A thermodynamic system undergoes cyclic process ABCDA as shown in figure. The work done by the system in the cycle is
1. ρoVo
2. 2ρoVo
3. ρoVo/2
4. zero
An ideal gas goes from state \(A\) to state \(B\) via three different processes, as indicated in the \(P\text-V\) diagram. If \(Q_1,Q_2,Q_3\) indicates the heat absorbed by the gas along the three processes and \(\Delta U_1, \Delta U_2, \Delta U_3\) indicates the change in internal energy along the three processes respectively, then:
1. | \({Q}_1>{Q}_2>{Q}_3 \) and \(\Delta {U}_1=\Delta {U}_2=\Delta {U}_3\) |
2. | \({Q}_3>{Q}_2>{Q}_1\) and \(\Delta {U}_1=\Delta {U}_2=\Delta {U}_3\) |
3. | \({Q}_1={Q}_2={Q}_3\) and \(\Delta {U}_1>\Delta {U}_2>\Delta {U}_3\) |
4. | \({Q}_3>{Q}_2>{Q}_1\) and \(\Delta {U}_1>\Delta {U}_2>\Delta {U}_3\) |
If the volume of the given mass of a gas is increased four times and the temperature is raised from 27°C to 127°C. The isothermal elasticity will become
1. 4 times
2. 1/4 times
3. 3 times
4. 1/3 times
A container of volume 1m3 is divided into two equal compartments by a partition. One of these compartments contains an ideal gas at 300 K. The other compartment is vaccum. The whole system is thermally isolated from its surroundings. The partition is removed and the gas expands to occupy the whole volume of the container. Its temperature now would be -
(1) 300 K
(2) 239 K
(3) 200 K
(4) 100 K
The second law of thermodynamics states that in a cyclic process:
1. Work cannot be converted into heat
2. Heat cannot be converted into work
3. Work cannot be completely converted into heat
4. Heat cannot be completely converted into work
First law of thermodynamics is a special case of
(1) Newton's law
(2) Law of conservation of energy
(3) Charle's law
(4) Law of heat exchange
A monoatomic gas of n-moles is heated from temperature T1 to T2 under two different conditions (i) at constant volume and (ii) at constant pressure. The change in internal energy of the gas is
(1) More for (i)
(2) More for (ii)
(3) Same in both cases
(4) Independent of number of moles
In isothermal expansion, the pressure is determined by:
1. | Temperature only |
2. | Compressibility only |
3. | Both temperature and compressibility |
4. | None of these |
1. | will be the same in both \(A\) and \(B\). |
2. | will be zero in both the gases. |
3. | of \(B\) will be more than that of \(A\). |
4. | of \(A\) will be more than that of \(B\). |
The work done in an adiabatic change in a gas depends only on
(1) Change is pressure
(2) Change is volume
(3) Change in temperature
(4) None of the above