Question 2.10: Show that Eq. (2.28) reduces to Eq. (2.3) for the case of a ...
Show that Eq. (2.28) reduces to Eq. (2.3) for the case of a closed system.
\frac{d(mU)_{CV} }{dt} + \Delta (H\dot{m} )_{fs} = \dot{Q } + \dot{W} (2.28)
\Delta U^{t} = Q + W (2.3)
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The second term of Eq. (2.28) is omitted in the absence of flowing streams:
\frac{d(mU)_{CV} }{dt} = \dot{Q} + \dot{W}
Integration over time gives
\Delta (mU)_{CV} = \int_{t_{1} }^{t_{2}}{\dot{\varrho} dt} + \int_{t_{1} }^{t_{2}}{\dot{W}dt}
or
\Delta U^{t} =Q + W
The Q and W terms are defined by the integrals of the preceding equation.
Note here that Δ indicates a change over time, not from an inlet to an outlet.
One must be aware of its context to discern its meaning.
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