| 1. | \(\Delta Q=\Delta U+\Delta W\) | 
| 2. | \(\Delta U=\Delta Q+\Delta W\) | 
| 3. | \(\Delta U=\Delta Q-\Delta W\) | 
| 4. | \(\Delta U+\Delta Q+\Delta W=0\) | 
| 1. | work done by the system is \(120~\text{J}.\) | 
| 2. | work done on the system is \(120~\text{J}.\) | 
| 3. | work done by the system is \(80~\text{J}.\) | 
| 4. | work done on the system is \(80~\text{J}.\) | 
If an average person jogs, he produces \(14.5 \times10^3\) cal/min. This is removed by the evaporation of sweat. The amount of sweat evaporated per minute (assuming \(1\) kg requires \(580 \times10^3\) cal for evaporation) is:
| 1. | \(0.25\) kg | 2. | \(0.50\) kg | 
| 3. | \(0.025\) kg | 4. | \(0.20\) kg | 
\(1~\text g\) 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. \(2256~\text J\) 
| 1. | \(U_0\mathrm{ln}(2)\) | 2. | \(\dfrac12U_0~\mathrm{ln}(2)\) | 
| 3. | \(\dfrac13U_0~\mathrm{ln}(2)\) | 4. | \(\dfrac23U_0~\mathrm{ln}(2)\) | 
The first law of thermodynamics is a statement of:
1. conservation of heat
2. conservation of work
3. conservation of momentum
4. conservation of energy
Consider the process on a system shown in the figure. During the process, the work done by the system:
           
| 1. | continuously increases | 
| 2. | continuously decreases | 
| 3. | first increases then decreases | 
| 4. | first decreases then increases | 
 
An ideal gas goes from the state \(i\) to the state \(f\) as shown in figure given below. The work done by the gas during the process,
   
 
| 1. | is positive | 
| 2. | is negative | 
| 3. | is zero | 
| 4. | cannot be obtained from this information | 
The molar specific heat at a constant pressure of an ideal gas is \(\dfrac{7}{2}R.\) The ratio of specific heat at constant pressure to that at constant volume is:
| 1. | \(\dfrac{7}{5}\) | 2. | \(\dfrac{8}{7}\) | 
| 3. | \(\dfrac{5}{7}\) | 4. | \(\dfrac{9}{7}\) |