1. | \(4\) | 2. | \(1\) |
3. | \(2\) | 4. | \(3\) |
A gas undergoes an isothermal process. The specific heat capacity of the gas in the process is:
1. | infinity | 2. | \(0.5\) |
3. | zero | 4. | \(1\) |
1. | \(\text{If}~P_1>P_2~\text{then}~T_1<T_2\) |
2. | \(\text{If}~V_2>V_1~\text{then}~T_2>T_1\) |
3. | \(\text{If}~V_2>V_1~\text{then}~T_2<T_1\) |
4. | \(\text{If}~P_1>P_2~\text{then}~V_1>V_2\) |
Two cylinders \(A\) and \(B\) of equal capacity are connected to each other via a stop cock. A contains an ideal gas at standard temperature and pressure. \(B\) is completely evacuated. The entire system is thermally insulated. The stop cock is suddenly opened. The process is:
1. adiabatic
2. isochoric
3. isobaric
4. isothermal
The \((P\text{-}V)\) diagram for an ideal gas in a piston-cylinder assembly undergoing a thermodynamic process is shown in the figure. The process is:
1. | adiabatic | 2. | isochoric |
3. | isobaric | 4. | isothermal |
1. | isochoric | 2. | isothermal |
3. | adiabatic | 4. | isobaric |
\(1~\text g\) of water of volume \(1~\text{cm}^3\) at \(100^\circ \text{C}\) is converted into steam at the same temperature under normal atmospheric pressure \(\approx 1\times10^{5}~\text{Pa}.\) The volume of steam formed equals \(1671~\text{cm}^3.\) If the specific latent heat of vaporization of water is \(2256~\text{J/g},\) the change in internal energy is:
1. \(2423~\text J\)
2. \(2089~\text J\)
3. \(167~\text J\)
4. \(2256~\text J\)