CN1215298C - Method for reducing resonance frequency of thermoacoustic system and its equipment - Google Patents
Method for reducing resonance frequency of thermoacoustic system and its equipment Download PDFInfo
- Publication number
- CN1215298C CN1215298C CN 02104157 CN02104157A CN1215298C CN 1215298 C CN1215298 C CN 1215298C CN 02104157 CN02104157 CN 02104157 CN 02104157 A CN02104157 A CN 02104157A CN 1215298 C CN1215298 C CN 1215298C
- Authority
- CN
- China
- Prior art keywords
- resonatron
- metal bellows
- bellows spring
- thermoacoustic
- resonant frequency
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired - Fee Related
Links
- 238000000034 method Methods 0.000 title abstract description 11
- 239000002184 metal Substances 0.000 claims abstract description 43
- 239000007787 solid Substances 0.000 claims abstract description 18
- 238000007789 sealing Methods 0.000 claims description 6
- 230000002349 favourable effect Effects 0.000 abstract 2
- 239000007789 gas Substances 0.000 description 24
- XKRFYHLGVUSROY-UHFFFAOYSA-N Argon Chemical compound [Ar] XKRFYHLGVUSROY-UHFFFAOYSA-N 0.000 description 16
- IJGRMHOSHXDMSA-UHFFFAOYSA-N Atomic nitrogen Chemical compound N#N IJGRMHOSHXDMSA-UHFFFAOYSA-N 0.000 description 16
- 239000001307 helium Substances 0.000 description 12
- 229910052734 helium Inorganic materials 0.000 description 12
- SWQJXJOGLNCZEY-UHFFFAOYSA-N helium atom Chemical compound [He] SWQJXJOGLNCZEY-UHFFFAOYSA-N 0.000 description 12
- 229910052786 argon Inorganic materials 0.000 description 8
- 229910052754 neon Inorganic materials 0.000 description 8
- GKAOGPIIYCISHV-UHFFFAOYSA-N neon atom Chemical compound [Ne] GKAOGPIIYCISHV-UHFFFAOYSA-N 0.000 description 8
- 229910052757 nitrogen Inorganic materials 0.000 description 8
- 229910001220 stainless steel Inorganic materials 0.000 description 6
- 239000010935 stainless steel Substances 0.000 description 6
- 238000006243 chemical reaction Methods 0.000 description 4
- 238000010586 diagram Methods 0.000 description 4
- 230000000694 effects Effects 0.000 description 4
- 229910000679 solder Inorganic materials 0.000 description 3
- CURLTUGMZLYLDI-UHFFFAOYSA-N Carbon dioxide Chemical compound O=C=O CURLTUGMZLYLDI-UHFFFAOYSA-N 0.000 description 2
- 239000000463 material Substances 0.000 description 2
- 240000007594 Oryza sativa Species 0.000 description 1
- 235000007164 Oryza sativa Nutrition 0.000 description 1
- 239000001569 carbon dioxide Substances 0.000 description 1
- 229910002092 carbon dioxide Inorganic materials 0.000 description 1
- 238000010276 construction Methods 0.000 description 1
- 230000007812 deficiency Effects 0.000 description 1
- 208000002925 dental caries Diseases 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 230000007613 environmental effect Effects 0.000 description 1
- 238000010438 heat treatment Methods 0.000 description 1
- 239000011261 inert gas Substances 0.000 description 1
- 231100000252 nontoxic Toxicity 0.000 description 1
- 230000003000 nontoxic effect Effects 0.000 description 1
- 238000005057 refrigeration Methods 0.000 description 1
- 235000009566 rice Nutrition 0.000 description 1
- 230000000630 rising effect Effects 0.000 description 1
- 210000001260 vocal cord Anatomy 0.000 description 1
Images
Classifications
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F25—REFRIGERATION OR COOLING; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS; MANUFACTURE OR STORAGE OF ICE; LIQUEFACTION SOLIDIFICATION OF GASES
- F25B—REFRIGERATION MACHINES, PLANTS OR SYSTEMS; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS
- F25B9/00—Compression machines, plants or systems, in which the refrigerant is air or other gas of low boiling point
- F25B9/14—Compression machines, plants or systems, in which the refrigerant is air or other gas of low boiling point characterised by the cycle used, e.g. Stirling cycle
- F25B9/145—Compression machines, plants or systems, in which the refrigerant is air or other gas of low boiling point characterised by the cycle used, e.g. Stirling cycle pulse-tube cycle
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F25—REFRIGERATION OR COOLING; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS; MANUFACTURE OR STORAGE OF ICE; LIQUEFACTION SOLIDIFICATION OF GASES
- F25B—REFRIGERATION MACHINES, PLANTS OR SYSTEMS; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS
- F25B2309/00—Gas cycle refrigeration machines
- F25B2309/14—Compression machines, plants or systems characterised by the cycle used
- F25B2309/1402—Pulse-tube cycles with acoustic driver
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F25—REFRIGERATION OR COOLING; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS; MANUFACTURE OR STORAGE OF ICE; LIQUEFACTION SOLIDIFICATION OF GASES
- F25B—REFRIGERATION MACHINES, PLANTS OR SYSTEMS; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS
- F25B2309/00—Gas cycle refrigeration machines
- F25B2309/14—Compression machines, plants or systems characterised by the cycle used
- F25B2309/1411—Pulse-tube cycles characterised by control details, e.g. tuning, phase shifting or general control
Abstract
The present invention relates to a method for reducing resonance frequencies of a thermoacoustics system and equipment thereof. In the method, an elastic vibration mass block subassembly is installed in a resonant tube of a thermoacoustics system, and a natural frequency of the thermoacoustics system is reduced through adding the effective vibration mass of the thermoacoustics system. The equipment comprises the resonant tube and at least one layer of multi-layer metal bellows spring, and is characterized in that the equipment also comprises a solid mass block. One end face of the solid mass block is connected with one end of the multi-layer metal bellows spring, and a subassembly composed of the solid mass block and the multi-layer metal bellows spring is arranged at any position of the resonant tube. The resonant frequency of the thermoacoustics system is effectively reduced through introducing the equivalent vibration mass to the thermoacoustics system. The dimension of the system is easily controlled, and the present invention is favourable for the miniaturization of a thermoacoustics engine. The present invention is favourable for practicality.
Description
Technical field
The present invention relates to a kind of device that reduces thermoacoustic system, particularly relate to a kind of device that reduces the thermoacoustic system resonant frequency.
Background technology
The operating frequency of thermoacoustic system can not be excessive, because the thermoacoustic system conversion efficiency generally reduces along with the rising of frequency, this can be shown by following sound merit generation rate equation:
The physical significance of relevant symbol can list of references [1] in this formula (Xiao Jiahua. " theoretical research of the hot machine of thermoacoustic effect and back-heating type (comprising refrigeration machine) ", the 24th page, Beijing: Inst. of Physics, CAS, 1991) year is introduced: in the following formula, first of the right is illustrated in following theoretical maximum merit that can produce of certain thermograde, and second and the 3rd then represent owing to limited exchange capability of heat and sound power consumption that viscous drag caused are diffusing.This formula shows that the power consumption that the deficiency of exchange capability of heat and viscous drag cause is loose to be increased along with the increase of frequency, so, for a thermoacoustic system, if can reduce frequency, will reduce to dissipate, improve the conversion efficiency of thermoacoustic system.
Usually, the resonant frequency of a sound system (comprising thermoacoustic system) depends mainly on three factors: the length dimension of the geometry, particularly system of (1) system; (2) boundary condition of system; (3) velocity of sound of the used working media characteristic, particularly working media of system.
The acoustic construction of existing thermoacoustic system mainly contains: (1) standing wave type half-wavelength (or claiming 1/2nd wavelength) sound system, as shown in Figure 1; (2) standing wave type quarter-wave system, as shown in Figure 2; (3) has the quarter-wave system in partial row ripple loop, as shown in Figure 3.
To half-wavelength sound system shown in Figure 1, its minimum natural reonant frequency is:
To quarter-wave sound system shown in Figure 2, its minimum natural reonant frequency is:
To the quarter-wave sound system with partial row ripple loop shown in Figure 3, its minimum natural reonant frequency is determined by following equation:
In (1), (2), (3) formula, f is the minimum natural reonant frequency of sound system; a
0The velocity of sound for working gas in the sound system; L is the length of pipe.
This shows that the lowest resonance frequency of these sound systems is mainly determined by the velocity of sound of working gas, the length of pipe and the boundary condition of sound system.
Table 1 has provided above-mentioned three kinds of sound systems in the minimum natural reonant frequency data that adopt under gas with various medium and the different pipe ranges.As can be seen from Table 1, for the resonant frequency that makes sound system is lower than 50 hertz, then the length of pipeline generally will be at (to helium) more than 5 meters, otherwise resonant frequency will be far above 50 hertz.As seen, be lower than 50 hertz acoustic resonance system if make a frequency, its size is general huger so, not only increases the occupation of land space of system but also consume lot of materials, is unfavorable for practicability.Do not increasing under the size situation of system, can take to change the gas working medium kind, its velocity of sound is reduced, thereby reducing the resonant frequency of thermoacoustic system.But the working medium that is applicable to thermoacoustic system usually generally all adopts environmental protection, nontoxic and safe inert gas, as helium, neon, argon gas, nitrogen, carbon dioxide etc.The molecular weight of these gases is generally less, is difficult to reduce effectively the velocity of sound.Particularly, in the sound-driving low-temperature thermoacoustic refrigerator of heat, the general helium that adopt could obtain low temperature as working media more, but the velocity of sound of helium is very high, reaches about 1000 meter per seconds.As seen, these two kinds of methods are limited in the ability that reduces frequency, reduce aspect the system dimension.
The relation of the minimum intrinsic frequency of the different sound systems of table 1 and working gas, pipeline length
Annotate: (in the calculating of table 1, helium, neon, argon gas and the nitrogen velocity of sound when temperature T=300K is respectively 1019.4m/s, 353m/s, 455.9m/s, 322.4m/s.In addition, row ripple loop length is 0.2m in the travelling-wave type quarter-wave system)
Summary of the invention
Purpose of the present invention: in order to solve the problem that above-mentioned prior art exists, when frequency of solution making was lower than 50 hertz acoustic resonance system (to helium), its size was huger, the problem of practical difficulty; It is generally less that next is to overcome the gas working medium kind molecular weight that is applicable to thermoacoustic system usually, is difficult to reduce effectively the problem of the velocity of sound; Thereby provide a kind of device that reduces the resonant frequency of thermoacoustic system by the effective mass that increases thermoacoustic system.
A kind of method that reduces the resonant frequency of various thermoacoustic systems provided by the invention: it is characterized in that: any part in the resonatron of thermoacoustic system is connected and fixed mass, for make mass in sound system with gas motion, also at an end face of solid masses piece or the spring of a reality of both ends of the surface connection, as the wavy metal bellows.
The employed device of method of the resonant frequency of the various thermoacoustic systems of reduction provided by the invention, comprise: the metal bellows spring of resonatron, at least one multilayer: it is characterized in that: also comprise a solid masses piece, one end face of this solid masses piece is connected with an end of the metal bellows spring of described multilayer, and the assembly of being made up of them is installed on the port of any part on the resonatron or resonatron along the tubular axis line.
When described assembly is installed in the resonatron centre, one section fracture fixation of the other end of solid masses piece and resonatron, the fracture fixation of the other end of the metal bellows spring of described multilayer and another section of resonatron, and connect as one the other port closed of resonatron.
When described assembly is installed in the resonatron port, also comprise a cavity, one end of the metal bellows spring of described multilayer is connected with an end face of solid masses piece, the other end of metal bellows spring is installed in a port of resonatron, metal bellows spring and resonatron fixedly are communicated as one, be fixed with a cavity on the resonatron one end outer cover of solid masses piece, and sealing and fixing.
The both ends of the surface that also are included in the solid masses piece are fixed the metal bellows spring of a multilayer respectively, wherein the metal bellows spring of each multilayer respectively with one section fracture fixation of resonatron, the other port closed of resonatron.
Described resonatron comprises: have thermic sound unit resonatron, have the resonatron in partial row ripple loop etc.
The device that the present invention proposes reduces the resonant frequency of an acoustics effectively, the principle that particularly is used for reducing the resonant frequency of various thermoacoustic systems is: the vibrational system that can regard a quality-spring to any one thermoacoustic system roughly as, wherein, gaseous mass in the system just is equivalent to the oscillating mass of this vibrational system, the compressibility of gas has then constituted the effective spring in this vibrational system, when the equivalent mass that can control this vibrational system and equivalent spring, so just might change the eigentone of this vibrational system, according to the General Principle of quality-spring vibration system, the quality that increases system just can reduce the intrinsic frequency of system.For this reason, reach the purpose of the resonant frequency that reduces thermoacoustic system.
The present invention is as follows to the benefit that existing hot vocal cords come:
(1) needn't solve existing thermoacoustic system because of the oversize difficulty that produces by increasing the intrinsic frequency that device size just can reduce thermoacoustic system significantly;
(2) add the size that measure of the present invention can greatly reduce existing thermoacoustic system, and reduce the intrinsic frequency of thermoacoustic system significantly; And hot acoustic frequency can improve the conversion efficiency that has thermoacoustic system now after reducing effectively.
(3) can increase the free degree that working medium is selected.For example, can mainly be conceived to the heat sound conversion performance of working medium and not necessarily pay close attention to the situation of its velocity of sound.
Description of drawings
Fig. 1 is common 1/2nd wavelength sound system schematic diagrames.
(this sound system is made of the equal diameter pipe of a closed at both ends.Tube length is L, and diameter is D)
Fig. 2 is common quarter-wave sound system schematic diagram.
(this sound system mainly is made up of much larger than the cavity of equal diameter pipe an isodiametric pipe and a volume, the end sealing of pipe, and the other end is connected with cavity; The length of pipe is L, and diameter is D)
Fig. 3 is for having the quarter-wave sound system schematic diagram in partial row ripple loop usually.
(this system has increased a partial row ripple loop on the basis of standing wave type 1/4th sound systems of Fig. 2, promptly an end of equal diameter pipe links to each other with cavity, and the other end then is connected with a belt pipeline)
Metal bellows spring-mass the assembly assumption diagram of Fig. 4 for using in the device of reduction thermoacoustic system resonant frequency of the present invention.
Fig. 5 a is a kind of structural representation that reduces the device (1/2nd wavelength thermoacoustic systems) of thermoacoustic system resonant frequency of the present invention.
Fig. 5 b is the another kind of device that reduces the thermoacoustic system resonant frequency of the present invention
Fig. 5 c is the minimum intrinsic frequency curve of device band metal bellows spring-mass assembly 1/2nd wavelength thermoacoustic systems with Fig. 5 a structure, this figure has provided the contrast of (band metal bellows spring-mass assembly and band metal bellows spring-mass assembly) intrinsic frequency under two kinds of situations, shows that method of the present invention can reduce the intrinsic frequency of 1/2nd wavelength thermoacoustic systems effectively.
Fig. 6 a is the structural representation that embodiments of the invention 2 reduce the thermoacoustic system resonant frequency.
Fig. 6 b is the minimum intrinsic frequency of embodiment 2 and the graph of relation of size, and this figure has provided the contrast of intrinsic frequency under two kinds of situations.
Fig. 7 a is the structural representation that embodiments of the invention 3 reduce the thermoacoustic system resonant frequency.
Fig. 7 b is the minimum intrinsic frequency of embodiment 3 and the graph of relation of size, and this figure has provided the contrast of intrinsic frequency under two kinds of situations.
The drawing explanation:
Folded-2 room temperature coolers-3 of high temperature heater (HTH)-1 heat plate
Resonatron-4 mass (metal derby)-5 metal bellows spring-6
Big cavity-7 thermal acoustic regenerator-8 thermal buffer tube-9
Feedback inertia tube-10
The expression prior art;
Expression the present invention;
The specific embodiment
Embodiment 1
Making is just like the reduction thermoacoustic system resonant frequency devices (1/2nd wavelength thermoacoustic systems) of the band metal bellows spring-mass assembly shown in Fig. 5 a, and method
This thermoacoustic system mainly comprises common thermic sound converting unit, resonatron and metal bellows spring-quality component of the present invention, this assembly by a mass 5 with it about two corrugated stainless steel tubing springs 6 being connected constituted; Wherein, thermic sound converting unit is folded 2 by high temperature heater (HTH) 1, heat sound plate, room temperature cooler 3, and by being disposed in order shown in Fig. 4 a sealing and fixing is installed and forms.Resonatron (4) is an isodiametric pipe, and two end faces all seal about it, metal bellows spring-quality component with it cut into about two sections, make thermic sound unit in the pipe on resonatron (4) left side.As further specifying of this embodiment, present embodiment provides a concrete structure size and relevant parameter designing, so that superiority of the present invention to be described.In the present embodiment, the diameter of resonatron (4) is 50 millimeters, a segment length L on the left side
1=0.2 meter, one section L on the right
2Length can change.Adopt the corrugated stainless steel tubing spring 6 of solder type, coefficient of elasticity is 2400N/m (Newton/meter), and the quality of the mass 5 that welds together with stainless steel wave bellows spring pipe 6 is 0.2kg (kilogram), and mass 5 is a stainless steel material.The working gas medium adopts helium, neon, argon gas and nitrogen respectively, and operating pressure is 2.0MPa.According to these conditions, can obtain resonant frequency and the relation curve that related parameter is arranged shown in Fig. 5 c.
According to above layout, can determine the minimum natural reonant frequency of this thermoacoustic system.Suppose that three assembly high-temperature heaters 1, heat sound plate in the heat sound unit is folded 2, the length of room temperature cooler 3 is much smaller than resonatron 4.Therefore, the overwhelming majority of this thermoacoustic system still is in room temperature state, and the velocity of sound of gas is corresponding to the velocity of sound under the room temperature.Because the dissipation effect of assembly can not change intrinsic frequency in the heat sound converting unit, so in fact the resonant frequency of this thermoacoustic system is equal to the sound system among Fig. 4 b.
For the sound system among Fig. 5 b,, can obtain its intrinsic frequency equation and be according to Principles of Acoustics:
In the following formula, the physical significance of relevant symbol is as follows:
M is the quality (kg, kilogram) of mass; K is the coefficient of elasticity (N/m, Newton/meter) of multiple layer metal bellows; ω is the sound system natural angular frequency, is 2 π times (1/s, 1/ second) of frequency f; L
1, L
2Be respectively the length (m, rice) of metal bellows the right and left resonatron; ρ
0Density (kg/m for gas working dielectric in the thermoacoustic system
3, kilograms per cubic meter); a
0The velocity of sound (m/s, meter per second) for gas; S is the sectional area (m of resonatron
2, square metre)
From Fig. 5 c as can be seen, when the two ends, the left and right sides of resonatron (4) length is 0.2 meter, if there is not the metal bellows assembly, then this system is when charging into helium, neon, argon gas and nitrogen, and its intrinsic lowest resonance frequency is respectively 1274.3 hertz, 572.7 hertz, 403.4 hertz and 441.4 hertz.But, when using elastic vibration mass assembly is installed in the resonatron at thermoacoustic system of the present invention, reach the method for the intrinsic frequency that reduces thermoacoustic system by the effective oscillating mass that increases thermoacoustic system, make the thermoacoustic system lowest resonance frequency be reduced to 92.5 hertz, 91.7 hertz, 90.8 hertz and 84.3 hertz respectively.As seen, use method of the present invention after, the resonant frequency of this thermoacoustic system is reduced significantly, reaches several times to tens times.Particularly, if the resonatron of thermoacoustic system is short more, the effect that then reduces frequency is just remarkable more.
Press shown in Fig. 6 a, make metal bellows spring-mass assembly and be installed in mainly the reduction thermoacoustic system resonant frequency devices of forming in the thermoacoustic system of making by thermic sound converting unit, resonatron and large volume cavity (quarter-wave thermoacoustic system)
Thermic sound unit is folded 2 by high temperature heater (HTH) 1, heat sound plate, room temperature cooler 3 forms by being disposed in order shown in Fig. 5 a.Resonatron 4 is an isodiametric pipe, thermic sound unit is arranged in the pipe on resonatron 4 left sides left side sealing; The both ends of the surface of solid masses piece 5 are fixed the metal bellows spring 6 of a multilayer respectively, wherein the metal bellows spring 6 of a multilayer is fixed with a port of resonatron 4, solid masses piece 5 is that resonatron 4 big cavitys 7 more than 10 times are connected with a volume, the gas of metal bellows assembly the right and left is sealing mutually, and cavity (7) completely cuts off with extraneous.
As further specifying of this embodiment, provide concrete structure size and relevant parameter designing, so that superiority of the present invention to be described.In the present embodiment, the diameter of resonatron (4) is 50 millimeters, and length L can change.Adopt the stainless steel wave bellows spring of solder type, coefficient of elasticity is 2400N/m (Newton/meter), and the quality of the mass M that welds together with spring is 0.2kg (kilogram).The working gas medium adopts helium, neon, argon gas and nitrogen respectively, and operating pressure is 2.0MPa.According to these conditions, can obtain resonant frequency and the relation curve that related parameter is arranged shown in Fig. 6 b.
From Fig. 6 b as can be seen, when the length of resonatron (4) is 0.5 meter, if there is not the metal bellows assembly, then this system is when charging into helium, neon, argon gas and nitrogen, and its intrinsic lowest resonance frequency is respectively 637.1 hertz, 286.4 hertz, 201.7 hertz and 220.7 hertz.But when adding the metal bellows assembly and using method of the present invention, the lowest resonance frequency of this thermoacoustic system is reduced to 48.6 hertz, 48.2 hertz, 47.8 hertz and 44.6 hertz respectively.The resonant frequency that can reduce this thermoacoustic system significantly reaches several times to tens times.
Shown in Fig. 7 a, make metal bellows spring-mass assembly and be installed in reduction thermoacoustic system resonant frequency devices (quarter-wave thermoacoustic system) with partial row ripple loop with partial row ripple loop
The thermoacoustic system of this reduction thermoacoustic system resonant frequency devices mainly is made of partial row's ripple loop thermic sound converting unit, resonatron and metal bellows spring-mass assembly.In Fig. 7 a, thermic sound unit, partial row ripple loop is formed by being disposed in order shown in Fig. 7 a by room temperature cooler 3, thermal acoustic regenerator 8, high temperature heater (HTH) 1, thermal buffer tube 9, room temperature cooler 3 and feedback inertia tube 10.Resonatron 4 is an isodiametric pipe, and its left side links together by a threeway with the outlet of time cooler, identical in the order of placement on the right of resonatron 4 and the example 3.
As further specifying of this embodiment, provide concrete structure size and relevant parameter designing, so that superiority of the present invention to be described.In the present embodiment, partial row ripple loop is the belt bend pipe of the equal diameter of 0.5 meter of length, 50 millimeters of diameters, and the diameter of resonatron (4) is 50 millimeters, and length L can change.Adopt the stainless steel wave bellows spring pipe of solder type, coefficient of elasticity is 2400N/m (Newton/meter).The quality of the mass M that welds together with spring is 0.2kg (kilogram).The working gas medium adopts helium, neon, argon gas and nitrogen respectively, and operating pressure is 2.0MPa.According to these conditions, can obtain resonant frequency and the relation curve that related parameter is arranged shown in Fig. 6 b.
From Fig. 7 b as can be seen, when the length of resonatron (4) is 0.5 meter, if there is not the metal bellows spring-mass assembly of present embodiment, then this system is when charging into helium, neon, argon gas and nitrogen, and its intrinsic lowest resonance frequency is respectively 682.3 hertz, 306.7 hertz, 216.1 hertz and 236.4 hertz.But after adding metal bellows spring-mass assembly, the lowest resonance frequency of this thermoacoustic system is reduced to 48.6 hertz, 48.3 hertz, 47.9 hertz and 44.6 hertz respectively.As seen, add metal bellows spring-mass assembly after, the resonant frequency of this thermoacoustic system is reduced significantly, reaches several times to tens times.Particularly, the resonatron of thermoacoustic system is short more, and the effect that then reduces frequency is more for remarkable.
Claims (5)
1. a device that reduces the thermoacoustic system resonant frequency comprises: the metal bellows spring of resonatron, at least one multilayer; It is characterized in that: also comprise a solid masses piece, one end face of this solid masses piece is connected with an end of the metal bellows spring of described multilayer, and the parts of being made up of them are installed in a optional position on the resonatron or a port of resonatron along the axis of resonatron.
2. press the device of the described reduction thermoacoustic system of claim 1 resonant frequency, it is characterized in that: described parts are installed in the middle of the resonatron, one section fracture fixation of the other end of solid masses piece and resonatron, the fracture fixation of the other end of the metal bellows spring of a described multilayer and another section of resonatron, and connect as one the other port closed of resonatron.
3. by the device of the described reduction thermoacoustic system of claim 1 resonant frequency, it is characterized in that: described parts are installed in the resonatron port, also comprise a cavity; Wherein an end of the metal bellows spring of a multilayer is connected with an end face of solid masses piece, the other end of metal bellows spring is installed in a port of resonatron, metal bellows spring and resonatron fixedly are communicated as one, be fixed with a cavity on the resonatron one end outer cover of solid masses piece, and sealing and fixing.
4. press the device of the described reduction thermoacoustic system of claim 1 resonant frequency, it is characterized in that: the both ends of the surface that also are included in the solid masses piece are fixed the metal bellows spring of a multilayer respectively, wherein the metal bellows spring of each multilayer respectively with one section fracture fixation of resonatron, the other port closed of resonatron.
5. by the isolated plant of the described reduction thermoacoustic system of claim 1 resonant frequency, it is characterized in that: described resonatron comprises: have thermic sound unit resonatron, have the resonatron in partial row ripple loop.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN 02104157 CN1215298C (en) | 2002-03-13 | 2002-03-13 | Method for reducing resonance frequency of thermoacoustic system and its equipment |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN 02104157 CN1215298C (en) | 2002-03-13 | 2002-03-13 | Method for reducing resonance frequency of thermoacoustic system and its equipment |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| CN1443998A CN1443998A (en) | 2003-09-24 |
| CN1215298C true CN1215298C (en) | 2005-08-17 |
Family
ID=27810840
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CN 02104157 Expired - Fee Related CN1215298C (en) | 2002-03-13 | 2002-03-13 | Method for reducing resonance frequency of thermoacoustic system and its equipment |
Country Status (1)
| Country | Link |
|---|---|
| CN (1) | CN1215298C (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US9523272B2 (en) | 2013-12-28 | 2016-12-20 | Halliburton Energy Services, Inc. | Amplification of data-encoded sound waves within a resonant area |
Families Citing this family (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN1332160C (en) * | 2004-09-03 | 2007-08-15 | 中国科学院理化技术研究所 | Coaxial travelling-wave thermo acoustic drive refrigerating system |
| CN1821048B (en) * | 2005-02-18 | 2014-01-15 | 中国科学院理化技术研究所 | Micronl nano thermoacoustic vibration excitor based on thermoacoustic conversion |
| JP5609159B2 (en) * | 2010-02-26 | 2014-10-22 | いすゞ自動車株式会社 | Thermoacoustic engine |
| CN101852513A (en) * | 2010-05-17 | 2010-10-06 | 苏州赛尔科凌空调有限公司 | Thermoacoustic refrigeration device of automobile |
| JP6781899B2 (en) * | 2016-10-18 | 2020-11-11 | 株式会社ジェイテクト | Thermoacoustic device |
| GB2576185B (en) * | 2018-08-08 | 2022-07-20 | Oxford Instruments Nanotechnology Tools Ltd | Noise reduction method for a cryogenic cooling system |
-
2002
- 2002-03-13 CN CN 02104157 patent/CN1215298C/en not_active Expired - Fee Related
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US9523272B2 (en) | 2013-12-28 | 2016-12-20 | Halliburton Energy Services, Inc. | Amplification of data-encoded sound waves within a resonant area |
Also Published As
| Publication number | Publication date |
|---|---|
| CN1443998A (en) | 2003-09-24 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| Bi et al. | Development of a 5 kW traveling-wave thermoacoustic electric generator | |
| Xu et al. | Study on a heat-driven thermoacoustic refrigerator for low-grade heat recovery | |
| US7389852B2 (en) | Integrated heat exchanger and muffler unit | |
| CN1215298C (en) | Method for reducing resonance frequency of thermoacoustic system and its equipment | |
| CN1659412A (en) | Compliant enclosure for thermoacoustic devices | |
| Chi et al. | Study of a gas-liquid-coupled heat-driven room-temperature thermoacoustic refrigerator with different working gases | |
| JP2012154251A (en) | Muffler | |
| Yang et al. | Performance of a looped thermoacoustic engine with multiple loads capable of utilizing heat source below 200° C | |
| CN2811865Y (en) | High frequency pulse tube refrigerator without gas storage device | |
| CN2557889Y (en) | thermoacoutic system with low resonance frequency and small size | |
| Tan et al. | Performance of an air‐cooled looped thermoacoustic engine capable of recovering low‐grade thermal energy | |
| Minner | Theoretical evaluation of the optimal performance of a thermoacoustic refrigerator | |
| CN2526750Y (en) | Assembly for reducing resonance frequency of thermoacoustic system | |
| CN218034630U (en) | Enhanced heat transfer device based on thermoacoustic effect | |
| JP2006118728A (en) | Thermoacoustic refrigeration machine | |
| JP2005265261A (en) | Pulse pipe refrigerator | |
| Chi et al. | A high-efficiency gas–liquid coupled heat-driven thermoacoustic heat pump | |
| CN1743767A (en) | Coaxial travelling-wave thermo acoustic drive refrigerating system | |
| Tew et al. | Recent Stirling engine loss-understanding results | |
| Ibrahim et al. | Constraints and challenges in the development of loudspeaker-driven thermoacoustic refrigerator | |
| CN100344920C (en) | Pressurizer of refrigerator driven by thermoacoustic engine | |
| CN207420873U (en) | Thermocompressor and its heat-exchange system | |
| Al-Mufti et al. | Thermoacoustic Refrigeration: Short Review | |
| Hamood et al. | Two-stage thermoacoustic electricity generator for waste heat recovery | |
| CN101619713B (en) | Thermoacoustic engine with spiral passageway resonance tube |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| C10 | Entry into substantive examination | ||
| SE01 | Entry into force of request for substantive examination | ||
| C06 | Publication | ||
| PB01 | Publication | ||
| C10 | Entry into substantive examination | ||
| SE01 | Entry into force of request for substantive examination | ||
| C14 | Grant of patent or utility model | ||
| GR01 | Patent grant | ||
| ASS | Succession or assignment of patent right |
Owner name: SHENZHEN CITY ZHONGKE LIHAN THERMOACOUSTIC TECHNOL Free format text: FORMER OWNER: PHYSICAL CHEMISTRY TECHNOLOGY INST., CHINESE ACADEMY OF SCIENCES Effective date: 20090626 |
|
| C41 | Transfer of patent application or patent right or utility model | ||
| TR01 | Transfer of patent right |
Effective date of registration: 20090626 Address after: No. 505, Pioneer Park, University Town, Taoyuan Li Shan Road, Shenzhen, Nanshan District Patentee after: Shenzhen Chinese Academy of Sciences Lihan Thermoacoustic Technology Engineering Research Center Co. Address before: No. 2, North Zhongguancun, Beijing, Haidian District Patentee before: Technical Institute of Physics and Chemistry, CAS |
|
| C56 | Change in the name or address of the patentee |
Owner name: ZHONGKE LIHAN (SHENZHEN) THERMOACOUSTIC TECHNOLOGY Free format text: FORMER NAME: SHENZHEN CHINESE ACADEMY OF SCIENCES LIHAN THERMOACOUSTIC TECHNOLOGY ENGINEERING RESEARCH CENTER CO., LTD. |
|
| CP01 | Change in the name or title of a patent holder |
Address after: 518055, No. 505, Pioneer Park, University Town, Mount Li, Nanshan District, Shenzhen, Taoyuan Patentee after: Shenzhen Zhongke Lihan Thermoacoustic Technology Engineering Research Center Co., Ltd. Address before: 518055, No. 505, Pioneer Park, University Town, Mount Li, Nanshan District, Shenzhen, Taoyuan Patentee before: Shenzhen Chinese Academy of Sciences Lihan Thermoacoustic Technology Engineering Research Center Co. |
|
| CF01 | Termination of patent right due to non-payment of annual fee |
Granted publication date: 20050817 Termination date: 20170313 |
|
| CF01 | Termination of patent right due to non-payment of annual fee |