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When an ideal gas in a cylinder was comp...

When an ideal gas in a cylinder was compreswsed isothermally by a piston, the work done on the gas found to be `1.5xx10^(4)` cal. During this process about

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To solve the problem, we need to analyze the isothermal compression of an ideal gas and understand the relationship between work done, heat transfer, and internal energy. ### Step-by-Step Solution: 1. **Understanding Isothermal Process**: In an isothermal process, the temperature of the gas remains constant. For an ideal gas, this means that the internal energy (U) does not change, i.e., \( \Delta U = 0 \). 2. **Work Done on the Gas**: The work done on the gas during isothermal compression is given as \( W = 1.5 \times 10^4 \) joules. 3. **First Law of Thermodynamics**: According to the first law of thermodynamics: \[ \Delta Q = \Delta U + W \] Since \( \Delta U = 0 \) for an isothermal process, we can simplify this to: \[ \Delta Q = W \] 4. **Substituting the Values**: We substitute the value of work done into the equation: \[ \Delta Q = 1.5 \times 10^4 \text{ J} \] 5. **Converting Joules to Calories**: To convert joules to calories, we use the conversion factor \( 1 \text{ cal} = 4.184 \text{ J} \): \[ \Delta Q = \frac{1.5 \times 10^4 \text{ J}}{4.184 \text{ J/cal}} \approx 3580.65 \text{ cal} \] 6. **Considering Heat Flow Direction**: Since the work is done on the gas, the gas loses heat to the surroundings. Therefore, the heat transfer \( \Delta Q \) will be negative: \[ \Delta Q \approx -3580.65 \text{ cal} \] 7. **Final Result**: Thus, the amount of heat that flowed out of the gas during the isothermal compression is approximately \( -3.58 \times 10^3 \) cal. ### Conclusion: The correct option, based on the calculations, is that approximately \( 3.6 \times 10^3 \) calories of heat flowed out from the gas.
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