A metal surface with work function is illuminated by monochromatic light of frequency $
uV_0m$, the maximum speed of the emitted photoelectrons is:
$\sqrt{\frac{2(h
u + \phi)}{m}}$
$\sqrt{\frac{2(h
u - \phi)}{m}}$
$\sqrt{\frac{h
u - \phi}{m}}$
$\frac{2(h
u - \phi)}{m}$
Related Questions
In Lenard's experiment, the stopping potential for photoelectrons emitted from a metal surface illuminated by light of wavelength is . When the wavelength is changed to (), the stopping potential becomes . If the work function of the metal is , which of the following relations is correct?
The collector plate in an experiment on photoelectric effect is kept vertically above the emitter plate. Light source is put on and a saturation photo current is recorded. An electric field is switched on which has a vertically downward direction
The photo current will increase
The kinetic energy of the electrons will increase
The stopping potential will decrease
The threshold wavelength will increase
The electrons are emitted in the photoelectric effect from a metal surface
Only if the frequency of the incident radiation is above a certain threshold value
Only if the temperature of the surface is high
At a rate that is independent of the nature of the metal
With a maximum velocity proportional to the frequency of the incident radiation
A metal plate gets heated when cathode rays strike against it due to
Kinetic energy of cathode rays
Potential energy of cathode rays
Linear velocity of cathode rays
Angular velocity of cathode rays
In Thomson mass spectrograph, singly and doubly ionised particles from similar parabola corresponding to magnetic fields of 0.8 T and 1.2 T for a constant electric field. The ratio of masses of ionised particles will be
In a photoelectric experiment, the incident light frequency is $3
u_0
u_01.5
u_0$ and the intensity is kept constant, how does the stopping potential change?
Becomes zero
Becomes one-fourth
Doubles
Remains the same
Planckβs constant has the dimensions of
Energy
Mass
Frequency
Angular momentum
When monochromatic radiation of intensity falls on a metal surface, the number of photoelectron and their maximum kinetic energy are and respectively. If the intensity of radiation is the number of emitted electrons and their maximum kinetic energy are respectively
and
and
and
and
When subjected to a transverse electric field, cathode rays move
Down the potential gradient
Up the potential gradient
Along a hyperbolic path
Along a circular path