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Chapter-5 2 nd Law

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Thermal efficiency<br />

Desired output<br />

In general performance = =<br />

required input<br />

What I Get<br />

What I pay for<br />

In heat engines the desired output = net work output =<br />

W<br />

net , out<br />

the required input = heat supplied to system =<br />

Qin<br />

Thermal<br />

efficiency<br />

<br />

th<br />

or<br />

<br />

<br />

W<br />

th<br />

net,<br />

out<br />

Q<br />

<br />

in<br />

W<br />

net,<br />

out<br />

Q<br />

<br />

H<br />

Q<br />

in<br />

Q<br />

Q<br />

in<br />

out<br />

Q<br />

1<br />

Q<br />

L<br />

H<br />

1<br />

Q<br />

Q<br />

out<br />

in<br />

can Q out 0?<br />

No, because a) the cycle will not be complete!<br />

b)violates Kelvin-Plank statement.

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