Problems and Solutions on Thermodynamics and Statistical Mechanics

(Ann) #1
Thermodynamics 65

Solution:


(1)
u=- s3
A3NV

(2) When no work is delivered, Tf will be maximum. Then

2
3

91 = /TTf c,dT = XfidT = -A(Tfi2 - ,


2
3
Q2 = /TT( c,dT = -A(TfI2 - Ti12).

Since 91 + 92 = 0, we have


The minimum of T corresponds to a reversible process; for which the change
in entropy of the system is zero. As

AS1 = c,dT/T = 2A(T;I2 - T;I2) ,


AS2 = l2 c,dT/T = 2A(T;12 - Tif2).


r
Tf

and AS1 + AS, = 0, we have


Hence
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