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Thermo-acoustic system driven by liquefied natural gas cold energy

A technology of liquefied natural gas and thermoacoustic system, applied in the field of thermoacoustic system, can solve the problems of low efficiency, large viscous resistance and high sound power loss of thermoacoustic engines, and achieves improving the utilization rate of cooling capacity, reducing viscous resistance, reducing sound The effect of power loss

Inactive Publication Date: 2015-12-02
TONGJI UNIV
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  • Summary
  • Abstract
  • Description
  • Claims
  • Application Information

AI Technical Summary

Problems solved by technology

The structure of this patent is simple and the cost is low, but its power loss is high and the efficiency of the thermoacoustic engine is low
This patent has a simple structure and low cost, but the cold-end heat exchanger and resonance tube of the thermoacoustic engine are both in the room temperature environment outside the LNG cold energy supply system, and the viscous resistance of the gas in the resonance tube is relatively large, so that the acoustic power Relatively high loss

Method used

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  • Thermo-acoustic system driven by liquefied natural gas cold energy
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  • Thermo-acoustic system driven by liquefied natural gas cold energy

Examples

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Effect test

Embodiment 1

[0022] A thermoacoustic system driven by cold energy of liquefied natural gas, the thermoacoustic system is a standing wave thermoacoustic system, and its structure is as follows figure 1 As shown, the standing wave thermoacoustic system includes a hot-end gas storage 5, a hot-end heat exchanger 1, a regenerator 2, a cold-end heat exchanger 3, a resonant tube 4, and a cold-end gas storage 6 connected in sequence. The heater 1 and the hot-end gas storage 5 are arranged in the heat source 7, the cold-end heat exchanger 3, the resonant tube 4 and the cold-end gas storage 6 are provided with a jacket 10, and the jacket 10 is provided with a liquefied natural gas in and out. At the inlet and outlet, the liquefied natural gas cold source 8 is set in the jacket 10, the temperature of the heat source 7 is 30°C, and the temperature of the liquefied natural gas cold source 8 is -160°C;

[0023] Using the temperature difference between the hot end heat exchanger 1 and the cold end heat e...

Embodiment 2

[0025] A thermoacoustic system driven by cold energy of liquefied natural gas, the thermoacoustic system is a traveling wave thermoacoustic system, and its structure is as follows figure 2 As shown, the traveling wave thermoacoustic system includes a hot-end heat exchanger 1, a regenerator 2, a cold-end heat exchanger 3, and a resonant tube 4 connected in sequence, and returns to the hot-end heat exchanger 1, and the hot-end heat exchanger 1 Set in the heat source 7, the cold end heat exchanger 3 and the resonant tube 4 are provided with a jacket 10 outside, and the jacket 10 is provided with an inlet and an outlet for the liquefied natural gas to enter and exit, and the liquefied natural gas cold source 8 is arranged in the jacket 10 , the temperature of the heat source 7 is 30°C, and the temperature of the LNG cold source 8 is -160°C;

[0026] Using the temperature difference between the hot end heat exchanger 1 and the cold end heat exchanger 3, a temperature gradient is e...

Embodiment 3

[0028] A thermoacoustic system driven by cold energy of liquefied natural gas. The thermoacoustic system is a traveling wave-standing wave hybrid thermoacoustic system. Its structure is as follows: image 3 As shown, the traveling wave-standing wave hybrid thermoacoustic system includes a thermal buffer tube 11, a hot end heat exchanger 1, a regenerator 2, a cold end heat exchanger 3, a feedback tube 9, and a resonance tube 4 connected in sequence. The buffer tube 11 is connected to the resonant tube 4, and the thermal buffer tube 11 is provided with an insulating tube 12 to ensure that the wall surface of the thermal buffer tube 11 is adiabatic. The hot end heat exchanger 1 is arranged in the heat source 7, and the cold end heat exchanger 3, feedback The pipe 9 and the resonant pipe 4 are provided with a jacket 10 outside, and the jacket 10 is provided with inlets and outlets for the entry and exit of liquefied natural gas. The cold source 8 of the liquefied natural gas is arr...

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Abstract

The invention relates to a thermo-acoustic system driven by a liquefied natural gas cold energy. The thermo-acoustic system comprises a heat source (7), a liquefied natural gas cold energy (8), a hot end heat exchanger (1), a heat regenerator (2), a cold end heat exchanger (3) and a resonant cavity, wherein the hot end heat exchanger, the heat regenerator, the cold end heat exchanger and the resonant cavity are connected in sequence; the hot end heat exchanger (1) is connected with the heat source (7); the cold end heat exchanger (3) and a resonant tube (4) are arranged in the liquefied natural gas cold energy (8); the temperature difference of the hot end heat exchanger (1) and the cold end heat exchanger (3) is utilized, and a temperature gradient is built inside the heat regenerator (2), so that pressure fluctuation is generated in the resonant tube (4), and cold energy is converted into acoustic power. Compared with the prior art, the thermo-acoustic system driven by the liquefied natural gas cold energy has the advantages that the structure is simple; the acoustic power loss is low; the efficiency of the thermo-acoustic system is high, and the like.

Description

technical field [0001] The invention relates to a thermoacoustic system, in particular to a thermoacoustic system driven by cold energy of liquefied natural gas. Background technique [0002] A thermoacoustic engine is a device that converts heat energy into sound work through the thermoacoustic effect. The advantages of a thermoacoustic engine are the absence of moving parts, low cost and ease of manufacture. However, the application of thermoacoustic engines is limited by their large size and low thermoacoustic conversion efficiency. In 1999, Backhaus and Swift of the Los Alamos National Laboratory in the United States published an article in Nature, introducing a thermoacoustic Stirling engine developed by them. Its thermal efficiency is as high as 0.3, which is completely comparable to the traditional internal combustion engine (0.25 —0.4) and piston Stirling engines (0.20-0.38). This has aroused the great attention of scientific researchers and industrial circles all...

Claims

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Application Information

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Patent Type & Authority Applications(China)
IPC IPC(8): F03G7/04
Inventor 林玉哲朱绍伟
Owner TONGJI UNIV
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