Presentation is loading. Please wait.

Presentation is loading. Please wait.

Stirling-type pulse-tube refrigerator for 4 K M.A. Etaati, R.M.M. Mattheij, A.S. Tijsseling, A.T.A.M. de Waele Eindhoven University of Technology Mathematics.

Similar presentations


Presentation on theme: "Stirling-type pulse-tube refrigerator for 4 K M.A. Etaati, R.M.M. Mattheij, A.S. Tijsseling, A.T.A.M. de Waele Eindhoven University of Technology Mathematics."— Presentation transcript:

1 Stirling-type pulse-tube refrigerator for 4 K M.A. Etaati, R.M.M. Mattheij, A.S. Tijsseling, A.T.A.M. de Waele Eindhoven University of Technology Mathematics & Computer Science Dept. May. 09 2006

2 Presentation Contents Introduction Project definition and physics of the problem Mathematical model Non-dimensionalization Conclusion and future of the work

3 Single-Stage PTR Stirling-Type Pulse-Tube Refrigerator (S-PTR)

4 Single-stage Stirling-PTR Heat of Compression Aftercooler Regenerator Cold Heat Exchanger Pulse Tube Hot Heat Exchanger Orifice Reservoir QQ Q Compressor Pressure-time Temperature-distance

5 Gas parcel path in the Pulse-Tube

6 Three-Stage PTR Stirling-Type Pulse-Tube Refrigerator (S-PTR)

7 Three-Stage Stirling-PTR Reservoir 1Reservoir 2Reservoir 3 Orifice 1 Pulse- Tube 1 Reg. 1 Reg. 2 Reg. 3 Aftercooler Compressor Orifice 3 Pulse- Tube 3 Orifice 2 Pulse- Tube 2 Stage 1

8 Single-stage Stirling-PTR Heat of Compression Aftercooler Regenerator Cold Heat Exchanger Pulse Tube Hot Heat Exchanger Orifice Reservoir QQ Q Compressor Continuum fluid flow Reciprocating flow Newtonian flow Ideal gas No external forces act on the gas

9 Mathematical model Conservation of mass Conservation of momentum Conservation of energy Equation of state (ideal gas) material derivative:

10 One-dimensional formulation The viscous stress tensor ( ) The heat flux The viscous dissipation term ( is the dynamic viscosity ) ( is the thermal conductivity )

11 One-dimensional formulation of Pulse-Tube

12 One-dimensional formulation of Regenerator

13 Non-dimensionalisation “ ”: a typical gas density “ T a ”: room temperature “ p 0 ”: average pressure “ ”: the amplitude of the pressure variation “ ”: the amplitude of the velocity variation “ ”: the angular frequency of the pressure variation “ ”: a typical viscosity “ ”: a typical thermal conductivity of the gas “ ”: a typical thermal conductivity of the regenerator material “ ”: a typical heat capacity of the regenerator material

14 Non-dimensionalised model of Pulse-Tube 2 2 dimensionless parameters:

15 Non-dimensionalised model of Regenerator dimensionless parameters:

16 Simplified System; Pulse-Tube Momentum equation:

17 Simplified System; Regenerator

18 Boundary Conditions ( Pulse-Tube ) velocity: Heat of Compression Aftercooler Regenerator Cold Heat Exchanger Pulse Tube Hot Heat Exchanger Orifice Reservoir QQ Q Compressor temperature:

19 Boundary Conditions (Regenerator) velocity: ( known as the interface condition with pulse-tube ) Heat of Compression Aftercooler Regenerator Cold Heat Exchanger Pulse Tube Hot Heat Exchanger Orifice Reservoir QQ Q Compressor gas temperature: material temperature: pressure: ( given in the compressor side ) ( Neumann or Dirichlet Boundary Condition )

20 Conclusion and future of the work Single-stage S-PTR Three-stage S-PTR One-dimensional analysis of S-PTR Consideration of wall interaction effects Two-dimensional analysis

21 Thank you for your attention


Download ppt "Stirling-type pulse-tube refrigerator for 4 K M.A. Etaati, R.M.M. Mattheij, A.S. Tijsseling, A.T.A.M. de Waele Eindhoven University of Technology Mathematics."

Similar presentations


Ads by Google