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Cv and Cp denote the molar specific heat...

`C_v and C_p` denote the molar specific heat capacities of a gas at constant volume and constant pressure, respectively. Then

A

`C_p - C_v` is larger for a diatomic ideal gas then for a monatomic ideal gas

B

`C_p + C_v` is larger for a diatomic ideal gas than for a monatomic ideal gas

C

`C_P//C_v` is larger for a diatomic ideal gas than for a monatomic ideal gas

D

`C_p C_v` is larger for a diatomic ideal gas than for a monatomic ideal gas

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To solve the question regarding the molar specific heat capacities \( C_v \) and \( C_p \) of gases, we need to analyze the statements provided and derive the necessary relationships. Here’s a step-by-step solution: ### Step 1: Understanding \( C_v \) and \( C_p \) - \( C_v \) is the molar specific heat capacity at constant volume. - \( C_p \) is the molar specific heat capacity at constant pressure. - For any ideal gas, the relationship between \( C_p \) and \( C_v \) is given by: \[ C_p - C_v = R \] where \( R \) is the universal gas constant. ### Step 2: Analyzing the first statement - The first statement claims that \( C_p - C_v \) is greater for diatomic gases than for monatomic gases. - Since \( C_p - C_v = R \) is a constant for all ideal gases, this statement is **false**. ### Step 3: Analyzing the second statement - The second statement claims that \( C_p + C_v \) is greater for diatomic gases than for monatomic gases. - We know: \[ C_v = \frac{f}{2} R \] where \( f \) is the degrees of freedom. - For monatomic gases, \( f = 3 \) (translational motion only), so: \[ C_v = \frac{3}{2} R \] and thus: \[ C_p = C_v + R = \frac{3}{2} R + R = \frac{5}{2} R \] - For diatomic gases, \( f = 5 \) (3 translational + 2 rotational), so: \[ C_v = \frac{5}{2} R \] and thus: \[ C_p = C_v + R = \frac{5}{2} R + R = \frac{7}{2} R \] - Therefore: \[ C_p + C_v = \frac{5}{2} R + \frac{7}{2} R = 6R \quad \text{(for diatomic)} \] \[ C_p + C_v = \frac{3}{2} R + \frac{5}{2} R = 4R \quad \text{(for monatomic)} \] - This statement is **true**. ### Step 4: Analyzing the third statement - The third statement claims that \( \frac{C_p}{C_v} \) is greater for monatomic gases than for diatomic gases. - We know: \[ \frac{C_p}{C_v} = 1 + \frac{R}{C_v} \] - For monatomic gases: \[ \frac{C_p}{C_v} = 1 + \frac{R}{\frac{3}{2}R} = 1 + \frac{2}{3} = \frac{5}{3} \] - For diatomic gases: \[ \frac{C_p}{C_v} = 1 + \frac{R}{\frac{5}{2}R} = 1 + \frac{2}{5} = \frac{7}{5} \] - Since \( \frac{5}{3} > \frac{7}{5} \), this statement is **false**. ### Step 5: Analyzing the fourth statement - The fourth statement claims that \( C_p \cdot C_v \) is greater for diatomic gases than for monatomic gases. - We calculate: \[ C_p \cdot C_v \text{ for monatomic} = \left(\frac{5}{2} R\right) \left(\frac{3}{2} R\right) = \frac{15}{4} R^2 \] \[ C_p \cdot C_v \text{ for diatomic} = \left(\frac{7}{2} R\right) \left(\frac{5}{2} R\right) = \frac{35}{4} R^2 \] - Since \( \frac{35}{4} R^2 > \frac{15}{4} R^2 \), this statement is **true**. ### Conclusion The correct statements are: - Statement 2: \( C_p + C_v \) is greater for diatomic gases than for monatomic gases. - Statement 4: \( C_p \cdot C_v \) is greater for diatomic gases than for monatomic gases.

To solve the question regarding the molar specific heat capacities \( C_v \) and \( C_p \) of gases, we need to analyze the statements provided and derive the necessary relationships. Here’s a step-by-step solution: ### Step 1: Understanding \( C_v \) and \( C_p \) - \( C_v \) is the molar specific heat capacity at constant volume. - \( C_p \) is the molar specific heat capacity at constant pressure. - For any ideal gas, the relationship between \( C_p \) and \( C_v \) is given by: \[ C_p - C_v = R ...
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