Question:

4.0 g of a gas occupies 22.4 litres at NTP. The specific heat capacity of the gas at constant volume is 5.0 $JK^{-1} \, mol^{-1}$. If the speed of sound in this gas at NTP is 952 $ms^{-1}$, then the heat capacity at constant pressure is (Take gas constant R = 8.3 $JK^{-1} \, mol^{-1}$ )

Updated On: Jul 19, 2024
  • $7.0 \, JK^{-1} \, mol^{-1}$
  • $8.5 \, JK^{-1} \, mol^{-1}$
  • $8.0 \, JK^{-1} \, mol^{-1}$
  • $7.5 \, JK^{-1} \, mol^{-1}$
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The Correct Option is C

Approach Solution - 1

Since 4.0 g of a gas occupies 22.4 litres at NTP, so the molecular mass of the gas is
$M = 4.0 \, g\, mol^{-1}$
As the speed of the sound in the gas is
$v=\sqrt{\frac{?RT}{M}}$
where $?$ is the ratio of two specific heats, R is the universal gas constant and T is the temperature of the gas.
$\therefore \, \gamma = \frac{Mv^2}{RT}$
Here, $ \, \, \, M = 4.0 \, g \, mol^{-1} = 4.0 \times 10^{-3}kg\, mol^{-1}$
$v=952 \, ms^{-1}, R = 8.3\, JK^{-1}\, mol^{-1}$,
$v= 952\, mol^{-1}, R = 8.3\,JK^{-1}\, mol^{-1} $
and T = 273 K (at NTP)
$\therefore \gamma= \frac{(4.0 \times 10^{-3} \,kg\, mol^{-1})(952\,ms^{-1})^2}{(8.3 JK^{-1} mol^{-1})(273\,K)}=1.6$
By definition,
$\gamma=\frac{C_P}{V_V}$ or $C_P = \gamma C_V$
But $\gamma=1.6$ and $C_V=5.0 \,JK^{-1} \, mol^{-1}$
$\therefore \, \, C_P = (1.6)(5.0 JK^{1} \, mol^{-1})$
$ \, \, \, \, =8.0 \,JK^{-1} mol^{-1}$
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Approach Solution -2

Ans: The relation between constant pressure of an ideal gas (Cp) and constant volume (Cv) for an idea gas can be  given by: 

Cp-Cv =R 

Here, R is the molar gas constant, with the value of R= 8.3 JK⁻¹mol⁻¹ 

In the question, the value of Cp is given as 5.0JK⁻¹mol⁻¹ 

Substituting the values in the formula, 

Cp = Cv + R 

Cp = 5.0JK⁻¹mol⁻¹  + 8.3JK⁻¹mol⁻¹ 

 Cp = 13.3JK⁻¹mol⁻¹ 

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Concepts Used:

Waves

Waves are a disturbance through which the energy travels from one point to another. Most acquainted are surface waves that tour on the water, but sound, mild, and the movement of subatomic particles all exhibit wavelike properties. inside the most effective waves, the disturbance oscillates periodically (see periodic movement) with a set frequency and wavelength.

Types of Waves:

Transverse Waves -

Waves in which the medium moves at right angles to the direction of the wave.

Examples of transverse waves:

  • Water waves (ripples of gravity waves, not sound through water)
  • Light waves
  • S-wave earthquake waves
  • Stringed instruments
  • Torsion wave

The high point of a transverse wave is a crest. The low part is a trough.

Longitudinal Wave -

A longitudinal wave has the movement of the particles in the medium in the same dimension as the direction of movement of the wave.

Examples of longitudinal waves:

  • Sound waves
  • P-type earthquake waves
  • Compression wave