equations - =-= = rev int 1 2 S S kJ/K units T Q S T Q dS...

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( 29 1 2 T T mc Q - = L H net L net Q Q W Q W - = + = = H Q out in 1 1 in put to have you what you want what - = - = - = = = H L th H L H H in out H net th Q Q Q Q Q Q W W Q W η H net Q W L H L in net L AC R Q Q Q W Q COP - = = , , in net H HP W Q COP , = H L Q Q - = 1 H L rev T T - = 1 1 1 - = - = L H L H L R Q Q Q Q Q COP 1 1 , - = L H rev R T T COP 0 T Q δ 0 so engine heat Carnot a for but = - = = - = L L H H rev L H L H L L H H T Q T Q T Q T T Q Q T Q T Q T Q 0 get we cycles, le irreversib and reversible both the for Q input heat of value the assuming , , , H , , < - = - < - < L irr L H H irr rev L irr L rev L H irr L H rev irr T Q T Q T Q Q Q Q Q Q Q W W = = 0 0 dP dV ENTROPY call hich we property w a of al differenti the is so 0 rev rev T Q T Q =
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Unformatted text preview: =-= = rev int 1 2 S S kJ/K units T Q S T Q dS rev = =-T Q Q T S 1 S 1 2 never le irreversib reversible 2 1 1 2 &lt; = + =-= gen gen gen gen S S S S T Q S S S...
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This note was uploaded on 03/20/2011 for the course ME 114 taught by Professor Okamoto during the Spring '08 term at San Jose State University .

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