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.
Initial temperature, $T_1 = 0^\circ C = 273 \text{ K}$
Final volume, $V_2 = \dfrac{V_1}{4}$
Ratio of specific heats, $\gamma = \dfrac{C_p}{C_v} = \dfrac{3}{2}$
For a sudden (adiabatic) compression, $T_2 V_2^{\gamma - 1} = T_1 V_1^{\gamma - 1}$
$\displaystyle \frac{T_2}{T_1} = \left(\frac{V_1}{V_2}\right)^{\gamma - 1}$
$\displaystyle \frac{T_2}{273} = \left(\frac{V_1}{V_1/4}\right)^{\frac{3}{2} - 1}$
$\displaystyle \frac{T_2}{273} = 4^{\frac{1}{2}} = 2$
$T_2 = 2 \times 273 = 546 \text{ K}$
$\Delta T = T_2 - T_1 = 546 - 273 = 273 \text{ K}$
$\boxed{273\ \text{K}}$
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 \(\boxed{273 \text{ K}}\).
Match the LIST-I with LIST-II for an isothermal process of an ideal gas system. 
Choose the correct answer from the options given below:
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