Correct answer Carries: 4.
Wrong Answer Carries: -1.
What is the physical significance of the equation of state in thermodynamics?
The equation of state (e.g., \( P V = \mu R T \) for an ideal gas) relates state variables (pressure, volume, temperature), defining the equilibrium state of a system and showing their interdependence.
A gas expands adiabatically from \( 2 \, \text{atm} \) and \( 4 \, \text{L} \) to \( 1 \, \text{atm} \). What is the final volume? (\( \gamma = 1.33 \))
\( P_1 V_1^\gamma = P_2 V_2^\gamma \).
\( 2 \times 4^{1.33} = 1 \times V_2^{1.33} \).
\( V_2^{1.33} = 2 \times 4^{1.33} \).
\( V_2 = (2 \times 4^{1.33})^{1/1.33} = 2^{1/1.33} \times 4 \).
\( 2^{0.7519} \approx 1.681 \), \( V_2 \approx 1.681 \times 4 \approx 6.724 \, \text{L} \approx 6.7 \, \text{L} \).
How many calories are equivalent to \( 4186 \, \text{J} \) of heat? (1 cal = \( 4.186 \, \text{J} \))
\( \text{Heat in cal} = \frac{\text{Heat in J}}{4.186} \).
\( \frac{4186}{4.186} = 1000 \, \text{cal} \).
What is the change in internal energy for \( 0.6 \, \text{moles} \) of an ideal gas heated from \( 270 \, \text{K} \) to \( 320 \, \text{K} \) at constant volume? (\( C_v = 20.8 \, \text{J mol}^{-1} \text{K}^{-1} \))
\( \Delta U = \mu C_v \Delta T \).
\( \mu = 0.6 \), \( C_v = 20.8 \), \( \Delta T = 320 - 270 = 50 \).
\( \Delta U = 0.6 \times 20.8 \times 50 = 624 \, \text{J} \).
What is the molar specific heat capacity at constant volume for a diatomic gas if \( R = 8.3 \, \text{J mol}^{-1} \text{K}^{-1} \)?
For diatomic gas: \( C_v = \frac{5}{2} R \).
\( C_v = \frac{5}{2} \times 8.3 = 20.75 \, \text{J mol}^{-1} \text{K}^{-1} \).
A system releases \( 870 \, \text{J} \) of heat and performs \( 330 \, \text{J} \) of work. What is the change in internal energy?
First Law: \( \Delta Q = \Delta U + \Delta W \).
\( \Delta Q = -870 \) (heat released), \( \Delta W = 330 \) (work by system).
\( -870 = \Delta U + 330 \Rightarrow \Delta U = -870 - 330 = -1200 \, \text{J} \).
What is the primary reason a real gas deviates from the ideal gas equation?
Real gases deviate from the ideal gas equation (\( P V = \mu R T \)) due to intermolecular forces, which are negligible in ideal gases but significant in real gases, especially at high pressures or low temperatures.
A gas expands adiabatically from \( 10 \, \text{atm} \) and \( 5 \, \text{L} \) to \( 2 \, \text{atm} \). What is the final volume? (\( \gamma = 1.33 \))
\( 10 \times 5^{1.33} = 2 \times V_2^{1.33} \).
\( V_2^{1.33} = \frac{10}{2} \times 5^{1.33} = 5 \times 5^{1.33} \).
\( 5^{1.33} \approx 9.62 \), \( V_2^{1.33} = 5 \times 9.62 \approx 48.1 \).
\( V_2 = (48.1)^{1/1.33} \approx 14.5 \, \text{L} \).
A system releases \( 760 \, \text{J} \) of heat and performs \( 240 \, \text{J} \) of work. What is the change in internal energy?
\( \Delta Q = -760 \) (heat released), \( \Delta W = 240 \) (work by system).
\( -760 = \Delta U + 240 \Rightarrow \Delta U = -760 - 240 = -1000 \, \text{J} \).
0.15 moles of an ideal gas at 320 K expand isothermally from 3 L to 9 L. What is the work done by the gas? (\( R = 8.3 \, \text{J mol}^{-1} \text{K}^{-1} \))
Isothermal: \( W = \mu R T \ln\left(\frac{V_2}{V_1}\right) \). \( \mu = 0.15 \), \( T = 320 \), \( V_2 = 9 \), \( V_1 = 3 \). \( W = 0.15 \times 8.3 \times 320 \times \ln\left(\frac{9}{3}\right) = 398.4 \times 1.0986 \approx 438 \, \text{J} \).
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