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Battery Chargers and Management for Electric Vehicles

A special issue of Electronics (ISSN 2079-9292). This special issue belongs to the section "Electrical and Autonomous Vehicles".

Deadline for manuscript submissions: closed (30 June 2022) | Viewed by 60441

Special Issue Editor


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Faculty of Science and Technology Electrical Engineering Department, Universidade Nova de Lisboa, 1099-085 Lisbon, Portugal
Interests: HF and resonant power converters; wireless energy transfer to electric vehicles; energy management and storage in DC grids; efficient micro-power devices; energy harvesting; auto-supplied sensors
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Special Issue Information

Dear Colleagues,

The battery, a storage device for electrical energy, is by nature mostly chemical. The charging and discharging, however, is mostly electrical, with some chemical versions like the flow battery. One of the most important battery applications is that of the electric vehicle (EV). It is also the most expensive and problematic building block of the EV, progressing daily but remaining a fragile and sensitive yet expensive block to be managed. The cells of each battery are numerous, and the inter-cell management is already a problem in terms of aging, reliability, measurement, and prognostics. This is the case even in small devices like a laptop computers. In the EV, the problem is more serious as the propulsion battery must supply and absorb high power peak values that were unthinkable years ago. At the same time, the characteristics of the battery define the total available energy (autonomy) of the vehicle. The cost and weight of a 100 kWh EV battery are notably higher than the 55-litre fuel tank, and this brought to the market the hybrid EV (HEV) and its rechargeable plug-in (PHEV) version. These HEVs do not need the complete propulsion energy to be stored in their batteries as they also boast an internal combustion motor. Fast charging is another bottleneck of the management of the vehicle, keeping in mind the chemical nature of the battery. Even if the battery producer allows 20C speed, the client should keep the velocity to something like 1–2C if they want the battery to live longer and remain healthy. The reasons are mostly chemical and thermal, but some limitations come from the cabling: the highest current that a flexible cable is going to conduct is less than 500–600A. The problem is the flexibility of the charging cable. For this reason, many companies are looking at high frequency wireless energy transfer for the charging.

The topics of interest include but are not limited to the following:

  • new battery types with new types of charging;
  • control of the battery cells charge distribution;
  • state-of-charge (SoC) and state-of-health (SoH) determination;
  • wired and wireless energy transfer for battery charging;
  • power converters for regulating the charge of the battery;
  • bi-directional charging, especially for braking energy absorption;
  • wireless data transfer for the safe charging of batteries;
  • chargers applying solar energy;
  • general control system of the car and the charging control;
  • on-line charging (during the EV movement);
  • three-phase bi-directional convertor for propulsion/charging of EVs;
  • reliability of the batteries and chargers: parallel and series probability;
  • general influence of EV charging to the common grid;
  • how to recycle or continue using the old batteries;
  • mid-voltage “transformer-less” converters for charging EVs, future DC grids;
  • environmental conditions during charging and electromagnetic effects;
  • hydrogen based EVs and hydrogen grids;
  • other similar topics.

Prof. Dr. Stanimir Valtchev
Guest Editor

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Published Papers (7 papers)

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18 pages, 4182 KiB  
Article
A Quasi-Z-Source-Based Inductive Power Transfer System for Constant Current/Constant Voltage Charging Applications
by Vincenzo Castiglia, Nicola Campagna, Rosario Miceli, Fabio Viola and Frede Blaabjerg
Electronics 2021, 10(23), 2900; https://doi.org/10.3390/electronics10232900 - 24 Nov 2021
Cited by 3 | Viewed by 2195
Abstract
This article proposes a quasi-Z-source (qZS)-based Inductive Power Transfer (IPT) system for Electric Vehicles (EVs) charging applications. The IPT systems use the magnetic field to transfer power between two coils wirelessly, achieving improved reliability, safety and less environmental impact. Compared to the conventional [...] Read more.
This article proposes a quasi-Z-source (qZS)-based Inductive Power Transfer (IPT) system for Electric Vehicles (EVs) charging applications. The IPT systems use the magnetic field to transfer power between two coils wirelessly, achieving improved reliability, safety and less environmental impact. Compared to the conventional IPT system, the proposed qZS-IPT system simultaneously achieves DC/DC regulation and DC/AC conversion through a single-stage conversion, thus lowering the cost and complexity of the system. Moreover, the reliability of the system is improved thanks to the qZS network shoot-though immunity and the reduced number of switches. To ensure the battery efficient charging and long service life, the constant current/constant voltage (CC/CV) method is considered. With the proposed innovative modulation scheme, the qZS can easily change between buck and boost modes, respectively, lowering or increasing the secondary side current. A theoretical analysis is presented for system design. Simulation results based on a 25 kW (200 V/135 A) low duty EV charger are presented to verify the effectiveness of the proposed scheme. Experimental tests are performed on a 150 W scale-down prototype to validate the analysis and demonstrate the effectiveness of the proposed qZS-IPT system for CC/CV chargers. Full article
(This article belongs to the Special Issue Battery Chargers and Management for Electric Vehicles)
Show Figures

Figure 1

Figure 1
<p>IPT system architecture for EV charging applications.</p>
Full article ">Figure 2
<p>Circuit schematic of the qZS-based IPT system.</p>
Full article ">Figure 3
<p>Circuit schematic of the qZS-IPT system in different states. (<b>a</b>) Active state <math display="inline"><semantics> <msub> <mi>S</mi> <mn>1</mn> </msub> </semantics></math>, <math display="inline"><semantics> <msub> <mi>S</mi> <mn>4</mn> </msub> </semantics></math>. (<b>b</b>) Active state <math display="inline"><semantics> <msub> <mi>S</mi> <mn>2</mn> </msub> </semantics></math>, <math display="inline"><semantics> <msub> <mi>S</mi> <mn>3</mn> </msub> </semantics></math>. (<b>c</b>) Zero state <math display="inline"><semantics> <msub> <mi>S</mi> <mn>1</mn> </msub> </semantics></math>, <math display="inline"><semantics> <msub> <mi>S</mi> <mn>2</mn> </msub> </semantics></math>. (<b>d</b>) Zero state <math display="inline"><semantics> <msub> <mi>S</mi> <mn>3</mn> </msub> </semantics></math>, <math display="inline"><semantics> <msub> <mi>S</mi> <mn>4</mn> </msub> </semantics></math>. (<b>e</b>) Shoot-through state.</p>
Full article ">Figure 3 Cont.
<p>Circuit schematic of the qZS-IPT system in different states. (<b>a</b>) Active state <math display="inline"><semantics> <msub> <mi>S</mi> <mn>1</mn> </msub> </semantics></math>, <math display="inline"><semantics> <msub> <mi>S</mi> <mn>4</mn> </msub> </semantics></math>. (<b>b</b>) Active state <math display="inline"><semantics> <msub> <mi>S</mi> <mn>2</mn> </msub> </semantics></math>, <math display="inline"><semantics> <msub> <mi>S</mi> <mn>3</mn> </msub> </semantics></math>. (<b>c</b>) Zero state <math display="inline"><semantics> <msub> <mi>S</mi> <mn>1</mn> </msub> </semantics></math>, <math display="inline"><semantics> <msub> <mi>S</mi> <mn>2</mn> </msub> </semantics></math>. (<b>d</b>) Zero state <math display="inline"><semantics> <msub> <mi>S</mi> <mn>3</mn> </msub> </semantics></math>, <math display="inline"><semantics> <msub> <mi>S</mi> <mn>4</mn> </msub> </semantics></math>. (<b>e</b>) Shoot-through state.</p>
Full article ">Figure 4
<p>Combinatorial logic circuit for the proposed modulator.</p>
Full article ">Figure 5
<p>Closed—loop control scheme for CC/CV charging implementation.</p>
Full article ">Figure 6
<p>Steady—state voltage and current waveforms for (<b>a</b>) boost mode operation (<math display="inline"><semantics> <mrow> <mi>D</mi> <mo>=</mo> <mn>0.18</mn> </mrow> </semantics></math>) and (<b>b</b>) buck mode operation (<math display="inline"><semantics> <mrow> <mi>D</mi> <mo>=</mo> <mo>−</mo> <mn>0.57</mn> </mrow> </semantics></math>).</p>
Full article ">Figure 7
<p>Setup of the laboratory prototype for the proposed qZS-IPT system.</p>
Full article ">Figure 8
<p>Experimental waveforms of the qZS-IPT system in boost mode with <math display="inline"><semantics> <mrow> <mi>D</mi> <mo>=</mo> <mn>0.1</mn> </mrow> </semantics></math>. (<b>a</b>) Input voltage <math display="inline"><semantics> <msub> <mi>V</mi> <mrow> <mi>i</mi> <mi>n</mi> </mrow> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>i</mi> <mn>1</mn> </msub> </semantics></math>, DC-link voltage <math display="inline"><semantics> <msub> <mi>v</mi> <mrow> <mi>d</mi> <mi>c</mi> </mrow> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>i</mi> <mrow> <mi>d</mi> <mi>c</mi> </mrow> </msub> </semantics></math>. (<b>b</b>) primary side voltage <math display="inline"><semantics> <msub> <mi>v</mi> <mi>p</mi> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>i</mi> <mi>p</mi> </msub> </semantics></math>, secondary side voltage <math display="inline"><semantics> <msub> <mi>v</mi> <mi>s</mi> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>i</mi> <mi>s</mi> </msub> </semantics></math>. (<b>c</b>) Input voltage <math display="inline"><semantics> <msub> <mi>V</mi> <mrow> <mi>i</mi> <mi>n</mi> </mrow> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>i</mi> <mn>1</mn> </msub> </semantics></math>, output voltage <math display="inline"><semantics> <msub> <mi>V</mi> <mi>o</mi> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>I</mi> <mi>o</mi> </msub> </semantics></math>.</p>
Full article ">Figure 8 Cont.
<p>Experimental waveforms of the qZS-IPT system in boost mode with <math display="inline"><semantics> <mrow> <mi>D</mi> <mo>=</mo> <mn>0.1</mn> </mrow> </semantics></math>. (<b>a</b>) Input voltage <math display="inline"><semantics> <msub> <mi>V</mi> <mrow> <mi>i</mi> <mi>n</mi> </mrow> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>i</mi> <mn>1</mn> </msub> </semantics></math>, DC-link voltage <math display="inline"><semantics> <msub> <mi>v</mi> <mrow> <mi>d</mi> <mi>c</mi> </mrow> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>i</mi> <mrow> <mi>d</mi> <mi>c</mi> </mrow> </msub> </semantics></math>. (<b>b</b>) primary side voltage <math display="inline"><semantics> <msub> <mi>v</mi> <mi>p</mi> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>i</mi> <mi>p</mi> </msub> </semantics></math>, secondary side voltage <math display="inline"><semantics> <msub> <mi>v</mi> <mi>s</mi> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>i</mi> <mi>s</mi> </msub> </semantics></math>. (<b>c</b>) Input voltage <math display="inline"><semantics> <msub> <mi>V</mi> <mrow> <mi>i</mi> <mi>n</mi> </mrow> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>i</mi> <mn>1</mn> </msub> </semantics></math>, output voltage <math display="inline"><semantics> <msub> <mi>V</mi> <mi>o</mi> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>I</mi> <mi>o</mi> </msub> </semantics></math>.</p>
Full article ">Figure 9
<p>Experimental waveforms of the qZS-IPT system in boost mode with <math display="inline"><semantics> <mrow> <mi>D</mi> <mo>=</mo> <mn>0.2</mn> </mrow> </semantics></math>. (<b>a</b>) Input voltage <math display="inline"><semantics> <msub> <mi>V</mi> <mrow> <mi>i</mi> <mi>n</mi> </mrow> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>i</mi> <mn>1</mn> </msub> </semantics></math>, DC-link voltage <math display="inline"><semantics> <msub> <mi>v</mi> <mrow> <mi>d</mi> <mi>c</mi> </mrow> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>i</mi> <mrow> <mi>d</mi> <mi>c</mi> </mrow> </msub> </semantics></math>. (<b>b</b>) primary side voltage <math display="inline"><semantics> <msub> <mi>v</mi> <mi>p</mi> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>i</mi> <mi>p</mi> </msub> </semantics></math>, secondary side voltage <math display="inline"><semantics> <msub> <mi>v</mi> <mi>s</mi> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>i</mi> <mi>s</mi> </msub> </semantics></math>. (<b>c</b>) Input voltage <math display="inline"><semantics> <msub> <mi>V</mi> <mrow> <mi>i</mi> <mi>n</mi> </mrow> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>i</mi> <mn>1</mn> </msub> </semantics></math>, output voltage <math display="inline"><semantics> <msub> <mi>V</mi> <mi>o</mi> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>I</mi> <mi>o</mi> </msub> </semantics></math>.</p>
Full article ">Figure 9 Cont.
<p>Experimental waveforms of the qZS-IPT system in boost mode with <math display="inline"><semantics> <mrow> <mi>D</mi> <mo>=</mo> <mn>0.2</mn> </mrow> </semantics></math>. (<b>a</b>) Input voltage <math display="inline"><semantics> <msub> <mi>V</mi> <mrow> <mi>i</mi> <mi>n</mi> </mrow> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>i</mi> <mn>1</mn> </msub> </semantics></math>, DC-link voltage <math display="inline"><semantics> <msub> <mi>v</mi> <mrow> <mi>d</mi> <mi>c</mi> </mrow> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>i</mi> <mrow> <mi>d</mi> <mi>c</mi> </mrow> </msub> </semantics></math>. (<b>b</b>) primary side voltage <math display="inline"><semantics> <msub> <mi>v</mi> <mi>p</mi> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>i</mi> <mi>p</mi> </msub> </semantics></math>, secondary side voltage <math display="inline"><semantics> <msub> <mi>v</mi> <mi>s</mi> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>i</mi> <mi>s</mi> </msub> </semantics></math>. (<b>c</b>) Input voltage <math display="inline"><semantics> <msub> <mi>V</mi> <mrow> <mi>i</mi> <mi>n</mi> </mrow> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>i</mi> <mn>1</mn> </msub> </semantics></math>, output voltage <math display="inline"><semantics> <msub> <mi>V</mi> <mi>o</mi> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>I</mi> <mi>o</mi> </msub> </semantics></math>.</p>
Full article ">Figure 10
<p>Experimental waveforms of the qZS-IPT system in buck mode with <math display="inline"><semantics> <mrow> <mi>D</mi> <mo>=</mo> <mo>−</mo> <mn>0.2</mn> </mrow> </semantics></math>. (<b>a</b>) Input voltage <math display="inline"><semantics> <msub> <mi>V</mi> <mrow> <mi>i</mi> <mi>n</mi> </mrow> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>i</mi> <mn>1</mn> </msub> </semantics></math>, DC-link voltage <math display="inline"><semantics> <msub> <mi>v</mi> <mrow> <mi>d</mi> <mi>c</mi> </mrow> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>i</mi> <mrow> <mi>d</mi> <mi>c</mi> </mrow> </msub> </semantics></math>. (<b>b</b>) primary side voltage <math display="inline"><semantics> <msub> <mi>v</mi> <mi>p</mi> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>i</mi> <mi>p</mi> </msub> </semantics></math>, secondary side voltage <math display="inline"><semantics> <msub> <mi>v</mi> <mi>s</mi> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>i</mi> <mi>s</mi> </msub> </semantics></math>. (<b>c</b>) input voltage <math display="inline"><semantics> <msub> <mi>V</mi> <mrow> <mi>i</mi> <mi>n</mi> </mrow> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>i</mi> <mn>1</mn> </msub> </semantics></math>, output voltage <math display="inline"><semantics> <msub> <mi>V</mi> <mi>o</mi> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>I</mi> <mi>o</mi> </msub> </semantics></math>.</p>
Full article ">Figure 10 Cont.
<p>Experimental waveforms of the qZS-IPT system in buck mode with <math display="inline"><semantics> <mrow> <mi>D</mi> <mo>=</mo> <mo>−</mo> <mn>0.2</mn> </mrow> </semantics></math>. (<b>a</b>) Input voltage <math display="inline"><semantics> <msub> <mi>V</mi> <mrow> <mi>i</mi> <mi>n</mi> </mrow> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>i</mi> <mn>1</mn> </msub> </semantics></math>, DC-link voltage <math display="inline"><semantics> <msub> <mi>v</mi> <mrow> <mi>d</mi> <mi>c</mi> </mrow> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>i</mi> <mrow> <mi>d</mi> <mi>c</mi> </mrow> </msub> </semantics></math>. (<b>b</b>) primary side voltage <math display="inline"><semantics> <msub> <mi>v</mi> <mi>p</mi> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>i</mi> <mi>p</mi> </msub> </semantics></math>, secondary side voltage <math display="inline"><semantics> <msub> <mi>v</mi> <mi>s</mi> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>i</mi> <mi>s</mi> </msub> </semantics></math>. (<b>c</b>) input voltage <math display="inline"><semantics> <msub> <mi>V</mi> <mrow> <mi>i</mi> <mi>n</mi> </mrow> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>i</mi> <mn>1</mn> </msub> </semantics></math>, output voltage <math display="inline"><semantics> <msub> <mi>V</mi> <mi>o</mi> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>I</mi> <mi>o</mi> </msub> </semantics></math>.</p>
Full article ">Figure 11
<p>Experimental waveforms of the qZS-IPT system in buck mode with <math display="inline"><semantics> <mrow> <mi>D</mi> <mo>=</mo> <mo>−</mo> <mn>0.4</mn> </mrow> </semantics></math>. (<b>a</b>) Input voltage <math display="inline"><semantics> <msub> <mi>V</mi> <mrow> <mi>i</mi> <mi>n</mi> </mrow> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>i</mi> <mn>1</mn> </msub> </semantics></math>, DC-link voltage <math display="inline"><semantics> <msub> <mi>v</mi> <mrow> <mi>d</mi> <mi>c</mi> </mrow> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>i</mi> <mrow> <mi>d</mi> <mi>c</mi> </mrow> </msub> </semantics></math>. (<b>b</b>) Primary side voltage <math display="inline"><semantics> <msub> <mi>v</mi> <mi>p</mi> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>i</mi> <mi>p</mi> </msub> </semantics></math>, secondary side voltage <math display="inline"><semantics> <msub> <mi>v</mi> <mi>s</mi> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>i</mi> <mi>s</mi> </msub> </semantics></math>. (<b>c</b>) Input voltage <math display="inline"><semantics> <msub> <mi>V</mi> <mrow> <mi>i</mi> <mi>n</mi> </mrow> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>i</mi> <mn>1</mn> </msub> </semantics></math>, output voltage <math display="inline"><semantics> <msub> <mi>V</mi> <mi>o</mi> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>I</mi> <mi>o</mi> </msub> </semantics></math>.</p>
Full article ">Figure 11 Cont.
<p>Experimental waveforms of the qZS-IPT system in buck mode with <math display="inline"><semantics> <mrow> <mi>D</mi> <mo>=</mo> <mo>−</mo> <mn>0.4</mn> </mrow> </semantics></math>. (<b>a</b>) Input voltage <math display="inline"><semantics> <msub> <mi>V</mi> <mrow> <mi>i</mi> <mi>n</mi> </mrow> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>i</mi> <mn>1</mn> </msub> </semantics></math>, DC-link voltage <math display="inline"><semantics> <msub> <mi>v</mi> <mrow> <mi>d</mi> <mi>c</mi> </mrow> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>i</mi> <mrow> <mi>d</mi> <mi>c</mi> </mrow> </msub> </semantics></math>. (<b>b</b>) Primary side voltage <math display="inline"><semantics> <msub> <mi>v</mi> <mi>p</mi> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>i</mi> <mi>p</mi> </msub> </semantics></math>, secondary side voltage <math display="inline"><semantics> <msub> <mi>v</mi> <mi>s</mi> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>i</mi> <mi>s</mi> </msub> </semantics></math>. (<b>c</b>) Input voltage <math display="inline"><semantics> <msub> <mi>V</mi> <mrow> <mi>i</mi> <mi>n</mi> </mrow> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>i</mi> <mn>1</mn> </msub> </semantics></math>, output voltage <math display="inline"><semantics> <msub> <mi>V</mi> <mi>o</mi> </msub> </semantics></math> and current <math display="inline"><semantics> <msub> <mi>I</mi> <mi>o</mi> </msub> </semantics></math>.</p>
Full article ">Figure 12
<p>Experimental battery voltage and current during a complete CC/CV charge cycle.</p>
Full article ">
16 pages, 2987 KiB  
Article
ECO Driving Control for Intelligent Electric Vehicle with Real-Time Energy
by Hongli He, Dan Liu, Xiangyang Lu and Juncai Xu
Electronics 2021, 10(21), 2613; https://doi.org/10.3390/electronics10212613 - 26 Oct 2021
Cited by 12 | Viewed by 2421
Abstract
For the battery pack’s limited remaining power, two energy-aware ecological driving problems are discussed. A real-time energy-aware ecological driving control strategy is proposed to optimize energy consumption and meet the ECO driving demand. First, the vehicle longitudinal driving dynamics model and energy consumption [...] Read more.
For the battery pack’s limited remaining power, two energy-aware ecological driving problems are discussed. A real-time energy-aware ecological driving control strategy is proposed to optimize energy consumption and meet the ECO driving demand. First, the vehicle longitudinal driving dynamics model and energy consumption model are established. Then, the optimal control problem is constructed with the maximum driving distance and the shortest driving time as the objective functions, respectively. With the multinomial Radau pseudo-spectral method, the optimization results of residual power, vehicle speed, and acceleration are obtained. The results show that in the case of in-vehicle driving the remaining power of the battery pack can be sensed in real-time, and the driving of intelligent electric vehicles can be planned in real-time to realize the most ecological driving with the largest driving distance and shortest driving time. The energy consumptions of vehicles, traveling at the same distance, are compared. The consumption obtained through optimization, is 26% less than the consumption of the vehicle that has not been optimized. The results show that the optimization process has certain advantages. In the future, as one of intelligent vehicles’ autonomous driving control strategies, the results have guiding and practical significance. Full article
(This article belongs to the Special Issue Battery Chargers and Management for Electric Vehicles)
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<p>Schematic diagram of the path with energy-aware ecological driving control.</p>
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<p>The flow chart of solving the problem of real-time energy-sensing ecological driving control of the intelligent electric vehicle.</p>
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<p>Real car camera and configuration picture. (1) GPS/INS module. (2) IBEO LUX 2010. (3) LMS291. Four-battery group. (5) Planning decision computer. (6) Inverter and motor drive module. (7) Underlying control module. (8) Steering, throttle, and brake modules. (9) Camera. (10) DC energy meter.</p>
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<p>Power system structure diagram.</p>
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<p>Problem one optimization result: (<b>a</b>) the distance; (<b>b</b>) the speed; (<b>c</b>) the acceleration; (<b>d</b>) the power.</p>
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<p>Problem one optimization result: (<b>a</b>) the distance; (<b>b</b>) the speed; (<b>c</b>) the acceleration; (<b>d</b>) the power.</p>
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<p>Energy consumption compared with optimization and non-optimization.</p>
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<p>Energy-aware ecological driving control optimization results: (<b>a</b>) the distance; (<b>b</b>) the speed; (<b>c</b>) the acceleration; (<b>d</b>) the power.</p>
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<p>Optimization results of the multiphase pseudo-spectral method for energy-aware ecological driving control: (<b>a</b>) the distance; (<b>b</b>) the speed; (<b>c</b>) the acceleration; (<b>d</b>) the power.</p>
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<p>Optimization results of the multiphase pseudo-spectral method for energy-aware ecological driving control: (<b>a</b>) the distance; (<b>b</b>) the speed; (<b>c</b>) the acceleration; (<b>d</b>) the power.</p>
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<p>Driving time compares with optimization and non-optimization.</p>
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<p>Wiring diagram of energy consumption measurement. (<b>a</b>) The distance; (<b>b</b>) the max acceleration; (<b>c</b>) the min acceleration; (<b>d</b>) the speed; (<b>e</b>) the travel time.</p>
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<p>Wiring diagram of energy consumption measurement.</p>
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12 pages, 31689 KiB  
Article
The Hazards Analysis of Nickel-Rich Lithium-Ion Battery Thermal Runaway under Different States of Charge
by Kun Jiang, Pingwei Gu, Peng Huang, Ying Zhang, Bin Duan and Chenghui Zhang
Electronics 2021, 10(19), 2376; https://doi.org/10.3390/electronics10192376 - 28 Sep 2021
Cited by 8 | Viewed by 2701
Abstract
The lithium-ion battery industry has been developing rapidly, with energy density and capacity constantly improving. However, the ensuing safety accidents of lithium-ion power batteries have seriously threatened the personal safety of passengers. Therefore, more and more attention has been paid to the thermal [...] Read more.
The lithium-ion battery industry has been developing rapidly, with energy density and capacity constantly improving. However, the ensuing safety accidents of lithium-ion power batteries have seriously threatened the personal safety of passengers. Therefore, more and more attention has been paid to the thermal safety research of lithium-ion batteries, such as thermal runaway (TR) mechanism analysis and prevention methods, etc. In this paper, the nickel-rich 18650 lithium-ion batteries with Li[Ni0.8Co0.1Mn0.1]O2 cathode in different states of charge (SOC) are taken to investigate the TR characteristics using an extended volume plus acceleration calorimeter (EV+-ARC). In order to evaluate the TR characteristics, some characteristic parameters such as battery voltage, surface temperature, temperature rise rate, etc. are selected from the experiment to analyze the influence of SOC on the critical state of TR. It can be seen from the experiment results that the maximum temperature of the battery surface decreases with the decrease of SOC, while the self-generated heat temperature and TR trigger temperature increases with the decrease of SOC. Full article
(This article belongs to the Special Issue Battery Chargers and Management for Electric Vehicles)
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<p>The experimental platform for charging and discharging.</p>
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<p>The charging and discharging curves of the battery.</p>
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<p>The experimental platform for charging and discharging.</p>
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<p>The specific heat capacity experiment.</p>
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<p>The schematic diagram of the TR experiment.</p>
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<p>Temperature and voltage variation curves of different SOC batteries.</p>
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<p>Temperature and voltage variation curves of different SOC batteries.</p>
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<p>The comparison of TR of different SOC batteries.</p>
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<p>The photographs of the sample battery before and after the TR experiment.</p>
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15 pages, 1295 KiB  
Article
Overcoming Bottlenecks for Realizing a Vehicle-to-Grid Infrastructure in Europe through Standardization
by Sameer Chandrakant Fulari and Geerten van de Kaa
Electronics 2021, 10(5), 582; https://doi.org/10.3390/electronics10050582 - 2 Mar 2021
Cited by 7 | Viewed by 2864
Abstract
This paper focuses on committee–market standards battles for the case of vehicle-to-grid technology in Europe. In this battle, standards such as CHArge de MOve (CHAdeMO) and Combined Charging System (CCS) Combo are competing. The paper identifies relevant factors with the help of a [...] Read more.
This paper focuses on committee–market standards battles for the case of vehicle-to-grid technology in Europe. In this battle, standards such as CHArge de MOve (CHAdeMO) and Combined Charging System (CCS) Combo are competing. The paper identifies relevant factors with the help of a literature review and expert interviews. Furthermore, the importance weights were established for the factors. The paper ends with a discussion and conclusion in which the theoretical contributions, practical implications, limitations, and recommendations for further research are discussed. Full article
(This article belongs to the Special Issue Battery Chargers and Management for Electric Vehicles)
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<p>The best–worst method (BWM) procedure.</p>
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<p>A visualization of the results ranking the factors from most important to least important.</p>
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12 pages, 6477 KiB  
Article
Field-Oriented Driving/Braking Control for Electric Vehicles
by Shang-Ming Liu, Chia-Hung Tu, Chun-Liang Lin and Van-Tsai Liu
Electronics 2020, 9(9), 1484; https://doi.org/10.3390/electronics9091484 - 10 Sep 2020
Cited by 11 | Viewed by 8127
Abstract
Most electric vehicles use regenerative brakes, since this kind of braking system design recycles electromotive force to increase electric power endurance during braking. This research proposes a sensor-free, integrated driving and braking control system that uses a space-vector-pulse-width module to synthesize stator current [...] Read more.
Most electric vehicles use regenerative brakes, since this kind of braking system design recycles electromotive force to increase electric power endurance during braking. This research proposes a sensor-free, integrated driving and braking control system that uses a space-vector-pulse-width module to synthesize stator current by purpose. It calculates the rotor position angle of the motor by detecting variation in the stator current and completes a closed-loop control. When the motor receives a brake command, the controller changes the inverter-switching sequence to generate reverse torque and a magnetic field to complete the driving or braking function using field-oriented control (FOC). This provides a smoother and more accurate motor control than sinusoidal commands with Hall feedback. Compared to the regenerative brake and rheostatic brake, the proposed braking system has a powerful braking torque and shorter reaction time. Comparisons of reaction times for a modified four-wheel electric vehicle equipped with a permanent magnet synchronous motor under neutral-sliding-status, FOC based braking, and short-circuit braking were conducted. Full article
(This article belongs to the Special Issue Battery Chargers and Management for Electric Vehicles)
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<p>Structure of permanent magnet synchronous motor (PMSM). (<b>a</b>) Interior permanent magnet synchronous motor (IPMSM) and (<b>b</b>) surface-mounted permanent magnet synchronous motor (SPMSM).</p>
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<p>Equivalent circuit of the PMSM.</p>
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<p>Simplified inverter topology.</p>
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<p>SVPWM of V<sub>1</sub>–V<sub>6</sub>. (<b>a</b>) SVPWM of V1 (0,0,1); (<b>b</b>) SVPWM of V2 (0,1,1); (<b>c</b>) SVPWM of V3 (0,1,0); (<b>d</b>) SVPWM of V4 (1,1,0); (<b>e</b>) SVPWM of V5 (1,0,0); (<b>f</b>) SVPWM of V6 (1,0,1).</p>
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<p>Architecture of the braking control system.</p>
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<p>Electric vehicle modified from a gas-powered sedan for experimental tests.</p>
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<p>Twenty-five lead acid batteries assembled as the high-voltage power source.</p>
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<p>Hardware architecture.</p>
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<p>Integrated driving/braking inverter.</p>
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<p>PMSM used in the experimental electric vehicle.</p>
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<p>System architecture.</p>
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<p>PMSM working under sliding conditions. (<b>a</b>) 450 rpm; (<b>b</b>) 950 rpm.</p>
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<p>PMSM working under the FOC reverse-braking mode. (<b>a</b>) 450 rpm; (<b>b</b>) 950 rpm.</p>
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<p>PMSM working under short-circuit braking mode. (<b>a</b>) 450 rpm; (<b>b</b>) 950 rpm.</p>
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Review

Jump to: Research

31 pages, 59055 KiB  
Review
Hybrid Three-Phase Rectifiers with Active Power Factor Correction: A Systematic Review
by José Teixeira Gonçalves, Stanimir Valtchev, Rui Melicio, Alcides Gonçalves and Frede Blaabjerg
Electronics 2021, 10(13), 1520; https://doi.org/10.3390/electronics10131520 - 23 Jun 2021
Cited by 19 | Viewed by 6667
Abstract
The hybrid three-phase rectifiers (HTR) consist of parallel associations of two rectifiers (rectifier 1 and rectifier 2), each one of them with a distinct operation, while the sum of their input currents forms a sinusoidal or multilevel waveform. In general, rectifier 1 is [...] Read more.
The hybrid three-phase rectifiers (HTR) consist of parallel associations of two rectifiers (rectifier 1 and rectifier 2), each one of them with a distinct operation, while the sum of their input currents forms a sinusoidal or multilevel waveform. In general, rectifier 1 is a GRAETZ (full bridge) (can be combined with a BOOST converter) and rectifier 2 is combined with a DC-DC converter. In this HTR contest, this paper is intended to answer some important questions about those hybrid rectifiers. To obtain the correct answers, the study is conducted as an analysis of a systematic literature review. Thus, a search was carried out in the databases, mostly IEEE and IET, and 34 papers were selected as the best corresponding to the HTR theme. It is observed that the preferred form of power distribution in unidirectional hybrid three-phase rectifiers (UHTR) is 55%Po (rectifier 1) and 45%Po (rectifier 2). For the bidirectional hybrid three-phase rectifiers (BHTR), rectifier 1 preferably takes 90% of Po and 10% of Po is processed by rectifier 2. It is also observed that the UHTR that employ the single-ended primary-inductor converter (SEPIC) or VIENNA converter topologies in rectifier 2 can present sinusoidal input currents with low total harmonic distortion (THD) and high Power Factor (PF), even successfully complying with the international standards. The same can be said about the rectifier that employs a pulse-width (PWM) converter of BOOST topology in rectifier 2. In short, the HTR are interesting because they allow using the GRAETZ full bridge topology in rectifier 1, thus taking advantage of its characteristics, being simple, robust, and reliable. At the same time, the advantages of rectifier 2, i.e., high PF and low THD, are well used. In addition, this article also points out the future direction of research that is still unexplored in the literature, thus giving opportunities for future innovation. Full article
(This article belongs to the Special Issue Battery Chargers and Management for Electric Vehicles)
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<p>Classification of three-phase rectifiers with reduced harmonic content.</p>
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<p>Flow diagram of the systematic review (PRISMA).</p>
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<p>Number of papers published annually.</p>
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<p>GRAETZ bridge rectifier with BOOST converter and respective control system.</p>
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<p>Modular three-phase rectifier with BOOST converter and isolation transformer.</p>
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<p>Modular three-phase rectifier with BOOST converter and coupled inductor.</p>
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<p>Modular three-phase rectifier with SEPIC converter.</p>
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<p>VIENNA rectifier with PFC and respective control system.</p>
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<p>BOOST-type PWM rectifier with PFC and respective control system.</p>
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<p>Representation of the first mode for power distribution in the HTR using the K gain.</p>
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<p>Representation of the second mode for power distribution in the HTR using the K1 and K2 gains.</p>
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<p>Current waveforms in phase <span class="html-italic">a</span> of the HTR. (<b>a</b>) Input current in rectifier 1. (<b>b</b>) Input current in rectifier 2. (<b>c</b>) Input current (sinusoidal) in the HTR.</p>
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<p>Current waveforms in phase <span class="html-italic">a</span> of the HTR. (<b>a</b>) Input current in rectifier 1. (<b>b</b>) Input current in rectifier 2. (<b>c</b>) Input current (distorted sinusoidal) in the HTR.</p>
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<p>Current waveforms in phase <span class="html-italic">a</span> of the HTR. (<b>a</b>) Input current in rectifier 1. (<b>b</b>) Input current in rectifier 2. (<b>c</b>) Input current (sinusoidal) in the HTR.</p>
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<p>Current waveforms in phase a of the HTR. (<b>a</b>) Input current at rectifier 1. (<b>b</b>) Input current at rectifier 2. (<b>c</b>) Input current (sinusoidal) at BHTR.</p>
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<p>Configuration of the electrical circuit of the UHTR-BR1//BR2.</p>
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<p>Configuration of the electrical circuit of the UHTR-R1//BR2.</p>
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<p>Current waveforms in phase a of the HTR. (<b>a</b>) Input current at rectifier 1. (<b>b</b>) Input current at rectifier 2. (<b>c</b>) Input current (12 multilevels) at HTR.</p>
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<p>Configuration of the electrical circuit of UHTR-BR1//SR2.</p>
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<p>Current waveforms in phase <span class="html-italic">a</span> of the HTR. (<b>a</b>) Input current in rectifier 1. (<b>b</b>) Input current in rectifier 2. (<b>c</b>) Input current (sinusoidal) in the HTR.</p>
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<p>Configuration of the electrical circuit of UHTR-R1//SR2.</p>
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<p>Configuration of the electrical circuit of UHTR-BR1//VR2.</p>
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<p>Configuration of the electrical circuit of UHTR-BR1//DR2.</p>
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<p>Configuration of the electrical circuit of the UHTR-BR1//StR2.</p>
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<p>Configuration of the electrical circuit of BHTR-BR1//BR2.</p>
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<p>Configuration of the BHTR-R1//BR2 electrical circuit.</p>
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<p>Configuration of electrical circuit applied in HTR with sinusoidal current.</p>
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<p>Configuration of electrical circuit applied in HTR with multilevel current.</p>
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<p>Configuration of electrical circuit applied in HTR with sinusoidal current, using a reference signal generator.</p>
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44 pages, 10693 KiB  
Review
A Comprehensive Review of Li-Ion Battery Materials and Their Recycling Techniques
by Hee-Je Kim, TNV Krishna, Kamran Zeb, Vinodh Rajangam, Chandu V. V. Muralee Gopi, Sangaraju Sambasivam, Kummara Venkata Guru Raghavendra and Ihab M. Obaidat
Electronics 2020, 9(7), 1161; https://doi.org/10.3390/electronics9071161 - 17 Jul 2020
Cited by 136 | Viewed by 33848
Abstract
In the context of constant growth in the utilization of the Li-ion batteries, there was a great surge in the quest for electrode materials and predominant usage that lead to the retiring of Li-ion batteries. This review focuses on the recent advances in [...] Read more.
In the context of constant growth in the utilization of the Li-ion batteries, there was a great surge in the quest for electrode materials and predominant usage that lead to the retiring of Li-ion batteries. This review focuses on the recent advances in the anode and cathode materials for the next-generation Li-ion batteries. To achieve higher power and energy demands of Li-ion batteries in future energy storage applications, the selection of the electrode materials plays a crucial role. The electrode materials, such as carbon-based, semiconductor/metal, metal oxides/nitrides/phosphides/sulfides, determine appreciable properties of Li-ion batteries such as greater specific surface area, a minimal distance of diffusion, and higher conductivity. Various classifications of the anode materials such as the intercalation/de- intercalation, alloy/de-alloy, and various conversion materials are illustrated lucidly. Further, the cathode materials, such as nickel-rich LiNixCoyMnzO2 (NCM), were discussed. NCM members such as NCM 333, NCM 523 that enabled to advance for NCM622 and NCM81are reported. The nanostructured materials bridged the gap in the realization of next-generation Li-ion batteries. Li-ion batteries’ electrode nanostructure synthesis, performance, and reaction mechanisms were considered with great concern. The serious effects of Li-ion batteries disposal need to be cut significantly to reduce the detrimental effect on the environment. Hence, the recycling of spent Li-ion batteries has gained much attention in recent years. Various recycling techniques and their effect on the electroactive materials are illustrated. The key areas covered in this review are anode and cathode materials and recent advances along with their recycling techniques. In light of crucial points covered in this review, it constitutes a suitable reference for engineers, researchers, and designers in energy storage applications. Full article
(This article belongs to the Special Issue Battery Chargers and Management for Electric Vehicles)
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<p>Historical evolution and advances of Lithium-ion battery technologies.</p>
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<p>Schematic depiction of lithium insertion/de-insertion mechanism for current rechargeable lithium battery with various electrode materials.</p>
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<p>(<b>a</b>) Single-walled carbon nanotube (SWCNT) electrode voltage profile in extraction and initial insertion of the cycle on stainless steel. Nickel and Titanium coated cells at a current density of 74 mA g<sup>−1</sup> (<b>b</b>) Cycling stability of all three metal-coated cells at various current densities.</p>
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<p>Energies and structures of Li adsorbed on carbon nanotubes (CNTs) and defects. The balls show Li, and the sticks represent C lattice. The numbers are calculated as ε<sub>Li</sub> − ε<sub>Li-M</sub>, in eV. The energy of a single Li atom adsorption on pristine graphene (hexagon) is also shown for comparison. The plots show ε<sub>Li</sub> − ε<sub>Li-CNT</sub> as a function of diameter for (5, 5), (10, 10), and (15, 15) CNTs, for adsorption on inner or outer surfaces, at high (LiC<sub>6</sub>, solid lines) or low ((LiC<sub>∞</sub>, dashed lines) concentrations [<a href="#B104-electronics-09-01161" class="html-bibr">104</a>].</p>
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<p>Polyhedral view of (<b>a</b>) rutile, (<b>b</b>) anatase, and (<b>c</b>) bronze B TiO<sub>2</sub> (Reproduced with permission from Ref. [<a href="#B110-electronics-09-01161" class="html-bibr">110</a>], Copyright 2013 WILEY-VCH Verlag GmbH &amp; Co. KGaA, Weinheim).</p>
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<p>The capacity diagram of various lithium titanate (Reproduced with permission from Ref. [<a href="#B117-electronics-09-01161" class="html-bibr">117</a>].</p>
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<p>Self-supported Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub> nanowire arrays with high conductivity architectures.</p>
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<p>Simple synthesis and particle size effects of TiO<sub>2</sub> nanoparticle anodes for rechargeable lithium ion batteries (Reproduced with the permission from reference [<a href="#B129-electronics-09-01161" class="html-bibr">129</a>]).</p>
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<p>Schematic structure illustration in the bulk and at the surface for (<b>a</b>) Li and (<b>b</b>) Li - Mg alloy anodes during Li stripping/plating process.</p>
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<p>Stable Silicon anode for Lithium-ion batteries by Covalent Bond formation.</p>
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<p>During the slurry-casting process, sheets of MXene material combine with silicon particles to form a network that allows for a more orderly reception of lithium ions, which prevents the silicon anode from expanding and breaking.</p>
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<p>Schematic illustration of the d-SiO/vG during charge/discharge.</p>
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<p>(<b>a</b>) Schematic of the Ge/LCO full-cell. (<b>b</b>) Digital image of a light-emitting diode lighted by the Ge/LCO full-cell.</p>
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<p>Cyclic voltammogram of a flat SnO<sub>2</sub> model electrode with a schematic representation of the electrode composition, intermediate phases during lithiation, and redox features associated with interfacial reactions with the organic and inorganic part of the electrolyte. EC = ethylene carbonate, DMC = dimethyl carbonate. Reproduced with permission from Ref. [<a href="#B156-electronics-09-01161" class="html-bibr">156</a>].</p>
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<p>Open Circuit Voltage (OCV) and Closed Circuit Voltage (CCV) curves for the Li/L-BIOX(Biogenous Iron Oxide) cell in both the discharge and charge directions of the (<b>a</b>) first and (<b>b</b>) second cycles. 80 wt% L-BIOX, 10 wt% CNTs, 10 wt% Styrene-Butadiene Rubber/Carboxymethylcellulose (SBR/CMC). Hysteresis of the OCV curves for the first and second discharge-charge is shown in (<b>c</b>) and (<b>d</b>), respectively. Potential (OCV) dependence of cell resistance for the (<b>e</b>) first and (<b>f</b>) second cycles. The intercepts of the semicircle on the real axis at the low-frequency side in is attributed to the total resistance of the cells.</p>
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<p>Powder XRD patterns of CNS, Co<sub>3</sub>O<sub>4</sub>/CNS hybrids, and bare Co<sub>3</sub>O<sub>4.</sub></p>
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<p>(<b>a</b>) Schematic view of modification mechanism through the ultrathin Al<sub>2</sub>O<sub>3</sub> ALD coating (<b>b</b>) Schematic view of the electronic structure of uncoated and MgO-coated LCO/electrolyte interface upon electrolyte immersion (φ S and φ L are the electrochemical potentials of the electrode and electrolyte, respectively).</p>
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<p>Li[Ni<sub>1–x–y</sub>Co<sub>x</sub>Al<sub>y</sub>]O<sub>2</sub> (NCA) and Li[Ni<sub>1–x–y</sub>Co<sub>x</sub>Mn<sub>y</sub>]O<sub>2</sub> (NCM) cathodes have been the archetypes of current high-energy-density cathodes for Li-ion batteries [<a href="#B217-electronics-09-01161" class="html-bibr">217</a>].</p>
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<p>LMO particles size distribution in individual fractions according to the laser diffraction method: The specific surface area of particles in different samples.</p>
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<p>Schematic representation of the plot of Li-ion battery cathode material potentials vs. capacity. LiMPO<sub>4</sub>, Li<sub>2</sub>MSiO<sub>4</sub> and Li<sub>2</sub>MPO<sub>4</sub>F, where M ¼ Fe, Mn, Co, Ni, etc.; Li<sub>2</sub>MO<sub>3</sub>, where M ¼ Mn, Mo, Ir, Ru, etc. [<a href="#B236-electronics-09-01161" class="html-bibr">236</a>].</p>
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<p>[001] direction projection of four unit cells of phase FeF<sub>3·0.33</sub> H<sub>2</sub>O (<b>a</b>) and β-FeF<sub>3·3</sub>H<sub>2</sub>O (<b>b</b>) [<a href="#B244-electronics-09-01161" class="html-bibr">244</a>].</p>
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<p>Perspectives for LIBs recycling.</p>
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<p>Pre-treatments for lithium-ion recycling process [<a href="#B252-electronics-09-01161" class="html-bibr">252</a>,<a href="#B253-electronics-09-01161" class="html-bibr">253</a>].</p>
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<p>Pyrometallurgical and Hydrothermal Processes.</p>
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<p>Schematic flowsheet for the LithoRec battery recycling process [<a href="#B304-electronics-09-01161" class="html-bibr">304</a>].</p>
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