Introduction
The photoelectric effect is the emission of electrons from a metal surface when light of sufficient frequency shines on it. This phenomenon provided crucial evidence for the particle nature of light and earned Einstein the Nobel Prize in 1921.
Historical Context
Classical wave theory predicted:
- Higher intensity should give electrons more energy
- Any frequency should eventually cause emission
Experiments showed otherwise! This led to the quantum explanation.
Experimental Observations
Key Findings
Threshold frequency ($\nu_0$): Below this frequency, no electrons are emitted regardless of intensity
Instantaneous emission: Electrons are emitted immediately (within 10⁻⁹ s), not gradually
Intensity effect: More intensity = more electrons, but NOT higher kinetic energy
Frequency effect: Higher frequency = higher kinetic energy of emitted electrons
graph TD
A[Light hits metal] --> B{ν ≥ ν₀?}
B -->|Yes| C[Electrons emitted]
B -->|No| D[No emission]
C --> E[KE depends on frequency]
C --> F[Number depends on intensity]Einstein’s Explanation
Einstein (1905) proposed that light consists of photons, each carrying energy $E = h\nu$.
The Photoelectric Equation
$$\boxed{h\nu = \phi + \frac{1}{2}mv_{max}^2}$$or equivalently:
$$\boxed{h\nu = h\nu_0 + KE_{max}}$$where:
- $h\nu$ = Energy of incident photon
- $\phi = h\nu_0$ = Work function (minimum energy to remove electron)
- $\frac{1}{2}mv_{max}^2 = KE_{max}$ = Maximum kinetic energy of electron
- $\nu_0$ = Threshold frequency
Interactive Demo: Visualize Photoelectric Effect
See how light photons eject electrons from a metal surface based on frequency and intensity.
Understanding Work Function
The work function ($\phi$) is the minimum energy needed to remove an electron from the metal surface.
| Metal | Work Function (eV) |
|---|---|
| Cesium (Cs) | 2.14 |
| Potassium (K) | 2.30 |
| Sodium (Na) | 2.75 |
| Zinc (Zn) | 4.33 |
| Platinum (Pt) | 5.65 |
Stopping Potential
When a negative potential is applied to the collector, it can stop the most energetic electrons.
Definition
Stopping potential ($V_0$): The minimum negative potential needed to stop all photoelectrons.
$$\boxed{eV_0 = KE_{max} = h\nu - \phi}$$or:
$$V_0 = \frac{h\nu - \phi}{e} = \frac{h(\nu - \nu_0)}{e}$$Graphical Analysis
Plotting $V_0$ vs $\nu$:
- Slope = $\frac{h}{e}$ (universal constant)
- x-intercept = threshold frequency $\nu_0$
- y-intercept = $-\frac{\phi}{e}$
Threshold Wavelength
Since $\nu_0 = \frac{c}{\lambda_0}$, we can also define:
$$\boxed{\lambda_0 = \frac{hc}{\phi}}$$- If $\lambda < \lambda_0$: emission occurs
- If $\lambda > \lambda_0$: no emission
Remember:
- Threshold frequency is the minimum required
- Threshold wavelength is the maximum allowed
Don’t mix these up in problems!
Problem Solving Strategy
Step-by-step Approach
- Identify given values: frequency/wavelength, work function, KE
- Convert units: Ensure consistent units (eV or J)
- Apply Einstein’s equation: $h\nu = \phi + KE_{max}$
- Solve for unknown
Example 1: Finding KE
Problem: Light of wavelength 200 nm falls on a metal with work function 4.2 eV. Find the maximum KE of photoelectrons.
Solution:
Energy of photon:
$$E = \frac{hc}{\lambda} = \frac{6.626 \times 10^{-34} \times 3 \times 10^8}{200 \times 10^{-9}} = 9.94 \times 10^{-19} \text{ J}$$ $$E = \frac{9.94 \times 10^{-19}}{1.6 \times 10^{-19}} = 6.21 \text{ eV}$$Apply equation:
$$KE_{max} = E - \phi = 6.21 - 4.2 = 2.01 \text{ eV}$$
Example 2: Finding Threshold Frequency
Problem: The work function of sodium is 2.75 eV. Calculate its threshold wavelength.
Solution:
$$\lambda_0 = \frac{hc}{\phi} = \frac{6.626 \times 10^{-34} \times 3 \times 10^8}{2.75 \times 1.6 \times 10^{-19}}$$ $$\lambda_0 = 4.52 \times 10^{-7} \text{ m} = 452 \text{ nm}$$This is in the blue-violet region of visible light.
Important Points for JEE
- Photoelectric effect proves particle nature of light
- One photon ejects at most one electron
- Below threshold frequency: no emission regardless of intensity
- Stopping potential is independent of intensity
- Maximum KE depends only on frequency (not intensity)
Quick Formulas
| Quantity | Formula |
|---|---|
| Work function | $\phi = h\nu_0$ |
| Maximum KE | $KE_{max} = h\nu - \phi$ |
| Stopping potential | $V_0 = \frac{KE_{max}}{e}$ |
| Threshold wavelength | $\lambda_0 = \frac{hc}{\phi}$ |
| Maximum velocity | $v_{max} = \sqrt{\frac{2(h\nu - \phi)}{m}}$ |
Practice Problems
Light of frequency $1.5 \times 10^{15}$ Hz ejects electrons with maximum KE of 2 eV. Find the work function.
Two metals A and B have work functions 4 eV and 2 eV. What is the ratio of their threshold wavelengths?
If the intensity of light is doubled (keeping frequency same), how does the stopping potential change?