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When an ideal gas (gamma = 5//3) is heat...

When an ideal gas `(gamma = 5//3)` is heated under constant pressure, what percentage of given heat energy will be utilized in doing external work ?

A

`40%`

B

`30%`

C

`60%`

D

`20%`

Text Solution

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The correct Answer is:
To solve the problem of determining the percentage of heat energy utilized in doing external work when an ideal gas (with γ = 5/3) is heated under constant pressure, we can follow these steps: ### Step-by-Step Solution: 1. **Understand the First Law of Thermodynamics**: The first law states that the change in internal energy (ΔU) is equal to the heat added to the system (ΔQ) minus the work done by the system (ΔW): \[ \Delta Q = \Delta U + \Delta W \] 2. **Rearrange the Equation**: We can rearrange the equation to express the work done (ΔW) in terms of heat added (ΔQ) and change in internal energy (ΔU): \[ \Delta W = \Delta Q - \Delta U \] 3. **Express Work Done as a Fraction of Heat Added**: We want to find the fraction of heat energy that goes into doing work: \[ \frac{\Delta W}{\Delta Q} = 1 - \frac{\Delta U}{\Delta Q} \] 4. **Determine Expressions for ΔQ and ΔU**: For an ideal gas, the heat added at constant pressure (ΔQ) is given by: \[ \Delta Q = N C_p \Delta T \] where \(C_p\) is the specific heat at constant pressure. The change in internal energy (ΔU) for an ideal gas is given by: \[ \Delta U = N C_v \Delta T \] where \(C_v\) is the specific heat at constant volume. 5. **Substitute ΔQ and ΔU into the Fraction**: Now, substituting these expressions into our fraction: \[ \frac{\Delta W}{\Delta Q} = 1 - \frac{N C_v \Delta T}{N C_p \Delta T} \] Here, \(N\) and \(\Delta T\) cancel out: \[ \frac{\Delta W}{\Delta Q} = 1 - \frac{C_v}{C_p} \] 6. **Use the Relationship Between Cp and Cv**: We know that: \[ \frac{C_p}{C_v} = \gamma \] Therefore, we can express \(C_v\) in terms of \(C_p\): \[ C_v = \frac{C_p}{\gamma} \] 7. **Substitute into the Fraction**: Now substituting \(C_v\) into our fraction: \[ \frac{\Delta W}{\Delta Q} = 1 - \frac{C_p/\gamma}{C_p} = 1 - \frac{1}{\gamma} \] 8. **Calculate the Value**: Given that \(\gamma = \frac{5}{3}\): \[ \frac{\Delta W}{\Delta Q} = 1 - \frac{1}{5/3} = 1 - \frac{3}{5} = \frac{2}{5} \] 9. **Convert to Percentage**: To find the percentage of heat energy utilized in doing external work: \[ \text{Percentage} = \left(\frac{\Delta W}{\Delta Q}\right) \times 100 = \frac{2}{5} \times 100 = 40\% \] ### Final Answer: The percentage of the given heat energy that will be utilized in doing external work is **40%**.

To solve the problem of determining the percentage of heat energy utilized in doing external work when an ideal gas (with γ = 5/3) is heated under constant pressure, we can follow these steps: ### Step-by-Step Solution: 1. **Understand the First Law of Thermodynamics**: The first law states that the change in internal energy (ΔU) is equal to the heat added to the system (ΔQ) minus the work done by the system (ΔW): \[ \Delta Q = \Delta U + \Delta W ...
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