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Physics Strategy Reading Time: 12 min 4 Systematic Steps

Cracking Photoelectric Effect Problems in 4 Simple Steps

Master the systematic approach to solve any Photoelectric Effect problem in JEE Main and Advanced.

95%
Problem Coverage
3-4
Marks per Question
4
Key Steps
5min
Avg. Solve Time

Why This 4-Step Method Works

Photoelectric Effect questions follow predictable patterns in JEE. This systematic approach ensures you never miss key concepts and can solve even the trickiest problems efficiently.

🎯 JEE Relevance

Photoelectric Effect appears in 1-2 questions per JEE paper, carrying 3-4 marks each. Mastering this topic can give you a significant advantage in Modern Physics section.

Essential Formulas You Must Know

Einstein's Photoelectric Equation

$$ E_k = h\nu - h\nu_0 = h\nu - \phi $$

Where:
$E_k$ = Maximum kinetic energy of photoelectrons
$h$ = Planck's constant ($6.626 \times 10^{-34}$ Js)
$\nu$ = Frequency of incident light
$\nu_0$ = Threshold frequency
$\phi$ = Work function

Key Relationships

Stopping Potential:

$ eV_0 = E_k = h\nu - h\nu_0 $

Work Function:

$ \phi = h\nu_0 = \frac{hc}{\lambda_0} $

Kinetic Energy vs Frequency:

$ E_k = h(\nu - \nu_0) $

1

Identify Threshold Frequency (ν₀) or Work Function (φ)

Example Problem

A metal surface has work function 2.3 eV. Light of wavelength 400 nm is incident on it. Calculate the maximum kinetic energy of emitted electrons.

Step 1.1: Convert units if necessary

Work function: $\phi = 2.3$ eV

Convert to joules: $\phi = 2.3 \times 1.6 \times 10^{-19} = 3.68 \times 10^{-19}$ J

Step 1.2: Find threshold frequency

Using $\phi = h\nu_0$:

$\nu_0 = \frac{\phi}{h} = \frac{3.68 \times 10^{-19}}{6.626 \times 10^{-34}} = 5.55 \times 10^{14}$ Hz

💡 Key Insights

  • Threshold frequency is the minimum frequency needed for photoemission
  • If $\nu < \nu_0$, no photoelectrons are emitted regardless of intensity
  • Work function is a material property - different for each metal
  • Common conversions: 1 eV = $1.6 \times 10^{-19}$ J
2

Apply Einstein's Photoelectric Equation

Continuing Our Example

Step 2.1: Find frequency of incident light

Wavelength $\lambda = 400$ nm = $400 \times 10^{-9}$ m

$\nu = \frac{c}{\lambda} = \frac{3 \times 10^8}{400 \times 10^{-9}} = 7.5 \times 10^{14}$ Hz

Step 2.2: Apply Einstein's equation

$E_k = h\nu - h\nu_0 = h(\nu - \nu_0)$

$E_k = 6.626 \times 10^{-34} \times (7.5 - 5.55) \times 10^{14}$

$E_k = 6.626 \times 10^{-34} \times 1.95 \times 10^{14} = 1.29 \times 10^{-19}$ J

In eV: $E_k = \frac{1.29 \times 10^{-19}}{1.6 \times 10^{-19}} = 0.806$ eV

💡 Common Variations

  • Sometimes given in terms of wavelength: $E_k = \frac{hc}{\lambda} - \phi$
  • If $\nu < \nu_0$, $E_k$ is negative ⇒ no photoemission
  • Intensity affects number of photoelectrons, not their energy
  • Remember: $hc = 1240$ eV·nm (useful conversion)
3

Find Stopping Potential (V₀)

Complete the Calculation

Step 3.1: Use stopping potential relation

$eV_0 = E_k$

$V_0 = \frac{E_k}{e} = \frac{1.29 \times 10^{-19}}{1.6 \times 10^{-19}} = 0.806$ V

Final Answers:

  • Maximum kinetic energy = 0.806 eV
  • Stopping potential = 0.806 V
  • Threshold frequency = $5.55 \times 10^{14}$ Hz

💡 Physical Significance

  • Stopping potential measures maximum kinetic energy of photoelectrons
  • $V_0$ vs $\nu$ graph gives straight line with slope $h/e$
  • X-intercept gives threshold frequency
  • Y-intercept gives -φ/e
4

Analyze Graphs and Experimental Data

Key Graphs in Photoelectric Effect

1. $E_k$ vs $\nu$ Graph

Straight line with slope = h, intercept = -φ

Equation: $E_k = h\nu - \phi$

2. $V_0$ vs $\nu$ Graph

Straight line with slope = h/e

Equation: $eV_0 = h\nu - \phi$

3. Photocurrent vs Voltage Graphs

Saturation current depends on intensity, stopping potential depends on frequency

💡 Graph Analysis Tips

  • Slope of $V_0$ vs $\nu$ graph = $h/e$ (can be used to find h)
  • X-intercept = threshold frequency $\nu_0$
  • Changing intensity shifts saturation current, not stopping potential
  • Changing frequency shifts stopping potential and saturation current

Complete JEE-Level Problem

JEE Main 2022 Problem

Light of wavelength 248 nm is incident on a cesium surface ($\phi = 1.95$ eV). Calculate:

  1. Threshold wavelength for cesium
  2. Maximum kinetic energy of photoelectrons
  3. Stopping potential

Step 1: Find threshold wavelength

$\phi = 1.95$ eV = $1.95 \times 1.6 \times 10^{-19}$ J

$\lambda_0 = \frac{hc}{\phi} = \frac{6.626 \times 10^{-34} \times 3 \times 10^8}{1.95 \times 1.6 \times 10^{-19}} = 6.37 \times 10^{-7}$ m = 637 nm

Step 2: Apply Einstein's equation

Using $hc = 1240$ eV·nm (convenient units):

$E_k = \frac{hc}{\lambda} - \phi = \frac{1240}{248} - 1.95 = 5.0 - 1.95 = 3.05$ eV

Step 3: Find stopping potential

$V_0 = \frac{E_k}{e} = 3.05$ V

⚠️ Common Mistakes to Avoid

Conceptual Errors

  • Thinking intensity affects photoelectron energy
  • Confusing threshold frequency with threshold wavelength
  • Forgetting to convert eV to joules (or vice versa)
  • Mixing up slope interpretations in graphs

Calculation Errors

  • Using wrong value of Planck's constant
  • Not paying attention to units (nm vs m, eV vs J)
  • Sign errors in Einstein's equation
  • Misreading graph intercepts and slopes

📝 Practice Problems

Problem 1: A metal has work function 4.2 eV. Light of wavelength 200 nm is incident. Will photoemission occur? If yes, find stopping potential.

Hint: Compare incident energy with work function

Problem 2: The stopping potential for light of wavelength 4000 Å is 1.3 V. Find the work function of the metal.

Hint: Use $eV_0 = \frac{hc}{\lambda} - \phi$

Problem 3: Light of frequencies 1.5ν₀ and 2ν₀ are incident on a metal surface. Find the ratio of maximum kinetic energies of photoelectrons.

Hint: Use $E_k = h(\nu - \nu_0)$

📋 4-Step Method Summary

Step-by-Step Checklist

  1. Find ν₀/φ: Identify threshold frequency or work function
  2. Einstein's Eq: Apply $E_k = h\nu - \phi$
  3. Stopping Potential: Use $V_0 = E_k/e$
  4. Graph Analysis: Interpret slopes and intercepts

Key Constants & Formulas

  • $h = 6.626 \times 10^{-34}$ Js
  • $hc = 1240$ eV·nm
  • 1 eV = $1.6 \times 10^{-19}$ J
  • $\phi = h\nu_0 = hc/\lambda_0$
  • $E_k = h\nu - \phi = eV_0$

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