Practice MCQs for JEE Physics Thermodynamics
Review structured MCQ sets for JEE Physics Thermodynamics. Built according to official JEE guidelines, these downloadable questions support daily revision and core concept reinforcement.
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View or download the dedicated Thermodynamics MCQ resource below. Practicing these 50 objective questions regularly builds familiarity with standard exam patterns and helps secure higher marks in final Physics evaluations.
Multiple Choice Questions
(a) 600 K
(b) 300 K
(c) 373 K
(d) none of these
Show Answer & Explanation
Answer: (a) 600 K
Explanation:
1. \( \eta=1-\dfrac{T_2}{T_1}=\dfrac12\Rightarrow T_2=\dfrac{T_1}2 \).
2. New sink temperature \( T_2-100 \) gives \( \dfrac{T_2-100}{T_1}=\dfrac13 \): \( \dfrac12-\dfrac{100}{T_1}=\dfrac13 \).
3. \( \dfrac{100}{T_1}=\dfrac16\Rightarrow T_1=600\ \text{K} \).
Teacher's Note:
1. A change of 100 °C is the same as a change of 100 K. Write each efficiency as one minus the temperature ratio.
(a) 6 J
(b) 5 J
(c) 4 J
(d) 3 J
Show Answer & Explanation
Answer: (a) 6 J
Explanation:
1. \( \text{COP}=\dfrac{T_2}{T_1-T_2}=\dfrac{250}{300-250}=5 \), so 5 J is extracted from the cold space per joule of work.
2. Heat rejected = 5 + 1 = 6 J.
Teacher's Note:
1. Heat rejected equals heat removed plus the work done. Use kelvin temperatures.
(a) \( C_P=\dfrac{\gamma R}{\gamma-1} \)
(b) \( C_P-C_V=R \)
(c) \( \Delta U=\dfrac{P_fV_f-P_iV_i}{1-\gamma} \)
(d) \( C_V=\dfrac{R}{\gamma-1} \)
Show Answer & Explanation
Answer: (c) \( \Delta U=\dfrac{P_fV_f-P_iV_i}{1-\gamma} \)
Explanation:
1. For n moles \( \Delta U=nC_V\Delta T=\dfrac{nR\Delta T}{\gamma-1}=\dfrac{P_fV_f-P_iV_i}{\gamma-1} \).
2. Option (c) has \( 1-\gamma \) in the denominator, which gives the wrong sign. The other three are correct.
Teacher's Note:
1. Remember internal energy change as PV difference over gamma minus one. Check the sign with an adiabatic compression.
(a) Specific heat in a no heat exchange condition, \( C_A=0 \)
(b) Specific heat at constant temperature, \( C_T=\infty \)
(c) Specific heat at constant pressure, \( C_P=\dfrac{\gamma R}{\gamma-1} \)
(d) Specific heat at constant volume, \( C_V=\dfrac R\gamma \)
Show Answer & Explanation
Answer: (d) Specific heat at constant volume, \( C_V=\dfrac R\gamma \)
Explanation:
1. Adiabatic: dQ = 0, so C = 0. Isothermal: dT = 0, so \( C=dQ/dT=\infty \).
2. \( C_P=\dfrac{\gamma R}{\gamma-1} \) is correct.
3. \( C_V=\dfrac{R}{\gamma-1} \), not \( R/\gamma \), so (d) is incorrect.
Teacher's Note:
1. Cv is R over gamma minus one. Cp is gamma times Cv.
(a) \( C_V+\dfrac{R}{1+x} \)
(b) \( C_P+\dfrac{R}{1+x} \)
(c) \( C_V+\dfrac{R}{1-x} \)
(d) \( C_P+\dfrac{R}{1-x} \)
Show Answer & Explanation
Answer: (c) \( C_V+\dfrac{R}{1-x} \)
Explanation:
1. Work in a polytropic process: \( dW=\dfrac{R\,dT}{1-x} \).
2. First law: \( C=C_V+\dfrac{dW}{dT}=C_V+\dfrac{R}{1-x} \).
Teacher's Note:
1. Check the special cases. x = 0 gives Cp, x = 1 gives infinity (isothermal) and x = gamma gives zero (adiabatic).
(a) \( \dfrac{17R}{6} \)
(b) \( \dfrac{6R}{17} \)
(c) \( \dfrac{13R}{6} \)
(d) \( \dfrac{16R}{7} \)
Show Answer & Explanation
Answer: (a) \( \dfrac{17R}{6} \)
Explanation:
1. Write \( PV^{-2}=a \), so the polytropic index is \( x=-2 \).
2. \( C=C_V+\dfrac{R}{1-x}=\dfrac{5R}{2}+\dfrac R3=\dfrac{17R}{6} \).
Teacher's Note:
1. Identify x from the given relation, including its sign. A diatomic gas has Cv equal to 5R by 2.
(a) 11 J
(b) 22 J
(c) 33 J
(d) 50 J
Show Answer & Explanation
Answer: (a) 11 J
Explanation:
1. \( \dfrac{Q_{out}}{W}=\dfrac{T_1}{T_1-T_2}=\dfrac{300}{27}=11.1 \).
2. So about 11 J is delivered to the surroundings for each joule of work.
Teacher's Note:
1. For a reversible refrigerator the heat rejected scales as T1 over T1 minus T2. A small temperature difference means a large ratio.
(a) \( \dfrac{(\gamma-1)Mv^2}{4R} \)
(b) \( \dfrac{\gamma Mv^2}{2R} \)
(c) \( \dfrac{Mv^2}{2(\gamma-1)R} \)
(d) \( \dfrac{(\gamma-1)Mv^2}{2R} \)
Show Answer & Explanation
Answer: (d) \( \dfrac{(\gamma-1)Mv^2}{2R} \)
Explanation:
1. Mass of the gas = 2M, so kinetic energy \( =\tfrac12(2M)v^2=Mv^2 \).
2. This becomes internal energy at constant volume: \( Mv^2=nC_V\Delta T=2\cdot\dfrac{R}{\gamma-1}\Delta T \).
3. \( \Delta T=\dfrac{(\gamma-1)Mv^2}{2R} \).
Teacher's Note:
1. The ordered kinetic energy of the whole gas turns into random molecular energy. Use the molar heat capacity at constant volume.
(a) \( C_V(T_1-T_2) \)
(b) \( C_P(T_1-T_2) \)
(c) \( \dfrac{C_P+C_V}{2}(T_1-T_2) \)
(d) \( (C_P-C_V)(T_1-T_2) \)
Show Answer & Explanation
Answer: (a) \( C_V(T_1-T_2) \)
Explanation:
1. Internal energy of an ideal gas depends only on temperature: \( \Delta U=nC_V\Delta T \) for any process.
2. For one mole the decrease is \( C_V(T_1-T_2) \).
Teacher's Note:
1. Internal energy of an ideal gas depends only on temperature. The adiabatic condition is not needed for this result.
(a) \( 7/5 \)
(b) \( 5/3 \)
(c) \( 3/2 \)
(d) 2
Show Answer & Explanation
Answer: (c) \( 3/2 \)
Explanation:
1. \( dQ=C\,dT=4R\,dT \) and \( dW=2R\,dT \), so \( dU=dQ-dW=2R\,dT \) and \( C_V=2R \).
2. \( C_P=C_V+R=3R \), so \( \gamma=3R/2R=3/2 \).
Teacher's Note:
1. Use the first law to find Cv from the given heat capacity and work. Then add R to get Cp.
(a) \( \dfrac{RT_0}{2} \)
(b) \( RT_0 \)
(c) \( 2RT_0 \)
(d) \( \dfrac32RT_0 \)
Show Answer & Explanation
Answer: (c) \( 2RT_0 \)
Explanation:
1. \( \Delta U=\tfrac32R(2T_0-T_0)=\tfrac32RT_0 \).
2. Work \( =\int P\,dV=\dfrac K2(V_2^2-V_1^2)=\tfrac12(P_2V_2-P_1V_1)=\tfrac12R(2T_0-T_0)=\tfrac12RT_0 \).
3. \( Q=\Delta U+W=\tfrac32RT_0+\tfrac12RT_0=2RT_0 \).
Teacher's Note:
1. For P proportional to V the work is half the change in PV. Add it to the change in internal energy.
(a) 1 : 15
(b) 1 : 1
(c) 1 : 2
(d) 1.73 : 1
Show Answer & Explanation
Answer: (d) 1.73 : 1
Explanation:
1. \( \eta_1=\dfrac{473-273}{473}=\dfrac{200}{473} \) and \( \eta_2=\dfrac{273-73}{273}=\dfrac{200}{273} \).
2. \( \dfrac{\eta_2}{\eta_1}=\dfrac{473}{273}=1.73 \).
Teacher's Note:
1. Convert to kelvin before taking ratios. The same temperature difference is more efficient at lower temperatures.
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FAQs
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