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A gas expands adiabatically at constant ...

A gas expands adiabatically at constant pressure such that:
`T prop(1)/(sqrt(V))`
The value of `gamma` i.e., `(C_(P)//C_(V))` of the gas will be:

A

1.3

B

1.5

C

1.7

D

2

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The correct Answer is:
To solve the problem, we need to analyze the relationship between temperature (T) and volume (V) during an adiabatic expansion of a gas. The given relationship is that temperature is inversely proportional to the square root of volume, which can be expressed mathematically as: \[ T \propto \frac{1}{\sqrt{V}} \] ### Step-by-Step Solution: 1. **Express the relationship mathematically**: From the proportionality, we can write: \[ T = \frac{K}{\sqrt{V}} \] where K is a constant. 2. **Rearranging the equation**: We can rewrite the equation as: \[ T \cdot \sqrt{V} = K \] or equivalently: \[ T \cdot V^{1/2} = K \] 3. **Using the adiabatic condition**: According to the adiabatic process, we have the relation: \[ T V^{\gamma - 1} = \text{constant} \] Let’s denote this constant as \( C \). Therefore: \[ T V^{\gamma - 1} = C \] 4. **Equating the two expressions**: From our earlier expression, we have: \[ T \cdot V^{1/2} = K \] Now, we can equate the two expressions: \[ T V^{\gamma - 1} = T V^{1/2} \] 5. **Canceling T (assuming T ≠ 0)**: Since T appears in both sides, we can cancel it out: \[ V^{\gamma - 1} = V^{1/2} \] 6. **Equating the exponents**: Since the bases are the same, we can equate the exponents: \[ \gamma - 1 = \frac{1}{2} \] 7. **Solving for gamma**: Rearranging gives: \[ \gamma = 1 + \frac{1}{2} = \frac{3}{2} \] 8. **Conclusion**: Thus, the value of gamma, which is the ratio of specific heats \( \frac{C_P}{C_V} \), is: \[ \gamma = 1.5 \] ### Final Answer: The value of \( \gamma \) is \( \frac{3}{2} \) or 1.5.
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