Modern Physics: Edge Cases and Subtle Traps (3)

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Question

The work function of a metal is ϕ=2.5 eV\phi = 2.5 \text{ eV}. Light of wavelength λ=400 nm\lambda = 400 \text{ nm} falls on it. Find (a) the maximum kinetic energy of photoelectrons, (b) the stopping potential, (c) the maximum wavelength that can produce photoelectrons (threshold wavelength). Take h=6.63×1034 J sh = 6.63 \times 10^{-34} \text{ J s}, c=3×108 m/sc = 3 \times 10^8 \text{ m/s}, 1 eV=1.6×1019 J1 \text{ eV} = 1.6 \times 10^{-19} \text{ J}.

Solution — Step by Step

E=hc/λ=6.63×1034×3×108400×109=4.97×1019 JE = hc/\lambda = \frac{6.63 \times 10^{-34} \times 3 \times 10^8}{400 \times 10^{-9}} = 4.97 \times 10^{-19} \text{ J}

In eV: E=4.97×1019/(1.6×1019)=3.11 eVE = 4.97 \times 10^{-19} / (1.6 \times 10^{-19}) = 3.11 \text{ eV}.

(Quick shortcut: E(eV)=1240/λ(nm)=1240/400=3.1 eVE(\text{eV}) = 1240/\lambda(\text{nm}) = 1240/400 = 3.1 \text{ eV}.)

KEmax=Eϕ=3.12.5=0.6 eV=0.6×1.6×1019=9.6×1020 JKE_{max} = E - \phi = 3.1 - 2.5 = 0.6 \text{ eV} = 0.6 \times 1.6 \times 10^{-19} = 9.6 \times 10^{-20} \text{ J}.

eVs=KEmaxeV_s = KE_{max}, so Vs=KEmax/e=0.6 VV_s = KE_{max}/e = 0.6 \text{ V}.

At threshold, hc/λ0=ϕhc/\lambda_0 = \phi. So λ0(nm)=1240/ϕ(eV)=1240/2.5=496 nm\lambda_0(\text{nm}) = 1240/\phi(\text{eV}) = 1240/2.5 = 496 \text{ nm}.

Photons with λ>496 nm\lambda > 496 \text{ nm} cannot produce photoelectrons, no matter how intense the light.

Final answers: KEmax=0.6 eVKE_{max} = \mathbf{0.6 \text{ eV}}, Vs=0.6 VV_s = \mathbf{0.6 \text{ V}}, λ0=496 nm\lambda_0 = \mathbf{496 \text{ nm}}.

Why This Works

The photoelectric effect’s signature feature: energy per photon depends on frequency, not intensity. Below threshold (ν<ν0\nu < \nu_0, equivalently λ>λ0\lambda > \lambda_0), no photoelectrons emerge no matter how bright the light — each photon individually lacks enough energy to free an electron.

The shortcut E(eV)=1240/λ(nm)E(\text{eV}) = 1240/\lambda(\text{nm}) is gold for JEE/NEET. Memorize it. It comes from hc=1240 eV nmhc = 1240 \text{ eV nm}.

Alternative Method

Use λ0=hc/ϕ\lambda_0 = hc/\phi directly to get threshold first, then KEmax=(hc/λ)(1λ/λ0)=3.1(1400/496)=3.1×0.193=0.6 eVKE_{max} = (hc/\lambda)(1 - \lambda/\lambda_0) = 3.1(1 - 400/496) = 3.1 \times 0.193 = 0.6 \text{ eV}. Same answer, cleaner if you have λ0\lambda_0 already.

Common Mistake

A frequent NEET trap: students mix up frequency and wavelength conditions. “Threshold frequency” ν0\nu_0 is the minimum frequency for emission, but “threshold wavelength” λ0\lambda_0 is the maximum wavelength. Below λ0\lambda_0 — emission happens; above λ0\lambda_0 — no emission. Always cross-check with E=hc/λE = hc/\lambda.

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