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If Q amount of heat is given to a diatom...

If `Q` amount of heat is given to a diatomic ideal gas in a process in which the gas perform a work `(2Q)/(3)` on its surrounding. Find the molar heat capacity (in terms of `R`) for the process.

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To find the molar heat capacity \( C \) for the process involving a diatomic ideal gas, we can follow these steps: ### Step 1: Understand the relationship between heat, work, and internal energy According to the first law of thermodynamics, we have: \[ Q = \Delta U + W \] Where: - \( Q \) is the heat added to the system, - \( \Delta U \) is the change in internal energy, - \( W \) is the work done by the system. ### Step 2: Substitute the given values From the problem, we know: - \( Q \) is the amount of heat given to the gas, - The work done \( W = \frac{2Q}{3} \). Substituting this into the first law equation gives: \[ Q = \Delta U + \frac{2Q}{3} \] ### Step 3: Solve for change in internal energy \( \Delta U \) Rearranging the equation to solve for \( \Delta U \): \[ \Delta U = Q - \frac{2Q}{3} = \frac{Q}{3} \] ### Step 4: Relate internal energy change to temperature change For an ideal gas, the change in internal energy is also given by: \[ \Delta U = n C_V \Delta T \] Where: - \( n \) is the number of moles, - \( C_V \) is the molar heat capacity at constant volume, - \( \Delta T \) is the change in temperature. ### Step 5: Use the value of \( C_V \) for a diatomic gas For a diatomic ideal gas, the molar heat capacity at constant volume is: \[ C_V = \frac{5R}{2} \] Thus, we can write: \[ \Delta U = n \left(\frac{5R}{2}\right) \Delta T \] ### Step 6: Set the two expressions for \( \Delta U \) equal to each other Now we can equate the two expressions for \( \Delta U \): \[ \frac{Q}{3} = n \left(\frac{5R}{2}\right) \Delta T \] ### Step 7: Solve for \( n \Delta T \) Rearranging gives: \[ n \Delta T = \frac{Q}{3} \cdot \frac{2}{5R} = \frac{2Q}{15R} \] ### Step 8: Relate heat \( Q \) to molar heat capacity \( C \) The heat added can also be expressed as: \[ Q = n C \Delta T \] Substituting \( n \Delta T \) from the previous step: \[ Q = C \left(\frac{2Q}{15R}\right) \] ### Step 9: Solve for \( C \) Rearranging gives: \[ C = \frac{Q}{\frac{2Q}{15R}} = \frac{15R}{2} \] ### Final Answer Thus, the molar heat capacity \( C \) in terms of \( R \) is: \[ C = \frac{15R}{2} \quad \text{or} \quad C = 7.5R \]

To find the molar heat capacity \( C \) for the process involving a diatomic ideal gas, we can follow these steps: ### Step 1: Understand the relationship between heat, work, and internal energy According to the first law of thermodynamics, we have: \[ Q = \Delta U + W \] Where: ...
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