Electron Emission, Photo Electric Effect (Threshol Frequency Stopping Potential)
Dual nature of radiation and Matter

142019 Light of frequency $10^{15} \mathrm{~Hz}$ falls on metal surface of work function $2.5 \mathrm{eV}$. The stopping potential of photoelectrons in volts is

1 1.6
2 2.5
3 4.1
4 6.6
Dual nature of radiation and Matter

142020 When a metallic surface is illuminated by a light of wavelength $\lambda$, the stopping potential for the photoelectric current is $3 \mathrm{~V}$. When the same surface is illuminated by light of wavelength $2 \lambda$, the stopping potential is $1 \mathrm{~V}$. The threshold wavelength for this surface is

1 $4 \lambda$
2 $3.5 \lambda$
3 $3 \lambda$
4 $2.75 \lambda$
Dual nature of radiation and Matter

142021 In a photoelectric effect measurement, the stopping potential for a given metal is found to be $V_{0}$ volt when radiation of wavelength $\lambda_{0}$ is used. If radiation of wavelength $2 \lambda_{0}$ is used with the same metal then the stopping potential (in volt) will be :

1 $\frac{\mathrm{V}_{0}}{2}$
2 $2 \mathrm{~V}_{0}$
3 $\mathrm{V}_{0}+\frac{\mathrm{hc}}{2 \mathrm{e} \lambda_{0}}$
4 $\mathrm{V}_{0}-\frac{\mathrm{hc}}{2 \mathrm{e} \lambda_{0}}$
5 $\mathrm{V}_{0}$
Dual nature of radiation and Matter

142023 A radiation of energy $E$ falls on a perfectly reflecting surface. The momentum transferred to the surface is (let $c=$ speed of light)

1 $\frac{E}{c}$
2 $\frac{2 \mathrm{E}}{\mathrm{c}}$
3 Ec
4 $\frac{\mathrm{E}}{\mathrm{c}^{2}}$
Dual nature of radiation and Matter

142019 Light of frequency $10^{15} \mathrm{~Hz}$ falls on metal surface of work function $2.5 \mathrm{eV}$. The stopping potential of photoelectrons in volts is

1 1.6
2 2.5
3 4.1
4 6.6
Dual nature of radiation and Matter

142020 When a metallic surface is illuminated by a light of wavelength $\lambda$, the stopping potential for the photoelectric current is $3 \mathrm{~V}$. When the same surface is illuminated by light of wavelength $2 \lambda$, the stopping potential is $1 \mathrm{~V}$. The threshold wavelength for this surface is

1 $4 \lambda$
2 $3.5 \lambda$
3 $3 \lambda$
4 $2.75 \lambda$
Dual nature of radiation and Matter

142021 In a photoelectric effect measurement, the stopping potential for a given metal is found to be $V_{0}$ volt when radiation of wavelength $\lambda_{0}$ is used. If radiation of wavelength $2 \lambda_{0}$ is used with the same metal then the stopping potential (in volt) will be :

1 $\frac{\mathrm{V}_{0}}{2}$
2 $2 \mathrm{~V}_{0}$
3 $\mathrm{V}_{0}+\frac{\mathrm{hc}}{2 \mathrm{e} \lambda_{0}}$
4 $\mathrm{V}_{0}-\frac{\mathrm{hc}}{2 \mathrm{e} \lambda_{0}}$
5 $\mathrm{V}_{0}$
Dual nature of radiation and Matter

142023 A radiation of energy $E$ falls on a perfectly reflecting surface. The momentum transferred to the surface is (let $c=$ speed of light)

1 $\frac{E}{c}$
2 $\frac{2 \mathrm{E}}{\mathrm{c}}$
3 Ec
4 $\frac{\mathrm{E}}{\mathrm{c}^{2}}$
Dual nature of radiation and Matter

142019 Light of frequency $10^{15} \mathrm{~Hz}$ falls on metal surface of work function $2.5 \mathrm{eV}$. The stopping potential of photoelectrons in volts is

1 1.6
2 2.5
3 4.1
4 6.6
Dual nature of radiation and Matter

142020 When a metallic surface is illuminated by a light of wavelength $\lambda$, the stopping potential for the photoelectric current is $3 \mathrm{~V}$. When the same surface is illuminated by light of wavelength $2 \lambda$, the stopping potential is $1 \mathrm{~V}$. The threshold wavelength for this surface is

1 $4 \lambda$
2 $3.5 \lambda$
3 $3 \lambda$
4 $2.75 \lambda$
Dual nature of radiation and Matter

142021 In a photoelectric effect measurement, the stopping potential for a given metal is found to be $V_{0}$ volt when radiation of wavelength $\lambda_{0}$ is used. If radiation of wavelength $2 \lambda_{0}$ is used with the same metal then the stopping potential (in volt) will be :

1 $\frac{\mathrm{V}_{0}}{2}$
2 $2 \mathrm{~V}_{0}$
3 $\mathrm{V}_{0}+\frac{\mathrm{hc}}{2 \mathrm{e} \lambda_{0}}$
4 $\mathrm{V}_{0}-\frac{\mathrm{hc}}{2 \mathrm{e} \lambda_{0}}$
5 $\mathrm{V}_{0}$
Dual nature of radiation and Matter

142023 A radiation of energy $E$ falls on a perfectly reflecting surface. The momentum transferred to the surface is (let $c=$ speed of light)

1 $\frac{E}{c}$
2 $\frac{2 \mathrm{E}}{\mathrm{c}}$
3 Ec
4 $\frac{\mathrm{E}}{\mathrm{c}^{2}}$
Dual nature of radiation and Matter

142019 Light of frequency $10^{15} \mathrm{~Hz}$ falls on metal surface of work function $2.5 \mathrm{eV}$. The stopping potential of photoelectrons in volts is

1 1.6
2 2.5
3 4.1
4 6.6
Dual nature of radiation and Matter

142020 When a metallic surface is illuminated by a light of wavelength $\lambda$, the stopping potential for the photoelectric current is $3 \mathrm{~V}$. When the same surface is illuminated by light of wavelength $2 \lambda$, the stopping potential is $1 \mathrm{~V}$. The threshold wavelength for this surface is

1 $4 \lambda$
2 $3.5 \lambda$
3 $3 \lambda$
4 $2.75 \lambda$
Dual nature of radiation and Matter

142021 In a photoelectric effect measurement, the stopping potential for a given metal is found to be $V_{0}$ volt when radiation of wavelength $\lambda_{0}$ is used. If radiation of wavelength $2 \lambda_{0}$ is used with the same metal then the stopping potential (in volt) will be :

1 $\frac{\mathrm{V}_{0}}{2}$
2 $2 \mathrm{~V}_{0}$
3 $\mathrm{V}_{0}+\frac{\mathrm{hc}}{2 \mathrm{e} \lambda_{0}}$
4 $\mathrm{V}_{0}-\frac{\mathrm{hc}}{2 \mathrm{e} \lambda_{0}}$
5 $\mathrm{V}_{0}$
Dual nature of radiation and Matter

142023 A radiation of energy $E$ falls on a perfectly reflecting surface. The momentum transferred to the surface is (let $c=$ speed of light)

1 $\frac{E}{c}$
2 $\frac{2 \mathrm{E}}{\mathrm{c}}$
3 Ec
4 $\frac{\mathrm{E}}{\mathrm{c}^{2}}$