Evolution of temperature (adiabatic procsses)

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ted1986
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Hello,

I'm trying to derive a differential equation as requested in the attached exercise (thermal1.jpg).
I'm not quite sure my solution is the right answer (my_solution1.jpg).
How do I get rid of the energy dU ?

Thnks


Ted
 
Attachments
  • Printed exercise text stating the dimensionless entropy per particle satisfies dT/T (3σ + 3/2) − dρ/ρ (1 + σ) = ds, with instructions to derive a differential equation for T(ρ) in adiabatic processes and solve it for σ << 1 and σ >> 1.
    thermal1.jpg
    18.9 KB · Views: 443
  • Handwritten-style typeset derivation titled 'My solution:' showing ds = (dT/T)(3σ + 3/2) − (dρ/ρ)(1+σ), rewritten as dT/dρ = 2T/(3+6σ) (ds/dρ + (1+σ)/ρ), then ds = (dU + PdV)/T, leading to dT/dρ = 2/(3+6σ) (dU/dρ − PV/ρ + T(1+σ)/ρ).
    my_solution1.jpg
    16.8 KB · Views: 434
well in an adiabatic processes dQ = 0 so ds = 0 giving you quite a simple derivation of the differential equation
 
sgd37 said:
well in an adiabatic processes dQ = 0 so ds = 0 giving you quite a simple derivation of the differential equation


OK, It sure gives a simple derivation of the differential equation, but what is the physical explanation for that?

Thanks
 
it most generally means that it is a reversible process