Photoelectric Effect
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357751 For the photoelectric effect, the maximum kinetic energy \(E_{k}\) 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
supporting img

1 Charge of the electron
2 Work function of the metal
3 Planck's constant
4 Ratio of the Planck's constant to electronic charge
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357752 A photometal is illuminated by lights of wavelengths \(\lambda_{1}\) and \(\lambda_{2}\) respectively. The maximum kinetic energies of electrons emitted in the two cases are \(E_{1}\) and \(E_{2}\) respectively. The work function of metal is.

1 \(\dfrac{E_{2} \lambda_{1}+E_{1} \lambda_{2}}{\lambda_{1}}\)
2 \(\dfrac{E_{1} \lambda_{1}+E_{2} \lambda_{2}}{\lambda_{1}+\lambda_{2}}\)
3 \(\dfrac{E_{1} \lambda_{1}+E_{2} \lambda_{2}}{\lambda_{1}-\lambda_{2}}\)
4 \(\dfrac{E_{2} \lambda_{2}-E_{1} \lambda_{1}}{\lambda_{1}-\lambda_{2}}\)
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357753 The maximum kinetic energy of the photoelectrons depends only on

1 Incident angle
2 Potential
3 Pressure
4 Frequency
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357754 The correct graph between the maximum energy of a photoelectron and the inverse of wavelength of the incident radiation is given by the curve
supporting img

1 \(A\)
2 \(B\)
3 \(C\)
4 None of the above
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357755 Light of energy \({E}\) falls normally on a metal of work function \({E / 3}\). The kinetic energies \({(K)}\) of the photo electrons are

1 \({K=\dfrac{2 E}{3}}\)
2 \({K=\dfrac{E}{3}}\)
3 \({0 \leq K \leq \dfrac{2 E}{3}}\)
4 \({0 \leq K \leq \dfrac{E}{3}}\)
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357751 For the photoelectric effect, the maximum kinetic energy \(E_{k}\) 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
supporting img

1 Charge of the electron
2 Work function of the metal
3 Planck's constant
4 Ratio of the Planck's constant to electronic charge
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357752 A photometal is illuminated by lights of wavelengths \(\lambda_{1}\) and \(\lambda_{2}\) respectively. The maximum kinetic energies of electrons emitted in the two cases are \(E_{1}\) and \(E_{2}\) respectively. The work function of metal is.

1 \(\dfrac{E_{2} \lambda_{1}+E_{1} \lambda_{2}}{\lambda_{1}}\)
2 \(\dfrac{E_{1} \lambda_{1}+E_{2} \lambda_{2}}{\lambda_{1}+\lambda_{2}}\)
3 \(\dfrac{E_{1} \lambda_{1}+E_{2} \lambda_{2}}{\lambda_{1}-\lambda_{2}}\)
4 \(\dfrac{E_{2} \lambda_{2}-E_{1} \lambda_{1}}{\lambda_{1}-\lambda_{2}}\)
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357753 The maximum kinetic energy of the photoelectrons depends only on

1 Incident angle
2 Potential
3 Pressure
4 Frequency
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357754 The correct graph between the maximum energy of a photoelectron and the inverse of wavelength of the incident radiation is given by the curve
supporting img

1 \(A\)
2 \(B\)
3 \(C\)
4 None of the above
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357755 Light of energy \({E}\) falls normally on a metal of work function \({E / 3}\). The kinetic energies \({(K)}\) of the photo electrons are

1 \({K=\dfrac{2 E}{3}}\)
2 \({K=\dfrac{E}{3}}\)
3 \({0 \leq K \leq \dfrac{2 E}{3}}\)
4 \({0 \leq K \leq \dfrac{E}{3}}\)
NEET Test Series from KOTA - 10 Papers In MS WORD WhatsApp Here
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357751 For the photoelectric effect, the maximum kinetic energy \(E_{k}\) 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
supporting img

1 Charge of the electron
2 Work function of the metal
3 Planck's constant
4 Ratio of the Planck's constant to electronic charge
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357752 A photometal is illuminated by lights of wavelengths \(\lambda_{1}\) and \(\lambda_{2}\) respectively. The maximum kinetic energies of electrons emitted in the two cases are \(E_{1}\) and \(E_{2}\) respectively. The work function of metal is.

1 \(\dfrac{E_{2} \lambda_{1}+E_{1} \lambda_{2}}{\lambda_{1}}\)
2 \(\dfrac{E_{1} \lambda_{1}+E_{2} \lambda_{2}}{\lambda_{1}+\lambda_{2}}\)
3 \(\dfrac{E_{1} \lambda_{1}+E_{2} \lambda_{2}}{\lambda_{1}-\lambda_{2}}\)
4 \(\dfrac{E_{2} \lambda_{2}-E_{1} \lambda_{1}}{\lambda_{1}-\lambda_{2}}\)
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357753 The maximum kinetic energy of the photoelectrons depends only on

1 Incident angle
2 Potential
3 Pressure
4 Frequency
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357754 The correct graph between the maximum energy of a photoelectron and the inverse of wavelength of the incident radiation is given by the curve
supporting img

1 \(A\)
2 \(B\)
3 \(C\)
4 None of the above
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357755 Light of energy \({E}\) falls normally on a metal of work function \({E / 3}\). The kinetic energies \({(K)}\) of the photo electrons are

1 \({K=\dfrac{2 E}{3}}\)
2 \({K=\dfrac{E}{3}}\)
3 \({0 \leq K \leq \dfrac{2 E}{3}}\)
4 \({0 \leq K \leq \dfrac{E}{3}}\)
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357751 For the photoelectric effect, the maximum kinetic energy \(E_{k}\) 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
supporting img

1 Charge of the electron
2 Work function of the metal
3 Planck's constant
4 Ratio of the Planck's constant to electronic charge
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357752 A photometal is illuminated by lights of wavelengths \(\lambda_{1}\) and \(\lambda_{2}\) respectively. The maximum kinetic energies of electrons emitted in the two cases are \(E_{1}\) and \(E_{2}\) respectively. The work function of metal is.

1 \(\dfrac{E_{2} \lambda_{1}+E_{1} \lambda_{2}}{\lambda_{1}}\)
2 \(\dfrac{E_{1} \lambda_{1}+E_{2} \lambda_{2}}{\lambda_{1}+\lambda_{2}}\)
3 \(\dfrac{E_{1} \lambda_{1}+E_{2} \lambda_{2}}{\lambda_{1}-\lambda_{2}}\)
4 \(\dfrac{E_{2} \lambda_{2}-E_{1} \lambda_{1}}{\lambda_{1}-\lambda_{2}}\)
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357753 The maximum kinetic energy of the photoelectrons depends only on

1 Incident angle
2 Potential
3 Pressure
4 Frequency
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357754 The correct graph between the maximum energy of a photoelectron and the inverse of wavelength of the incident radiation is given by the curve
supporting img

1 \(A\)
2 \(B\)
3 \(C\)
4 None of the above
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357755 Light of energy \({E}\) falls normally on a metal of work function \({E / 3}\). The kinetic energies \({(K)}\) of the photo electrons are

1 \({K=\dfrac{2 E}{3}}\)
2 \({K=\dfrac{E}{3}}\)
3 \({0 \leq K \leq \dfrac{2 E}{3}}\)
4 \({0 \leq K \leq \dfrac{E}{3}}\)
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357751 For the photoelectric effect, the maximum kinetic energy \(E_{k}\) 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
supporting img

1 Charge of the electron
2 Work function of the metal
3 Planck's constant
4 Ratio of the Planck's constant to electronic charge
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357752 A photometal is illuminated by lights of wavelengths \(\lambda_{1}\) and \(\lambda_{2}\) respectively. The maximum kinetic energies of electrons emitted in the two cases are \(E_{1}\) and \(E_{2}\) respectively. The work function of metal is.

1 \(\dfrac{E_{2} \lambda_{1}+E_{1} \lambda_{2}}{\lambda_{1}}\)
2 \(\dfrac{E_{1} \lambda_{1}+E_{2} \lambda_{2}}{\lambda_{1}+\lambda_{2}}\)
3 \(\dfrac{E_{1} \lambda_{1}+E_{2} \lambda_{2}}{\lambda_{1}-\lambda_{2}}\)
4 \(\dfrac{E_{2} \lambda_{2}-E_{1} \lambda_{1}}{\lambda_{1}-\lambda_{2}}\)
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357753 The maximum kinetic energy of the photoelectrons depends only on

1 Incident angle
2 Potential
3 Pressure
4 Frequency
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357754 The correct graph between the maximum energy of a photoelectron and the inverse of wavelength of the incident radiation is given by the curve
supporting img

1 \(A\)
2 \(B\)
3 \(C\)
4 None of the above
PHXII11:DUAL NATURE OF RADIATION AND MATTER

357755 Light of energy \({E}\) falls normally on a metal of work function \({E / 3}\). The kinetic energies \({(K)}\) of the photo electrons are

1 \({K=\dfrac{2 E}{3}}\)
2 \({K=\dfrac{E}{3}}\)
3 \({0 \leq K \leq \dfrac{2 E}{3}}\)
4 \({0 \leq K \leq \dfrac{E}{3}}\)