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1 Jun Watanabe 2015.6.29 R&D status of highly efficient Stirling-type cryocooler for superconducting drive motor J Watanabe, T Nakamura, S Iriyama, T Ogasa,

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Presentation on theme: "1 Jun Watanabe 2015.6.29 R&D status of highly efficient Stirling-type cryocooler for superconducting drive motor J Watanabe, T Nakamura, S Iriyama, T Ogasa,"— Presentation transcript:

1 1 Jun Watanabe 2015.6.29 R&D status of highly efficient Stirling-type cryocooler for superconducting drive motor J Watanabe, T Nakamura, S Iriyama, T Ogasa, N Amemiya(Kyoto University, Japan); Y Ohashi(AISHIN SEIKI Co.,Ltd, Japan) CEC/ICMC 2015 June 29-July 4 2015 JW Marriott Starr Pass Resort & Spa, Tucson, Arizona

2 Outline 1. Background and objective 2. Specifications of developed compressor 3. Analytical and experimental method 4. Results and discussion 5. Development and test of pulse-tube cryocooler 6. Conclusion 2 Jun Watanabe 2015.6.29

3 3 1. Background and objective Advantages ・ High efficiency thanks to synchronous rotation ・ High torque density ・ Stable Rotation High Temperature Superconductor Induction/Synchronous Machine HTS-ISM Target ; Drive motor for the next generation electric vehicle Direct-drive without transmission gears

4 4 Jun Watanabe 2015.6.29 Fig.1 Schematic diagram of direct-derived power train system HTS ISM Inverter Battery Control unit Cryocooler 1. Background and objective Necessary functions of the cryocooler for HTS-ISM system ・ High efficiency ・ Light weight ・ Robustness against vibration Development of highly efficient Stirling-type cryocooler Development of linear actuator-type compressor

5 5 Jun Watanabe 2015.6.29 Input3000 W Coil Wire diameter1.6 mm Turn number of coil210 DC resistance0.6 Ω Rated stroke length±10 mm Piston diameter40 mm Table1 Specifications of compressor Fig.2 Schematic diagram of compressor Outer yoke Inner yoke Compression zone Piston Flexure bearing Permanent magnet Coil Moving magnet type linear actuator 2. Specifications of the developed actuator

6 Outer yoke Coil Shaft Permanent magnet 6 Jun Watanabe 2015.6.29 Finite element method analysis model S N S N x r Analysis by commercial software(JMAG-Designer Ⓡ ) Stator (Analysis conditions) External circuit : Single-phase current source Mover motion : Forced displacement Inner yoke Fig.3 Axisymmetric analysis model of the linear actuator 3. Analytical and experimental method Mover

7 7 Jun Watanabe 2015.6.29 Non-linear spring characteristic of the flexure bearing Orifice effect between piston and cylinder α Pressure changes in Stirling-cycle space Dumping of the drive coil Rigidity of the electromagnetic force ….etc Mover (piston+motor) Electrical input : Sinusoidal wave Fig.4 Analysis model of the actuator Electromagnetic field analysis code coupled with kinetic equation 3. Analytical and experimental method

8 8 Jun Watanabe 2015.6.29 8 Experimental method under no-load condition Fig.5 Schematic diagram of experiment under no-load condition Fig.6 Photograph of compressor assembly Voltage controlled inverter Compression - zone

9 9 Jun Watanabe 2015.6.29 Pressure gauge Needle valve Laser displacement sensor Buffer tank Load test of the compressor with He gas Fig.7 Photograph of experimental system under load condition Fig.9 PV work Fig.8 Laser displacement sensor Pressure Volume 3. Analytical and experimental method

10 10 (c) Current (a) Displacement x a =5 mm (b) Voltage x a =10 mm Drive frequency 42 Hz, Displacement 5 mm, 10 mm (experimental results) In case of x a =10 mm, the current waveform was distorted. Detailed examination by analysis The power factor was decreased because phase of the current waveform lagged. Jun Watanabe 2015.6.29 4. Results and discussion Fig.10 Experimental results under no-load condition

11 11 Fig.11 Power spectrum of current waveform The FFT analysis of the current waveform →Third harmonic component was highly included Current waveform obtained by superimposing the third harmonic (a) Effective power (b) Voltage Agreement between experimental and analysis results Reason for the current waveform distortion Fundamental only Third harmonic superimposed Fig.12 Experimental and analysis results under no-load condition Jun Watanabe 2015.6.29 4. Results and discussion

12 12 Fig.13 Analysis results of counter-electromotive force (a) Waveform (b) Effective value The counter-electromotive force in the case of forced displacement (analysis results) → Distortion of the waveform caused by nonlinear B-H curve Out of the linear Distortion Jun Watanabe 2015.6.29 4. Results and discussion Counter-electromotive force E s (V)

13 13 Jun Watanabe 2015.6.29 Output characteristics (analysis results) Fig.14 Output characteristics (analysis results) → Possibility of high efficiency and power factor Displacement 10.0 mm, Frequency 58 Hz, Current - displacement phase difference 90 ° 4. Results and discussion Mechanical output 2495 W Efficiency 90 % Power factor 0.83 Power P (W)

14 Frequency 59 Hz Pressure 2.5 MPa Input 200 V 14 Jun Watanabe 2015.6.29 Fig.15 Experimental results under load condition (a) Input power and PV work (b) Displacement (c) Efficiency and power factor Next target: ・ Improvement of efficiency ・ Comparison of analysis results 4. Results and discussion ・ Test at the rated displacement Power P (W) Displacement x ( mm )

15 5. Development and test of the pulse-tube cryocooler 15 Jun Watanabe 2015.6.29 z Heat exchanger Cold stage Pulse-tube Hot stage Fig.16 Photograph of pulse-tube cryocooler Cooling test of the pulse-tube cryocooler coupled with the compressor

16 16 Jun Watanabe 2015.6.29 Buffer tank volume 3485 cm 3 (1 gal) Copper pipe length 2 m Evaluation of pulse-tube cryocooler at 77 K Fig.17 Schematic diagram of experiment of pulse-tube cryocooler Table2 Specifications of buffer unit 5. Development and test of the pulse-tube cryocooler Voltage controlled inverter Compression - zone

17 Pressure 2.5 MPa, Input 160 V, Operational temperature 77 K 17 Jun Watanabe 2015.6.29 Fig.18 Experimental results of pulse-tube cryocooler Output 31.603 W COP 0.0276 (a) Input power and PV work (b) Cryocooler output (c) COP Next target: Re-try of cooling test with the improved compressor 5. Development and test of the pulse-tube cryocooler

18 18 Jun Watanabe 2015.6.29 6. Conclusion ・ Development of linear actuator-type compressor for cryocooler ・ Agreement between experimental and analytical results by considering the nonlinear B-H curve of the iron core ・ Modeling the linear actuator by the use of electromagnetic field analysis code coupled with kinetic equation ・ Obtaining analytical results which show possibility of high efficiency as well as high power factor ・ Conducting cooling test of the pulse-tube cryocooler

19 19 Jun Watanabe 2015.6.29 Future plan ・ Experiment at the rated displacement and development of analysis code considering thermodynamics of He gas ・ Development of Stirling-type cryocooler for HTS-ISM system 6. Conclusion


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