To determine the nature of the graph of
B2 vs.
rac1λ, we start by analyzing the given problem using the photoelectric effect and the behavior of electrons in a magnetic field.
Photoelectric Effect and Kinetic Energy
The energy of the incident light is given by:
E=λhcwhere
h is Planck's constant,
c is the speed of light, and
λ is the wavelength of the incident light.
The kinetic energy (
K.E.) of the emitted photoelectrons, given the work function
ϕ, is:
K.E.=λhc−ϕ Electron in a Magnetic Field
When these electrons enter a perpendicular magnetic field
B, they experience a force that causes them to move in a circular path. The centripetal force required for this motion is provided by the Lorentz force:
racmv2R=evB where:
m is the mass of the electron,
v is the velocity of the electron,
R is the radius of the circular path,
e is the charge of the electron.
From the above equation, we can solve for
v :
v=meBR Relationship between Kinetic Energy and Velocity
The kinetic energy of the electrons can also be expressed as:
K.E.=21mv2Substituting
v=meBR into the kinetic energy equation, we get:
21m(meBR)2=21me2B2R2K.E.=2me2B2R2 Combining Both Expressions for Kinetic Energy
We already have:
K.E.=λhc−ϕEquating both expressions for kinetic energy:
2me2B2R2=λhc−ϕRearranging to isolate
B2 :
B2=e2R22m(λhc−ϕ)B2=e2R22mhc⋅λ1−e2R22mϕ Form of the Graph
This equation is in the form of a straight line
y=mx+c where:
y=B2x=λ1m=e2R22mhcc=−e2R22mϕ Thus, the graph of
B2 vs.
rac1λ will be a straight line with a positive slope and a negative
y-intercept.
The correct graph will be a straight line with a positive slope and negative
y-intercept:
Option C