The threshold frequency of a metal is \(f _0\) When the light of frequency \(2 f _0\) is incident on the metal plate, the maximum velocity of photoelectrons is \(v_1\) When the frequency of incident radiation is increased to \(5 f _0\), the maximum velocity of photoelectrons emitted is \(v_2\) The ratio of \(v_1\) to \(v_2\) is :
Remember Einstein’s photoelectric equation and how to relate the maximum kinetic energy of photoelectrons to their velocity.
\(\frac{v_1}{v_2}=\frac{1}{8}\)
\(\frac{v_1}{v_2}=\frac{1}{4}\)
\(\frac{v_1}{v_2}=\frac{1}{16}\)
\(\frac{v_1}{v_2}=\frac{1}{2}\)
To solve this problem, let's use the photoelectric effect equation. According to Einstein's photoelectric equation:
\(E_k = hf - \phi\)
where:
From the kinetic energy, the maximum velocity \(v\) of the emitted photoelectrons is given by:
\(E_k = \frac{1}{2} mv^2\)
For frequency \(2f_0\):
\(E_{k1} = h(2f_0) - hf_0 = hf_0\)
This gives:
\(\frac{1}{2}mv_1^2 = hf_0\)
For frequency \(5f_0\):
\(E_{k2} = h(5f_0) - hf_0 = 4hf_0\)
This gives:
\(\frac{1}{2}mv_2^2 = 4hf_0\)
Let us find the ratio \(\frac{v_1}{v_2}\):
\(\frac{v_1^2}{v_2^2} = \frac{hf_0 / \frac{1}{2}m}{4hf_0 / \frac{1}{2}m} = \frac{1}{4}\)
Taking the square root on both sides:
\(\frac{v_1}{v_2} = \frac{1}{2}\)
Hence, the correct option is \(\frac{v_1}{v_2}=\frac{1}{2}\).
| List I (Spectral Lines of Hydrogen for transitions from) | List II (Wavelength (nm)) | ||
| A. | n2 = 3 to n1 = 2 | I. | 410.2 |
| B. | n2 = 4 to n1 = 2 | II. | 434.1 |
| C. | n2 = 5 to n1 = 2 | III. | 656.3 |
| D. | n2 = 6 to n1 = 2 | IV. | 486.1 |