If 300 J of heat energy is used to raise the temperature of one mole of an ideal gas by 10 K at constant pressure, then heat energy required to raise its temperature by 10 K at constant volume is $(R=8.3\text{ J mol}^{-1}\text{K}^{-1})$
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Logic Tip: You can calculate this even faster without finding $C_p$ explicitly. The difference in heat is simply the work done: $Q_p - Q_v = nR\Delta T$. Therefore, $Q_v = Q_p - nR\Delta T = 300 - (1)(8.3)(10) = 300 - 83 = 217$ J.
Concept:
The heat energy required to change the temperature of a gas is given by:
$Q_p = n C_p \Delta T$ (at constant pressure)
$Q_v = n C_v \Delta T$ (at constant volume)
The molar specific heats are related by Mayer's relation: $C_p - C_v = R$, where $R$ is the universal gas constant.
Step 1: Calculate the molar heat capacity at constant pressure ($C_p$).
We are given:
$Q_p = 300\text{ J}$
$n = 1\text{ mole}$
$\Delta T = 10\text{ K}$
Using the formula $Q_p = n C_p \Delta T$:
$$300 = (1) \cdot C_p \cdot (10)$$
$$C_p = \frac{300}{10} = 30\text{ J mol}^{-1}\text{K}^{-1}$$
Step 2: Calculate the molar heat capacity at constant volume ($C_v$).
Using Mayer's relation $C_p - C_v = R$:
$$C_v = C_p - R$$
Substitute $C_p = 30$ and $R = 8.3$:
$$C_v = 30 - 8.3$$
$$C_v = 21.7\text{ J mol}^{-1}\text{K}^{-1}$$
Step 3: Calculate the heat required at constant volume ($Q_v$).
We need the heat to raise the temperature of the same 1 mole of gas by 10 K at constant volume:
$$Q_v = n C_v \Delta T$$
$$Q_v = (1) \cdot (21.7) \cdot (10)$$
$$Q_v = 217\text{ J}$$