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Question: In a photoelectric experiment the stopping potential V is plotted against applied frequency v for th...

In a photoelectric experiment the stopping potential V is plotted against applied frequency v for three different materials A, B and C as shown. Which of the following materials has largest threshold wavelength ?

A

A

B

B

C

C

D

All have same

Answer

C

Explanation

Solution

The photoelectric effect is described by Einstein's equation:

Kmax=hνϕ0K_{max} = h\nu - \phi_0

where KmaxK_{max} is the maximum kinetic energy of the emitted photoelectrons, hh is Planck's constant, ν\nu is the frequency of the incident light, and ϕ0\phi_0 is the work function of the material.

The stopping potential VsV_s is related to the maximum kinetic energy by:

eVs=KmaxeV_s = K_{max}

where ee is the charge of an electron.

Combining these equations, we get:

eVs=hνϕ0eV_s = h\nu - \phi_0

Dividing by ee, we express the stopping potential as a function of frequency:

Vs=(he)ν(ϕ0e)V_s = \left(\frac{h}{e}\right)\nu - \left(\frac{\phi_0}{e}\right)

This equation represents a straight line in a VsV_s vs ν\nu graph, with:

  • Slope m=hem = \frac{h}{e} (which is a universal constant for all materials).
  • Y-intercept c=ϕ0ec = -\frac{\phi_0}{e}.

The threshold frequency (ν0\nu_0) is the minimum frequency of incident light required to eject electrons, at which Kmax=0K_{max} = 0 and thus Vs=0V_s = 0. Setting Vs=0V_s = 0 in the equation:

0=(he)ν0(ϕ0e)0 = \left(\frac{h}{e}\right)\nu_0 - \left(\frac{\phi_0}{e}\right) (he)ν0=(ϕ0e)\left(\frac{h}{e}\right)\nu_0 = \left(\frac{\phi_0}{e}\right) hν0=ϕ0h\nu_0 = \phi_0

This means the threshold frequency ν0\nu_0 is the x-intercept (the point where the line crosses the ν\nu-axis, i.e., Vs=0V_s = 0) of the graph.

From the given graph:

  • The lines for materials A, B, and C are parallel, indicating they have the same slope he\frac{h}{e}, which is consistent.
  • We need to find the threshold frequencies for each material by observing their x-intercepts.
    • For material C, the line intersects the ν\nu-axis at the smallest frequency. So, ν0C\nu_{0C} is the smallest.
    • For material B, the line intersects at an intermediate frequency. So, ν0B\nu_{0B} is intermediate.
    • For material A, the line intersects at the largest frequency. So, ν0A\nu_{0A} is the largest.

Therefore, we have the order of threshold frequencies:

ν0C<ν0B<ν0A\nu_{0C} < \nu_{0B} < \nu_{0A}

The threshold wavelength (λ0\lambda_0) is related to the threshold frequency by:

λ0=cν0\lambda_0 = \frac{c}{\nu_0}

where cc is the speed of light.

This inverse relationship means that a smaller threshold frequency corresponds to a larger threshold wavelength. Since ν0C\nu_{0C} is the smallest threshold frequency, material C will have the largest threshold wavelength.

Thus, the order of threshold wavelengths is:

λ0C>λ0B>λ0A\lambda_{0C} > \lambda_{0B} > \lambda_{0A}

Material C has the largest threshold wavelength.