CN105909598A - Full-frequency-band hydraulic system pressure pulsating suppression device - Google Patents

Abstract

The invention relates to a pressure pulsation suppression device for a full-frequency hydraulic system. The input pipe and the output pipe are respectively connected to two ends of the casing and extend into the casing; the elastic thin wall is installed in the casing; the elastic thin wall and the casing form a series connection Resonance chambers I, II and parallel resonance chambers; series resonance chambers I and II are separated by an elastic partition; the elastic thin wall is evenly opened with a number of tapered damping holes in the axial direction; the elastic partition is close to the input There is a tapered insertion tube on the side of the tube, and the tapered insertion tube connects the series resonance chamber I and II; the plug-in H-type filter is located in the parallel resonance chamber; the plug-in series H-type filter is located in the series resonance chamber I and II Inside, it is arranged axially symmetrically with the plug-in H-type filter. The invention can attenuate the pulsating pressure in the high, middle and low frequency bands in the hydraulic system, so as to play the role of self-adaptive filtering in the working conditions of the whole frequency band.

Description

A full-band hydraulic system pressure pulsation suppression device

【Technical field】

The invention relates to a pressure pulsation suppressing device for a hydraulic system, in particular to a pressure pulsation suppressing device for a full-frequency hydraulic system, which belongs to the technical field of hydraulic equipment.

【Background technique】

The hydraulic system has the characteristics of high power density and good operation stability, and has been widely used in the engineering field. With the development of hydraulic technology towards high pressure, high speed and large flow, the influence of pressure pulsation inherent in hydraulic system is becoming more and more prominent. Relevant studies have shown that when the pressure pulsation amplitude exceeds 10% of the working pressure of the hydraulic system, the pipeline will form a higher pressure and cause damage to the pipeline system; when the pressure pulsation amplitude exceeds 2-10% of the hydraulic system working pressure , pipelines and valves will wear and tear, endangering the reliability of the entire hydraulic system.

The pressure pulsation is generated by the flow pulsation passing through the system impedance, and the flow pulsation originates from the pulsation of the output flow of the hydraulic pump. Eliminating the pressure pulsation at the hydraulic pump is the most direct method of hydraulic filtering. Scholars at home and abroad have done a lot of research on this. Although many improvement measures have been taken, it is impossible to eradicate flow pulsation due to the constraints of the periodic oil discharge mechanism of the hydraulic pump. In addition to considering how to attenuate the pulsation from the source, you can also consider it from the perspective of the system load. Installing a hydraulic filter on the pipeline can reduce the input impedance of the system (that is, reduce the output impedance of the pump) and increase the attenuation and reduction of pressure pulsation. absorb.

The hydraulic filter starts from the load system to attenuate the pressure pulsation, and can be divided into two categories: resistive filter and resistive filter from the mechanism of action. The principle of resistive filtering is to use the impedance mismatch to make the pressure wave reflect at the interface where the impedance changes suddenly to achieve the purpose of filtering. But the current resistance filter has the following disadvantages: (1) The pressure pulsation in the hydraulic pipeline is a function of time and position, and the hydraulic filter installed in the position cannot adapt to the variable working conditions; (2) the resistance filter is only suitable for Specific frequency points and narrow frequency bands have good filtering effects, and broad-spectrum filtering cannot be achieved; (3) The attenuation effect of hydraulic filters on pressure pulsations is not ideal; (4) There is no filtering effect on flow pulsations.

In order to solve the above problems, Patent Document 1 (Chinese Patent Application for Invention, Publication No. CN101614231) discloses a vibration damping muffler for a hydraulic system. , there is a damping hole on the mass body, so that the resonant leaf spring with different mass bodies and the damping hole form a "mass + spring + damping" centralized parameter coupling spring vibration system, so as to achieve a broad-spectrum filtering effect. The filtering effect of the vibration damping muffler of this patent is closely related to the radius and thickness of each filter unit on the elastic thin plate. Since there are multiple filter units on the elastic thin plate to achieve broad-spectrum filtering, the radius and thickness of each unit are different. It is limited, so it affects the filtering effect; at the same time, the vibration damping muffler of this patent does not solve the problem that the pressure pulsation changes with the position, and the adaptability to changing working conditions is not good; it has no filtering effect on the flow pulsation.

Therefore, in order to solve the above technical problems, it is indeed necessary to provide an innovative full-band hydraulic system pressure pulsation suppression device to overcome the above-mentioned defects in the prior art.

【Content of invention】

In order to solve the above-mentioned technical problems, the object of the present invention is to provide a pressure pulsation suppression device for a full-frequency hydraulic system, which can track the pressure fluctuation of the hydraulic system, automatically change the filter structure to attenuate the pulsation pressure of the high, medium and low frequency bands in the hydraulic system, So as to play the role of self-adaptive filtering in the whole frequency band.

In order to achieve the above purpose, the technical solution adopted by the present invention is: a pressure pulsation suppression device for a full-band hydraulic system, which includes an input pipe, a casing, an output pipe, an elastic thin wall, a plug-in H-type filter, and a plug-in series H-type Filter; wherein, the input pipe is connected to one end of the casing, which extends into the casing; the output pipe is connected to the other end of the casing, which extends into the casing; the elastic thin wall is installed in the casing along the radial direction of the casing The input pipe, the output pipe and the elastic thin wall jointly form a double-tube plug-in filter; the series resonance volume I, the series resonance volume II and the parallel resonance volume are formed between the elastic thin wall and the shell; The series resonance chamber I and the series resonance chamber II are separated by an elastic partition; the elastic thin wall is evenly opened with a number of tapered damping holes in the axial direction; the elastic partition is provided with A tapered insertion tube, the tapered insertion tube communicates with the series resonance cavity I and the series resonance cavity II; the plug-in H-type filter is located in the parallel resonance cavity, which communicates with the tapered damping hole; the The plug-in series H-type filter is located in the series resonance cavity I and the series resonance cavity II, which are also connected to the tapered damping hole; the plug-in H-type filter and the plug-in series H-type filter are in the axial direction Set symmetrically, and form a plug-in series-parallel H-type filter.

The pressure pulsation suppressing device of the full-frequency hydraulic system of the present invention is further configured such that: the axes of the input pipe and the output pipe are not on the same axis.

The pressure pulsation suppressing device of the full-frequency hydraulic system of the present invention is further configured as follows: the wide opening of the tapered damping hole is located in the series resonance cavity I and the parallel resonance cavity, and the taper angle is 10°.

The pressure pulsation suppressing device of the full-frequency hydraulic system of the present invention is further configured as follows: the wider opening of the tapered insertion tube is located in the series resonance cavity II, and its taper angle is 10°.

The pressure pulsation suppressing device of the full-frequency hydraulic system of the present invention is further set as follows: a colloidal damping layer is provided on the inner side of the elastic thin wall; the inner layer and the outer layer of the colloidal damping layer are respectively the outer elastic thin wall and the inner elastic Thin wall, the outer elastic thin wall and the inner elastic thin wall are fixedly connected by several pillars; the interlayer between the outer elastic thin wall and the inner elastic thin wall is filled with pure water with antifreeze, pure Porous silica gel is suspended in the water.

The pressure pulsation suppressing device of the full-frequency hydraulic system of the present invention is further configured as follows: the end of the colloidal damping layer close to the output pipe is connected to the casing; the end of the colloidal damping layer close to the output pipe is provided with a piston.

Compared with the prior art, the present invention has the following beneficial effects:

1. The present invention has plug-in series-parallel H-type filter banks with different natural frequencies, forming a flat attenuation band in the frequency range of medium and low frequency pressure fluctuations; between the two resonant cavities of plug-in series-connected H-type filters The elastic partitions are separated to widen the attenuation bandwidth; the resonance cavity of the filter spans the entire adaptive filter, so that a larger volume of the resonance cavity can be obtained and the attenuation effect is strengthened; the tapered damping hole and the tapered The insertion tube is inserted into the corresponding resonance cavity, and the taper angle is 10°, which broadens the filter frequency range and makes the overall structure more compact; the tapered insertion tube is opened on the elastic partition near the input tube side, making the resonance cavity 1 and 2 form an asymmetric structure to reduce the natural resonance frequency of the filter.

2. The present invention adopts the combination of the colloidal damping layer and the double-tube plug-in filter structure, absorbs the flow pulsation while attenuating the pressure, and has better flow pulsation attenuation efficiency, and the input pipe and output pipe of the filter are not on the same axis , improving the filtering effect by more than 10%.

3. The axial length of the filter of the present invention is designed to be greater than the pressure pulsation wavelength, and a plurality of tapered damping holes with the same parameters are evenly opened in the axial direction of the elastic thin wall, which ensures three filtering structures in the filter It has a consistent pressure pulsation attenuation effect within the axial length range, making the filter self-adaptive to working conditions. The axial dimensions of the three filtering structures are the same as those of the filter, and their larger dimensions also ensure the filtering performance of the hydraulic filter.

4. The present invention adopts a plug-in series-parallel H-type filter group, a double-tube plug-in filter, an elastic thin-wall filter, and a colloidal damping layer to form a whole, so that the filter has full-band working conditions adaptive pressure pulsation filtering and flow pulsation filtering performance.

【Description of drawings】

Fig. 1 is a schematic structural diagram of a pressure pulsation suppressing device for a full-frequency hydraulic system according to the present invention.

Fig. 2 is a sectional view along A-A in Fig. 1 .

FIG. 3 is a schematic diagram of the plug-in H-type filter in FIG. 2 .

FIG. 4 is a schematic diagram of the plug-in series H-type filter in FIG. 2 .

Fig. 5 is a combination diagram of the frequency characteristics of the plug-in H-type filter and the plug-in series H-type filter. Among them, the solid line is the frequency characteristic of the plug-in series H-type filter.

Figure 6 is a frequency characteristic diagram of the plug-in series-parallel H-type filter.

Fig. 7 is a schematic structural diagram of a double-tube insertion filter.

Fig. 8 is a schematic cross-sectional view of the elastic thin wall.

Fig. 9 is a schematic longitudinal sectional view of the colloidal damping layer.

【detailed description】

Please refer to accompanying drawings 1 to 9 of the description, the present invention is a pressure pulsation suppression device for a full-frequency hydraulic system, which consists of an input pipe 1, a casing 9, an output pipe 11, an elastic thin wall 7, a plug-in H-type filter The device 12 and the plug-in series H-type filter 13 are composed of several parts.

Wherein, the input pipe 1 is connected to one end of the casing 9, and the length extending into the casing 9 is l1; the output pipe 11 is connected to the other end of the casing 9, and the length extending into the casing 9 is l2. The elastic thin wall 7 is installed inside the casing 9 along the radial direction of the casing. The axes of the input pipe 1 and the output pipe 11 are not on the same axis, which can improve the filtering effect by more than 10%.

The input pipe 1, the output pipe 11 and the elastic thin wall 7 jointly form a double-pipe plug-in filter, thereby attenuating high-frequency pressure pulsation of the hydraulic system. The filter transmission coefficient obtained after processing according to the lumped parameter method is:

$\mathrm{<span\; class="notranslate">\; \&gamma;</span>}<span\; class="notranslate">\; =</span>\frac{<span\; class="notranslate">\; |</span>\mathrm{<span\; class="notranslate">\; Z</span>}{<span\; class="notranslate">\; |</span>}^{\mathrm{<span\; class="notranslate">\; 2</span>}}}{<span\; class="notranslate">\; |</span>\mathrm{<span\; class="notranslate">\; Z</span>}{<span\; class="notranslate">\; |</span>}^{\mathrm{<span\; class="notranslate">\; 2</span>}}<span\; class="notranslate">\; +</span>{<span\; class="notranslate">\; (</span>\frac{\mathrm{<span\; class="notranslate">\; 2</span>}\mathrm{<span\; class="notranslate">\; \&rho;</span>}\mathrm{<span\; class="notranslate">\; a</span>}}{{\mathrm{<span\; class="notranslate">\; \&pi;d</span>}}_{\mathrm{<span\; class="notranslate">\; 1</span>}}^{\mathrm{<span\; class="notranslate">\; 2</span>}}}<span\; class="notranslate">\; )</span>}^{\mathrm{<span\; class="notranslate">\; 2</span>}}}$

a—speed of sound in the medium ρ—fluid density d ₁ —diameter of input pipe Z—characteristic impedance

$\mathrm{<span\; class="notranslate">\; Z</span>}<span\; class="notranslate">\; =</span>\frac{\mathrm{<span\; class="notranslate">\; 1</span>}}{\frac{\mathrm{<span\; class="notranslate">\; 1</span>}}{{\mathrm{<span\; class="notranslate">\; Z</span>}}_{\mathrm{<span\; class="notranslate">\; 1</span>}}}<span\; class="notranslate">\; +</span>\frac{\mathrm{<span\; class="notranslate">\; 1</span>}}{{\mathrm{<span\; class="notranslate">\; Z</span>}}_{\mathrm{<span\; class="notranslate">\; 2</span>}}}<span\; class="notranslate">\; +</span>\frac{\mathrm{<span\; class="notranslate">\; 1</span>}}{{\mathrm{<span\; class="notranslate">\; Z</span>}}_{\mathrm{<span\; class="notranslate">\; 3</span>}}}}$

${\mathrm{<span\; class="notranslate">\; Z</span>}}_{\mathrm{<span\; class="notranslate">\; 1</span>}}<span\; class="notranslate">\; =</span>\frac{{\mathrm{<span\; class="notranslate">\; \&rho;l</span>}}_{\mathrm{<span\; class="notranslate">\; 1</span>}}\mathrm{<span\; class="notranslate">\; the\; s</span>}}{\frac{\mathrm{<span\; class="notranslate">\; \&pi;</span>}}{\mathrm{<span\; class="notranslate">\; 4</span>}}<span\; class="notranslate">\; (</span>{\mathrm{<span\; class="notranslate">\; D.</span>}}^{\mathrm{<span\; class="notranslate">\; 2</span>}}<span\; class="notranslate">\; -</span>{{\mathrm{<span\; class="notranslate">\; d</span>}}_{\mathrm{<span\; class="notranslate">\; 1</span>}}}^{\mathrm{<span\; class="notranslate">\; 2</span>}}<span\; class="notranslate">\; )</span>}<span\; class="notranslate">\; +</span>\frac{{\mathrm{<span\; class="notranslate">\; \&rho;a</span>}}^{\mathrm{<span\; class="notranslate">\; 2</span>}}}{\frac{\mathrm{<span\; class="notranslate">\; \&pi;</span>}}{\mathrm{<span\; class="notranslate">\; 4</span>}}<span\; class="notranslate">\; (</span>{\mathrm{<span\; class="notranslate">\; D.</span>}}^{\mathrm{<span\; class="notranslate">\; 2</span>}}<span\; class="notranslate">\; -</span>{{\mathrm{<span\; class="notranslate">\; d</span>}}_{\mathrm{<span\; class="notranslate">\; 1</span>}}}^{\mathrm{<span\; class="notranslate">\; 2</span>}}<span\; class="notranslate">\; )</span>{\mathrm{<span\; class="notranslate">\; l</span>}}_{\mathrm{<span\; class="notranslate">\; 1</span>}}\mathrm{<span\; class="notranslate">\; the\; s</span>}}$

${\mathrm{<span\; class="notranslate">\; Z</span>}}_{\mathrm{<span\; class="notranslate">\; 2</span>}}<span\; class="notranslate">\; =</span>\frac{\mathrm{<span\; class="notranslate">\; \&rho;</span>}\mathrm{<span\; class="notranslate">\; L</span>}\mathrm{<span\; class="notranslate">\; the\; s</span>}}{\frac{\mathrm{<span\; class="notranslate">\; \&pi;</span>}}{\mathrm{<span\; class="notranslate">\; 4</span>}}{\mathrm{<span\; class="notranslate">\; D.</span>}}^{\mathrm{<span\; class="notranslate">\; 2</span>}}}<span\; class="notranslate">\; +</span>\frac{{\mathrm{<span\; class="notranslate">\; \&rho;a</span>}}^{\mathrm{<span\; class="notranslate">\; 2</span>}}}{\frac{\mathrm{<span\; class="notranslate">\; \&pi;</span>}}{\mathrm{<span\; class="notranslate">\; 4</span>}}{\mathrm{<span\; class="notranslate">\; D.</span>}}^{\mathrm{<span\; class="notranslate">\; 2</span>}}\mathrm{<span\; class="notranslate">\; L</span>}\mathrm{<span\; class="notranslate">\; the\; s</span>}}$

${\mathrm{<span\; class="notranslate">\; Z</span>}}_{\mathrm{<span\; class="notranslate">\; 3</span>}}<span\; class="notranslate">\; =</span>\frac{{\mathrm{<span\; class="notranslate">\; \&rho;l</span>}}_{\mathrm{<span\; class="notranslate">\; 2</span>}}\mathrm{<span\; class="notranslate">\; the\; s</span>}}{\frac{\mathrm{<span\; class="notranslate">\; \&pi;</span>}}{\mathrm{<span\; class="notranslate">\; 4</span>}}<span\; class="notranslate">\; (</span>{\mathrm{<span\; class="notranslate">\; D.</span>}}^{\mathrm{<span\; class="notranslate">\; 2</span>}}<span\; class="notranslate">\; -</span>{{\mathrm{<span\; class="notranslate">\; d</span>}}_{\mathrm{<span\; class="notranslate">\; 2</span>}}}^{\mathrm{<span\; class="notranslate">\; 2</span>}}<span\; class="notranslate">\; )</span>}<span\; class="notranslate">\; +</span>\frac{{\mathrm{<span\; class="notranslate">\; \&rho;a</span>}}^{\mathrm{<span\; class="notranslate">\; 2</span>}}}{\frac{\mathrm{<span\; class="notranslate">\; \&pi;</span>}}{\mathrm{<span\; class="notranslate">\; 4</span>}}<span\; class="notranslate">\; (</span>{\mathrm{<span\; class="notranslate">\; D.</span>}}^{\mathrm{<span\; class="notranslate">\; 2</span>}}<span\; class="notranslate">\; -</span>{{\mathrm{<span\; class="notranslate">\; d</span>}}_{\mathrm{<span\; class="notranslate">\; 2</span>}}}^{\mathrm{<span\; class="notranslate">\; 2</span>}}<span\; class="notranslate">\; )</span>{\mathrm{<span\; class="notranslate">\; l</span>}}_{\mathrm{<span\; class="notranslate">\; 2</span>}}\mathrm{<span\; class="notranslate">\; the\; s</span>}}$

d ₂ —diameter of output tube D—diameter of cavity l ₁ —length of insertion tube at input end l ₂ —length of insertion tube at output end L—the difference between the total length of cavity and the sum of the length of insertion tube at input end and output end

It can be seen from the above formula that the effect of the double-tube plug-in cavity filter is similar to that of the capacitor in the circuit. When pressure pulsation waves of different frequencies pass through the filter, the transmission coefficient varies with frequency. The higher the frequency, the smaller the transmission coefficient, which indicates that the high-frequency pressure pulsation wave is attenuated more strongly when passing through the filter, thereby eliminating the high-frequency pressure pulsation.

The design principle of the double-pipe plug-in filter is as follows: when the pressure pulsation frequency in the pipeline is high, the pressure pulsation acts on the fluid to produce a compression effect on the fluid. When the changing flow rate enters the double-tube insertion cavity through the input tube, the liquid flow exceeds the average flow rate, and the enlarged cavity can absorb the excess liquid flow, and release the liquid flow when the flow rate is lower than the average flow rate, thereby absorbing the pressure pulsation energy.

The elastic thin wall 7 weakens the high-frequency pressure pulsation in the hydraulic system by forced mechanical vibration. The natural frequency of elastic thin-wall obtained after processing according to the lumped parameter method is:

${\mathrm{<span\; class="notranslate">\; f</span>}}_{\mathrm{<span\; class="notranslate">\; m</span>}}<span\; class="notranslate">\; =</span>\frac{{\mathrm{<span\; class="notranslate">\; k</span>}}^{\mathrm{<span\; class="notranslate">\; 2</span>}}\mathrm{<span\; class="notranslate">\; h</span>}}{\mathrm{<span\; class="notranslate">\; 2</span>}{\mathrm{<span\; class="notranslate">\; \&pi;R</span>}}^{\mathrm{<span\; class="notranslate">\; 2</span>}}}<span\; class="notranslate">\; \&CenterDot;</span>\sqrt{\frac{\mathrm{<span\; class="notranslate">\; E.</span>}}{\mathrm{<span\; class="notranslate">\; 12</span>}\mathrm{<span\; class="notranslate">\; \&rho;</span>}<span\; class="notranslate">\; (</span>\mathrm{<span\; class="notranslate">\; 1</span>}<span\; class="notranslate">\; +</span>\mathrm{<span\; class="notranslate">\; \&eta;</span>}<span\; class="notranslate">\; )</span><span\; class="notranslate">\; (</span>\mathrm{<span\; class="notranslate">\; 1</span>}<span\; class="notranslate">\; -</span>{\mathrm{<span\; class="notranslate">\; \&mu;</span>}}^{\mathrm{<span\; class="notranslate">\; 2</span>}}<span\; class="notranslate">\; )</span>}}$

k—coefficient of elastic thin-wall structure h—thickness of elastic thin-wall R—radius of elastic thin-wall

E—Young's modulus of elastic thin wall ρ—mass density of elastic thin wall

η—the current carrying factor of the elastic thin wall μ—the Poisson's ratio of the elastic thin wall.

Substituting the actual parameters and performing simulation analysis on the above formula, it can be found that the natural frequency of the elastic thin wall 7 is usually higher than that of the H-type filter, and its attenuation frequency band is also wider than that of the H-type filter. In a relatively wide frequency band, the elastic thin wall has a good attenuation effect on pressure pulsation. At the same time, the elastic thin wall in the filter structure of the present invention has a larger and thinner radius, and its natural frequency is closer to the middle frequency band, which can effectively attenuate the middle and high frequency pressure fluctuations in the hydraulic system.

The design principle of the elastic thin wall 7 is as follows: when medium-frequency pressure pulsation occurs in the pipeline, the attenuation ability of the double-tube insertion cavity filter to the pressure fluctuation is weak, and the periodic pulsation pressure flowing into the double-tube insertion cavity continues to act On the inner and outer walls of the elastic thin wall, due to the fixed connection of the pillars between the inner and outer walls, the inner and outer elastic thin walls vibrate periodically according to the frequency of the pulsating pressure. The forced vibration consumes the pressure pulsation energy of the fluid, thereby realizing the middle frequency range Pressure filtering. According to the principle of virtual work, the ability of the elastic thin wall to consume fluid pulsating pressure energy is directly related to the sum of potential energy and kinetic energy when it is forced to vibrate. In order to improve the filtering performance in the middle frequency band, the radius of the elastic thin wall is designed to be much larger than the pipe radius. And the thickness of the thin wall is relatively small, typically less than 0.1mm.

Further, a series resonant cavity I4, a series resonant cavity II3 and a parallel resonant cavity 5 are formed between the elastic thin wall 7 and the housing 9, and the cavities 3, 4, and 5 span the entire filter, thereby A larger volume of the resonant cavity can be obtained, and the attenuation effect can be enhanced. The series resonance chamber I4 and the series resonance chamber II5 are separated by an elastic partition 10 . A plurality of tapered damping holes 6 are evenly opened in the axial direction of the elastic thin wall 7, and the wider openings of the tapered damping holes 6 are located in the series resonance cavity I4 and the parallel resonance cavity 5, and the taper angle is 10 °. The elastic partition 10 is provided with a tapered insertion tube 2 on the side close to the input tube 1, and the tapered insertion tube 2 communicates with the series resonance cavity I4 and the series resonance cavity II3. The wider opening of the tapered insertion tube 2 is located in the series resonance volume II3, and its taper angle is 10°.

The plug-in H-type filter 12 is located in the parallel resonant cavity 5 , which communicates with the tapered damping hole 6 . The natural angular frequency of the filter obtained after processing according to the lumped parameter method is:

$\begin{array}{cc}{\mathrm{<span\; class="notranslate">\; \&omega;</span>}}_{\mathrm{<span\; class="notranslate">\; r</span>}}<span\; class="notranslate">\; =</span>\mathrm{<span\; class="notranslate">\; a</span>}\sqrt{\frac{\mathrm{<span\; class="notranslate">\; S</span>}}{\mathrm{<span\; class="notranslate">\; L</span>}<span\; class="notranslate">\; (</span>\mathrm{<span\; class="notranslate">\; V</span>}<span\; class="notranslate">\; -</span>\mathrm{<span\; class="notranslate">\; L</span>}\mathrm{<span\; class="notranslate">\; S</span>}<span\; class="notranslate">\; )</span>}}& <span\; class="notranslate">\; (</span>\mathrm{<span\; class="notranslate">\; r</span>}\mathrm{<span\; class="notranslate">\; a</span>}\mathrm{<span\; class="notranslate">\; d</span>}<span\; class="notranslate">\; /</span>\mathrm{<span\; class="notranslate">\; the\; s</span>}<span\; class="notranslate">\; )</span>\end{array}<span\; class="notranslate">\; -</span><span\; class="notranslate">\; -</span><span\; class="notranslate">\; -</span><span\; class="notranslate">\; (</span>\mathrm{<span\; class="notranslate">\; 1</span>}<span\; class="notranslate">\; )</span>$

a—speed of sound in medium L—length of damping hole S—cross-sectional area of damping hole V—volume of parallel resonance cavity.

The plug-in series H-type filter 13 is located in the series resonance cavity I4 and the series resonance cavity II3 , which are also connected to the tapered damping hole 6 . After processing according to the lumped parameter method, the two natural corner frequencies of the filter are:

${\mathrm{<span\; class="notranslate">\; \&omega;</span>}}_{\mathrm{<span\; class="notranslate">\; 1</span>}}<span\; class="notranslate">\; =</span>\frac{\sqrt{\mathrm{<span\; class="notranslate">\; \&pi;</span>}}\mathrm{<span\; class="notranslate">\; a</span>}}{\sqrt{\mathrm{<span\; class="notranslate">\; 2</span>}}\sqrt{{\mathrm{<span\; class="notranslate">\; k</span>}}_{\mathrm{<span\; class="notranslate">\; 1</span>}}<span\; class="notranslate">\; +</span>{\mathrm{<span\; class="notranslate">\; k</span>}}_{\mathrm{<span\; class="notranslate">\; 2</span>}}<span\; class="notranslate">\; +</span>\sqrt{{<span\; class="notranslate">\; \&lsqb;</span>{\mathrm{<span\; class="notranslate">\; k</span>}}_{\mathrm{<span\; class="notranslate">\; 1</span>}}<span\; class="notranslate">\; -</span>{\mathrm{<span\; class="notranslate">\; k</span>}}_{\mathrm{<span\; class="notranslate">\; 2</span>}}<span\; class="notranslate">\; \&rsqb;</span>}^{\mathrm{<span\; class="notranslate">\; 2</span>}}<span\; class="notranslate">\; +</span>\frac{\mathrm{<span\; class="notranslate">\; 4</span>}{<span\; class="notranslate">\; (</span>{\mathrm{<span\; class="notranslate">\; V</span>}}_{\mathrm{<span\; class="notranslate">\; 4</span>}}<span\; class="notranslate">\; -</span>\frac{\mathrm{<span\; class="notranslate">\; 1</span>}}{\mathrm{<span\; class="notranslate">\; 4</span>}}{{\mathrm{<span\; class="notranslate">\; \&pi;d</span>}}_{\mathrm{<span\; class="notranslate">\; 3</span>}}}^{\mathrm{<span\; class="notranslate">\; 2</span>}}{\mathrm{<span\; class="notranslate">\; l</span>}}_{\mathrm{<span\; class="notranslate">\; 3</span>}}<span\; class="notranslate">\; )</span>}^{\mathrm{<span\; class="notranslate">\; 2</span>}}{\mathrm{<span\; class="notranslate">\; l</span>}}_{\mathrm{<span\; class="notranslate">\; 1</span>}}{\mathrm{<span\; class="notranslate">\; l</span>}}_{\mathrm{<span\; class="notranslate">\; 3</span>}}}{{\mathrm{<span\; class="notranslate">\; d</span>}}_{\mathrm{<span\; class="notranslate">\; 1</span>}}^{\mathrm{<span\; class="notranslate">\; 2</span>}}{\mathrm{<span\; class="notranslate">\; d</span>}}_{\mathrm{<span\; class="notranslate">\; 3</span>}}^{\mathrm{<span\; class="notranslate">\; 2</span>}}}}}}<span\; class="notranslate">\; -</span><span\; class="notranslate">\; -</span><span\; class="notranslate">\; -</span><span\; class="notranslate">\; (</span>\mathrm{<span\; class="notranslate">\; 2</span>}<span\; class="notranslate">\; )</span>$

${\mathrm{<span\; class="notranslate">\; \&omega;</span>}}_{\mathrm{<span\; class="notranslate">\; 2</span>}}<span\; class="notranslate">\; =</span>\frac{\sqrt{\mathrm{<span\; class="notranslate">\; \&pi;</span>}}\mathrm{<span\; class="notranslate">\; a</span>}}{\sqrt{\mathrm{<span\; class="notranslate">\; 2</span>}}\sqrt{{\mathrm{<span\; class="notranslate">\; k</span>}}_{\mathrm{<span\; class="notranslate">\; 1</span>}}<span\; class="notranslate">\; +</span>{\mathrm{<span\; class="notranslate">\; k</span>}}_{\mathrm{<span\; class="notranslate">\; 2</span>}}<span\; class="notranslate">\; -</span>\sqrt{{<span\; class="notranslate">\; \&lsqb;</span>{\mathrm{<span\; class="notranslate">\; k</span>}}_{\mathrm{<span\; class="notranslate">\; 1</span>}}<span\; class="notranslate">\; -</span>{\mathrm{<span\; class="notranslate">\; k</span>}}_{\mathrm{<span\; class="notranslate">\; 2</span>}}<span\; class="notranslate">\; \&rsqb;</span>}^{\mathrm{<span\; class="notranslate">\; 2</span>}}<span\; class="notranslate">\; +</span>\frac{\mathrm{<span\; class="notranslate">\; 4</span>}{<span\; class="notranslate">\; (</span>{\mathrm{<span\; class="notranslate">\; V</span>}}_{\mathrm{<span\; class="notranslate">\; 4</span>}}<span\; class="notranslate">\; -</span>\frac{\mathrm{<span\; class="notranslate">\; 1</span>}}{\mathrm{<span\; class="notranslate">\; 4</span>}}{{\mathrm{<span\; class="notranslate">\; \&pi;d</span>}}_{\mathrm{<span\; class="notranslate">\; 3</span>}}}^{\mathrm{<span\; class="notranslate">\; 2</span>}}{\mathrm{<span\; class="notranslate">\; l</span>}}_{\mathrm{<span\; class="notranslate">\; 3</span>}}<span\; class="notranslate">\; )</span>}^{\mathrm{<span\; class="notranslate">\; 2</span>}}{\mathrm{<span\; class="notranslate">\; l</span>}}_{\mathrm{<span\; class="notranslate">\; 1</span>}}{\mathrm{<span\; class="notranslate">\; l</span>}}_{\mathrm{<span\; class="notranslate">\; 3</span>}}}{{\mathrm{<span\; class="notranslate">\; d</span>}}_{\mathrm{<span\; class="notranslate">\; 1</span>}}^{\mathrm{<span\; class="notranslate">\; 2</span>}}{\mathrm{<span\; class="notranslate">\; d</span>}}_{\mathrm{<span\; class="notranslate">\; 3</span>}}^{\mathrm{<span\; class="notranslate">\; 2</span>}}}}}}<span\; class="notranslate">\; -</span><span\; class="notranslate">\; -</span><span\; class="notranslate">\; -</span><span\; class="notranslate">\; (</span>\mathrm{<span\; class="notranslate">\; 3</span>}<span\; class="notranslate">\; )</span>$

in:

${\mathrm{<span\; class="notranslate">\; k</span>}}_{\mathrm{<span\; class="notranslate">\; 1</span>}}<span\; class="notranslate">\; =</span>\frac{{\mathrm{<span\; class="notranslate">\; l</span>}}_{\mathrm{<span\; class="notranslate">\; 1</span>}}<span\; class="notranslate">\; (</span>{\mathrm{<span\; class="notranslate">\; V</span>}}_{\mathrm{<span\; class="notranslate">\; 2</span>}}<span\; class="notranslate">\; +</span>{\mathrm{<span\; class="notranslate">\; V</span>}}_{\mathrm{<span\; class="notranslate">\; 4</span>}}<span\; class="notranslate">\; -</span>\frac{\mathrm{<span\; class="notranslate">\; 1</span>}}{\mathrm{<span\; class="notranslate">\; 4</span>}}{{\mathrm{<span\; class="notranslate">\; \&pi;d</span>}}_{\mathrm{<span\; class="notranslate">\; 1</span>}}}^{\mathrm{<span\; class="notranslate">\; 2</span>}}{\mathrm{<span\; class="notranslate">\; l</span>}}_{\mathrm{<span\; class="notranslate">\; 1</span>}}<span\; class="notranslate">\; -</span>\frac{\mathrm{<span\; class="notranslate">\; 1</span>}}{\mathrm{<span\; class="notranslate">\; 4</span>}}{{\mathrm{<span\; class="notranslate">\; \&pi;d</span>}}_{\mathrm{<span\; class="notranslate">\; 3</span>}}}^{\mathrm{<span\; class="notranslate">\; 2</span>}}{\mathrm{<span\; class="notranslate">\; l</span>}}_{\mathrm{<span\; class="notranslate">\; 3</span>}}<span\; class="notranslate">\; )</span>}{{{\mathrm{<span\; class="notranslate">\; d</span>}}_{\mathrm{<span\; class="notranslate">\; 1</span>}}}^{\mathrm{<span\; class="notranslate">\; 2</span>}}}$

${\mathrm{<span\; class="notranslate">\; k</span>}}_{\mathrm{<span\; class="notranslate">\; 2</span>}}<span\; class="notranslate">\; =</span>\frac{<span\; class="notranslate">\; (</span>{\mathrm{<span\; class="notranslate">\; V</span>}}_{\mathrm{<span\; class="notranslate">\; 4</span>}}<span\; class="notranslate">\; -</span>\frac{\mathrm{<span\; class="notranslate">\; 1</span>}}{\mathrm{<span\; class="notranslate">\; 4</span>}}{{\mathrm{<span\; class="notranslate">\; \&pi;d</span>}}_{\mathrm{<span\; class="notranslate">\; 3</span>}}}^{\mathrm{<span\; class="notranslate">\; 2</span>}}{\mathrm{<span\; class="notranslate">\; l</span>}}_{\mathrm{<span\; class="notranslate">\; 3</span>}}<span\; class="notranslate">\; )</span>{\mathrm{<span\; class="notranslate">\; l</span>}}_{\mathrm{<span\; class="notranslate">\; 3</span>}}}{{{\mathrm{<span\; class="notranslate">\; d</span>}}_{\mathrm{<span\; class="notranslate">\; 3</span>}}}^{\mathrm{<span\; class="notranslate">\; 2</span>}}}$

a—speed of sound in medium l ₁ —length of damping hole d ₁ —diameter of damping hole l ₃ —length of insertion tube

d ₃ —the diameter of the insertion tube V ₂ —the volume of the series resonance chamber 1 V ₄ —the volume of the series resonance chamber 2.

The plug-in H-type filter 12 and the plug-in series H-type filter 13 are arranged axially symmetrically, and form a plug-in series-parallel H-type filter, which is used to broaden the filtering frequency range and make the overall structure more compact. In the present invention, a plurality of plug-in series-parallel H-type filters (only two are shown in the figure) are distributed along the circumferential interface, separated by partitions 20 .

It can be found from the frequency characteristics of the plug-in H-type filter and the plug-in series H-type filter and the formula (1)(2)(3) in Figure 5 that the plug-in series H-type filter has two natural angular frequencies, which are at the peak The filtering effect is better at the peak, but there is basically no filtering effect at the valley; the plug-in H-type filter has a natural angular frequency, and the filtering effect is better at the peak, but there is basically no filtering effect at the valley; choose a suitable filter parameters, so that the natural corner frequency of the plug-in H-type filter just falls between the two natural corner frequencies of the plug-in series H-type filter, as shown in Figure 6, which forms a Three adjacent natural resonance frequency peaks, within this frequency range, no matter the pressure pulsation frequency is at the peak or the trough, it can ensure a better filtering effect. A filter bank composed of multiple plug-in series-parallel H-type filters can cover the entire low-to-medium frequency band and realize full-spectrum filtering of the low-to-medium frequency band.

A colloidal damping layer 8 is provided on the inner side of the elastic thin wall 7 . The inner layer and the outer layer of the colloidal damping layer 8 are an outer elastic thin wall 81 and an inner elastic thin wall 82 respectively, and several pillars 14 are fixedly connected between the outer elastic thin wall 81 and the inner elastic thin wall 82 . The interlayer between the outer elastic thin wall 81 and the inner elastic thin wall 82 is filled with pure water 16 with antifreeze, and porous silica gel 15 is suspended in the pure water 16 . One end of the colloidal damping layer 8 close to the output pipe 11 is connected to the housing 9 ; the end of the colloidal damping layer 8 close to the output pipe 11 is also provided with a piston 17 .

Because the distance between the outer elastic thin wall 81 and the inner elastic thin wall 82 is very small and they are fixedly connected by the struts 14, when the pressure pulsation acts perpendicularly on the thin wall, the inner and outer walls deform almost uniformly, and the thickness of the colloidal damping layer remains almost unchanged. , has no damping effect on the pressure pulsation; the piston 17 of the colloidal damping layer 8 only senses the flow pulsation in the horizontal direction. The nanoscale delivery channel enters the micron-scale central space; when the flow pulsation weakens, the piston 17 is under back pressure, and the colloidal damping layer expands at this time, and the water in the colloidal damping layer is discharged from the central space through the channel. In this process, due to the mechanical effect of silica gel 15 microchannel adsorption, the roughness effect of the channel surface molecular scale and the chemical heterogeneity effect, the piston follows the colloidal damping layer during the contraction and expansion process to form a "gas-liquid-solid" boundary interface Work, so as to attenuate the flow pulsation, which is essentially a parallel R-type filter. Compared with the general liquid damper, the advantage of this filter is that it attenuates the flow pulsation through the interface work of the "gas-liquid-solid" boundary, and can absorb a large amount of mechanical energy without generating heat, and the energy consumption does not depend on With respect to piston speed, the decay efficiency has been significantly improved.

The invention can also self-adaption pressure pulsation attenuation under continuous working conditions. When the working condition of the hydraulic system changes, the sudden stop or operation of the actuator and the change of the opening of the valve will cause a sudden change in the characteristic impedance of the pipeline system, so that the curve of the original pipeline pressure with time and position will also change , the position of the pressure peak also changes. Because the axial length of the filter of the present invention is designed to be greater than the main pressure pulsation wavelength of the system, and the length of the cavity of the plug-in series-parallel H-type filter bank of the filter, the length and elastic thickness of the double-tube plug-in cavity filter The length of the wall is equal to the length of the filter axis, which ensures that the pressure peak position is always within the effective range of the filter; while the tapered damping hole of the plug-in series-parallel H-type filter is opened on the elastic thin wall, and is uniform along the axis direction. Distribution, so that the change of the pressure peak position has almost no impact on the performance of the filter, thus realizing the adaptive filtering function of working conditions. Considering that the axial dimensions of the three filter structures are equivalent to those of the filter, this larger size also ensures that the hydraulic filter has a strong pressure pulsation attenuation capability.

The method for hydraulic pulsation filtering by using the pressure pulsation suppression device of the present invention is as follows:

1), the hydraulic fluid enters the double-tube plug-in filter through the input pipe, and the enlarged cavity absorbs excess liquid flow to complete the filtering of high-frequency pressure pulsation;

2), through the forced vibration of the elastic thin wall 7, the pressure pulsation energy of the fluid is consumed, and the filtering of the intermediate frequency pressure pulsation is completed;

3), through the plug-in series-parallel H-type filter group, through the tapered damping hole, the tapered insertion tube and the fluid to generate resonance, consume pulsation energy, and complete the filtering of low-frequency pressure pulsation;

4), the axial length of the filter is designed to be greater than the main pressure pulsation wavelength of the hydraulic system, and the length of the plug-in series-parallel H-type filter, the length of the double-tube plug-in filter and the length of the elastic thin-walled 7 are equal to the filter length, Make the pressure peak position always within the effective range of the filter, and realize the filtering of the pressure pulsation when the working condition of the system changes.

The specific implementation above is only a preferred embodiment of this creation, and is not intended to limit this creation. Any modifications, equivalent replacements, improvements, etc. made within the spirit and principles of this creation should be included in this creation. within the scope of protection.

Claims (6)

1. a full frequency band Research of Pressure Ripple for Hydraulic Systems restraining device, it is characterised in that: include input pipe, shell, outlet tube, elastic thin-wall, plug-in type H mode filter and plug-in type cascaded H mode filter；Wherein, described input pipe is connected to one end of shell, and it extends in shell；Described outlet tube is connected to the other end of shell, and it extends in shell；Described elastic thin-wall is installed in shell along the radial direction of shell；Described input pipe, outlet tube and elastic thin-wall are collectively forming a two-tube slip-on filter；Resonance series cavity volume I, resonance series cavity volume II and parallel resonance cavity volume is formed between described elastic thin-wall and shell；Separated by an elastic baffle between described resonance series cavity volume I and resonance series cavity volume II；Some conical damping holes are uniformly had in the axial direction of described elastic thin-wall；Described elastic baffle is provided with taper near input tube side and inserts pipe, and pipe connection resonance series cavity volume I and resonance series cavity volume II is inserted in described taper；Described plug-in type H mode filter is positioned at parallel resonance cavity volume, and it is connected with conical damping hole；Described plug-in type cascaded H mode filter is positioned at resonance series cavity volume I and resonance series cavity volume II, and it is also connected with conical damping hole；Described plug-in type H mode filter and plug-in type cascaded H mode filter are axially symmetrical set, and form plug-in type connection in series-parallel H mode filter.

2. full frequency band Research of Pressure Ripple for Hydraulic Systems restraining device as claimed in claim 1, it is characterised in that: the axis of described input pipe and outlet tube is the most on the same axis.

3. full frequency band Research of Pressure Ripple for Hydraulic Systems restraining device as claimed in claim 1, it is characterised in that: the described wider place of conical damping hole opening is positioned at resonance series cavity volume I and parallel resonance cavity volume, and its taper angle is 10 °.

4. full frequency band Research of Pressure Ripple for Hydraulic Systems restraining device as claimed in claim 1, it is characterised in that: described taper is inserted the wider place of tube opening and is positioned at resonance series cavity volume II, and its taper angle is 10 °.

5. full frequency band Research of Pressure Ripple for Hydraulic Systems restraining device as claimed in claim 1, it is characterised in that: the inner side of described elastic thin-wall is provided with colloid damping layer；The internal layer of described colloid damping layer and outer layer are respectively outer layer elastic thin-wall and internal layer elastic thin-wall, are connected by some pillars are fixing between outer layer elastic thin-wall and internal layer elastic thin-wall；It is filled with, in interlayer between described outer layer elastic thin-wall and internal layer elastic thin-wall, the pure water adding antifreezing agent, in pure water, is suspended with Bio-sil.

6. full frequency band Research of Pressure Ripple for Hydraulic Systems restraining device as claimed in claim 5, it is characterised in that: described colloid damping layer is connected with shell near one end of outlet tube；Described colloid damping layer is provided with a piston near one end of outlet tube.