A light of wavelength \(\lambda \) is incident on the metal surface and the ejected fastest electron has speed \(v.\) If the wavelength is changed to \(\frac{3\lambda}{4},\) then the speed of the fastest emitted electron will be:
| 1. | smaller than \(\sqrt{\frac{4}{3}}v\) |
| 2. | greater than \(\sqrt{\frac{4}{3}}v\) |
| 3. | \(2v\) |
| 4. | zero |
The work functions for metals \(A,B,\) and \(C\) are respectively \(1.92\) eV, \(2.0\) eV, and \(5\) eV. According to Einstein's equation, the metals that will emit photoelectrons for a radiation of wavelength \(4100~\mathring{A}\) is/are:
| 1. | None | 2. | \(A\) only |
| 3. | \(A\) and \(B\) only | 4. | All the three metals |
| 1. | \(1.2\) eV | 2. | \(0.98\) eV |
| 3. | \(0.45\) eV | 4. | \(0\) eV |
According to Einstein's photoelectric equation, the graph between the kinetic energy of photoelectrons ejected and the frequency of incident radiation is:
| 1. | ![]() |
2. | ![]() |
| 3. | ![]() |
4. | ![]() |
The current conduction in a discharge tube is due to:
1. electrons only
2. +ve ions and –ve ions
3. –ve ions and electrons
4. +ve ions and electrons
If a light of amplitude A and wavelength λ is incident on a metallic surface, then the saturation current flow is proportional to (assume cut-off wavelength = ):
1.
2.
3.
4.
| 1. | less than \(0.5 ~\text{eV}\). |
| 2. | \(0.5 ~\text{eV}\). |
| 3. | greater than \(0.5 ~\text{eV}\). |
| 4. | the photoelectric effect does not occur. |
The value of Planck's constant is:
| 1. | \(6.63\times 10^{-34}~\text{J/s}\) | 2. | \(6.63\times 10^{-34}~\text{kg-}\text{m}^2\text{/s}\) |
| 3. | \(6.63\times 10^{-34}~\text{kg-}\text{m}^2\) | 4. | \(6.63\times 10^{-34}~\text{J-s}^2\) |