The present invention includes an acoustic power amplifier and a pulse tube cryocooler with inertance tube phase modulation, especially an acoustic power amplifier used in the modulating phase via inertance tube and a pulse tube cryocooler with the acoustic power amplifier.
The pulse tube cryocoolers do not have moving parts under a low temperature, and have advantages of a simple structure, low cost, low mechanical vibration, high reliability, and a long life. These advantages make the research of pulse tube cryocoolers popular. Compared with G-M type pulse tube cryocoolers, Stirling type pulse tube cryocooler is smaller and more compact, hence attracts more attention. As the enthalpy phase modulation theory indicates, the phase difference between the mass flow and the pressure wave can significantly affect the cooling performance of the pulse tube cryocooler. Thus, it is crucial to choose appropriate device for phase modulation. There are three kinds of phase modulation for pulse tube cryocoolers at present, namely the orifice, the double inlets and the inertance tube. Compared to the orifice, the inertance tube uses the inertance effect of the oscillating gas inside a long and thin tube to adjust the phase difference, which has better performance and wider range of phase modulation. Compared with the method of using double inlets, there are no direct current flows inside the inertance tube. This can eliminate the vibration at the cold end of the pulse tube caused by the direct current flow. Therefore, the inertance tube for phase modulation is better for Stirling type high-frequency pulse tube cryocoolers.
Researches by Radebaugh and some other people indicate that: when the phase of the mass flow and pressure wave in the middle of the regenerator is the same, the cooling efficiency of the pulse tube cryocooler is the highest. At the same time, at the hot end of the regenerator, the phase of the mass flow leads in advance the phase of the pressure wave about 30 degrees. And at the cold end, the phase of the pressure wave lags the phase of the mass flow about 30 degrees. These combined means that at the inlet of the inertance tube, the phase of the mass flow should lags the pressure wave about 60 degrees. Therefore, the inertance tube should be capable of at least 60 degrees of phase modulation. But for pulse tube cryocoolers which have smaller PV work, it is not realistic to realize that the phase of the mass flow lags the pressure wave about 60 degrees. Thus, it is urgently necessary to increase the acoustic power at the hot end of pulse tube and will improve the phase modulation capability of the inertance tube, in order to provide a proper angle for pulse tube cryocoolers.
For an ideal regenerator, the ratio of the acoustic power at the hot end to the acoustic power at the cold end is proportional to the ratio of the temperature at the hot end to the cold end. According to this principle, putting regenerative materials inside the pulse tube at proper position will function as an acoustic power amplifier for the cold end. This is the core content of the present invention, which will offer necessary phase modulation for the inertance tube at the hot end in the pulse tube.
The object of the present invention is to overcome the shortcomings of present technology and provide an acoustic power amplifier for the phase modulation of the inertance tube and the pulse tube cryocooler.
The acoustic power amplifier for inertance tube phase modulation is: a metal tube filled its inside with regenerative materials, said tube being located at a distance X from the pulse tube; or regenerative materials inside the pulse tube, the regenerative materials having a length of L and a distance to the hot end of the pulse tube being X, satisfying the requirement of X−L>0.
A pulse tube cryocooler with an acoustic power amplifier consists of a first stage compressor, a first stage regenerator, a first stage pulse tube, a first stage acoustic power amplifier, a first stage inertance tube, and a first stage reservoir. The first stage compressor connects with the hot end of the first stage regenerator. The cold end of the first stage regenerator connects with the cold end of the first stage pulse tube. The hot end of the first stage pulse tube connects with the first stage reservoir through the first stage inertance tube. The first stage acoustic power amplifier is inside the first stage pulse tube. The distance between the first stage acoustic power amplifier and the hot end of the pulse tube is X. The length of the first stage acoustic power amplifier is L. X−L>0.
A pulse tube cryocooler with an acoustic power amplifier consists of a first stage compressor, a first stage regenerator, a first stage pulse tube, a first stage acoustic power amplifier, a first stage inertance tube, a first stage reservoir, a second stage compressor, a precooling section of second stage regenerator, a section of second stage regenerator, a second stage pulse tube, a second stage acoustic power amplifier, a second stage inertance tube, a second stage reservoir, and a thermal bridge. The first stage compressor connects of the hot end of the first stage regenerator. The cold end of the first stage regenerator connects with the cold end of the first stage pulse tube. The hot end of the first stage pulse tube connects with the first stage reservoir through the first stage inertance tube. The first stage acoustic power amplifier is inside the first stage pulse tube. The distance between the hot end of the first stage pulse tube and the first stage acoustic power amplifier is X. The length of the first stage acoustic power amplifier is L. X−L>0. The second stage compressor connects the hot end of the precooling section of the second stage regenerator. The cold end of the precooling section of the second stage connects with the hot end of the second stage regenerator. The cold end of the second stage regenerator connects with the cold end of the second stage pulse tube. The hot end of the second stage pulse tube connects with the second stage reservoir through the second stage inertance tube. The second stage acoustic power amplifier is inside the second stage pulse tube. The distance between the acoustic power amplifier and the hot end of the pulse tube is X. The length of the second stage acoustic power amplifier is L. X−L>0. The cold end of the precooling section of the second regenerator connects with the cold end of the first stage through a thermal bridge.
A pulse tube cryocooler with an acoustic power amplifier consists of a first stage pulse tube, a first stage acoustic power amplifier, a first stage inertance tube, a first stage reservoir, a second stage compressor, a precooling section of the second stage regenerator, a second stage regenerator, a second stage pulse tube, a second stage acoustic power amplifier, a second stage inertance tube, a second stage reservoir and a thermal bridge. The cold end of the first stage pulse tube connects with the precooling section of the second stage regenerator. The hot end of the first stage pulse tube connects with the first stage reservoir through the first stage inertance tube. The first stage acoustic power amplifier is inside the pulse tube. The distance between the first stage acoustic power amplifier and the hot end of the pulse tube is X. The length of the first stage acoustic power amplifier is L. X−L>0. The second stage compressor connects with the hot end of the precooling section of the second stage regenerator. The cold end of the precooling section of the second stage regenerator connects with the hot end of the second stage regenerator. The cold end of the second stage regenerator connects with the cold end of the second stage pulse tube. The hot end of the second stage pulse tube connects with the second stage reservoir through the second stage inertance tube. The second stage acoustic power amplifier is inside the second stage pulse tube. The distance between the acoustic power amplifier and the hot end of the second stage pulse tube is X. The length of the second stage acoustic power amplifier is L. X−L>0.
The present invention improves the performance of the cryocooler through the addition of acoustic power amplifier, which increases the acoustic power at the hot end of the pulse tube hence increase the angle of phase modulation of the inertance tube. For an ideal regenerator, the ratio of the acoustic power at the hot end to the acoustic power at the cold end is proportional to the ratio of the temperature at the hot end to the cold end. According to this principle, putting regenerative materials inside the pulse tube at a proper position will function as an acoustic power amplifier for the cold end. It is the core content of the present invention. This will offer the necessary phase modulation for the inertance tube at the hot end in the pulse tube.
In the figures, C1 is the first stage linear compressor; RG1 is the first stage regenerator; PT1 is the first stage pulse; R1 is the first stage reservoir; I1 is the first stage inertance tube (ambient temperature); C2 is the second stage linear compressor; RG2 is the precooling section of the second stage regenerator; RG22 is the working section of the second stage regenerator; PT2 is the second stage pulse tube; R2 is the second stage reservoir (ambient temperature); I2 is the second stage inertance tube (ambient temperature); TB is a thermal bridge.
The acoustic power amplifier for inertance tube phase modulation is: a metal tube filled its inside with regenerative materials, said tube being located at a distance X from the pulse tube; or regenerative materials inside the pulse tube, the regenerative materials having a length of L and a distance to the hot end of the pulse tube being X, satisfying the requirement of X−L>0.
As shown in
As shown in
As shown in
In summary, the present invention includes two main parts. The first part is an acoustic power amplifier which is characterized as a metal tube filled with regenerative materials. The acoustic power amplifier can be inside the pulse tube and the distance between the acoustic power amplifier and the hot end of the pulse tube is X. Alternatively, the filling regenerative materials inside the pulse tube, whose length is L and distant X from the hot end, forms an acoustic power amplifier, where X−L>0. The second part is the acoustic power amplifier can be used separately or correspondently in single or multi stage thermal-coupled or gas-coupled pulse tube cryocoolers. The length L of acoustic power amplifier can be freely chosen according to specific requirements.
A comparison is offered below to illustrate the advantages of acoustic power amplifier for phase modulation in inertance tube. Three Stirling type high-frequency pulse tube cryocooler working at 35K are selected, one adopting an ambient temperature inertance tube for phase modulation, another adopting a low temperature inertance tube for phase modulation, and still another adopting an ambient temperature inertance tube with acoustic power amplifier for phase modulation. The acoustic power amplifier in the third one locates in the middle ⅓ of the pulse tube. Assuming the frequency is 40 Hz, charging pressure is 1.25 MP; adiabatic temperature at the hot end is 300 k. The volume of the reservoir is infinite. Pressure ratio of the cold end is 1.15.
1Acoustic power at the cold end of the pulse tube;
2Acoustic power the hot end of the pulse tube
3Pressure ratio at the hot end of the pulse tube;
4Phase difference provided by the inertance tube
From the above calculation, adding acoustic power amplifier not only improve the acoustic power at the hot end of pulse tube significantly but also decrease the pressure ratio, both of which benefit phase modulation of the system while avoiding the complexity of low temperature phase modulation.
Number | Date | Country | Kind |
---|---|---|---|
200910100287.4 | Jun 2009 | CN | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
---|---|---|---|---|
PCT/CN2010/071028 | 3/12/2010 | WO | 00 | 12/29/2011 |