We only have to substitute the solution for the integral of the work when the pressure remains constant:
W=∫V1V2pdV=pΔV=p(V2−V1) then, we substitute and find the value for W:W=0.5lb(50psia)(8−4)ft3 finally, we use the relation between the variables to find the value for W in Btu/lb:W=400lbpsia⋅ft3×5.40362psia⋅ft31BtuW=74.0244lbBtu
In conclusion, we find that the work done is equal to W=74.0244 But/lb.
Reference:
- Sears, F. W., & Zemansky, M. W. (1973). University physics.
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