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Isothermal process on p-V, T-V, and p-T diagrams

Isothermal process on p-V, T-V, and p-T diagrams

Isothermal process on p-V, T-V, and p-T diagrams

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p<br />

a<br />

Q in<br />

W < 0<br />

Q out<br />

For a refrigerator, the<br />

cycle is always<br />

counterclockwise.<br />

Expansi<strong>on</strong> happens at<br />

low pressure,<br />

compressi<strong>on</strong> at high<br />

pressure <strong>and</strong> this takes<br />

work. Heat is drawn in at<br />

T C <strong>and</strong> expelled at T H .<br />

c<br />

V<br />

Refrigerators (heat pumps)<br />

Q C = Q in<br />

Q H = Q out<br />

W in = –W<br />

PHYS 1101, Winter 2009, Prof. Clarke 37<br />

p<br />

a<br />

S 1<br />

T C<br />

S2 Qout d<br />

adiabats<br />

b<br />

isotherms<br />

T H<br />

Q in<br />

c<br />

V<br />

As for an engine, the most<br />

optimal thermodynamical<br />

cycle for a refrigerator is the<br />

Carnot cycle traversed in<br />

the counterclockwise<br />

directi<strong>on</strong> (opposite to the<br />

engine).

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