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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
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Presentation Contents Introduction Project definition and physics of the problem Mathematical model Non-dimensionalization Conclusion and future of the work
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Single-Stage PTR Stirling-Type Pulse-Tube Refrigerator (S-PTR)
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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
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Gas parcel path in the Pulse-Tube
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Three-Stage PTR Stirling-Type Pulse-Tube Refrigerator (S-PTR)
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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
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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
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Mathematical model Conservation of mass Conservation of momentum Conservation of energy Equation of state (ideal gas) material derivative:
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One-dimensional formulation The viscous stress tensor ( ) The heat flux The viscous dissipation term ( is the dynamic viscosity ) ( is the thermal conductivity )
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One-dimensional formulation of Pulse-Tube
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One-dimensional formulation of Regenerator
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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
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Non-dimensionalised model of Pulse-Tube 2 2 dimensionless parameters:
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Non-dimensionalised model of Regenerator dimensionless parameters:
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Simplified System; Pulse-Tube Momentum equation:
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Simplified System; Regenerator
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Boundary Conditions ( Pulse-Tube ) velocity: Heat of Compression Aftercooler Regenerator Cold Heat Exchanger Pulse Tube Hot Heat Exchanger Orifice Reservoir QQ Q Compressor temperature:
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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 )
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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
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Thank you for your attention
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