all the formula for work done in thermodynamics in all types of processes
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Explanation:
With the adiabatic condition of Equation 3.7. 14, we may write p as K/Vγ, where K=p1Vγ1=p2Vγ2. The work is therefore W=∫V2V1KVγdV=K1−γ(1Vγ−12−1Vγ−11)=11−γ(p2Vγ2Vγ−12−p1Vγ1Vγ−11)=11−γ(p2V2−p1V1)=11−1.40[(1.23×106N/m2)(40×10−6m3)−(1.00×105N/m2)(240×10−6m3)]=−63J.
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