Einstein s Photo Electric Equation and Energy Quantity Of Radiation (KE, Vmax, Work Function)
Dual nature of radiation and Matter

142239 It takes $4.6 \mathrm{eV}$ to remove one of the least tightly bound electrons from a metal surface. When monochromatic photons strike the metal surface, electrons having kinetic energy from zero to $2.2 \mathrm{eV}$ are ejected. What is the energy of the incident photons?

1 $2.4 \mathrm{eV}$
2 $2.2 \mathrm{eV}$
3 $6.8 \mathrm{eV}$
4 $4.6 \mathrm{eV}$
5 $5.8 \mathrm{eV}$
Dual nature of radiation and Matter

142240 Find the frequency of light which ejects electron from a metal surface fully stopped by a retarding potential of $3 \mathrm{~V}$. The photoelectric effect begins in this metal at a frequency of $6 \times 10^{14} \mathrm{~Hz}$.

1 $1.324 \times 10^{15} \mathrm{~Hz}$
2 $2.295 \times 10^{16} \mathrm{~Hz}$
3 $3.678 \times 10^{18} \mathrm{~Hz}$
4 $2.7 \times 10^{14} \mathrm{~Hz}$
Dual nature of radiation and Matter

142241 An atom of mass $M$ which is in the state of rest emits a photon of wavelength $\lambda$. As a result, the atom will deflect with the kinetic energy equal to ( $h$ is Planck's constant)

1 $\frac{\mathrm{h}^{2}}{\mathrm{M} \lambda^{2}}$
2 $\frac{1}{2} \frac{\mathrm{h}^{2}}{\mathrm{M} \lambda^{2}}$
3 $\frac{\mathrm{h}}{\mathrm{M} \lambda}$
4 $\frac{1}{2} \frac{\mathrm{h}}{\mathrm{M} \lambda}$
Dual nature of radiation and Matter

142242 For a photoelectric cell, the graph showing the variation of cut-off voltage $\left(V_{0}\right)$ with frequency $v$ of incident light is

1 (i)
2 (ii)
3 (iii)
4 (iv)
Dual nature of radiation and Matter

142243 The maximum wavelength of radiation that can produce photoelectric effect in a certain metal is 200nm. The maximum kinetic energy acquired by electron due to radiation of wavelength $100 \mathrm{~nm}$ will be

1 $12.4 \mathrm{eV}$
2 $6.2 \mathrm{eV}$
3 $100 \mathrm{eV}$
4 $200 \mathrm{eV}$
Dual nature of radiation and Matter

142239 It takes $4.6 \mathrm{eV}$ to remove one of the least tightly bound electrons from a metal surface. When monochromatic photons strike the metal surface, electrons having kinetic energy from zero to $2.2 \mathrm{eV}$ are ejected. What is the energy of the incident photons?

1 $2.4 \mathrm{eV}$
2 $2.2 \mathrm{eV}$
3 $6.8 \mathrm{eV}$
4 $4.6 \mathrm{eV}$
5 $5.8 \mathrm{eV}$
Dual nature of radiation and Matter

142240 Find the frequency of light which ejects electron from a metal surface fully stopped by a retarding potential of $3 \mathrm{~V}$. The photoelectric effect begins in this metal at a frequency of $6 \times 10^{14} \mathrm{~Hz}$.

1 $1.324 \times 10^{15} \mathrm{~Hz}$
2 $2.295 \times 10^{16} \mathrm{~Hz}$
3 $3.678 \times 10^{18} \mathrm{~Hz}$
4 $2.7 \times 10^{14} \mathrm{~Hz}$
Dual nature of radiation and Matter

142241 An atom of mass $M$ which is in the state of rest emits a photon of wavelength $\lambda$. As a result, the atom will deflect with the kinetic energy equal to ( $h$ is Planck's constant)

1 $\frac{\mathrm{h}^{2}}{\mathrm{M} \lambda^{2}}$
2 $\frac{1}{2} \frac{\mathrm{h}^{2}}{\mathrm{M} \lambda^{2}}$
3 $\frac{\mathrm{h}}{\mathrm{M} \lambda}$
4 $\frac{1}{2} \frac{\mathrm{h}}{\mathrm{M} \lambda}$
Dual nature of radiation and Matter

142242 For a photoelectric cell, the graph showing the variation of cut-off voltage $\left(V_{0}\right)$ with frequency $v$ of incident light is

1 (i)
2 (ii)
3 (iii)
4 (iv)
Dual nature of radiation and Matter

142243 The maximum wavelength of radiation that can produce photoelectric effect in a certain metal is 200nm. The maximum kinetic energy acquired by electron due to radiation of wavelength $100 \mathrm{~nm}$ will be

1 $12.4 \mathrm{eV}$
2 $6.2 \mathrm{eV}$
3 $100 \mathrm{eV}$
4 $200 \mathrm{eV}$
Dual nature of radiation and Matter

142239 It takes $4.6 \mathrm{eV}$ to remove one of the least tightly bound electrons from a metal surface. When monochromatic photons strike the metal surface, electrons having kinetic energy from zero to $2.2 \mathrm{eV}$ are ejected. What is the energy of the incident photons?

1 $2.4 \mathrm{eV}$
2 $2.2 \mathrm{eV}$
3 $6.8 \mathrm{eV}$
4 $4.6 \mathrm{eV}$
5 $5.8 \mathrm{eV}$
Dual nature of radiation and Matter

142240 Find the frequency of light which ejects electron from a metal surface fully stopped by a retarding potential of $3 \mathrm{~V}$. The photoelectric effect begins in this metal at a frequency of $6 \times 10^{14} \mathrm{~Hz}$.

1 $1.324 \times 10^{15} \mathrm{~Hz}$
2 $2.295 \times 10^{16} \mathrm{~Hz}$
3 $3.678 \times 10^{18} \mathrm{~Hz}$
4 $2.7 \times 10^{14} \mathrm{~Hz}$
Dual nature of radiation and Matter

142241 An atom of mass $M$ which is in the state of rest emits a photon of wavelength $\lambda$. As a result, the atom will deflect with the kinetic energy equal to ( $h$ is Planck's constant)

1 $\frac{\mathrm{h}^{2}}{\mathrm{M} \lambda^{2}}$
2 $\frac{1}{2} \frac{\mathrm{h}^{2}}{\mathrm{M} \lambda^{2}}$
3 $\frac{\mathrm{h}}{\mathrm{M} \lambda}$
4 $\frac{1}{2} \frac{\mathrm{h}}{\mathrm{M} \lambda}$
Dual nature of radiation and Matter

142242 For a photoelectric cell, the graph showing the variation of cut-off voltage $\left(V_{0}\right)$ with frequency $v$ of incident light is

1 (i)
2 (ii)
3 (iii)
4 (iv)
Dual nature of radiation and Matter

142243 The maximum wavelength of radiation that can produce photoelectric effect in a certain metal is 200nm. The maximum kinetic energy acquired by electron due to radiation of wavelength $100 \mathrm{~nm}$ will be

1 $12.4 \mathrm{eV}$
2 $6.2 \mathrm{eV}$
3 $100 \mathrm{eV}$
4 $200 \mathrm{eV}$
NEET Test Series from KOTA - 10 Papers In MS WORD WhatsApp Here
Dual nature of radiation and Matter

142239 It takes $4.6 \mathrm{eV}$ to remove one of the least tightly bound electrons from a metal surface. When monochromatic photons strike the metal surface, electrons having kinetic energy from zero to $2.2 \mathrm{eV}$ are ejected. What is the energy of the incident photons?

1 $2.4 \mathrm{eV}$
2 $2.2 \mathrm{eV}$
3 $6.8 \mathrm{eV}$
4 $4.6 \mathrm{eV}$
5 $5.8 \mathrm{eV}$
Dual nature of radiation and Matter

142240 Find the frequency of light which ejects electron from a metal surface fully stopped by a retarding potential of $3 \mathrm{~V}$. The photoelectric effect begins in this metal at a frequency of $6 \times 10^{14} \mathrm{~Hz}$.

1 $1.324 \times 10^{15} \mathrm{~Hz}$
2 $2.295 \times 10^{16} \mathrm{~Hz}$
3 $3.678 \times 10^{18} \mathrm{~Hz}$
4 $2.7 \times 10^{14} \mathrm{~Hz}$
Dual nature of radiation and Matter

142241 An atom of mass $M$ which is in the state of rest emits a photon of wavelength $\lambda$. As a result, the atom will deflect with the kinetic energy equal to ( $h$ is Planck's constant)

1 $\frac{\mathrm{h}^{2}}{\mathrm{M} \lambda^{2}}$
2 $\frac{1}{2} \frac{\mathrm{h}^{2}}{\mathrm{M} \lambda^{2}}$
3 $\frac{\mathrm{h}}{\mathrm{M} \lambda}$
4 $\frac{1}{2} \frac{\mathrm{h}}{\mathrm{M} \lambda}$
Dual nature of radiation and Matter

142242 For a photoelectric cell, the graph showing the variation of cut-off voltage $\left(V_{0}\right)$ with frequency $v$ of incident light is

1 (i)
2 (ii)
3 (iii)
4 (iv)
Dual nature of radiation and Matter

142243 The maximum wavelength of radiation that can produce photoelectric effect in a certain metal is 200nm. The maximum kinetic energy acquired by electron due to radiation of wavelength $100 \mathrm{~nm}$ will be

1 $12.4 \mathrm{eV}$
2 $6.2 \mathrm{eV}$
3 $100 \mathrm{eV}$
4 $200 \mathrm{eV}$
Dual nature of radiation and Matter

142239 It takes $4.6 \mathrm{eV}$ to remove one of the least tightly bound electrons from a metal surface. When monochromatic photons strike the metal surface, electrons having kinetic energy from zero to $2.2 \mathrm{eV}$ are ejected. What is the energy of the incident photons?

1 $2.4 \mathrm{eV}$
2 $2.2 \mathrm{eV}$
3 $6.8 \mathrm{eV}$
4 $4.6 \mathrm{eV}$
5 $5.8 \mathrm{eV}$
Dual nature of radiation and Matter

142240 Find the frequency of light which ejects electron from a metal surface fully stopped by a retarding potential of $3 \mathrm{~V}$. The photoelectric effect begins in this metal at a frequency of $6 \times 10^{14} \mathrm{~Hz}$.

1 $1.324 \times 10^{15} \mathrm{~Hz}$
2 $2.295 \times 10^{16} \mathrm{~Hz}$
3 $3.678 \times 10^{18} \mathrm{~Hz}$
4 $2.7 \times 10^{14} \mathrm{~Hz}$
Dual nature of radiation and Matter

142241 An atom of mass $M$ which is in the state of rest emits a photon of wavelength $\lambda$. As a result, the atom will deflect with the kinetic energy equal to ( $h$ is Planck's constant)

1 $\frac{\mathrm{h}^{2}}{\mathrm{M} \lambda^{2}}$
2 $\frac{1}{2} \frac{\mathrm{h}^{2}}{\mathrm{M} \lambda^{2}}$
3 $\frac{\mathrm{h}}{\mathrm{M} \lambda}$
4 $\frac{1}{2} \frac{\mathrm{h}}{\mathrm{M} \lambda}$
Dual nature of radiation and Matter

142242 For a photoelectric cell, the graph showing the variation of cut-off voltage $\left(V_{0}\right)$ with frequency $v$ of incident light is

1 (i)
2 (ii)
3 (iii)
4 (iv)
Dual nature of radiation and Matter

142243 The maximum wavelength of radiation that can produce photoelectric effect in a certain metal is 200nm. The maximum kinetic energy acquired by electron due to radiation of wavelength $100 \mathrm{~nm}$ will be

1 $12.4 \mathrm{eV}$
2 $6.2 \mathrm{eV}$
3 $100 \mathrm{eV}$
4 $200 \mathrm{eV}$