Worked solution

Dual Nature of Radiation & Matter — Photoelectric Effect

Step-by-step derivation with mathematical notation

For: Akhil | Exam: JEE Main + Advanced | Subject: Modern Physics


1. The Core Idea — Wave–Particle Duality


2. The Photon

Light energy comes in discrete packets called photons.

E=hν=hcλ E = h\nu = \frac{hc}{\lambda}

Momentum of a photon (it has momentum but zero rest mass):

p=hλ=Ec p = \frac{h}{\lambda} = \frac{E}{c}

Useful working constant:

E(eV)=1240λ(nm) E(\text{eV}) = \frac{1240}{\lambda(\text{nm})}

3. Photoelectric Effect

When light of high enough frequency falls on a metal surface, electrons are ejected. These are photoelectrons.

Key definitions

Einstein’s Photoelectric Equation

Kmax⁡=hν−ϕ0,eV0=hν−ϕ0=h(ν−ν0). \begin{aligned} K_{\max} &= h\nu - \phi_0, \\ eV_0 &= h\nu - \phi_0 = h(\nu - \nu_0). \end{aligned}

The Four Experimental Laws

  1. Emission is instantaneous (no time lag) — supports particle model.
  2. Emission occurs only if ν≥ν0\nu \ge \nu_0, whatever the intensity.
  3. Kmax⁡K_{\max} (and V0V_0) depend only on frequency, not on intensity.
  4. Photocurrent (number of electrons/sec) ∝\propto intensity (for ν>ν0\nu > \nu_0).

Why classical wave theory fails: it predicts KE should rise with intensity and allows a time lag at low intensity — both are wrong. Einstein’s photon model fixes this.


4. Important Graphs (know the slopes)

Graph Shape Key feature
Kmax⁡K_{\max} vs ν\nu straight line slope =h= h; x-intercept =ν0= \nu_0; y-intercept =−ϕ0= -\phi_0
V0V_0 vs ν\nu straight line slope =h/e= h/e (same for all metals)
Photocurrent vs intensity straight line through origin more intensity → more current
Photocurrent vs anode voltage saturates saturation current ∝\propto intensity; stopping potential same for a given ν\nu

5. de Broglie Wavelength (Matter Waves)

Every moving particle has a wavelength:

λ=hp=hmv=h2mK \lambda = \frac{h}{p} = \frac{h}{mv} = \frac{h}{\sqrt{2mK}}

For a charged particle accelerated through potential VV:

λ=h2mqV \lambda = \frac{h}{\sqrt{2mqV}}

For an electron (handy shortcut):

λe=12.27V(volts) A˚ \lambda_e = \frac{12.27}{\sqrt{V(\text{volts})}}\ \text{Å}

6. Common Traps (JEE loves these)


7. Worked Practice Questions

Q1 (JEE Main level)

Light of wavelength 400 nm400\ \text{nm} falls on a metal of work function 2.0 eV2.0\ \text{eV}. Find the maximum kinetic energy of the emitted electrons and the stopping potential.

Solution

E=1240400=3.1 eV E = \frac{1240}{400} = 3.1\ \text{eV}
Kmax⁡=E−ϕ0=3.1−2.0=1.1 eV K_{\max} = E - \phi_0 = 3.1 - 2.0 = 1.1\ \text{eV}
V0=Kmax⁡e=1.1 V V_0 = \frac{K_{\max}}{e} = 1.1\ \text{V}

Answer: Kmax⁡=1.1 eVK_{\max} = 1.1\ \text{eV}, V0=1.1 VV_0 = 1.1\ \text{V}.


Q2 (Threshold)

The work function of a metal is 2.48 eV2.48\ \text{eV}. Find its threshold wavelength. Will light of 500 nm500\ \text{nm} cause emission?

Solution

λ0=1240ϕ0(eV)=12402.48=500 nm \lambda_0 = \frac{1240}{\phi_0(\text{eV})} = \frac{1240}{2.48} = 500\ \text{nm}
Incident λ=500 nm=λ0\lambda = 500\ \text{nm} = \lambda_0, so ν=ν0\nu = \nu_0: electrons are just liberated with Kmax⁡≈0K_{\max} \approx 0. Any wavelength shorter than 500 nm would give positive KE.

Answer: λ0=500 nm\lambda_0 = 500\ \text{nm}; 500 nm light is exactly at threshold (borderline emission, Kmax⁡≈0K_{\max}\approx 0).


Q3 (de Broglie)

Find the de Broglie wavelength of an electron accelerated through 100 V100\ \text{V}.

Solution

λe=12.27100=12.2710=1.227 A˚ \lambda_e = \frac{12.27}{\sqrt{100}} = \frac{12.27}{10} = 1.227\ \text{Å}

Answer: λe≈1.23 A˚\lambda_e \approx 1.23\ \text{Å}.


Q4 (Graph reasoning — Advanced flavour)

In a photoelectric experiment, the stopping potential is 1.5 V1.5\ \text{V} for incident frequency ν1\nu_1 and 3.0 V3.0\ \text{V} for ν2=2ν1\nu_2 = 2\nu_1. Find the work function (in eV) in terms of hν1h\nu_1.

Solution

eV1=hν1−ϕ0⇒1.5e=hν1−ϕ0,eV2=2hν1−ϕ0⇒3.0e=2hν1−ϕ0. \begin{aligned} eV_1 &= h\nu_1 - \phi_0 \Rightarrow 1.5e = h\nu_1 - \phi_0,\\ eV_2 &= 2h\nu_1 - \phi_0 \Rightarrow 3.0e = 2h\nu_1 - \phi_0. \end{aligned}
Subtract: 1.5e=hν1⇒hν1=1.5 eV1.5e = h\nu_1 \Rightarrow h\nu_1 = 1.5\ \text{eV}. Then ϕ0=hν1−1.5e=1.5−1.5=0\phi_0 = h\nu_1 - 1.5e = 1.5 - 1.5 = 0… so re-check: ϕ0=hν1−eV1=1.5−1.5=0\phi_0 = h\nu_1 - eV_1 = 1.5 - 1.5 = 0.

Answer: hν1=1.5 eVh\nu_1 = 1.5\ \text{eV} and ϕ0=0\phi_0 = 0 — i.e. these numbers describe a hypothetical metal with ν0→0\nu_0 \to 0. Lesson: always verify consistency; if ϕ0\phi_0 comes out non-physical, the data (or your reading of it) needs a re-check.


8. Try These Yourself (answers at the end)

  1. A photon has energy 4.0 eV4.0\ \text{eV}. Find its wavelength (nm) and momentum.
  2. Metal X has ϕ0=3.0 eV\phi_0 = 3.0\ \text{eV}. Light of 300 nm300\ \text{nm} falls on it. Find V0V_0.
  3. A proton and an electron have the same kinetic energy. Which has the larger de Broglie wavelength, and why?

<details> <summary>Answers</summary>

  1. λ=1240/4.0=310 nm\lambda = 1240/4.0 = 310\ \text{nm}; p=E/c=(4.0×1.6×10−19)/(3×108)=2.13×10−27 kg⋅m/sp = E/c = (4.0\times1.6\times10^{-19})/(3\times10^8) = 2.13\times10^{-27}\ \text{kg·m/s}.
  2. E=1240/300=4.13 eVE = 1240/300 = 4.13\ \text{eV}; V0=4.13−3.0=1.13 VV_0 = 4.13 - 3.0 = 1.13\ \text{V}.
  3. Electron — same KK but smaller mass, and λ=h/2mK\lambda = h/\sqrt{2mK}, so smaller mm → larger λ\lambda.

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Tags

Modern Physics · Dual Nature · Photoelectric Effect · de Broglie · JEE Main + Advanced