Question:

An ideal gas initially at 0°C temperature, is compressed suddenly to one fourth of its volume. If the ratio of specific heat at constant pressure to that at constant volume is \( \frac{3}{2} \), the change in temperature due to the thermodynamics process is         K.

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The change in temperature can be derived using the thermodynamic relation between pressure, volume, and temperature for adiabatic processes. Use the initial and final conditions to calculate the change.
Updated On: Oct 31, 2025
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Approach Solution - 1

Given Data: 

Initial temperature, $T_1 = 0^\circ C = 273 \text{ K}$ 
Final volume, $V_2 = \dfrac{V_1}{4}$ 
Ratio of specific heats, $\gamma = \dfrac{C_p}{C_v} = \dfrac{3}{2}$

Step 1: Relation for adiabatic process

For a sudden (adiabatic) compression, $T_2 V_2^{\gamma - 1} = T_1 V_1^{\gamma - 1}$

Step 2: Substitute given values

$\displaystyle \frac{T_2}{T_1} = \left(\frac{V_1}{V_2}\right)^{\gamma - 1}$ 

$\displaystyle \frac{T_2}{273} = \left(\frac{V_1}{V_1/4}\right)^{\frac{3}{2} - 1}$ 

$\displaystyle \frac{T_2}{273} = 4^{\frac{1}{2}} = 2$

Step 3: Calculate final temperature

$T_2 = 2 \times 273 = 546 \text{ K}$

Step 4: Change in temperature

$\Delta T = T_2 - T_1 = 546 - 273 = 273 \text{ K}$

Final Answer:

$\boxed{273\ \text{K}}$

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Approach Solution -2

To determine the temperature change during an adiabatic compression of an ideal gas, we follow these steps:

1. Initial Conditions:
- Initial temperature (T₁) = 0°C = 273 K
- Initial volume (V₁)
- Final volume (V₂) = V₁/4
- Ratio of specific heats (γ) = Cₚ/Cᵥ = 3/2

2. Adiabatic Process Relation:
For an adiabatic process, we use:

\[ T V^{\gamma - 1} = \text{constant} \]
Which gives the relation:

\[ T_1 V_1^{\gamma - 1} = T_2 V_2^{\gamma - 1} \]

3. Calculate Final Temperature:
Solving for the final temperature T₂:

\[ T_2 = T_1 \left( \frac{V_1}{V_2} \right)^{\gamma - 1} = 273 \left( \frac{V_1}{V_1/4} \right)^{1/2} = 273 \times (4)^{1/2} = 273 \times 2 = 546 \text{ K} \]

4. Determine Temperature Change:
The change in temperature is:

\[ \Delta T = T_2 - T_1 = 546 \text{ K} - 273 \text{ K} = 273 \text{ K} \]

Key Points:
- The process is adiabatic (no heat transfer)
- Volume reduces to 1/4th of original
- Temperature doubles due to the compression
- γ = 3/2 indicates a monatomic ideal gas

Final Answer:
The temperature increases by \(\boxed{273 \text{ K}}\).

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