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A diamtomic molecule can be modelled as ...

A diamtomic molecule can be modelled as two rigid balls connected with a spring such that the balls can vibrate with respect to the center of mass of the system ( spring+balls) . Consider a diamtomic gas made of such diatomic molecules. If the gas performs 20 J of work under isobaric condition, then heat given to the gas ( in J ) is

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To solve the problem, we need to find the heat given to a diatomic gas that performs 20 J of work under isobaric conditions. ### Step-by-Step Solution: 1. **Understanding the System**: We have a diatomic gas that can be modeled as two rigid balls connected by a spring. The diatomic gas has 5 degrees of freedom (3 translational and 2 rotational). 2. **Specific Heat Capacities**: - The specific heat at constant volume (Cv) for a diatomic gas is given by: \[ C_v = \frac{fR}{2} = \frac{5R}{2} \] - The specific heat at constant pressure (Cp) can be calculated using the relation: \[ C_p = C_v + R = \frac{5R}{2} + R = \frac{7R}{2} \] 3. **Work Done by the Gas**: The work done by the gas (W) is given as 20 J. 4. **Using the First Law of Thermodynamics**: The first law of thermodynamics states: \[ Q = \Delta U + W \] Where \(Q\) is the heat added to the system, \(\Delta U\) is the change in internal energy, and \(W\) is the work done by the system. 5. **Change in Internal Energy**: For an ideal gas, the change in internal energy (\(\Delta U\)) at constant volume can be expressed as: \[ \Delta U = N C_v \Delta T \] However, we will express \(\Delta T\) in terms of work done since we are dealing with an isobaric process. 6. **Relating Work and Temperature Change**: Under isobaric conditions, the work done can also be expressed as: \[ W = P \Delta V = N R \Delta T \] Therefore, we can express \(\Delta T\) as: \[ \Delta T = \frac{W}{N R} \] 7. **Substituting into the First Law**: Substitute \(\Delta T\) into the equation for \(\Delta U\): \[ \Delta U = N C_v \left(\frac{W}{N R}\right) = C_v \frac{W}{R} \] Now substituting this into the first law: \[ Q = C_v \frac{W}{R} + W \] 8. **Calculating Heat (Q)**: Substitute \(C_v = \frac{5R}{2}\) and \(W = 20 J\): \[ Q = \frac{5R}{2} \cdot \frac{20}{R} + 20 \] Simplifying: \[ Q = 50 + 20 = 70 J \] ### Final Answer: The heat given to the gas is **70 J**.
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