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One mole of an ideal gas with gamma=1.4,...

One mole of an ideal gas with `gamma`=1.4, is adiabatically compressed so that its temperature rises from `27^@C` to `35^@C`. The change in the internal energy of the gas is (R = 8.3J/mol.K)

A

-166 J

B

166 J

C

-168 J

D

168 J

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The correct Answer is:
To solve the problem of finding the change in internal energy of one mole of an ideal gas undergoing adiabatic compression, we can follow these steps: ### Step 1: Understand the relationship for internal energy change For an ideal gas, the change in internal energy (\( \Delta U \)) during an adiabatic process can be expressed as: \[ \Delta U = nC_V \Delta T \] Where: - \( n \) = number of moles of gas (1 mole in this case) - \( C_V \) = molar specific heat at constant volume - \( \Delta T \) = change in temperature ### Step 2: Calculate the change in temperature Convert the temperatures from Celsius to Kelvin: - Initial temperature \( T_1 = 27^\circ C = 27 + 273 = 300 \, K \) - Final temperature \( T_2 = 35^\circ C = 35 + 273 = 308 \, K \) Now, calculate the change in temperature: \[ \Delta T = T_2 - T_1 = 308 \, K - 300 \, K = 8 \, K \] ### Step 3: Determine \( C_V \) using \( \gamma \) The relationship between \( C_V \) and \( R \) (the universal gas constant) is given by: \[ C_V = \frac{R}{\gamma - 1} \] Given \( R = 8.3 \, J/(mol \cdot K) \) and \( \gamma = 1.4 \): \[ C_V = \frac{8.3}{1.4 - 1} = \frac{8.3}{0.4} = 20.75 \, J/(mol \cdot K) \] ### Step 4: Calculate the change in internal energy Now we can substitute the values into the equation for \( \Delta U \): \[ \Delta U = nC_V \Delta T = 1 \cdot 20.75 \cdot 8 = 166 \, J \] ### Conclusion The change in internal energy of the gas is: \[ \Delta U = 166 \, J \]

To solve the problem of finding the change in internal energy of one mole of an ideal gas undergoing adiabatic compression, we can follow these steps: ### Step 1: Understand the relationship for internal energy change For an ideal gas, the change in internal energy (\( \Delta U \)) during an adiabatic process can be expressed as: \[ \Delta U = nC_V \Delta T \] Where: ...
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