[Physics] internal energy calculation of superheated vapor

thermodynamics

I know that steam behaves like an ideal gas. Thus, the internal energy is a function only of temperature. I also know that $U=C_{V}(T_2-T_1)$, where
$C_V$ is the specific heat at constant volume. My question is:
Since $C_V$ is a function of temperature, which value of $C_V$ should I take, or should I just use the values of internal energies on the steam tables? Thanks in advance!

Best Answer

When the specific heat varies with temperature, you need an integral to compute the change in internal energy:

$$ \Delta U = \int_{T_1}^{T_2} c_V(T) \, dT $$

If you have a table of the specific heats at various temperatures, you can make a numerical estimate of this integral using the trapezoidal rule. For example, suppose that we are trying to find the change in internal energy between 400 K and 600 K and we know that the specific heat is $1.901 \frac{\text{kJ}}{\text{kg} \cdot \text{K}}$ at 400 K; $1.954 \frac{\text{kJ}}{\text{kg} \cdot \text{K}}$ at 500 K; and $2.015 \frac{\text{kJ}}{\text{kg} \cdot \text{K}}$ at 600 K. Then $\Delta U$ is approximately

\begin{align} &\frac{1.901 \frac{\text{kJ}}{\text{kg} \cdot \text{K}} + 1.954 \frac{\text{kJ}}{\text{kg} \cdot \text{K}}}{2} \cdot (500 \,\text{K} - 400 \,\text{K}) \\ + \,&\frac{1.954 \frac{\text{kJ}}{\text{kg} \cdot \text{K}} + 2.015 \frac{\text{kJ}}{\text{kg} \cdot \text{K}}}{2} \cdot (600 \,\text{K} - 500 \,\text{K}) \\ = \,&391.2 \,\frac{\text{kJ}}{\text{kg}} \end{align}

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