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Problems · Problem 2.9

Q.The threshold frequency ν0\nu_0 for a metal is 7.0×1014 s−17.0 \times 10^{14}\ s^{-1}. Calculate the kinetic energy of an electron emitted when radiation of frequency ν=1.0×1015 s−1\nu = 1.0 \times 10^{15}\ s^{-1} hits the metal.

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The kinetic energy of the emitted electron is found using the photoelectric equation: K=h(ν−ν0)K = h(\nu - \nu_0). Substituting the given frequencies and Planck’s constant gives K=1.99×10−19 JK = 1.99 \times 10^{-19}\ \text{J}.

The photoelectric effect is a beautiful example of light behaving as a particle. When a photon strikes a metal surface, it transfers its entire energy to an electron. But the electron needs a minimum energy just to escape the metal — that’s the work function, ϕ=hν0\phi = h\nu_0. Any leftover energy becomes the electron’s kinetic energy.

So the core idea is simple: photon energy in, work function out, kinetic energy left over.


  1. Write down the photoelectric equation. Einstein’s photoelectric equation states:

K=hν−ϕK = h\nu - \phi

where KK is the maximum kinetic energy of the emitted electron, hh is Planck’s constant, ν\nu is the frequency of incident radiation, and ϕ\phi is the work function of the metal.

  1. Express the work function in terms of threshold frequency. The work function is the minimum energy needed to eject an electron, given by:

ϕ=hν0\phi = h\nu_0

where ν0=7.0×1014 s−1\nu_0 = 7.0 \times 10^{14}\ \text{s}^{-1} is the threshold frequency.

  1. Substitute into the equation. This gives:

K=hν−hν0=h(ν−ν0)K = h\nu - h\nu_0 = h(\nu - \nu_0)

  1. Plug in the numbers. Planck’s constant h=6.626×10−34 J⋅sh = 6.626 \times 10^{-34}\ \text{J·s}. The incident frequency ν=1.0×1015 s−1\nu = 1.0 \times 10^{15}\ \text{s}^{-1}. So:

ν−ν0=(1.0×1015)−(7.0×1014)=3.0×1014 s−1\nu - \nu_0 = (1.0 \times 10^{15}) - (7.0 \times 10^{14}) = 3.0 \times 10^{14}\ \text{s}^{-1}

  1. Calculate the kinetic energy.

K=(6.626×10−34)×(3.0×1014)K = (6.626 \times 10^{-34}) \times (3.0 \times 10^{14})

K=1.9878×10−19 JK = 1.9878 \times 10^{-19}\ \text{J} …

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