Thermodynamics
- During an isothermal expansion, a confined ideal gas does –150 J of work against its surroundings. This implies that
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If a process is expansion then work done is positive so answer will be (a).
But in question work done by gas is given –150J so that according to it answer will be (d).Correct Option: E
If a process is expansion then work done is positive so answer will be (a).
But in question work done by gas is given –150J so that according to it answer will be (d).
- If ∆U and ∆W represent the increase in internal energy and work done by the system respectively in a thermodynamical process, which of the following is true?
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By first law of thermodynamics,
∆Q = ∆U - ∆W
In adiabatic process, ∆Q = 0
∴ ∆U = -∆W
In isothermal process, ∆U = 0
∴ ∆Q = ∆WCorrect Option: A
By first law of thermodynamics,
∆Q = ∆U - ∆W
In adiabatic process, ∆Q = 0
∴ ∆U = -∆W
In isothermal process, ∆U = 0
∴ ∆Q = ∆W
- In thermodynamic processes which of the following statements is not true?
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In an isochoric process volume remains constant whereas pressure remains constant in isobaric process.
Correct Option: A
In an isochoric process volume remains constant whereas pressure remains constant in isobaric process.
- If Q, E and W denote respectively the heat added, change in internal energy and the work done in a closed cyclic process, then :
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In a cyclic process, the initial state coincides with the final state. Hence, the change in internal energy is zero, as it depends only on the initial and final states. But Q & W are non-zero during a cycle process.
Correct Option: C
In a cyclic process, the initial state coincides with the final state. Hence, the change in internal energy is zero, as it depends only on the initial and final states. But Q & W are non-zero during a cycle process.
- One mole of an ideal gas at an initial temperature of T K does 6R joules of work adiabatically. If the ratio of specific heats of this gas at constant pressure and at constant volume is 5/3, the final temperature of gas will be
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T1 = T , W = 6R joules , γ = 5 3 W = P1V1 - P2V2 = nRT1 - nRT2 γ - 1 γ - 1 = nR(T1 - T2) γ - 1 n = 1 , T1 = T ⇒ R(T - T2) = 6R (5 / 3) - 1
⇒ T2 = ( T–4)KCorrect Option: A
T1 = T , W = 6R joules , γ = 5 3 W = P1V1 - P2V2 = nRT1 - nRT2 γ - 1 γ - 1 = nR(T1 - T2) γ - 1 n = 1 , T1 = T ⇒ R(T - T2) = 6R (5 / 3) - 1
⇒ T2 = ( T–4)K