JEE Challenger
More from Dual Nature of Radiation and Matter

Variation of Stopping Potential with Wavelength and Inverse Wavelength

In a photoelectric effect experiment with incident photon wavelength λ\lambda, the stopping potential is denoted by V0V_0. Select the correct graphical representation(s) showing the variation of V0V_0 with λ\lambda and 1/λ1/\lambda.

Options

A
Option A Diagram 1
Correct
B
Option B Diagram 1
C
Option C Diagram 1
Correct
D
Option D Diagram 1

Step-by-Step Solution

According to Einstein's photoelectric equation, the maximum kinetic energy of the emitted photoelectrons is given by:

eV0=hν−ϕ=hcλ−ϕe V_0 = h\nu - \phi = \frac{hc}{\lambda} - \phi

where:

  • V0V_0 is the stopping potential,
  • ee is the magnitude of charge on an electron,
  • hh is Planck's constant,
  • cc is the speed of light in vacuum,
  • λ\lambda is the wavelength of the incident photon,
  • ϕ\phi is the work function of the metal.

Photoelectric emission takes place only when the incident wavelength λ\lambda is less than or equal to the threshold wavelength λ0\lambda_0 (where λ0=hcϕ\lambda_0 = \frac{hc}{\phi}).


1. Variation of V0V_0 with 1/λ1/\lambda:

Rearranging the equation in terms of 1λ\frac{1}{\lambda}:

V0=(hce)1λ−ϕefor 1λ≥1λ0V_0 = \left( \frac{hc}{e} \right) \frac{1}{\lambda} - \frac{\phi}{e} \quad \text{for } \frac{1}{\lambda} \ge \frac{1}{\lambda_0}

  • For 1λ<1λ0\frac{1}{\lambda} < \frac{1}{\lambda_0}, no photoelectrons are emitted, so V0=0V_0 = 0.
  • For 1λ≥1λ0\frac{1}{\lambda} \ge \frac{1}{\lambda_0}, V0V_0 increases linearly with 1λ\frac{1}{\lambda} with a positive slope (hce)\left(\frac{hc}{e}\right) and an intercept on the horizontal axis at 1λ=1λ0\frac{1}{\lambda} = \frac{1}{\lambda_0}.

This linear behavior with a non-zero threshold intercept is correctly represented in graph (C).


2. Variation of V0V_0 with λ\lambda:

Rearranging the equation in terms of λ\lambda:

V0=hceλ−ϕefor 0<λ≤λ0V_0 = \frac{hc}{e\lambda} - \frac{\phi}{e} \quad \text{for } 0 < \lambda \le \lambda_0

  • For λ>λ0\lambda > \lambda_0, no photoelectrons are emitted, so V0=0V_0 = 0.
  • For 0<λ≤λ00 < \lambda \le \lambda_0, V0V_0 decreases non-linearly as λ\lambda increases.
  • Taking the derivatives with respect to λ\lambda: dV0dλ=−hceλ2<0\frac{dV_0}{d\lambda} = -\frac{hc}{e\lambda^2} < 0 d2V0dλ2=2hceλ3>0\frac{d^2V_0}{d\lambda^2} = \frac{2hc}{e\lambda^3} > 0

Since d2V0dλ2>0\frac{d^2V_0}{d\lambda^2} > 0, the curve is convex downwards, decreasing continuously to zero as λ→λ0\lambda \to \lambda_0, and remaining zero for λ>λ0\lambda > \lambda_0.

This non-linear, concave-upward decaying curve is correctly represented in graph (A).


Thus, the correct option(s) are (A) and (C).