A real heat engine operates between temperatures TcTcT_c and ThThT_h. During a certain time, an amount QcQcQ_c of heat is released to the cold reservoir. During that time, what is the maximum amount of work WmaxWmaxW_max that the engine might have performed

Respuesta :

The maximum amount of work performed is

[tex]W_{max}=\frac{T_H-T_C}{T_C}Q_C[/tex]

Explanation:

The efficiency of a real heat engine is given by the equation:

[tex]\eta = 1-\frac{T_C}{T_H}[/tex] (1)

where

[tex]T_C[/tex] is the temperature of the cold reservoir

[tex]T_H[/tex] is the temperature of the hot reservoir

However, the efficiency of a real heat engine can be also written as:

[tex]\eta = \frac{W_{max}}{Q_H}[/tex]

where

[tex]W_{max}[/tex] is the maximum work done

[tex]Q_H[/tex] is the heat absorbed from the hot reservoir

[tex]Q_H[/tex] can be written as

[tex]Q_H=W_{max}+Q_C[/tex]

where

[tex]Q_C[/tex]is the heat released to the cold reservoir

So the previous equation can be also written as

[tex]\eta=\frac{W_{max}}{W_{max}+Q_C}[/tex] (2)

By combining eq.(1) and (2) we get

[tex]1-\frac{T_C}{T_H}=\frac{W_{max}}{W_{max}+Q}[/tex]

And re-arranging the equation and solving for [tex]W_{max}[/tex], we find

[tex]W_{max}=\frac{T_H-T_C}{T_C}Q_C[/tex]

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