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An ideal gas is heated by 160J at consta...

An ideal gas is heated by `160J` at constant pressure, its temperature rises by `50^@` and if `240J` of heat is supplied at constant volume, temperature rises by `100^@C` , then its degree of freedom should be

A

3

B

5

C

6

D

7

Text Solution

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The correct Answer is:
To solve the problem, we will follow these steps: ### Step 1: Understand the relationship between heat, temperature change, and specific heat at constant pressure (Cp). When heat \( Q \) is added to an ideal gas at constant pressure, the relationship is given by: \[ Q = n C_p \Delta T \] where: - \( Q \) is the heat added, - \( n \) is the number of moles, - \( C_p \) is the specific heat at constant pressure, - \( \Delta T \) is the change in temperature. ### Step 2: Apply the equation for the first scenario (constant pressure). From the problem, we know: - \( Q = 160 \, J \) - \( \Delta T = 50 \, °C \) Substituting these values into the equation: \[ 160 = n C_p (50) \] This simplifies to: \[ n C_p = \frac{160}{50} = 3.2 \quad \text{(1)} \] ### Step 3: Understand the relationship for heat at constant volume (Cv). Similarly, when heat \( Q \) is added at constant volume: \[ Q = n C_v \Delta T \] where: - \( C_v \) is the specific heat at constant volume. ### Step 4: Apply the equation for the second scenario (constant volume). From the problem, we know: - \( Q = 240 \, J \) - \( \Delta T = 100 \, °C \) Substituting these values into the equation: \[ 240 = n C_v (100) \] This simplifies to: \[ n C_v = \frac{240}{100} = 2.4 \quad \text{(2)} \] ### Step 5: Relate Cp and Cv to the degree of freedom (F). The relationship between \( C_p \) and \( C_v \) is given by: \[ C_p - C_v = R \] Also, we know: \[ \gamma = \frac{C_p}{C_v} = 1 + \frac{2}{F} \] ### Step 6: Express \( C_p \) and \( C_v \) in terms of \( n \). From equations (1) and (2): \[ C_p = \frac{3.2}{n} \quad \text{and} \quad C_v = \frac{2.4}{n} \] ### Step 7: Substitute \( C_p \) and \( C_v \) into the equation for \( \gamma \). Using the relationship: \[ \gamma = \frac{C_p}{C_v} = \frac{\frac{3.2}{n}}{\frac{2.4}{n}} = \frac{3.2}{2.4} = \frac{32}{24} = \frac{4}{3} \] ### Step 8: Solve for \( F \). Using the equation: \[ \frac{4}{3} = 1 + \frac{2}{F} \] Subtracting 1 from both sides: \[ \frac{4}{3} - 1 = \frac{2}{F} \] This simplifies to: \[ \frac{1}{3} = \frac{2}{F} \] Cross-multiplying gives: \[ F = 6 \] ### Final Answer: The degree of freedom \( F \) of the gas is **6**. ---
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