First slide
Heat engine
Question

The below P-V digram represents the  thermodynamic cycle of an engine, operating with and ideal monoatomic gas. The amount of heat extracted from the source in a single cycle is     

Easy
Solution

{Q_{DA}} = ncv\Delta T = \frac{{nR\Delta T}}{{\gamma - 1}} = \frac{{3{P_0}{V_0}}}{2}

{Q_{AB}} = n{C_p}\Delta T = n\frac{{\gamma R}}{{\left( {\gamma - 1} \right)}}\Delta T

\Rightarrow {Q_{AB}} = \frac{5}{2}\left( {4{P_0}{V_0} - 2{P_0}{V_0}} \right)

= 5P0V0

{Q_{DA}} + {Q_{AB}} = \frac{{3{P_0}{V_0}}}{2} + 5{P_0}{V_0} = \frac{{13{P_0}{V_0}}}{2}

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