142337 A metal surface is illuminated by a radiation of wavelength $4500 \AA$. The ejected photo-electron enters a constant magnetic field of $2 \mathrm{mT}$ making an angle of $90^{\circ}$ with the magnetic field. If it starts revolving in a circular path of radius $2 \mathrm{~mm}$. the work function of the metal is approximately:
142346
Assertion: When ultraviolet light is incident on a photocell, its stopping potential is $\mathrm{V}_{0}$ and the maximum kinetic energy of the photoelectrons is $\mathrm{K}_{\max }$. When the ultraviolet light is replaced by Xrays, both $\mathrm{V}_{0}$ and $\mathrm{K}_{\max }$ increase.
Reason: Photoelectrons are emitted with speeds ranging from zero to a maximum value because of the range of frequencies present in the incident light.
142337 A metal surface is illuminated by a radiation of wavelength $4500 \AA$. The ejected photo-electron enters a constant magnetic field of $2 \mathrm{mT}$ making an angle of $90^{\circ}$ with the magnetic field. If it starts revolving in a circular path of radius $2 \mathrm{~mm}$. the work function of the metal is approximately:
142346
Assertion: When ultraviolet light is incident on a photocell, its stopping potential is $\mathrm{V}_{0}$ and the maximum kinetic energy of the photoelectrons is $\mathrm{K}_{\max }$. When the ultraviolet light is replaced by Xrays, both $\mathrm{V}_{0}$ and $\mathrm{K}_{\max }$ increase.
Reason: Photoelectrons are emitted with speeds ranging from zero to a maximum value because of the range of frequencies present in the incident light.
142337 A metal surface is illuminated by a radiation of wavelength $4500 \AA$. The ejected photo-electron enters a constant magnetic field of $2 \mathrm{mT}$ making an angle of $90^{\circ}$ with the magnetic field. If it starts revolving in a circular path of radius $2 \mathrm{~mm}$. the work function of the metal is approximately:
142346
Assertion: When ultraviolet light is incident on a photocell, its stopping potential is $\mathrm{V}_{0}$ and the maximum kinetic energy of the photoelectrons is $\mathrm{K}_{\max }$. When the ultraviolet light is replaced by Xrays, both $\mathrm{V}_{0}$ and $\mathrm{K}_{\max }$ increase.
Reason: Photoelectrons are emitted with speeds ranging from zero to a maximum value because of the range of frequencies present in the incident light.
142337 A metal surface is illuminated by a radiation of wavelength $4500 \AA$. The ejected photo-electron enters a constant magnetic field of $2 \mathrm{mT}$ making an angle of $90^{\circ}$ with the magnetic field. If it starts revolving in a circular path of radius $2 \mathrm{~mm}$. the work function of the metal is approximately:
142346
Assertion: When ultraviolet light is incident on a photocell, its stopping potential is $\mathrm{V}_{0}$ and the maximum kinetic energy of the photoelectrons is $\mathrm{K}_{\max }$. When the ultraviolet light is replaced by Xrays, both $\mathrm{V}_{0}$ and $\mathrm{K}_{\max }$ increase.
Reason: Photoelectrons are emitted with speeds ranging from zero to a maximum value because of the range of frequencies present in the incident light.
142337 A metal surface is illuminated by a radiation of wavelength $4500 \AA$. The ejected photo-electron enters a constant magnetic field of $2 \mathrm{mT}$ making an angle of $90^{\circ}$ with the magnetic field. If it starts revolving in a circular path of radius $2 \mathrm{~mm}$. the work function of the metal is approximately:
142346
Assertion: When ultraviolet light is incident on a photocell, its stopping potential is $\mathrm{V}_{0}$ and the maximum kinetic energy of the photoelectrons is $\mathrm{K}_{\max }$. When the ultraviolet light is replaced by Xrays, both $\mathrm{V}_{0}$ and $\mathrm{K}_{\max }$ increase.
Reason: Photoelectrons are emitted with speeds ranging from zero to a maximum value because of the range of frequencies present in the incident light.