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NEET PHYSICSMedium

4.0 g4.0 \text{ g} of a gas occupies 22.4 L22.4 \text{ L} at NTP. The specific heat capacity of the gas at constant volume is 5.0 J K1mol15.0 \text{ J K}^{-1}\text{mol}^{-1}. If the speed of sound in this gas at NTP is 952 ms1952 \text{ ms}^{-1}, then the heat capacity at constant pressure is: (Take gas constant R=8.3 J K1mol1R = 8.3 \text{ J K}^{-1}\text{mol}^{-1})

A

8.0 J K1mol18.0 \text{ J K}^{-1}\text{mol}^{-1}

B

7.5 J K1mol17.5 \text{ J K}^{-1}\text{mol}^{-1}

C

7.0 J K1mol17.0 \text{ J K}^{-1}\text{mol}^{-1}

D

8.5 J K1mol18.5 \text{ J K}^{-1}\text{mol}^{-1}

Step-by-Step Solution

  1. Find Molar Mass (MM): At NTP (Normal Temperature and Pressure, T=273 K,P=1 atmT = 273 \text{ K}, P = 1 \text{ atm}), 1 mole1 \text{ mole} of an ideal gas occupies 22.4 L22.4 \text{ L}. Given that 4.0 g4.0 \text{ g} of the gas occupies 22.4 L22.4 \text{ L}, the molar mass of the gas is: M=4.0 g mol1=4.0×103 kg mol1M = 4.0 \text{ g mol}^{-1} = 4.0 \times 10^{-3} \text{ kg mol}^{-1}
  2. Calculate the Ratio of Specific Heats (γ\gamma): The speed of sound vv in a gas is given by Laplace's formula : v=γRTMv = \sqrt{\frac{\gamma R T}{M}} Squaring both sides and solving for γ\gamma: γ=v2MRT\gamma = \frac{v^2 M}{R T} Substitute the given values (v=952 ms1v = 952 \text{ ms}^{-1}, M=4.0×103 kg mol1M = 4.0 \times 10^{-3} \text{ kg mol}^{-1}, R=8.3 J K1mol1R = 8.3 \text{ J K}^{-1}\text{mol}^{-1}, T=273 KT = 273 \text{ K}): γ=(952)2×4.0×1038.3×273=906304×0.0042265.9=3625.2162265.91.6\gamma = \frac{(952)^2 \times 4.0 \times 10^{-3}}{8.3 \times 273} = \frac{906304 \times 0.004}{2265.9} = \frac{3625.216}{2265.9} \approx 1.6
  3. Calculate Heat Capacity at Constant Pressure (CpC_p): We know that the ratio of molar heat capacities is γ=CpCv\gamma = \frac{C_p}{C_v} . Given Cv=5.0 J K1mol1C_v = 5.0 \text{ J K}^{-1}\text{mol}^{-1}, we can find CpC_p: Cp=γ×Cv=1.6×5.0=8.0 J K1mol1C_p = \gamma \times C_v = 1.6 \times 5.0 = 8.0 \text{ J K}^{-1}\text{mol}^{-1}
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