Question 2.17: A) Using the steam tables, find the change in specific entha...

Liquid water enters a steady-state heat exchanger at P=10 bar and T=80°C, and exits as saturated water vapor at P=10 bar.

A) Using the steam tables, find the change in specific enthalpy for this process.
B) Using the approximation that \hat { { C }_{ p } } = 4.19 J/g·K for liquid water, find the change in enthalpy when liquid water is heated from 80°C to its boiling point at P = 10 bar.
C) How do the answers to parts A and B compare to each other? What is the reason for the difference between them?

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A) Water at 10 bar and 80^{\circ} \mathrm{C} \rightarrow 335.77 \frac{\mathrm{kJ}}{\mathrm{kg}}

Saturated vapor at 10 \mathrm{bar} \rightarrow 2777.11 \frac{\mathrm{kJ}}{\mathrm{kg}}

\begin{aligned}&\Delta \widehat{\mathrm{H}}=\widehat{\mathrm{H}}_{\mathrm{out}}-\widehat{\mathrm{H}}_{\mathrm{in}}\\&2777.11 \frac{\mathrm{kJ}}{\mathrm{kg}}-335.77 \frac{\mathrm{kJ}}{\mathrm{kg}}=\mathbf{2 4 4 1 . 3 4} \frac{\mathbf{k J}}{\mathbf{k g}}\end{aligned}

B) The boiling point of water at 10 bar, according to the steam tables, is 179.88°C, or 453 K. Thus, the increase in temperature (ΔT) is almost exactly 100°C.

\begin{aligned}\Delta \widehat{\mathrm{H}} & =\int_{\mathrm{T}_{\mathrm{in}}}^{\mathrm{T}_{\text {out }}} \hat{C}_{P} \mathrm{dT} \\\Delta \widehat{\mathrm{H}} & =\int_{353 \mathrm{~K}}^{453 \mathrm{~K}} 4.19 \frac{\mathrm{J}}{\mathrm{gK}} \mathrm{dT}=4.19 \frac{\mathrm{J}}{\mathrm{g} \mathrm{K}}(453 \mathrm{~K}-353 \mathrm{~K})=\bf 419 \frac{\mathbf{J}}{\mathbf{g}}=\mathbf{4 1 9} \frac{\mathbf{k J}}{\mathbf{k g}}\end{aligned}

C) There is a large difference between the answers to A and B. The value found through the steam tables is the change in specific enthalpy from 80°C liquid that has been heated to its boiling point (at 10 bar) and then converted to a vapor. This extra heat added to convert a liquid to a vapor is very significant. In part b), we ignored this step—the final state was liquid water at its boiling point (at 10 bar).

We must always remember, the expression \mathrm{d} \underline{\mathrm{H}}=\mathrm{C}_{\mathrm{P}} \mathrm{dT}, or \mathrm{d} \widehat{\mathrm{H}}=\hat{C}_{P} \mathrm{dT}, is valid when a temperature change is the only thing occurring in a process-it does not account for changes in pressure or changes in phase.

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