring chains through six terephthalate bridges. While, the structure of MS7b is constructed from double inorganic chains, and each chain is, in turn, related symmetrically to the adjacent one through the c glide plane. These chains are formed by infinitely alternating {LiO4} and {TbO8} polyhedra through (O2-O3) edges to create Tb–O–Li connectivity along the c-axis. Both MS1-6,7a and MS7b structures possess a 3D framework with 1D trigonal channels running along the a and c axes, containing water molecules and anhydrous, respectively. Topological studies revealed that MS1-6 and MS7a have a new 2-nodal 3,10-c net, while MS7b generates a 3D net with unusual ?-Sn topology. The photoluminescence properties Eu- and Tb-doped compounds (MS5-6) are also investigated, exhibiting strong red and green light emissions, respectively, which are attributed to the efficient energy transfer process from the BDC ligand to Eu3+ and Tb3+. Full article
(This article belongs to the Special Issue Coordination Polymers: New Materials for Multiple Applications)
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<p>PXRD patterns of <b>MS1-6</b> compared with the calculated for <b>MS2</b>; (*) shows the peak of an unidentified phase.</p>
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<p>PXRD pattern of <b>MS7</b>, compared with the calculated for <b>MS1</b> and <b>MS7b</b>; (*) shows the peaks of an unidentified phase.</p>
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<p>Perspective view of the coordination environments of Ln<sup>3+</sup> and Li<sup>+</sup> cations in <b>MS1–6</b> (<b>a</b>,<b>b</b>) and <b>MS7b</b> (<b>c</b>,<b>d</b>) and coordination modes of BDC ligand (<b>e</b>).</p>
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<p>Perspective view of the coordination environments of Ln<sup>3+</sup> and Li<sup>+</sup> cations in <b>MS1–6</b> (<b>a</b>,<b>b</b>) and <b>MS7b</b> (<b>e</b>,<b>f</b>); the secondary building unit for <b>MS1–6</b> (<b>c</b>) and <b>MS7b</b> (<b>g</b>), and the infinite chains along the <span class="html-italic">a</span> and <span class="html-italic">c</span> axes for <b>MS1–6</b> (<b>d</b>) and <b>MS7b</b> (<b>h</b>).</p>
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<p>Projection of the structure along the <span class="html-italic">a</span> and <span class="html-italic">c</span> axes for <b>MS1–6</b> (<b>a</b>) and <b>MS7b</b> (<b>b</b>), respectively. Topological representations of <b>MS1–6</b> (<b>c</b>) and <b>MS7b</b> (<b>d</b>).</p>
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<p>IR spectra of <b>MS1–4</b> and <b>MS7</b>.</p>
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<p>TGA curves of <b>MS3</b> (Er) and <b>MS4</b> (Yb).</p>
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<p>Excitation spectra for <b>MS5</b> (<b>a</b>) and <b>MS6</b> (<b>c</b>) detecting luminescence at 615 and 545 nm, respectively. Emission spectra for <b>MS5</b> (<b>b</b>) and <b>MS6</b> (<b>d</b>) upon excitation at 260 and 275 nm. Emission decay curves excited at 260 nm and monitored at 616 and 545 nm for <b>MS5</b> (<b>e</b>) and <b>MS6</b> (<b>f</b>), respectively.</p>
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<p>Excitation spectra for <b>MS5</b> (<b>a</b>) and <b>MS6</b> (<b>c</b>) detecting luminescence at 615 and 545 nm, respectively. Emission spectra for <b>MS5</b> (<b>b</b>) and <b>MS6</b> (<b>d</b>) upon excitation at 260 and 275 nm. Emission decay curves excited at 260 nm and monitored at 616 and 545 nm for <b>MS5</b> (<b>e</b>) and <b>MS6</b> (<b>f</b>), respectively.</p>
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<p>Optical microscopic images under UV light of single crystals of Eu-doped compound <b>MS5</b> (<b>a</b>,<b>b</b>) and Tb-doped compound <b>MS6</b> (<b>c</b>,<b>d</b>).</p>
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2764 KiB  
Article
Systematic Limitations in Concentration Analysis via Anomalous Small-Angle X-ray Scattering in the Small Structure Limit
by Guenter Goerigk, Sebastian Lages and Klaus Huber
Polymers 2016, 8(3), 85; https://doi.org/10.3390/polym8030085 - 16 Mar 2016
Cited by 2 | Viewed by 11052
Abstract
Anomalous small angle scattering measurements have been applied to diluted solutions of anionic polyacrylates decorated by specifically-interacting Pb2+ cations, revealing partial collapse of the polyacrylate into pearl-like subdomains with a size on the order of a few nanometers. From the pure-resonant scattering [...] Read more.
Anomalous small angle scattering measurements have been applied to diluted solutions of anionic polyacrylates decorated by specifically-interacting Pb2+ cations, revealing partial collapse of the polyacrylate into pearl-like subdomains with a size on the order of a few nanometers. From the pure-resonant scattering contribution of the Pb2+ cations, and from subsequent analysis of the resonant-invariant, the amount of Pb2+ cations condensed onto the polyanions with respect to the total amount of Pb2+ cations in the solvent was estimated. In order to scrutinize systematic limitations in the determination of the chemical concentrations of resonant scattering counterions in the collapsed phase, Monte Carlo simulations have been performed. The simulations are based on structural confinements at variable size in the range of few nanometers, which represent the collapsed subdomains in the polyanions. These confinements were gradually filled to a high degree of the volume fraction with resonant scattering counterions giving access to a resonant-invariant at a variable degree of filling. The simulations revealed in the limit of small structures a significant underestimation of the true degree of filling of the collapsed subdomains when determining chemical concentrations of Pb2+ cations from the resonant invariant. Full article
(This article belongs to the Collection Polyelectrolytes)
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<p>(<b>a</b>) SAXS curves of samples FRM01 and FRM02 measured at three different X-ray energies in the vicinity of the LIII-absorption edge of Pb at 13,035 eV. The curves with the label “total” represent the total scattering, while the curves with label “pure” represent the form factor of the pure-resonant contribution. Note that the separated form factor of the pure-resonant scattering contribution is more than three orders of magnitude smaller with a cross-section down towards 10<sup>–5</sup> cm<sup>−1</sup> (!) when compared to the total scattering (factor 2000); (<b>b</b>) SANS curve of the sample FRM02. The solid lines running through the symbols of the scattering curves are fitted their respective scaled model functions representing the “freely jointed chain pearl necklace” FJC-PN model (see text).</p>
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<p>The resonant invariant of the Pb counterions. From the integral the Pbconcentrations in the condensed phase is deduced. The blue lines represent the FJC-PN model (see text).</p>
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<p>XANES spectrum of FRM02 measured at the Pb L<sub>III</sub>-edge at 13,035 eV. The solid (black) line represents the XANES spectrum of a Pb-metal foil (<span class="html-italic">y</span>-axis on the left). The FRM02 spectrum reveals a chemical shift of about 5 eV. Δμ<span class="html-italic">d</span> is the difference of the absorption coefficient times the sample thickness and represents the Pb-L<sub>III</sub>-edge of the sample taken from the <span class="html-italic">y</span>-axis on the right.</p>
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<p>Kratky plot of scattering curves calculated from scattering curves of Pb<sup>2+</sup> ions confined in a cube of 1 nm side length by Monte Carlo simulation under the condition of a standard SAXS experiment (<b>a</b>). For the Pb<sup>2+</sup> ions a spherical form factor with a radius of 0.119 nm was assumed. The structure factor of 5, 20, 40, 80, and 100 Pb ions with randomly-distributed distances inside a real gas was simulated. The curves are normalized to N. The same simulations have been repeated for the real gas under the condition of ASAXS measurements using point-like scattering centers. For <span class="html-italic">q</span>-values beyond 20 nm<sup>−1</sup> the simulated curves are divided by 10 in order to better visualize (<b>b</b>).</p>
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<p>Two integrals of normalized ASAXS and SAXS Kratky plots have been calculated for four different cubic confinements (1, 2, 4, and 6.5 nm) under the condition of a standard small-angle scattering experiment over the two integration intervals 0&lt; <span class="html-italic">q</span> &lt; 10 nm<sup>−1</sup> (<b>a</b>) and 0&lt; <span class="html-italic">q</span> &lt; 2 nm<sup>−1</sup> (<b>b</b>). The grey parallelogram represents the area of small confinements with low filling degrees compatible with results from the RI-analysis and XANES (see text).</p>
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2999 KiB  
Article
Enzymatic Synthesis and Characterization of Hydrophilic Sugar Based Polyesters and Their Modification with Stearic Acid
by Muhammad Humayun Bilal, Marko Prehm, Andrew Efraim Njau, Muhammad Haris Samiullah, Annette Meister and Jörg Kressler
Polymers 2016, 8(3), 80; https://doi.org/10.3390/polym8030080 - 16 Mar 2016
Cited by 22 | Viewed by 9817
Abstract
Biodegradable and hydrophilic functional polyesters were synthesized enzymatically using xylitol or d-sorbitol together with divinyl adipate and lipase B from Candida antartica (CAL-B). The resulting polyesters had pendant OH-groups from their sugar units which were esterified to different degrees with stearic acid [...] Read more.
Biodegradable and hydrophilic functional polyesters were synthesized enzymatically using xylitol or d-sorbitol together with divinyl adipate and lipase B from Candida antartica (CAL-B). The resulting polyesters had pendant OH-groups from their sugar units which were esterified to different degrees with stearic acid chloride. The structure and the degrees of polymerization of the resulting graft copolymers based on poly(xylitol adipate) and poly(d-sorbitol adipate) were characterized by 1H NMR spectroscopy and SEC. DSC, WAXS and SAXS measurements indicated that a phase separation between polymer backbone and stearoyl side chains occurred in the graft copolymers, and, additionally, the side chains were able to crystallize which resulted in the formation of a lamellar morphology. Additionally, nanoparticles of the graft copolymers in an aqueous environment were studied by DLS and negative stain TEM. Full article
(This article belongs to the Special Issue Polymers for Aqueous Media)
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<p><sup>1</sup>H NMR spectra of (<b>a</b>) grafted and non-grafted poly(xylitol adipate) and (<b>b</b>) grafted and non-grafted poly(<span class="html-small-caps">d</span>-sorbitol adipate), recorded at 25 °C using CDCl<sub>3</sub> and DMSO-d<sub>6</sub> as solvent for grafted and non-grafted polymers, respectively.</p>
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<p>Size exclusion chromatography (SEC) traces of (<b>a</b>) stearoyl grafed poly(xylitol adipate) in THF; (<b>b</b>) SEC traces of stearoyl grafted poly(<span class="html-small-caps">d</span>-sorbitol adipate) in THF. The insets show the SEC traces of the polymer backbones PXA and PDSA, respectively, in DMF.</p>
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<p>DSC traces of (<b>a</b>) grafted and non-grafted PXA and (<b>b</b>) grafted and non-grafted PDSA. The measurements are carried out with a heating rate of 10 K·min<sub>−1</sub>.</p>
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<p>Combined SAXS and WAXS traces during heating and cooling cycles (5 K step from 25 °C to 70 °C and back to 25 °C) of (<b>a</b>) PXA-<span class="html-italic">g</span>-S15; (<b>b</b>) PXA-<span class="html-italic">g</span>-S36; (<b>c</b>) PDSA-<span class="html-italic">g</span>-S68; and (<b>d</b>) PDSA-<span class="html-italic">g</span>-S10.</p>
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<p>(<b>a</b>) Hydrodynamic radius distribution of PXA-<span class="html-italic">g</span>-S15 nanoparticles in water with a concentration of 1 g∙L<sup>−1</sup> at 25 °C; (<b>b</b>) hydrodynamic radius distribution of PDSA-<span class="html-italic">g</span>-S10 nanoparticles (1g∙L<sup>−1</sup> in water at 25 °C).</p>
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<p>Negative-staining electron micrographs, (<b>a</b>) 0.1% dispersion of PXA-<span class="html-italic">g</span>-S15; (<b>b</b>) 0.1% dispersion of PDSA-<span class="html-italic">g</span>-S10.</p>
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<p>Synthetic route to stearoyl grafted poly(xylitol adipate) (PXA-<span class="html-italic">g</span>-S) and poly(<span class="html-small-caps">d</span>-sorbitol adipate) (PDSA-<span class="html-italic">g</span>-S).</p>
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1755 KiB  
Article
Hybrid Polymer-Network Hydrogels with Tunable Mechanical Response
by Sebastian Czarnecki, Torsten Rossow and Sebastian Seiffert
Polymers 2016, 8(3), 82; https://doi.org/10.3390/polym8030082 - 15 Mar 2016
Cited by 35 | Viewed by 10250
Abstract
Hybrid polymer-network gels built by both physical and covalent polymer crosslinking combine the advantages of both these crosslinking types: they exhibit high mechanical strength along with excellent fracture toughness and extensibility. If these materials are extensively deformed, their physical crosslinks can break such [...] Read more.
Hybrid polymer-network gels built by both physical and covalent polymer crosslinking combine the advantages of both these crosslinking types: they exhibit high mechanical strength along with excellent fracture toughness and extensibility. If these materials are extensively deformed, their physical crosslinks can break such that strain energy is dissipated and irreversible fracturing is restricted to high strain only. This mechanism of energy dissipation is determined by the kinetics and thermodynamics of the physical crosslinking contribution. In this paper, we present a poly(ethylene glycol) (PEG) based material toolkit to control these contributions in a rational and custom fashion. We form well-defined covalent polymer-network gels with regularly distributed additional supramolecular mechanical fuse links, whose strength of connectivity can be tuned without affecting the primary polymer-network composition. This is possible because the supramolecular fuse links are based on terpyridine–metal complexation, such that the mere choice of the fuse-linking metal ion adjusts their kinetics and thermodynamics of complexation–decomplexation, which directly affects the mechanical properties of the hybrid gels. We use oscillatory shear rheology to demonstrate this rational control and enhancement of the mechanical properties of the hybrid gels. In addition, static light scattering reveals their highly regular and well-defined polymer-network structures. As a result of both, the present approach provides an easy and reliable concept for preparing hybrid polymer-network gels with rationally designed properties. Full article
(This article belongs to the Special Issue Polymers for Aqueous Media)
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<p>Formation of hybrid polymer-network gels that contain both covalent and physical crosslinks. For this purpose, linear poly(ethylene glycol) (PEG) is functionalized with both azide (N<sub>3</sub>) and terpyridine (TPy) moieties at each end, and tetra-arm PEG is functionalized with cyclooctynes (CyOct) capped to each arm. After mixing aqueous solutions of both these PEG compounds, gelation occurs by strain-promoted azide–alkyne cycloaddition forming triazole linking units sketched as blue pentagons in the schematic. Addition of metal(II) ions, sketched as red circles in the schematic, leads to formation of intramolecular or intermolecular mechanical fuse links due to complexation to the additional terpyridine moieties on the polymer. Upon stretching, these hybrid gel-networks first respond in a linear rubbery-elastic fashion, before overstretching results in breakage of the transient metal–terpyridine bis-complexes, thereby dissipating strain energy, while leaving the covalent polymer crosslinking intact. Upon de-stretching, the metal–terpyridine bis-complexes are reformed. The illustrated hybrid polymer-network is drawn in an idealized fashion without loops or dangling chains; the data presented in this work indeed support this ideal picture and suggest the minor extent of such imperfection.</p>
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<p><sup>1</sup>H-NMR spectra of PEG-hydroxy-azide (<b>top</b>), PEG-hydroxy-terpyridine (<b>center</b>) and PEG-terpyridinyl-azide (<b>bottom</b>) in a chemical-shift range of 4–9 ppm, where the signals of the compounds differ most significantly.</p>
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<p>Frequency-dependent shear moduli of the (<b>A</b>) purely covalent gel and the (<b>B</b>) Zn<sup>2+</sup>-, (<b>C</b>) Mn<sup>2+</sup>-; and (<b>D</b>) Co<sup>2+</sup>-terpyridine-enforced hybrid gels, each probed at a total polymer concentration of 100 g L<sup>−1</sup> in water. All plots show the elastic (full symbols, <span class="html-italic">G</span>′) and viscous (open symbols, <span class="html-italic">G</span>′′) parts of the complex shear modulus, <span class="html-italic">G</span>, as a function of the test frequency, ω. Grey triangles denote data obtained at 10 °C, while black diamonds denote data obtained at 25 °C. All data are superimposed by shifting the 10 °C data along the frequency axes to obtain master curves according to the principle of time-temperature-superposition, referenced to 25 °C. The vertical dashed red line in (<b>B</b>) denotes ω = k<span class="html-italic"><sub>diss.</sub></span> of the Zn<sup>2+</sup>–terpyridine complexes.</p>
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<p>Amplitude-dependent shear moduli of the (<b>A</b>) purely covalent gel and the (<b>B</b>) Zn<sup>2+</sup>-, (<b>C</b>) Mn<sup>2+</sup>-; and (<b>D</b>) Co<sup>2+</sup>-terpyridine-enforced hybrid gels, each probed at a total polymer concentration of 100 g L<sup>−1</sup> in water. All plots show the elastic (full symbols, <span class="html-italic">G</span>′) and viscous (open symbols, <span class="html-italic">G</span>′′) parts of the complex shear modulus, <span class="html-italic">G</span>, as a function of the shear-deformation amplitude, γ, at 25 °C.</p>
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<p>Static light scattering data used to evaluate the spatial polymer network inhomogeneity of the (<b>A,E</b>) purely covalent gel and of the (<b>B</b>,<b>F</b>) Zn<sup>2+</sup>-, (<b>C</b>,<b>G</b>) Mn<sup>2+</sup>-, and (<b>D</b>,<b>H</b>) Co<sup>2+</sup>-terpyridine-enforced hybrid gels, each probed at a total polymer concentration of 100 g·L<sup>−1</sup> in water. (<b>A</b>–<b>D</b>) Rayleigh ratios, <span class="html-italic">R</span><sub>θ</sub>, of the gels (full symbols) and of an uncrosslinked reference sample (open symbols); (<b>E</b>–<b>H</b>) Debye-Bueche plots of the excess scattering intensities, <span class="html-italic">R</span><sub>E</sub>(<span class="html-italic">q</span>), calculated as the difference between the angle-resolved Rayleigh ratios of the crosslinked and uncrosslinked samples.</p>
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<p>Synthesis of (<b>A</b>) linear PEG-azide (<b>1</b>), (<b>B</b>) propargyl-terpyridine (<b>2</b>); (<b>C</b>) linear PEG-terpyridinyl-azide (<b>5</b>); and (<b>D</b>) tetra-arm PEG-bicyclo[6.1.0]non-4-yn-9-ylmethyl carbamate (<b>8</b>).</p>
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2747 KiB  
Article
Polymer Inclusion Membranes (PIM) for the Recovery of Potassium in the Presence of Competitive Cations
by Anna Casadellà, Olivier Schaetzle, Kitty Nijmeijer and Katja Loos
Polymers 2016, 8(3), 76; https://doi.org/10.3390/polym8030076 - 15 Mar 2016
Cited by 31 | Viewed by 13565
Abstract
Potassium is an important nutrient used in fertilizers but is not always naturally available We investigated the properties of polymer inclusion membranes (PIM) regarding their selective recovery of K+ over competitive ions typically present in urine (Na+ and NH4+ [...] Read more.
Potassium is an important nutrient used in fertilizers but is not always naturally available We investigated the properties of polymer inclusion membranes (PIM) regarding their selective recovery of K+ over competitive ions typically present in urine (Na+ and NH4+). The greatest flux was observed when the ratio of mass 2-nitrophenyl octyl ether (2-NPOE) used as plasticizer to cellulose triacetate (CTA) used as polymer was 0.25. The highest flux was achieved with a content of 24.8 wt % of dicyclohexan-18-crown-6 (DCH18C6) used as carrier, although the highest selectivity was observed with a content of 14.0 wt % of DCH18C6. We also studied whether the transport mechanism occurring in our system was based on co-transport of a counter-ion or ion exchange. Two different receiving phases (ultrapure water and 100 mM HCl) were tested. Results on transport mechanisms suggest that co-transport of cations and anions is taking place across our PIMs. The membrane deteriorated and lost its properties when the receiving phase was acidic; we suggested that this was due to hydrolysis of CTA. The greatest flux and selectivity were observed in ultrapure water as receiving phase. Full article
(This article belongs to the Special Issue Polymer Thin Films and Membranes 2015)
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<p>Scheme of the transport across a PIM for a cation (M<sub>n</sub><sup>+</sup>) and an anion (X<sub>n</sub><sup>−</sup>): co-transport of a counter-ion (<b>left</b>); and ion-exchange (<b>right</b>).</p>
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<p>Scheme of the diffusion cell.</p>
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<p>Effect of DCH18C6 content on the flux of the optimized PIM after 50 h. Results correspond to PIM-6 (1.56 wt %), -7 (14.0 wt %), -8 (24.8 wt %) and -9 (33.2 wt %).</p>
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<p>SEM images (magnification: 2500×) of cross-section PIMs with contents of DCH18C6 of 14.0 wt % (<b>a</b>); 24.8 wt % (<b>b</b>); and 33.2 wt % (<b>c</b>).</p>
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<p>Evolution using PIM-8 of [K<sup>+</sup>] in the receiving compartment in two different receiving phases: ultrapure water and 100 mM HCl.</p>
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<p>Evolution using PIM-8 of [NO<sub>3</sub><sup>−</sup>] in the receiving compartment in two different receiving phases: ultrapure water and 100 mM HCl.</p>
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<p>Comparison of the transported [K<sup>+</sup>] and [NO<sub>3</sub><sup>−</sup>] in the receiving phase of ultrapure water using PIM-8.</p>
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<p>Comparison of the transported [H<sup>+</sup>] and [Cl<sup>−</sup>] in the feed phase using PIM-8.</p>
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<p>Comparison of the transported [H<sup>+</sup>] into the feed phase and [K<sup>+</sup>] in the receiving phase using PIM-8.</p>
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<p>Comparison of the transported [Cl<sup>−</sup>] into the feed phase and [NO<sub>3</sub><sup>−</sup>] into the receiving phase using PIM-8.</p>
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<p>Chemical structure of 2-NPOE (<b>a</b>); CTA (<b>b</b>); and DCH18C6 (<b>c</b>).</p>
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<p>Release of DCH18C6 from PIM in three receiving phases: water, 10 mM HCl and 100 mM HCl.</p>
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3238 KiB  
Article
Surface Property Modification of Silver Nanoparticles with Dopamine-Functionalized Poly(pentafluorostyrene) via RAFT Polymerization
by Ka Wai Fan and Anthony Michael Granville
Polymers 2016, 8(3), 81; https://doi.org/10.3390/polym8030081 - 14 Mar 2016
Cited by 15 | Viewed by 8887
Abstract
This research aims to synthesize a dopamine-functionalized macromolecular anchor to perform surface modification on the target nanostructures. A molecular anchor, 3,4-dichloro-1-[2-(3,4-dihydroxyphenyl)ethyl]-1H-pyrrole-2,5-dione, was successfully synthesized from dopamine and 2,3-dichloromaleic anhydride. The anchor acted as a linkage to couple the chains of poly(pentafluorostyrene) [...] Read more.
This research aims to synthesize a dopamine-functionalized macromolecular anchor to perform surface modification on the target nanostructures. A molecular anchor, 3,4-dichloro-1-[2-(3,4-dihydroxyphenyl)ethyl]-1H-pyrrole-2,5-dione, was successfully synthesized from dopamine and 2,3-dichloromaleic anhydride. The anchor acted as a linkage to couple the chains of poly(pentafluorostyrene) (PPFS) which were synthesized via reversible addition fragmentation chain transfer (RAFT) polymerization. Modification was successfully performed to silver nanoparticles (AgNPs) by deposition of the dopamine-functionalized coupled PPFS onto the surface of the particles. The modified AgNPs had demonstrated improved dispersibility in organic solvent due to the hydrophobic nature of PPFS. To modify the surface chemistry of the nanoparticles further, thioglucose was grafted onto the structure of the coupled PPFS via thiol-fluoro nucleophilic substitution at the para-position of the pentafluorophenyl groups on the monomer units. The presence of sugar moieties on the coupled PPFS increased its hydrophilicity, which allowed the modified AgNPs to be readily dispersed in aqueous solvent. Full article
(This article belongs to the Special Issue Controlled/Living Radical Polymerization)
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<p>Gel Permeation Chromatography (GPC) analysis of PPFS chains (black) and coupled PPFS (blue) with DA-DCMA anchor.</p>
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<p>Attenuated Total Reflectance Fourier Transform Infrared (ATR-FTIR) analysis of coupled PPFS and anchored PPFS@AgNPs.</p>
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<p>SEM image of AgNPs (<b>left</b>) and PPFS coupled AgNPs (PPFS@AgNPs) (<b>right</b>).</p>
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<p>TGA analysis of bare AgNP, RAFT generated DA-DCMA coupled PPFS chains, and PPFS coupled to AgNPs (PPFS@AgNPs).</p>
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<p>Dispersion of modified GPPFS@AgNPs in water before (<b>left</b>) and after (<b>right</b>) sonication.</p>
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<p>TGA analysis of bare AgNP, DA-DCMA coupled glycosylated PPFS (GPPFS) chains, and GPPFS coupled to AgNPs (GPPFS@AgNPs).</p>
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<p>Reaction steps for generating poly(pentafluorostyrene) (PPFS) y-brush with dopamine based anchor.</p>
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488 KiB  
Article
The Backfolded Odijk Regime for Wormlike Chains Confined in Rectangular Nanochannels
by Abhiram Muralidhar, Michael J. Quevillon and Kevin D. Dorfman
Polymers 2016, 8(3), 79; https://doi.org/10.3390/polym8030079 - 14 Mar 2016
Cited by 23 | Viewed by 7009
Abstract
We confirm Odijk’s scaling laws for (i) the average chain extension; (ii) the variance about the average extension; and (iii) the confinement free energy of a wormlike chain confined in a rectangular nanochannel smaller than its chain persistence length through pruned-enriched Rosenbluth method [...] Read more.
We confirm Odijk’s scaling laws for (i) the average chain extension; (ii) the variance about the average extension; and (iii) the confinement free energy of a wormlike chain confined in a rectangular nanochannel smaller than its chain persistence length through pruned-enriched Rosenbluth method (PERM) simulations of asymptotically long, discrete wormlike chains. In the course of this analysis, we also computed the global persistence length of ideal wormlike chains for the modestly rectangular channels that are used in many experimental systems. The results are relevant to genomic mapping systems that confine DNA in channel sizes around 50 nm, since fabrication constraints generally lead to rectangular cross-sections. Full article
(This article belongs to the Special Issue Semiflexible Polymers)
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Full article ">Figure 1
<p>Schematic illustration of a wormlike chain confined in a rectangular nanochannel of depth <span class="html-italic">D</span> and width <math display="inline"> <mrow> <mi>A</mi> <mo>&gt;</mo> <mi>D</mi> </mrow> </math>. The global persistence length <span class="html-italic">g</span> is the typical distance between hairpin bends, while the deflection segment length <span class="html-italic">λ</span> arises from the deflections off the channel walls. The excluded volume is given by a hardcore interaction with width <span class="html-italic">w</span> equal to the diameter of the chain. The global persistence length and deflection segment length are not drawn to scale.</p>
Full article ">Figure 2
<p>(<b>a</b>) Illustration of our method for obtaining the global persistence length. The curves here correspond to a subset of Set 1a (see <a href="#polymers-08-00079-t001" class="html-table">Table 1</a>) of our data for a fixed aspect ratio of <math display="inline"> <mrow> <mi>A</mi> <mo>/</mo> <mi>D</mi> <mo>=</mo> <mn>2</mn> </mrow> </math> and <math display="inline"> <mrow> <msub> <mi>L</mi> <mi>p</mi> </msub> <mo>/</mo> <mi>b</mi> <mspace width="3.33333pt"/> <mo>=</mo> <mspace width="3.33333pt"/> <mn>10</mn> </mrow> </math>. The solid curves are our simulation data and the dashed lines are the best fits for Equation (17). The red curve corresponds to the smallest channel size <math display="inline"> <mrow> <mi>D</mi> <mo>/</mo> <msub> <mi>L</mi> <mi>p</mi> </msub> <mo>=</mo> <mn>0</mn> <mo>.</mo> <mn>5</mn> </mrow> </math> and the black curve corresponds to the biggest channel size of <math display="inline"> <mrow> <mi>D</mi> <mo>/</mo> <msub> <mi>L</mi> <mi>p</mi> </msub> <mo>=</mo> <mn>1</mn> <mo>.</mo> <mn>94</mn> </mrow> </math>. The channel size increases from top to bottom; (<b>b</b>) the global persistence length thus obtained for all our data in <a href="#polymers-08-00079-t001" class="html-table">Table 1</a> against dimensionless channel size. The five colors represent the five aspect ratios considered here. The different point types correspond to <math display="inline"> <mrow> <msub> <mi>L</mi> <mi>p</mi> </msub> <mo>/</mo> <mi>b</mi> <mo>=</mo> <mn>10</mn> </mrow> </math> (□), <math display="inline"> <mrow> <msub> <mi>L</mi> <mi>p</mi> </msub> <mo>/</mo> <mi>b</mi> <mo>=</mo> <mn>12</mn> <mo>.</mo> <mn>5</mn> </mrow> </math> (▽), <math display="inline"> <mrow> <msub> <mi>L</mi> <mi>p</mi> </msub> <mo>/</mo> <mi>b</mi> <mo>=</mo> <mn>15</mn> </mrow> </math> (◯), <math display="inline"> <mrow> <msub> <mi>L</mi> <mi>p</mi> </msub> <mo>/</mo> <mi>b</mi> <mo>=</mo> <mn>17</mn> <mo>.</mo> <mn>5</mn> </mrow> </math> (⋄) and <math display="inline"> <mrow> <msub> <mi>L</mi> <mi>p</mi> </msub> <mo>/</mo> <mi>b</mi> <mo>=</mo> <mn>20</mn> </mrow> </math> (△). The dashed lines are from Equation (21). The horizontal black line indicates <math display="inline"> <mrow> <mi>g</mi> <mo>=</mo> <msub> <mi>L</mi> <mi>p</mi> </msub> </mrow> </math>, which should be the limiting value of <span class="html-italic">g</span> for <math display="inline"> <mrow> <mi>D</mi> <mo>≫</mo> <msub> <mi>L</mi> <mi>p</mi> </msub> </mrow> </math>.</p>
Full article ">Figure 3
<p>(<b>a</b>) Fractional extension against the scaling variable <span class="html-italic">ξ</span>. The vertical dashed line shows the boundary between the classic and backfolded Odijk regimes according to the scaling theory, <math display="inline"> <mrow> <mi>ξ</mi> <mo>=</mo> <mn>1</mn> </mrow> </math>. A power law fit to our data for <math display="inline"> <mrow> <mi>ξ</mi> <mo>&lt;</mo> <mn>0</mn> <mo>.</mo> <mn>3</mn> </mrow> </math> yields an exponent of <math display="inline"> <mrow> <mn>0</mn> <mo>.</mo> <mn>333</mn> <mo>±</mo> <mn>0</mn> <mo>.</mo> <mn>007</mn> </mrow> </math>; (<b>b</b>) normalized variance of extension <span class="html-italic">versus ξ</span>. The horizontal dashed line corresponds to <math display="inline"> <mrow> <mi>δ</mi> <msup> <mrow> <mi>X</mi> </mrow> <mn>2</mn> </msup> <mo>/</mo> <mi>L</mi> <mi>g</mi> <mo>=</mo> <mn>0</mn> <mo>.</mo> <mn>2</mn> </mrow> </math>. In both the panels, the <math display="inline"> <mrow> <msub> <mi>L</mi> <mi>p</mi> </msub> <mo>/</mo> <mi>w</mi> </mrow> </math> values shown are <math display="inline"> <mrow> <msub> <mi>L</mi> <mi>p</mi> </msub> <mo>/</mo> <mi>w</mi> <mo>=</mo> <mn>10</mn> </mrow> </math> (□), <math display="inline"> <mrow> <msub> <mi>L</mi> <mi>p</mi> </msub> <mo>/</mo> <mi>w</mi> <mo>=</mo> <mn>12</mn> <mo>.</mo> <mn>5</mn> </mrow> </math> (▽), <math display="inline"> <mrow> <msub> <mi>L</mi> <mi>p</mi> </msub> <mo>/</mo> <mi>w</mi> <mo>=</mo> <mn>15</mn> </mrow> </math> (◯), <math display="inline"> <mrow> <msub> <mi>L</mi> <mi>p</mi> </msub> <mo>/</mo> <mi>w</mi> <mo>=</mo> <mn>17</mn> <mo>.</mo> <mn>5</mn> </mrow> </math> (⋄) and <math display="inline"> <mrow> <msub> <mi>L</mi> <mi>p</mi> </msub> <mo>/</mo> <mi>w</mi> <mo>=</mo> <mn>20</mn> </mrow> </math> (△). Different colors indicate different <math display="inline"> <mrow> <msub> <mi>A</mi> <mtext>eff</mtext> </msub> <mo>/</mo> <msub> <mi>D</mi> <mtext>eff</mtext> </msub> </mrow> </math> ratios: red (1), purple (1.5), brown (2), green (3) and blue (4). All the data points satisfy the condition <math display="inline"> <mrow> <msub> <mi>D</mi> <mtext>eff</mtext> </msub> <mo>≤</mo> <msub> <mi>A</mi> <mtext>eff</mtext> </msub> <mo>≤</mo> <mn>2</mn> <msub> <mi>L</mi> <mi>p</mi> </msub> </mrow> </math>.</p>
Full article ">Figure 4
<p>Confinement free energy of ideal chains in various channel sizes. The black solid line is the confinement free energy in the classic Odijk regime valid in the limit <math display="inline"> <mrow> <mi>D</mi> <mo>≪</mo> <msub> <mi>L</mi> <mi>p</mi> </msub> </mrow> </math> and <math display="inline"> <mrow> <mi>A</mi> <mo>≪</mo> <msub> <mi>L</mi> <mi>p</mi> </msub> </mrow> </math> (Equation (4)). The <math display="inline"> <mrow> <msub> <mi>L</mi> <mi>p</mi> </msub> <mo>/</mo> <mi>b</mi> </mrow> </math> values for ideal chains shown here are <math display="inline"> <mrow> <msub> <mi>L</mi> <mi>p</mi> </msub> <mo>/</mo> <mi>b</mi> <mo>=</mo> <mn>10</mn> </mrow> </math> (□), <math display="inline"> <mrow> <msub> <mi>L</mi> <mi>p</mi> </msub> <mo>/</mo> <mi>b</mi> <mo>=</mo> <mn>12</mn> <mo>.</mo> <mn>5</mn> </mrow> </math> (▽), <math display="inline"> <mrow> <msub> <mi>L</mi> <mi>p</mi> </msub> <mo>/</mo> <mi>b</mi> <mo>=</mo> <mn>15</mn> </mrow> </math> (◯), <math display="inline"> <mrow> <msub> <mi>L</mi> <mi>p</mi> </msub> <mo>/</mo> <mi>b</mi> <mo>=</mo> <mn>17</mn> <mo>.</mo> <mn>5</mn> </mrow> </math> (⋄) and <math display="inline"> <mrow> <msub> <mi>L</mi> <mi>p</mi> </msub> <mo>/</mo> <mi>b</mi> <mo>=</mo> <mn>20</mn> </mrow> </math> (△). Different colors indicate different <math display="inline"> <mrow> <mi>A</mi> <mo>/</mo> <mi>D</mi> </mrow> </math> ratios: red (1), purple (1.5), brown (2), green (3) and blue (4). All the data points satisfy the condition <math display="inline"> <mrow> <mi>D</mi> <mo>≤</mo> <mi>A</mi> <mo>≤</mo> <mn>2</mn> <msub> <mi>L</mi> <mi>p</mi> </msub> </mrow> </math>.</p>
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<p>The excess free energy of real chains confined in rectangular channels. The <math display="inline"> <mrow> <msub> <mi>L</mi> <mi>p</mi> </msub> <mo>/</mo> <mi>w</mi> </mrow> </math> values shown are <math display="inline"> <mrow> <msub> <mi>L</mi> <mi>p</mi> </msub> <mo>/</mo> <mi>w</mi> <mo>=</mo> <mn>10</mn> </mrow> </math> (□), <math display="inline"> <mrow> <msub> <mi>L</mi> <mi>p</mi> </msub> <mo>/</mo> <mi>w</mi> <mo>=</mo> <mn>12</mn> <mo>.</mo> <mn>5</mn> </mrow> </math> (▽), <math display="inline"> <mrow> <msub> <mi>L</mi> <mi>p</mi> </msub> <mo>/</mo> <mi>w</mi> <mo>=</mo> <mn>15</mn> </mrow> </math> (◯), <math display="inline"> <mrow> <msub> <mi>L</mi> <mi>p</mi> </msub> <mo>/</mo> <mi>w</mi> <mo>=</mo> <mn>17</mn> <mo>.</mo> <mn>5</mn> </mrow> </math> (⋄) and <math display="inline"> <mrow> <msub> <mi>L</mi> <mi>p</mi> </msub> <mo>/</mo> <mi>w</mi> <mo>=</mo> <mn>20</mn> </mrow> </math> (△). Different colors indicate different <math display="inline"> <mrow> <msub> <mi>A</mi> <mtext>eff</mtext> </msub> <mo>/</mo> <msub> <mi>D</mi> <mtext>eff</mtext> </msub> </mrow> </math> ratios: red (1), purple (1.5), brown (2), green (3) and blue (4). A power law fit of our data for <math display="inline"> <mrow> <mi>ξ</mi> <mo>&lt;</mo> <mn>0</mn> <mo>.</mo> <mn>1</mn> </mrow> </math> reveals an exponent of <math display="inline"> <mrow> <mn>0</mn> <mo>.</mo> <mn>559</mn> <mo>±</mo> <mn>0</mn> <mo>.</mo> <mn>016</mn> </mrow> </math>. All the data points satisfy the condition <math display="inline"> <mrow> <msub> <mi>D</mi> <mtext>eff</mtext> </msub> <mo>≤</mo> <msub> <mi>A</mi> <mtext>eff</mtext> </msub> <mo>≤</mo> <mn>2</mn> <msub> <mi>L</mi> <mi>p</mi> </msub> </mrow> </math>.</p>
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<p>Schematic illustration of genome mapping in nanochannel arrays [<a href="#B38-polymers-08-00079" class="html-bibr">38</a>]. The green color corresponds to the fluorescent dye inserted into the DNA backbone, and the red color corresponds to sequence-specific labels inserted into the DNA. The goal of the experiment is to construct a consensus genome map by assembling the measurements of many fragments of the genome that have been stretched in the nanochannel.</p>
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2627 KiB  
Article
Highly Active Copolymerization of Ethylene and N-Acetyl-O-(?-Alkenyl)-l-Tyrosine Ethyl Esters Catalyzed by Titanium Complex
by Jing Wang, Hongming Li, Runcong Zhang, Xianghui Shi, Jianjun Yi, Jian Wang, Qigu Huang and Wantai Yang
Polymers 2016, 8(3), 64; https://doi.org/10.3390/polym8030064 - 10 Mar 2016
Cited by 5 | Viewed by 8116
Abstract
A series of N-acetyl-O-(?-alkenyl)-l-tyrosine ethyl esters were synthesized by the reaction of vinyl bromides (4-bromo-1-butene, 6-bromo-1-hexene, 8-bromo-1-octene and 10-bromo-1-decene) with N-acetyl-l-tyrosine ethyl ester. 1H NMR, elemental analysis, FT-IR, and mass spectra were performed for [...] Read more.
A series of N-acetyl-O-(?-alkenyl)-l-tyrosine ethyl esters were synthesized by the reaction of vinyl bromides (4-bromo-1-butene, 6-bromo-1-hexene, 8-bromo-1-octene and 10-bromo-1-decene) with N-acetyl-l-tyrosine ethyl ester. 1H NMR, elemental analysis, FT-IR, and mass spectra were performed for these N-acetyl-O-(?-alkenyl)-l-tyrosine ethyl esters. The novel titanium complex can catalyze the copolymerization of ethylene and N-acetyl-O-(?-alkenyl)-l-tyrosine ethyl esters efficiently and the highest catalytic activity was up to 6.86 × 104 gP·(molTi)?1·h?1. The structures and properties of the obtained copolymers were characterized by FT-IR, (1H)13C NMR, GPC, DSC, and water contact angle. The results indicated that the obtained copolymers had a uniformly high average molecular weight of 2.85 × 105 g·mol?1 and a high incorporation ratio of N-acetyl-O-(but-3-enyl)-l-tyrosine ethyl ester of 2.65 mol % within the copolymer chain. The units of the comonomer were isolated within the copolymer chains. The insertion of the polar comonomer into a copolymer chain can effectively improve the hydrophilicity of a copolymer. Full article
(This article belongs to the Special Issue Metal-Mediated Polymer Synthesis)
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<p>Structure of titanium complex.</p>
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<p>Activity diagrams for the copolymerization of ethylene and different comonomers with titanium complex.</p>
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<p>FT-IR spectra of ethylene homopolymer (<b>A</b>, run 1 in <a href="#polymers-08-00064-t001" class="html-table">Table 1</a>) and ethylene/<span class="html-italic">N</span>-acetyl-<span class="html-italic">O</span>-(but-3-enyl)-<span class="html-small-caps">l</span>-tyrosine ethyl ester copolymer (<b>B</b>, run 3 in <a href="#polymers-08-00064-t001" class="html-table">Table 1</a>).</p>
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<p>DSC spectra (the second heating) of ethylene homopolymer (<b>A</b>, run 1 in <a href="#polymers-08-00064-t001" class="html-table">Table 1</a>) and ethylene/<span class="html-italic">N</span>-acetyl-<span class="html-italic">O</span>-(but-3-enyl)-<span class="html-small-caps">l</span>-tyrosine ethyl ester copolymers (<b>B</b>, run 3 in <a href="#polymers-08-00064-t001" class="html-table">Table 1</a>).</p>
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<p>High-temperature solution<sup>13</sup>C NMR spectra (<b>A</b>); and expandedview (δ = 10–40 ppm) (<b>B</b>) of the copolymer of ethylene/<span class="html-italic">N</span>-acetyl-<span class="html-italic">O</span>-(but-3-enyl)-<span class="html-small-caps">l</span>-tyrosine ethyl ester with comonomer insertion ratio 2.24 mol % from run 3 in <a href="#polymers-08-00064-t001" class="html-table">Table 1</a>.</p>
Full article ">Figure 6
<p><sup>1</sup>H NMR spectrum of the copolymer of ethylene/<span class="html-italic">N</span>-acetyl-<span class="html-italic">O</span>-(but-3-enyl)-<span class="html-small-caps">l</span>-tyrosine ethyl ester from run 3 in <a href="#polymers-08-00064-t002" class="html-table">Table 2</a>.</p>
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<p>Water contact angle of polyethylene (<b>A</b>, PE) from run 1 in <a href="#polymers-08-00064-t001" class="html-table">Table 1</a> ethylene/<span class="html-italic">N</span>-acetyl-<span class="html-italic">O</span>-(but-3-enyl)-<span class="html-small-caps">l</span>-tyrosine ethyl ester copolymers; (<b>B</b>) comonomer insertion ratio of 1.16 mol % from run 2 in <a href="#polymers-08-00064-t001" class="html-table">Table 1</a>; (<b>C</b>) comonomer insertion ratio of 2.24 mol % from run 3 in <a href="#polymers-08-00064-t001" class="html-table">Table 1</a>; (<b>D</b>) comonomer insertion ratio of 2.65 mol % from run 4 in <a href="#polymers-08-00064-t001" class="html-table">Table 1</a>).</p>
Full article ">Figure 8
<p>Copolymerization of ethylene and <span class="html-italic">N</span>-acetyl-<span class="html-italic">O</span>-(ω-alkenyl)-<span class="html-small-caps">l</span>-tyrosine ethyl esters. <span class="html-italic">n</span> = 1, 3, 5, 7.</p>
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1536 KiB  
Communication
Polylactide/Montmorillonite Hybrid Latex as a Barrier Coating for Paper Applications
by Davide Bandera, Veronika R. Meyer, David Prevost, Tanja Zimmermann and Luciano F. Boesel
Polymers 2016, 8(3), 75; https://doi.org/10.3390/polym8030075 - 4 Mar 2016
Cited by 19 | Viewed by 7440
Abstract
We developed a paper coating for the potential application in food packaging based on polylactide and montmorillonite. It is applied to the paper in the form of a stable, water-based latex with a solid content of 25–28 wt %. The latex is prepared [...] Read more.
We developed a paper coating for the potential application in food packaging based on polylactide and montmorillonite. It is applied to the paper in the form of a stable, water-based latex with a solid content of 25–28 wt %. The latex is prepared from a commercially available polylactide, surfactants, montmorillonite, a plasticizer, chloroform (to be removed later) and water by an emulsion/solvent evaporation procedure. This coating formulation is applied to the paper substrate by bar-coating, followed by hot-pressing at 150 °C. The coated papers achieved up to an 85% improvement in water vapor transmission rates when compared to the pristine papers. The coating latex is prepared from inexpensive materials and can be used for a solvent-free coating process. In addition, the ingredients of the latex are non-toxic; thus, the coated papers can be safely used for food packaging. Full article
(This article belongs to the Special Issue Biodegradable Polymers)
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<p>SEM image of a PLA/MMT hybrid latex.</p>
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<p>DSC curves (1st and 2nd heating) of PLA/MMT films after one and eight weeks of latex ageing. The curves were displaced vertically for easier reading.</p>
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<p>Top: SEM photo of a burst (due to high temperatures during sample preparation) PLA/MMT hybrid latex particle. <b>Bottom left</b>: EDX spectrum of the PLA region. <b>Bottom right</b>: EDX spectrum of the MMT region, which is only located at the original surface of the spherule.</p>
Full article ">Figure 4
<p>XRD spectra of clays and their mixtures with PLA. The d<sub>001</sub> are 1.1 nm (MMT), 2.1 nm (organically-modified MMT (OMMT)) and 3.1 nm (PLA/OMMT). The hybrid latex presents two diffraction peaks, similar to the d<sub>001</sub> of both clays (MMT and OMMT). The spectra were vertically adjusted to display similar count values.</p>
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4387 KiB  
Article
Fabrication of Alkoxyamine-Functionalized Magnetic Core-Shell Microspheres via Reflux Precipitation Polymerization for Glycopeptide Enrichment
by Meng Yu, Yi Di, Ying Zhang, Yuting Zhang, Jia Guo, Haojie Lu and Changchun Wang
Polymers 2016, 8(3), 74; https://doi.org/10.3390/polym8030074 - 4 Mar 2016
Cited by 11 | Viewed by 9105
Abstract
As a facile method to prepare hydrophilic polymeric microspheres, reflux precipitation polymerization has been widely used for preparation of polymer nanogels. In this article, we synthesized a phthalamide-protected N-aminooxy methyl acrylamide (NAMAm-p) for preparation of alkoxyamine-functionalized polymer composite microspheres via [...] Read more.
As a facile method to prepare hydrophilic polymeric microspheres, reflux precipitation polymerization has been widely used for preparation of polymer nanogels. In this article, we synthesized a phthalamide-protected N-aminooxy methyl acrylamide (NAMAm-p) for preparation of alkoxyamine-functionalized polymer composite microspheres via reflux precipitation polymerization. The particle size and functional group density of the composite microspheres could be adjusted by copolymerization with the second monomers, N-isopropyl acrylamide, acrylic acid or 2-hydroxyethyl methacrylate. The resultant microspheres have been characterized by TEM, FT-IR, TGA and DLS. The experimental results showed that the alkoxyamine group density of the microspheres could reach as high as 1.49 mmol/g, and these groups showed a great reactivity with ketone/aldehyde compounds. With the aid of magnetic core, the hybrid microspheres could capture and magnetically isolate glycopeptides from the digested mixture of glycopeptides and non-glycopeptides at a 1:100 molar ratio. After that, we applied the composite microspheres to profile the glycol-proteome of a normal human serum sample, 95 unique glycopeptides and 64 glycoproteins were identified with these enrichment substrates in a 5 ?L of serum sample. Full article
(This article belongs to the Special Issue Selected Papers from ASEPFPM2015)
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<p><sup>1</sup>H NMR spectra of (<b>a</b>) PNAMAm-<span class="html-italic">p</span>; (<b>b</b>) PNAMAm, and; (<b>c</b>) PNAMAm-m; GPC spectra of; (<b>d</b>) PNAMAm-<span class="html-italic">p</span> (PDI = 1.36), and; (<b>e</b>) PANAMAm (PDI = 1.37); (<b>f</b>) FT-IR spectra of (I) NAMAm-<span class="html-italic">p</span>; (II) PNAMAm-<span class="html-italic">p</span>; and (III) PNAMAm. The labelled peaks are (i) 1790 cm<sup>−1</sup>; (ii) 1735 cm<sup>−1</sup> and (iii) 1633 cm<sup>−1</sup>.</p>
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<p>TEM images of PNAMAm with different amount of MBA as crosslinker: (<b>a</b>) 20%; (<b>b</b>) 30%; (<b>c</b>) 40%; (<b>d</b>) 50%. The scale bar is 200 nm.</p>
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<p>TEM images of (<b>a</b>) MSP (magnetic supraparticle); (<b>b</b>) MSP@PNAMAm-<span class="html-italic">p</span>; (<b>c</b>) MSP@PNAMAm. The scale bar is 100 nm.</p>
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<p>(<b>a</b>) TGA and; (<b>b</b>) VSM curves of (i) MSP; (ii) MSP@PNAMAm-<span class="html-italic">p</span>; (iii) MSP@PNAMAm.</p>
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<p>TEM images of MSP@PNAMAm with different thickness of polymeric shell prepared with different solid contents of (<b>a</b>) 0.25%; (<b>b</b>) 0.375%; (<b>c</b>) 0.5%; (<b>d</b>) 0.625%, the scale bar is 100 nm; (<b>e</b>) DLS results of (i) MSP and MSP@PNAMAm prepared with different solid contents; (ii) 0.25%; (iii) 0.375%; (iv) 0.5%; (v) 0.625%.</p>
Full article ">Figure 6
<p>TEM images of (<b>a</b>) MSP@PNAMAm-<span class="html-italic">p</span>-<span class="html-italic">co</span>-PNIPAm; (<b>b</b>) MSP@PNAMAm-<span class="html-italic">p</span>-<span class="html-italic">co</span>-PAA; (<b>c</b>) MSP@PNAMAm-<span class="html-italic">p</span>-<span class="html-italic">co</span>-HEMA. The scale bar is 100 nm.</p>
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<p>SDS–PAGE analysis of the model glycoprotein proteins before and after treatment with MSP@PNAMAm-1 core-shell microspheres. M stands for protein marker; Lane 1 represents the RNase B; Lane 2 represents the supernatant after enrichment with MSP@PNAMAm-1; Lane 3 represents the released deglycoslated RNB after enrichment; Lane 4 represents the protein mixture of BSA, RNB(RNase B)and LYS(The amount of BSA:RNB:LYS = 1:1:1); Lane 5 represents the supernatant of the protein mixture after enrichment; Lane 6 represents the released deglycosylated RNB after enrichment.</p>
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<p>MALDI-TOF mass spectra of the tryptic digest mixture of ASF (asialofetuin) and MYO (myoglobin), the mole ratio of ASF:MYO = 1:10. (<b>a</b>) direct analysis; (<b>b</b>) analysis after enrichment by MSP@NAMAm-1 and deglycosylation by PNGase F; (<b>c</b>) analysis after enrichment by MSP@NAMAm-4 and deglycosylation by PNGase F. The symbols * denote the deglycosylated peptides.</p>
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<p>Synthesis of (<b>a</b>) monomer NAMAm-<span class="html-italic">p</span> and; (<b>b</b>) polymer PNAMAm.</p>
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<p>Preparation of the crosslinked PNAMAm micropsheres, MSP@PNAMAm core–shell microspheres, and the core-shell microspheres with varying functional groups (MSP@PNAMAm-R).</p>
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<p>Mechanism of glycoprotein and glycopeptide enrichment with magnetic core–shell microspheres (MSP@PNAMAm-1).</p>
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Article
Processing-Induced Inhomogeneity of Yield Stress in Polycarbonate Product and Its Influence on the Impact Behavior
by Yingjie Xu, Huan Lu, Tenglong Gao and Weihong Zhang
Polymers 2016, 8(3), 72; https://doi.org/10.3390/polym8030072 - 4 Mar 2016
Cited by 9 | Viewed by 6104
Abstract
In this study, an integrated methodology for impact analysis of polycarbonate (PC) product is proposed which incorporates the processing-induced inhomogeneity of yield stress. A previously developed model is extended to predict the inhomogeneous yield stress distribution along the specimen by using the thermal [...] Read more.
In this study, an integrated methodology for impact analysis of polycarbonate (PC) product is proposed which incorporates the processing-induced inhomogeneity of yield stress. A previously developed model is extended to predict the inhomogeneous yield stress distribution along the specimen by using the thermal history experienced during injection molding. A strain rate-dependent elastic-plastic model combining the processing-induced yield stress is applied to model the mechanical behavior of PC. Finite element simulation for notched Izod impact test is then conducted to analyze the impact behaviors of PC specimens with different thermal histories. Numerical results of the fracture energies are compared with experimental measurements. Full article
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<p>Illustration of the notched Izod impact test.</p>
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<p>Illustration of the integrative simulation framework.</p>
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<p>Finite element model of the specimen.</p>
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<p>Cooling profiles of material elements at the center cross-section.</p>
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<p>Distributions of yield stress within the center cross-section.</p>
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<p>Yield stress distributions of the specimens with different mold temperatures.</p>
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<p>Finite element models of the specimen and pendulum hammer.</p>
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<p>The distribution of plastic strain of the undamaged specimen with different model temperatures: (<b>a</b>) 60 °C; (<b>b</b>) 80 °C; (<b>c</b>) 120 °C.</p>
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<p>Internal energy variation of specimen with different mold temperatures during the impacting.</p>
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<p>Fracture process of the specimen with 60 °C mold temperature: (<b>a</b>) 1.54 ms; (<b>b</b>) 4 ms; (<b>c</b>) 5.8 ms; (<b>d</b>) 7.8 ms.</p>
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<p>Fracture process of the specimen with 60 °C mold temperature: (<b>a</b>) 1.54 ms; (<b>b</b>) 4 ms; (<b>c</b>) 5.8 ms; (<b>d</b>) 7.8 ms.</p>
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6678 KiB  
Article
Polyelectrolyte Threading through a Nanopore
by Pai-Yi Hsiao
Polymers 2016, 8(3), 73; https://doi.org/10.3390/polym8030073 - 3 Mar 2016
Cited by 12 | Viewed by 6821
Abstract
Threading charged polymers through a nanopore, driven by electric fields E, is investigated by means of Langevin dynamics simulations. The mean translocation time ? ? ? is shown to follow a scaling law N?, and the exponent ? increases monotonically from [...] Read more.
Threading charged polymers through a nanopore, driven by electric fields E, is investigated by means of Langevin dynamics simulations. The mean translocation time ? ? ? is shown to follow a scaling law N?, and the exponent ? increases monotonically from 1.16 (4) to 1.40 (3) with E. The result is double-checked by the calculation of mean square displacement of translocation coordinate, which asserts a scaling behavior t? (for t near ?) with ? complying with the relation ?? = 2. At a fixed chain length N, ??? displayed a reciprocal scaling behavior E?1 in the weak and also in the strong fields, connected by a transition E?1.64(5) in the intermediate fields. The variations of the radius of gyration of chain and the positions of chain end are monitored during a translocation process; far-from-equilibrium behaviors are observed when the driving field is strong. A strong field can strip off the condensed ions on the chain when it passes the pore. The total charges of condensed ions are hence decreased. The studies for the probability and density distributions reveal that the monomers in the trans-region are gathered near the wall and form a pancake-like density profile with a hump cloud over it in the strong fields, due to fast translocation. Full article
(This article belongs to the Collection Polyelectrolytes)
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<p>(<b>a</b>) Snapshot of a system of <math display="inline"> <mrow> <mi>N</mi> <mo>=</mo> <mn>128</mn> </mrow> </math>, where <span class="html-italic">N</span> refers to the number of monomers; (<b>b</b>) the membrane wall viewed from the trans side of the system. A pore is punched through the wall at the center. The gray beads represent the wall. The yellow, white, and green beads represent the monomers, cations, and anions, respectively.</p>
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<p>(<b>a</b>) Snapshot of a system of <math display="inline"> <mrow> <mi>N</mi> <mo>=</mo> <mn>128</mn> </mrow> </math>, where <span class="html-italic">N</span> refers to the number of monomers; (<b>b</b>) the membrane wall viewed from the trans side of the system. A pore is punched through the wall at the center. The gray beads represent the wall. The yellow, white, and green beads represent the monomers, cations, and anions, respectively.</p>
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<p>Snapshots of a typical translocation run for <math display="inline"> <mrow> <mi>N</mi> <mo>=</mo> <mn>128</mn> </mrow> </math> in <math display="inline"> <mrow> <mi>E</mi> <mo>=</mo> <mn>0.5</mn> </mrow> </math> at time <math display="inline"> <mrow> <mi>t</mi> <mo>=</mo> <mn>0.1</mn> <mi>τ</mi> </mrow> </math>, <math display="inline"> <mrow> <mn>0.4</mn> <mi>τ</mi> </mrow> </math>, <math display="inline"> <mrow> <mn>0.7</mn> <mi>τ</mi> </mrow> </math>, and <math display="inline"> <mrow> <mn>1.0</mn> <mi>τ</mi> </mrow> </math>. The color scheme is the same as described in <a href="#polymers-08-00073-f001" class="html-fig">Figure 1</a>.</p>
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<p>Mean translocation time <math display="inline"> <mrow> <mo stretchy="false">〈</mo> <mi>τ</mi> <mo stretchy="false">〉</mo> </mrow> </math> as a function of (<b>a</b>) chain length <span class="html-italic">N</span> at a given <span class="html-italic">E</span>, and (<b>b</b>) field strength <span class="html-italic">E</span> at a given <span class="html-italic">N</span>. The error bar is smaller than the data symbol.</p>
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<p><math display="inline"> <mrow> <mi>w</mi> <mo>/</mo> <mo stretchy="false">〈</mo> <mi>τ</mi> <mo stretchy="false">〉</mo> </mrow> </math> as a function of <span class="html-italic">E</span> for different <span class="html-italic">N</span>. (Inset) Probability distributions <math display="inline"> <mrow> <mi>P</mi> <mo>(</mo> <mi>τ</mi> <mo>)</mo> </mrow> </math> of translocation time at <math display="inline"> <mrow> <mi>E</mi> <mo>=</mo> <mn>4.0</mn> </mrow> </math>. The number <span class="html-italic">N</span> is indicated near the curve.</p>
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<p><math display="inline"> <mover accent="true"> <mi>t</mi> <mo>˜</mo> </mover> </math>-variation of the averaged <math display="inline"> <msub> <mi>R</mi> <mi mathvariant="normal">g</mi> </msub> </math> for the chain of <math display="inline"> <mrow> <mi>N</mi> <mo>=</mo> <mn>128</mn> </mrow> </math> in the cis-(I), the trans-(III), and the whole (tot) region at <math display="inline"> <mrow> <mi>E</mi> <mo>=</mo> <mn>0.2</mn> </mrow> </math>, <math display="inline"> <mrow> <mn>2.0</mn> </mrow> </math>, <math display="inline"> <mrow> <mn>4.0</mn> </mrow> </math>, <math display="inline"> <mrow> <mn>16.0</mn> </mrow> </math>, and <math display="inline"> <mrow> <mn>32.0</mn> </mrow> </math>. The gray-colored region denotes the distribution range of a curve.</p>
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<p>Averaged z-coordinates of chain end, <math display="inline"> <mrow> <mo stretchy="false">〈</mo> <msub> <mi>z</mi> <mn>1</mn> </msub> <mo stretchy="false">〉</mo> </mrow> </math> and <math display="inline"> <mrow> <mo stretchy="false">〈</mo> <msub> <mi>z</mi> <mi>N</mi> </msub> <mo stretchy="false">〉</mo> </mrow> </math>, and the difference <math display="inline"> <mrow> <mo stretchy="false">〈</mo> <msub> <mi>z</mi> <mn>1</mn> </msub> <mo>−</mo> <msub> <mi>z</mi> <mi>N</mi> </msub> <mo stretchy="false">〉</mo> </mrow> </math>, as a function of <math display="inline"> <mover accent="true"> <mi>t</mi> <mo>˜</mo> </mover> </math> at different field strengths for <math display="inline"> <mrow> <mi>N</mi> <mo>=</mo> <mn>128</mn> </mrow> </math>. The gray region denotes the distribution range of a curve.</p>
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<p><math display="inline"> <mover accent="true"> <mi>t</mi> <mo>˜</mo> </mover> </math>-variation of the averaged <math display="inline"> <msub> <mi>N</mi> <mi mathvariant="normal">m</mi> </msub> </math> for <math display="inline"> <mrow> <mi>N</mi> <mo>=</mo> <mn>128</mn> </mrow> </math> in the cis-region (I); the pore-region (II); and the trans-region (III). The field strength <span class="html-italic">E</span> is indicated in the figure.</p>
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<p>MSD <math display="inline"> <mrow> <mo stretchy="false">〈</mo> <msup> <mrow> <mo>(</mo> <msub> <mi>N</mi> <mrow> <mi mathvariant="normal">m</mi> <mo>,</mo> <mi>III</mi> </mrow> </msub> <mrow> <mo>(</mo> <mi>t</mi> <mo>)</mo> </mrow> <mo>−</mo> <msub> <mi>N</mi> <mrow> <mi mathvariant="normal">m</mi> <mo>,</mo> <mi>III</mi> </mrow> </msub> <mrow> <mo>(</mo> <mn>0</mn> <mo>)</mo> </mrow> <mo>)</mo> </mrow> <mn>2</mn> </msup> <mo stretchy="false">〉</mo> </mrow> </math> at <math display="inline"> <mrow> <mi>E</mi> <mo>=</mo> <mn>0.5</mn> </mrow> </math>, plotted with the normalized time <math display="inline"> <mover accent="true"> <mi>t</mi> <mo>˜</mo> </mover> </math>, for <math display="inline"> <mrow> <mi>N</mi> <mo>=</mo> <mn>128</mn> </mrow> </math>, 256, and 384. (Inset) Exponent <span class="html-italic">β</span> vs. <span class="html-italic">E</span> for different <span class="html-italic">N</span>.</p>
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<p>(Left) Variations of the average number of condensed counterions <math display="inline"> <msubsup> <mi>N</mi> <mrow> <mi mathvariant="normal">c</mi> </mrow> <mrow> <mo>(</mo> <mo>+</mo> <mn>1</mn> <mo>)</mo> </mrow> </msubsup> </math> in the cis-region (I), the pore-region (II), and the trans-region (III) for <math display="inline"> <mrow> <mi>N</mi> <mo>=</mo> <mn>128</mn> </mrow> </math>. (Right) Fraction of charges neutralized on the chain, <math display="inline"> <mrow> <mo stretchy="false">〈</mo> <mo>|</mo> <msub> <mi>Q</mi> <mi mathvariant="normal">c</mi> </msub> <mo>/</mo> <mi>N</mi> <mi>e</mi> <mo>|</mo> <mo stretchy="false">〉</mo> </mrow> </math>, during a translocation process. The field strength <span class="html-italic">E</span> is indicated in the legend.</p>
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<p>Probability distributions in the <span class="html-italic">z</span>-direction for (<b>a</b>) monomers; (<b>b</b>) counterions; and (<b>c</b>) coions; at <math display="inline"> <mrow> <mi>E</mi> <mo>=</mo> <mn>0.2</mn> </mrow> </math>, <math display="inline"> <mrow> <mn>2.0</mn> </mrow> </math>, and <math display="inline"> <mrow> <mn>16.0</mn> </mrow> </math> (<math display="inline"> <mrow> <mi>N</mi> <mo>=</mo> <mn>128</mn> </mrow> </math>). The gray color denotes the <span class="html-italic">z</span>-location of the pore. The value given near a curve is the normalized time <math display="inline"> <mover accent="true"> <mi>t</mi> <mo>˜</mo> </mover> </math> at which the probability density was calculated. For clarity, the curves have been shifted upward with a fixed step value, one curve after the others.</p>
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<p>Density distributions of monomer, viewed along <span class="html-italic">x</span>-axis, at (Left) <math display="inline"> <mrow> <mi>E</mi> <mo>=</mo> <mn>0.2</mn> </mrow> </math>, (Middle) <math display="inline"> <mrow> <mi>E</mi> <mo>=</mo> <mn>2.0</mn> </mrow> </math>, and (Right) <math display="inline"> <mrow> <mi>E</mi> <mo>=</mo> <mn>16.0</mn> </mrow> </math>. The chain length is <math display="inline"> <mrow> <mi>N</mi> <mo>=</mo> <mn>128</mn> </mrow> </math>. The value of <math display="inline"> <mover accent="true"> <mi>t</mi> <mo>˜</mo> </mover> </math> is indicated in the figure.</p>
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5619 KiB  
Article
Near Surface Mounted Composites for Flexural Strengthening of Reinforced Concrete Beams
by Md. Akter Hosen, Mohd Zamin Jumaat, Ubagaram Johnson Alengaram, A. B. M. Saiful Islam and Huzaifa Bin Hashim
Polymers 2016, 8(3), 67; https://doi.org/10.3390/polym8030067 - 3 Mar 2016
Cited by 35 | Viewed by 10931
Abstract
Existing structural components require strengthening after a certain period of time due to increases in service loads, errors in design, mechanical damage, and the need to extend the service period. Externally-bonded reinforcement (EBR) and near-surface mounted (NSM) reinforcement are two preferred strengthening approach. [...] Read more.
Existing structural components require strengthening after a certain period of time due to increases in service loads, errors in design, mechanical damage, and the need to extend the service period. Externally-bonded reinforcement (EBR) and near-surface mounted (NSM) reinforcement are two preferred strengthening approach. This paper presents a NSM technique incorporating NSM composites, namely steel and carbon fiber-reinforced polymer (CFRP) bars, as reinforcement. Experimental and analytical studies carried out to explore the performance of reinforced concrete (RC) members strengthened with the NSM composites. Analytical models were developed in predicting the maximum crack spacing and width, concrete cover separation failure loads, and deflection. A four-point bending test was applied on beams strengthened with different types and ratios of NSM reinforcement. The failure characteristics, yield, and ultimate capacities, deflection, strain, and cracking behavior of the beams were evaluated based on the experimental output. The test results indicate an increase in the cracking load of 69% and an increase in the ultimate load of 92% compared with the control beam. The predicted result from the analytical model shows good agreement with the experimental result, which ensures the competent implementation of the present NSM-steel and CFRP technique. Full article
(This article belongs to the Collection Fiber-Reinforced Polymer Composites in Structural Engineering)
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<p>Beam specimen details.</p>
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<p>Experimental setup.</p>
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<p>Load <span class="html-italic">vs.</span> deflection at midspan for all beams.</p>
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<p>Load <span class="html-italic">vs.</span> crack width for all beams.</p>
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<p>Modes of failure of all beams. (<b>a</b>) CB; (<b>b</b>) N-1; (<b>c</b>) N-2; (<b>d</b>) N-3; (<b>e</b>) N-4; and (<b>f</b>) N-5.</p>
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<p>Load <span class="html-italic">vs.</span> compressive strain of concrete at midspan for all beams.</p>
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<p>Load <span class="html-italic">vs.</span> tensile strain in main reinforcements at midspan for all beams.</p>
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<p>Digital extensometer for measure the sectional strain.</p>
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<p>Sectional strain variation at mid-span during loading on strengthen beams. (<b>a</b>) CB; (<b>b</b>) N1; (<b>c</b>) N2; (<b>d</b>) N3; (<b>e</b>) N4; and (<b>f</b>) N5.</p>
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<p>Sectional strain variation at mid-span during loading on strengthen beams. (<b>a</b>) CB; (<b>b</b>) N1; (<b>c</b>) N2; (<b>d</b>) N3; (<b>e</b>) N4; and (<b>f</b>) N5.</p>
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<p>The effect of NSM reinforcement amount.</p>
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<p>The effect of type of NSM reinforcement.</p>
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<p>The effect of the number of grooves.</p>
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<p>Distribution of stress in the NSM bars and concrete between the last two adjacent cracks at the end of the NSM bars.</p>
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<p>Comparison of experimental and predicted failure loads.</p>
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<p>Comparison of experimental and predicted deflection.</p>
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<p>Comparison of experimental and predicted crack spacing.</p>
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<p>Comparison of experimental and predicted crack width.</p>
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Review
Biopolymeric Mucin and Synthetic Polymer Analogs: Their Structure, Function and Role in Biomedical Applications
by Sundar P. Authimoolam and Thomas D. Dziubla
Polymers 2016, 8(3), 71; https://doi.org/10.3390/polym8030071 - 2 Mar 2016
Cited by 64 | Viewed by 21809
Abstract
Mucin networks are viscoelastic fibrillar aggregates formed through the complex self-association of biopolymeric glycoprotein chains. The networks form a lubricious, hydrated protective shield along epithelial regions within the human body. The critical role played by mucin networks in impacting the transport properties of [...] Read more.
Mucin networks are viscoelastic fibrillar aggregates formed through the complex self-association of biopolymeric glycoprotein chains. The networks form a lubricious, hydrated protective shield along epithelial regions within the human body. The critical role played by mucin networks in impacting the transport properties of biofunctional molecules (e.g., biogenic molecules, probes, nanoparticles), and its effect on bioavailability are well described in the literature. An alternate perspective is provided in this paper, presenting mucin’s complex network structure, and its interdependent functional characteristics in human physiology. We highlight the recent advances that were achieved through the use of mucin in diverse areas of bioengineering applications (e.g., drug delivery, biomedical devices and tissue engineering). Mucin network formation is a highly complex process, driven by wide variety of molecular interactions, and the network possess structural and chemical variations, posing a great challenge to understand mucin’s bulk behavior. Through this review, the prospective potential of polymer based analogs to serve as mucin mimic is suggested. These analog systems, apart from functioning as an artificial model, reducing the current dependency on animal models, can aid in furthering our fundamental understanding of such complex structures. Full article
(This article belongs to the Special Issue Polymers Applied in Tissue Engineering)
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<p>Mucin glycoprotein’s molecular properties, and its network formation ability. (<b>a</b>) A simplified scheme shows the composition of mucin glycoproteins, its subunit, monomer, and dimer; (<b>b</b>) Progression of higher order complexation of mucin glycoproteins resulting in the formation of a mucin network over oral mucosal surface. This scheme demonstrates the progression of high-order complexation process, which results in formation of mucin aggregates. Mucin aggregates invariably contain two-distinct zones: the more intact adherent mucin layers, and loosely-held (expanded) mucin layers of high free-volume. The illustrated scheme is adapted from References [<a href="#B22-polymers-08-00071" class="html-bibr">22</a>,<a href="#B23-polymers-08-00071" class="html-bibr">23</a>,<a href="#B24-polymers-08-00071" class="html-bibr">24</a>].</p>
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<p>Mucin network thickness varies based upon its physiological location and role. Based on findings from References [<a href="#B39-polymers-08-00071" class="html-bibr">39</a>,<a href="#B40-polymers-08-00071" class="html-bibr">40</a>,<a href="#B41-polymers-08-00071" class="html-bibr">41</a>]. Inset figure shows cryo-SEM imaging of pulmonary mucin, demonstrating heterogeneous mesh size distribution. Reprinted with permission from Reference [<a href="#B42-polymers-08-00071" class="html-bibr">42</a>]. Copyright © 2009, National Academy of Sciences.</p>
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<p>Illustrative scheme highlighting mucin network prevalence and its key functional properties across different regions within human body. The respiratory-gastrointestinal figure outline was taken from Reference [<a href="#B46-polymers-08-00071" class="html-bibr">46</a>].</p>
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<p>(Left) CMP at different stages of pregnancy (<b>a</b>) (left to right) at 20th day, 5 weeks, 2-1/2 months, and last week of pregnancy. Cervical mucin network density increases progressively during the gestation period, and forms a more compact interconnected fibrillar networks. The mucus functions as a selectively permeable plug that blocks pathogens and allows nutrients and growth factor to transport. Reprinted with permission from [<a href="#B80-polymers-08-00071" class="html-bibr">80</a>]. Copyright © 2011, John Wiley &amp; Sons, Inc.; (<b>b</b>) Figure showing bulk structure of cervical mucus plug discharged during labor. Reprinted with permission from [<a href="#B77-polymers-08-00071" class="html-bibr">77</a>]. Copyright © 2010, John Wiley &amp; Sons, Inc.</p>
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<p>Schematic of mucin network’s (cervical region) ability to impact transport properties of various biogenic materials, synthetic structures or pathogens across its physical barrier. Figure also illustrates the mucopenetration effects, which can arise as a result of differences in network mesh size, or its adhesive interactions with transport molecules. Figure was adapted from References [<a href="#B105-polymers-08-00071" class="html-bibr">105</a>,<a href="#B106-polymers-08-00071" class="html-bibr">106</a>].</p>
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<p>A comparison of native cell bound mucin coats with biomimetic carbon nanotubes possessing cell bound mucin coats. The bioengineered carbon nanotubes mimics the native cell bound mucin functional property, and can be used in preventing non-specific protein binding (antibiofouling), or immobilizing specific functional molecules to CNT via specific biomolecular recognition with mucin chains, or as coatings for developing stable dispersions. Reprinted with permission from Reference [<a href="#B148-polymers-08-00071" class="html-bibr">148</a>]. Copyright © 2004, Wiley-VCH Verlag GmbH &amp; Co. KGaA, Weinheim.</p>
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<p>Glass-bound glycopolymer based hydrogels used as a model mucin network mimics in recreating the mucosal surface interfacial property. Scanning electron micrographs clearly shows highly porous structure of the hydrogels, these structures mimics membrane-bound mucin networks that were formed from glycoprotein chains. Reprinted with permission from Reference [<a href="#B201-polymers-08-00071" class="html-bibr">201</a>]. Copyright © 2015, The Royal Society of Chemistry.</p>
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<p>Synthetically derived mucin mimetic system formed from controlled Layer-by-layer (LBL) deposition of polymeric filomicelle, and its structural and functional relevance to natural mucin networks. (<b>a</b>) Overall simplified scheme showing natural mucin networks and biomimetic synthetic counterpart (filomicelle networks); (<b>b</b>) Fluorescence microscopic visualization of curcumin encapsulated biotinylated filomicelle. Similar to glycoprotein chains in natural systems, the filamentous micelles forms key building block in formation of synthetic networks; (<b>c</b>) Morphological relevance of natural mucin structures with synthetic mucin networks formed from filomicelle LBL depositions; (<b>d</b>) Controlled thickness growth in synthetic mucin networks can be achieved, by adjusting the number of LBL depositions. Figure shows during filomicelle network, where even with relatively lesser no. of micelle LBL additions (~7), network with significant barrier thickness (~4 um) is achieved; (<b>e</b>) Filomicelle networks mimicked the nanoporous mesh size (average range ~110–340 nm) observable in the natural mucin; (<b>f</b>) Synthetic mucin networks formed from PEG-based diblock copolymers displayed excellent surface hydration tendency. With synthetic mucin network depositions, the hydrophobic polystyrene (model synthetic interface) translated into a more hydrophilic, hydrating surface, this can be observed with lowering of contact angle from gonimetry study. Reprinted with permission from Reference [<a href="#B84-polymers-08-00071" class="html-bibr">84</a>] (Copyright 2015, Wiley-VCH Verlag GmbH &amp; Co. KGaA, Weinheim), and [<a href="#B15-polymers-08-00071" class="html-bibr">15</a>] (Copyright © 2014, American Chemical Society).</p>
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<p>Potential synthetic mucin analogs as a tunable drug releasing network (<b>a</b>) Scheme showing use of filomicelle networks formed from crosslinking of biotinylated micelles with streptavidin, as a synthetic mucin analog. And, modification of those analog systems using polymeric capping barriers formed atop synthetic mucin. Capping barriers are formed from crosslinking of biotinylated polymer poly(acrylic acid) with streptavidin via LBL depositions; (<b>b</b>) Figure shows modification of drug release capacity from synthetic mucin systems for localized oral drug delivery applications. By developing polymeric capping barrier, the drug release from micelle-based network was greatly hindered, suggesting its capable potential to serve as tunable release systems for mucosal specific regenerative applications such as xerostomia and oral mucositis. Reprinted with permission from Reference [<a href="#B84-polymers-08-00071" class="html-bibr">84</a>]. Copyright © 2015, Wiley-VCH Verlag GmbH &amp; Co. KGaA, Weinheim.</p>
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142 KiB  
Editorial
Organic Photovoltaics: More than Ever, an Interdisciplinary Field
by Laure Biniek and Christian B. Nielsen
Polymers 2016, 8(3), 70; https://doi.org/10.3390/polym8030070 - 2 Mar 2016
Cited by 3 | Viewed by 4680
Abstract
Despite the growing interest and rapid advancement of alternative photovoltaic (PV) technologies such as perovskite based PV devices, we still believe that organic photovoltaic (OPV) devices have a significant potential for stable, low-cost solar power generation. [...] Full article
(This article belongs to the Special Issue Organic Photovoltaics)
759 KiB  
Article
ICAR ATRP of Acrylonitrile under Ambient and High Pressure
by Zhicheng Huang, Jing Chen, Lifen Zhang, Zhenping Cheng and Xiulin Zhu
Polymers 2016, 8(3), 59; https://doi.org/10.3390/polym8030059 - 2 Mar 2016
Cited by 25 | Viewed by 7990
Abstract
It is well known that well-defined polyacrylonitrile (PAN) with high molecular weight (Mw > 106 g·mol?1) is an excellent precursor for high performance carbon fiber. In this work, a strategy for initiators for a continuous activator regeneration atom transfer [...] Read more.
It is well known that well-defined polyacrylonitrile (PAN) with high molecular weight (Mw > 106 g·mol?1) is an excellent precursor for high performance carbon fiber. In this work, a strategy for initiators for a continuous activator regeneration atom transfer radical polymerization (ICAR ATRP) system for acrylonitrile (AN) was firstly established by using CuCl2·2H2O as the catalyst and 2,2?-azobis(2-methylpropionitrile) (AIBN) as the thermal initiator in the presence of ppm level catalyst under ambient and high pressure (5 kbar). The effect of catalyst concentration and polymerization temperature on the polymerization behaviors was investigated. It is important that PAN with ultrahigh viscosity and average molecular weight (M? = 1,034,500 g·mol?1) could be synthesized within 2 h under high pressure. Full article
(This article belongs to the Special Issue Controlled/Living Radical Polymerization)
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<p>ln([M]<sub>0</sub>/[M]) as a function of time (<b>a</b>) and number-average molecular weight and molecular weight distribution (<span class="html-italic">M</span><sub>w</sub>/<span class="html-italic">M</span><sub>n</sub>) <span class="html-italic">versus</span> monomer conversion (<b>b</b>) for the initiators for a continuous activator regeneration atom transfer radical polymerization (ICAR ATRP) of acrylonitrile (AN) under ambient pressure; (<b>c</b>) The <sup>1</sup>H NMR spectrum of polyacrylonitrile (PAN) (<span class="html-italic">M</span><sub>n,GPC</sub> = 28,400 g·mol<sup>−1</sup>, <span class="html-italic">M</span><sub>w</sub>/<span class="html-italic">M</span><sub>n</sub> = 1.06, conversion = 40.8%) with dimethylsulfoxide (DMSO) as the solvent and tetramethylsilane (TMS) as the internal standard. Polymerization conditions: [AN]<sub>0</sub>:[BMPB<sub>2</sub>]<sub>0</sub>:[CuCl<sub>2</sub>·2H<sub>2</sub>O]<sub>0</sub>:[TPMA]<sub>0</sub>:[AIBN]<sub>0</sub> = 500:1:0.01:0.1:0.2, <span class="html-italic">V</span><sub>AN</sub> = 1.5 mL, <span class="html-italic">V</span><sub>DMSO</sub> = 3.0 mL, <span class="html-italic">T</span> = 30 °C under ambient pressure.</p>
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<p>The proposed mechanism of initiators for continuous activator regeneration atom transfer radical polymerization (ICAR ATRP).</p>
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<p>The structure of chemicals used in this work.</p>
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Article
Homo- and Copolymerization of Ethylene and Norbornene with Anilido–Imine Chromium Catalysts
by Lixia Pei, Yong Tang and Haiyang Gao
Polymers 2016, 8(3), 69; https://doi.org/10.3390/polym8030069 - 1 Mar 2016
Cited by 16 | Viewed by 7466
Abstract
A series of anilido–imine chromium complexes have been used as precursors to catalyze homo- and copolymerization of ethylene and norbornene. The chromium complexes activated with methylalumoxane (MAO) exhibit good activities for homopolymerization of ethylene (E) to produce linear polyethylene and moderate activities for [...] Read more.
A series of anilido–imine chromium complexes have been used as precursors to catalyze homo- and copolymerization of ethylene and norbornene. The chromium complexes activated with methylalumoxane (MAO) exhibit good activities for homopolymerization of ethylene (E) to produce linear polyethylene and moderate activities for norbornene (N) polymerization to afford vinyl-type polynorbornene. Ethylene–norbornene copolymers with high incorporation of norbornene can be also produced by these catalysts. 13C NMR and differential scanning calorimetry (DSC) analyses show that the copolymers are random products, and –NNN– and –EEE– units can be observed in the microstructure of the copolymers. Full article
(This article belongs to the Special Issue Metal-Mediated Polymer Synthesis)
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Graphical abstract

Graphical abstract
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<p><sup>13</sup>C NMR spectra of PE obtained by <b>1</b>/MAO at different temperatures.</p>
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<p>DSC curves of PE obtained by <b>1</b>/MAO at different temperatures.</p>
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<p>IR (<b>A</b>) and <sup>1</sup>H NMR (<b>B</b>) spectroscopy of the polynorbornene (TMS: tetramethylsilane).</p>
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<p><sup>13</sup>C NMR spectra of E–N copolymers obtained at different ethylene pressures (up: 20 atm (entry 4), down: 0.5 atm (entry 7)).</p>
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<p>DSC curves of E–N copolymers with different norbornene incorporations.</p>
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<p>WAXD curves of polymers.</p>
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<p>Synthesis of anilido–imino chromium complexes <b>1–3.</b></p>
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