To determine the heat capacity at constant pressure, we can use the basic principles of thermodynamics related to ideal gases. Given data includes:
First, we need to determine the molar mass of the gas. At Normal Temperature and Pressure (NTP), 1 mole of an ideal gas occupies 22.4 L. Hence, the molar mass of the gas can be calculated as:
\text{Molar mass} = \frac{\text{mass of gas}}{\text{moles of gas}} = \frac{4.0 \, g}{1 \, mol} = 4.0 \, g/mol.
Next, we use the relation between the speed of sound, the adiabatic index (γ), and the specific heat capacities:
v = \sqrt{\frac{\gamma \cdot R \cdot T}{M}}
where γ is the adiabatic index, given by \gamma = \frac{C_p}{C_v}, and M is the molar mass in kg/mol.
Rearranging the speed of sound formula:
v^2 = \frac{\gamma \cdot R \cdot T}{M}
NTP conditions give us the temperature T = 273 \, K and the molar mass M = 0.004 \, kg/mol.
Using the speed of sound formula:
\gamma = \frac{v^2 \cdot M}{R \cdot T}
Insert the values:
\gamma = \frac{(952)^2 \cdot 0.004}{8.3 \times 273}
Calculating γ:
\gamma = \frac{(952)^2 \cdot 0.004}{8.3 \times 273} \approx 1.6
Now, using the relationship between gamma, C_p, and C_v:
\gamma = \frac{C_p}{C_v}
C_p = \gamma \cdot C_v
Substitute γ and C_v to find C_p:
C_p = 1.6 \times 5.0 \, JK^{-1} \, mol^{-1} = 8.0 \, JK^{-1} \, mol^{-1}
Therefore, the heat capacity at constant pressure is 8.0 \, JK^{-1} \, mol^{-1}, which matches the correct answer option.