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Exercises · 11.11

Q.Light of wavelength 488 nm488\ \text{nm} is produced by an argon laser which is used in the photoelectric effect. When light from this spectral line is incident on the emitter, the stopping (cut-off) potential of photoelectrons is 0.38 V0.38\ \text{V}. Find the work function of the material from which the emitter is made.

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Einstein's equation gives ϕ=hcλ−eV0=2.54 eV−0.38 eV=2.16 eV\phi = \dfrac{hc}{\lambda}-eV_0 = 2.54\ \text{eV}-0.38\ \text{eV} = 2.16\ \text{eV}.

Einstein's photoelectric equation

When a photon of energy hc/λhc/\lambda frees an electron, part goes to overcome the work function ϕ\phi and the rest becomes kinetic energy. The stopping potential V0V_0 just halts the fastest electrons, so Kmax⁡=eV0K_{\max}=eV_0:

hcλ=ϕ+eV0.\frac{hc}{\lambda} = \phi + eV_0.

Step 1 — Photon energy of the 488 nm line

Using hc≈1240 eV⋅nmhc \approx 1240\ \text{eV·nm},

E=hcλ=1240 eV⋅nm488 nm=2.54 eV.E = \frac{hc}{\lambda} = \frac{1240\ \text{eV·nm}}{488\ \text{nm}} = 2.54\ \text{eV}.

Step 2 — Maximum kinetic energy

The cut-off (stopping) potential is V0=0.38V_0 = 0.38 V, so

Kmax⁡=eV0=0.38 eV.K_{\max} = eV_0 = 0.38\ \text{eV}. …

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