Question:

An ideal gas is compressed in volume by a factor of 2,while keeping its temperature constant. The speed of sound in it is: 

Updated On: Apr 7, 2025
  • doubled

  • unchanged 

  • reduced to half

  • increased by 4 times 

  • reduced by 4 times 

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The Correct Option is B

Approach Solution - 1

Given:

  • An ideal gas is compressed in volume by a factor of 2 (V → V/2).
  • The temperature (T) is kept constant during this process.
  • We need to determine how the speed of sound in the gas changes.

Step 1: Speed of Sound in an Ideal Gas

The speed of sound (c) in an ideal gas is given by:

\[ c = \sqrt{\frac{\gamma RT}{M}} \]

where:

  • γ = adiabatic index (ratio of specific heats)
  • R = universal gas constant
  • T = absolute temperature
  • M = molar mass of the gas

 

Step 2: Analyze the Given Conditions

Key observations:

  1. The temperature T is constant (given).
  2. γ, R, and M are properties of the gas that remain unchanged.
  3. The volume change affects density, but not the speed of sound directly.

 

Step 3: Conclusion

Since none of the terms in the speed of sound equation (γ, R, T, M) are changing, the speed of sound remains unchanged despite the volume compression.

Final Answer: The speed of sound in the gas is unchanged.

Answer: \(\boxed{B}\)

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Approach Solution -2

When an ideal gas undergoes isothermal compression (i.e., the temperature remains constant) and its volume is reduced by a factor of 2, we can determine the effect on the speed of sound in the gas.

The speed of sound in an ideal gas is given by the equation:
\[ v = \sqrt{\frac{\gamma P}{\rho}} \]

where:
- \( v \) is the speed of sound,
- \( \gamma \) is the adiabatic index (ratio of specific heats),
- \( P \) is the pressure,
- \( \rho \) is the density of the gas.

For an ideal gas, we have the relation \( P = \rho RT \), where \( R \) is the specific gas constant and \( T \) is the temperature. The density \( \rho \) can be expressed in terms of pressure and temperature:
\[ \rho = \frac{P}{RT} \]

Substituting this into the speed of sound equation:
\[ v = \sqrt{\frac{\gamma P}{\frac{P}{RT}}} = \sqrt{\gamma RT} \]

Notice that in this form, the speed of sound \( v \) in an ideal gas depends only on the temperature \( T \) and the gas constant \( R \). It does not explicitly depend on the pressure or the volume of the gas.

Given that the temperature \( T \) remains constant during the isothermal compression and \( R \) is a constant for a given gas, the speed of sound in the gas does not change due to the isothermal compression.

Therefore, even though the volume is compressed by a factor of 2, the speed of sound in the gas remains the same as before the compression.

Thus, the speed of sound in the gas after the isothermal compression remains unchanged.
So The correct answer is Option is (B):unchanged 

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Concepts Used:

Work Done Thermodynamics

In thermodynamics, work is a way of energy transfer from a system to surroundings, under the influence of external factors such gravity, electromagnetic forces, pressure/volume etc.

Energy (ΔU) can cross the boundary of a system in two forms -> Work (W) and Heat (q). Both work and heat refer to processes by which energy is transferred to or from a substance.

ΔU=W+q

Work done by a system is defined as the quantity of energy exchanged between a system and its surroundings. It is governed by external factors such as an external force, pressure or volume or change in temperature etc.

Work (W) in mechanics is displacement (d) against a resisting force (F).

Work has units of energy (Joule, J)