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An ideal gas is taken through a process ...

An ideal gas is taken through a process `PT^3` = constant . The coefficient of thermal expansion of the gas in the given process in n/T. Find n.

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To solve the problem, we need to find the coefficient of thermal expansion of an ideal gas undergoing a process where \( P T^3 = \text{constant} \). We will denote the coefficient of thermal expansion as \( \gamma \). ### Step-by-Step Solution: 1. **Understand the Coefficient of Thermal Expansion**: The coefficient of thermal expansion \( \gamma \) is defined as: \[ \gamma = \frac{1}{V} \frac{dV}{dT} \] 2. **Relate Pressure and Volume**: From the given process \( P T^3 = \text{constant} \), we can express pressure \( P \) in terms of volume \( V \) and temperature \( T \). Using the ideal gas law \( PV = nRT \), we can write: \[ P = \frac{nRT}{V} \] Therefore, substituting into the process equation gives: \[ \frac{nRT}{V} T^3 = C \quad \text{(where C is a constant)} \] Simplifying this, we get: \[ \frac{nR T^4}{V} = C \] Rearranging gives: \[ V = \frac{nR T^4}{C} \] 3. **Differentiate Volume with Respect to Temperature**: To find \( \frac{dV}{dT} \), we differentiate \( V \) with respect to \( T \): \[ V = \frac{nR}{C} T^4 \] Thus, \[ \frac{dV}{dT} = \frac{nR}{C} \cdot 4T^3 \] 4. **Substituting into the Coefficient of Thermal Expansion**: Now, substituting \( \frac{dV}{dT} \) back into the expression for \( \gamma \): \[ \gamma = \frac{1}{V} \frac{dV}{dT} = \frac{1}{\frac{nR}{C} T^4} \cdot \left( \frac{nR}{C} \cdot 4T^3 \right) \] Simplifying this gives: \[ \gamma = \frac{4T^3}{T^4} = \frac{4}{T} \] 5. **Identifying \( n \)**: We are given that \( \gamma = \frac{n}{T} \). From our calculation, we have: \[ \gamma = \frac{4}{T} \] Therefore, comparing both expressions: \[ \frac{n}{T} = \frac{4}{T} \] This leads us to conclude: \[ n = 4 \] ### Final Answer: \[ n = 4 \]
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