Photoelectric emission is observed from a metallic surface for frequencies ${\mathrm{v}}_1$ and ${\mathrm{v}}_2$ of the incident light rays $\left({\mathrm{v}}_1>{\mathrm{v}}_2\right)$. If the maximum values of kinetic energy of the photoelectrons emitted in the two cases are in the ratio of 1:k, then the threshold frequency of the metallic surface is

(1) $\frac{{\mathrm{v}}_1-{\mathrm{v}}_2}{\mathrm{k}-1}$          

(2) $\frac{{\mathrm{kv}}_1-{\mathrm{v}}_2}{\mathrm{k}-1}$

(3) $\frac{{\mathrm{kv}}_2-{\mathrm{v}}_1}{\mathrm{k}-1}$         

(4) $\frac{{\mathrm{v}}_2-{\mathrm{v}}_1}{\mathrm{k}}$

The ratio of de-Broglie wavelengths of molecules of hydrogen and helium which are at temperature 27 $°\mathrm{C}$ and 127 $°\mathrm{C}$ respectively is
(1) $\frac{1}{2}$               

(2) $\sqrt{\frac{3}{8}}$

(3) $\sqrt{\frac{8}{3}}$             

(4) 1

A photon of wavelength 6630 Å is incident on a totally reflecting surface. The momentum delivered by the photon is equal to

(1) $6.63\times {10}^{-27}$ kg-m/sec                           

(2) $2\times {10}^{-27}$ kg-m/sec

(3) ${10}^{-27}$ kg-m/sec                                     

(4) None of these

The ratio of de-Broglie wavelength of a $\mathrm{\alpha }$-particle to that of a proton being subjected to the same magnetic field so that the radii of their path are equal to each other assuming the field induction vector $\overrightarrow{\mathrm{B}}$ is perpendicular to the velocity vectors of the $\mathrm{\alpha }$-particle and the proton is
1. 1                     

2. $\frac{1}{4}$

3. $\frac{1}{2}$                   

4. 2

In a photocell bichromatic light of wavelength 2475 Å and 6000 Å are incident on cathode whose work function is 4.8 eV. If a uniform magnetic field of $3\times {10}^{-5}$ Tesla exists parallel to the plate, the radius of the path described by the photoelectron will be (mass of electron = $9\times {10}^{-31}$ kg)

(1) 1 cm                     

(2) 5 cm

(3) 10 cm                     

(4) 25 cm

The figure shows the variation of photocurrent with anode potential for a photo-sensitive surface for three different radiations. Let ${\mathrm{I}}_{\mathrm{a}},{\mathrm{I}}_{\mathrm{b}}$ and ${\mathrm{I}}_{\mathrm{c}}$ be the intensities and ${\mathrm{f}}_{\mathrm{a}},{\mathrm{f}}_{\mathrm{b}}$ and ${\mathrm{f}}_{\mathrm{c}}$ be the frequencies for the curves a, b and c respectively. Then-

1. ${\mathrm{f}}_{\mathrm{a}}={\mathrm{f}}_{\mathrm{b}} \mathrm{and} {\mathrm{I}}_{\mathrm{a}}\ne {\mathrm{I}}_{\mathrm{b}}$ 
2. ${\mathrm{f}}_{\mathrm{a}}={\mathrm{f}}_{\mathrm{c}} \mathrm{and} {\mathrm{I}}_{\mathrm{a}}={\mathrm{I}}_{\mathrm{c}}$
3. ${\mathrm{f}}_{\mathrm{a}}={\mathrm{f}}_{\mathrm{b}} \mathrm{and} {\mathrm{I}}_{\mathrm{a}}={\mathrm{I}}_{\mathrm{c}}$
4. ${\mathrm{f}}_{\mathrm{a}}={\mathrm{f}}_{\mathrm{b}} \mathrm{and} {\mathrm{I}}_{\mathrm{a}}={\mathrm{I}}_{\mathrm{b}}$

According to Einstein's photoelectric equation, the graph between the kinetic energy of photoelectrons ejected and the frequency of incident radiation is

For the photoelectric effect, the maximum kinetic energy ${\mathrm{E}}_1$ of the emitted photoelectrons is plotted against the frequency v of the incident photons as shown in the figure. The slope of the curve gives

(a) Charge of the electron

(b) Work function of the metal

(c) Planck's constant

(d) Ratio of the Planck’s constant to electronic charge

The stopping potential \(V\) for photoelectric emission from a metal surface is plotted along the \(Y\text-\)axis and the frequency \(\nu\) of incident light along the \(X\text-\)axis. A straight line is obtained as shown in the figure. Planck's constant is given by:
             

In an experiment on the photoelectric effect, the frequency \(f\) of the incident light is plotted against the stopping potential \(V_0.\) The work function of the photoelectric surface is given by:
(\(e\) is an electronic charge)