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Concepts Of Physics MCQ Edition [Volume 2]
Exam
Concepts Of Physics MCQ Edition [Volume 2]
Subject
Physics
Chapter
Specific Heat Capacities of Gases

Concepts Of Physics MCQ Edition [Volume 2] · Physics · Specific Heat Capacities of Gases

A Kundt tube is filled with an ideal gas having a density of 1.7 ×...

A Kundt tube is filled with an ideal gas having a density of 1.7×10−3 g cm−31.7 \times 10^{-3} \text{ g cm}^{-3} at a pressure of 1.5×105 Pa1.5 \times 10^5 \text{ Pa}. When the gas is resonated at a frequency of 3.0 kHz3.0 \text{ kHz}, nodes form at a separation of 6.0 cm6.0 \text{ cm}. Determine the molar heat capacities CpC_p and CVC_V of the gas.

Options

  1. A26 J K−1 mol−126 \text{ J K}^{-1} \text{ mol}^{-1} and 17.7 J K−1 mol−117.7 \text{ J K}^{-1} \text{ mol}^{-1}
  2. B29.1 J K−1 mol−129.1 \text{ J K}^{-1} \text{ mol}^{-1} and 20.8 J K−1 mol−120.8 \text{ J K}^{-1} \text{ mol}^{-1}
  3. C17.7 J K−1 mol−117.7 \text{ J K}^{-1} \text{ mol}^{-1} and 26 J K−1 mol−126 \text{ J K}^{-1} \text{ mol}^{-1}
  4. D20.8 J K−1 mol−120.8 \text{ J K}^{-1} \text{ mol}^{-1} and 12.5 J K−1 mol−112.5 \text{ J K}^{-1} \text{ mol}^{-1}

Correct answer

A. 26 J K−1 mol−126 \text{ J K}^{-1} \text{ mol}^{-1} and 17.7 J K−1 mol−117.7 \text{ J K}^{-1} \text{ mol}^{-1}

Step-by-step solution

The distance between two consecutive nodes in a Kundt tube is λ2\dfrac{\lambda}{2}.

λ2=6.0 cm⇒λ=12.0 cm=0.12 m\dfrac{\lambda}{2} = 6.0 \text{ cm} \Rightarrow \lambda = 12.0 \text{ cm} = 0.12 \text{ m}

The speed of sound in the gas is given by:

v=fλ=3000 Hz×0.12 m=360 m s−1v = f \lambda = 3000 \text{ Hz} \times 0.12 \text{ m} = 360 \text{ m s}^{-1}

The density of the gas is ρ=1.7×10−3 g cm−3=1.7 kg m−3\rho = 1.7 \times 10^{-3} \text{ g cm}^{-3} = 1.7 \text{ kg m}^{-3}.

The speed of sound is also given by v=γPρv = \sqrt{\dfrac{\gamma P}{\rho}}.

Squaring both sides and solving for γ\gamma:

γ=v2ρP=(360)2×1.71.5×105=129600×1.7150000=1.4688\gamma = \dfrac{v^2 \rho}{P} = \dfrac{(360)^2 \times 1.7}{1.5 \times 10^5} = \dfrac{129600 \times 1.7}{150000} = 1.4688

Using the relation Cp−CV=RC_p - C_V = R and CpCV=γ\dfrac{C_p}{C_V} = \gamma:

CV=Rγ−1=8.3141.4688−1=8.3140.4688≈17.7 J K−1 mol−1C_V = \dfrac{R}{\gamma - 1} = \dfrac{8.314}{1.4688 - 1} = \dfrac{8.314}{0.4688} \approx 17.7 \text{ J K}^{-1} \text{ mol}^{-1}

Cp=CV+R=17.7+8.314≈26.0 J K−1 mol−1C_p = C_V + R = 17.7 + 8.314 \approx 26.0 \text{ J K}^{-1} \text{ mol}^{-1}

Thus, Cp=26 J K−1 mol−1C_p = 26 \text{ J K}^{-1} \text{ mol}^{-1} and CV=17.7 J K−1 mol−1C_V = 17.7 \text{ J K}^{-1} \text{ mol}^{-1}.
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