| 1. |  | 2. |  | 
| 3. |  | 4. |  | 
The value of stopping potential in the following diagram is given by:
    
| 1. | \(-4\) V | 2. | \(-3\) V | 
| 3. | \(-2\) V | 4. | \(-1\) V | 
 
| 1. | Curves \(a\) and \(b\) represent incident radiations of different frequencies and different intensities. | 
| 2. | Curves \(a\) and \(b\) represent incident radiation of the same frequency but of different intensities. | 
| 3. | Curves \(b\) and \(c\) represent incident radiation of different frequencies and different intensities. | 
| 4. | Curves \(b\) and \(c\) represent incident radiations of the same frequency having the same intensity. | 
| 1. | \(N\) and \(2T\) | 2. | \(2N\) and \(T\) | 
| 3. | \(2N\) and \(2T\) | 4. | \(N\) and \(T\) | 
The number of photo-electrons emitted per second from a metal surface increases when:
| 1. | The energy of incident photons increases. | 2. | The frequency of incident light increases. | 
| 3. | The wavelength of the incident light increases. | 4. | The intensity of the incident light increases. | 
| 1. |  | 2. |  | 
| 3. |  | 4. |  | 
The stopping potential as a function of the frequency of the incident radiation is plotted for two different photoelectric surfaces \(A\) and \(B\). The graphs demonstrate that \(A\)'s work function is:
           
| 1. | Greater than that of \(B\). | 2. | Smaller than that of \(B\). | 
| 3. | Equal to that of \(B\). | 4. | No inference can be drawn about their work functions from the given graphs. | 
| 1. |  | 2. |  | 
| 3. |  | 4. |  | 
| 1. |  | 2. |  | 
| 3. |  | 4. |  | 
The figure shows different graphs between stopping potential \(V_0\) and frequency (\(\nu\)) for the photosensitive surfaces of cesium, potassium, sodium and lithium. The plots are parallel.
 
 
| 1. | Cesium | 
| 2. | Potassium | 
| 3. | Sodium | 
| 4. | Lithium | 
| 1. | (i) > (ii) > (iii) > (iv) | 2. | (i) > (iii) > (ii) > (iv) | 
| 3. | (iv) > (iii) > (ii) > (i) | 4. | (i) = (iii) > (ii) = (iv) |