PHOTOELECTRIC EFFECT & CIRCUIT LABORATORY

Investigate the quantized nature of light by firing photons at diverse metal cathodes. Construct the full experimental schematic, monitor the photocurrent, and plot your findings dynamically to verify Planck's constant and experimental stopping potentials.

Circuit Status: INCOMPLETE (OPEN)
Photon Energy: 3.10 eV
Applied Voltage (V): 0.00 V
Photocurrent (I): 0.00 μA
Theo. Stop Pot. (V∞): 0.96 V

Experimental ControlsΦ = 2.14 eV

Experimental Data Logger

# Emitter Wavelength (nm) Freq (×10¹⁴ Hz) Applied Voltage (V) Current (μA) Exp. Stop Pot. (V) Max KE (eV)
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How to Operate the Simulator

A critical part of the photoelectric experiment is building the circuit and finding the exact voltage that brings the escaping photoelectrons to a halt.

  • Wiring Tab: Click and drag components to arrange them. Click any terminal to begin routing a wire, and click another terminal to close the connection. For help, press the Auto-Wire button in the controls panel.
  • Lab Tab: Wait until the status says ACTIVE (CLOSED LOOP). Select your Emitter Metal and adjust the Wavelength of the incident light. If the photon energy exceeds the Work Function (Φ), electrons will be emitted.
  • Stopping Potential: Slide the Applied Voltage towards the negative (retarding) range. Carefully observe the Digital Ammeter Reader. When the current reads precisely 0.00 μA, you have found the boundary where electrons are stopped.
  • Click Record Data. Your Experimental Stopping Potential will be logged, and automatically plotted onto the V∞ vs Frequency characteristic graph in the Graphs Tab.

Scientific Theory & Working Principles

The Photoelectric Effect occurs when light is shined on a metal surface, causing the emission of electrons (photoelectrons). Classical physics predicted that the energy of the emitted electrons should depend on the intensity (brightness) of the light. However, experiments showed that the kinetic energy of emitted electrons depends entirely on the frequency (color) of the light, not the intensity.

In 1905, Albert Einstein explained this by proposing that light behaves as discrete packets of energy called photons. Each photon has an energy proportional to its frequency. For an electron to escape the metal surface, it must absorb a single photon with energy greater than the metal's binding energy, known as the Work Function (Φ). Any leftover energy becomes the kinetic energy of the escaping electron.

Mathematical Foundations & Formulas

Use the following equations to govern your calculations in the simulator:

Photon Energy: E = h × f = (h × c) / λ

Maximum Kinetic Energy: K_max = E - Φ

Stopping Potential: V_0 = K_max / e

Constants applied:

  • Planck's Constant (h) = 6.626 × 10 ⁻³⁴ J·s  (or 4.136 × 10 ⁻¹⁵ eV·s)
  • Speed of Light (c) = 3 × 10 ⁸ m/s
  • For convenience in eV and nm, hc ≈ 1240 eV·nm

Real-World Engineering & Industrial Applications

  • Solar Panels (Photovoltaics): Rely heavily on similar principles, utilizing semiconductor materials to absorb photons and generate electron flow for electricity.
  • Night Vision Goggles: Use photocathodes that turn faint ambient photons into electrons, which are then multiplied and smashed into a phosphor screen to produce a visible image.
  • Photomultiplier Tubes: Used in medical imaging and astronomical detectors to detect single photons by converting them into a measurable current cascade.

Practice Problems & Diagnostic Tasks

Test your quantitative comprehension using the five laboratory exercises below:

Task 1: Basic Energy Calculation

Using the formula E = hc / λ, calculate the energy (in eV) of a photon of light with a wavelength of 400 nm. Assume hc = 1240 eV·nm.

Task 2: Kinetic Energy Threshold

If you shine that same 400 nm light onto a Sodium (Na) target which has a Work Function (Φ) of 2.36 eV, what is the maximum kinetic energy of the emitted photoelectrons?

Task 3: Determining Stopping Potential

Based on your answer to Task 2, what applied retarding voltage (Stopping Potential, V_0) must be applied to the circuit to bring the current exactly to 0.00 μA?

Task 4: Effect of Intensity Variations

If the intensity of the light in the previous tasks is doubled from 50% to 100%, what happens to the Stopping Potential? What happens to the maximum flowing current?

Task 5: Reverse Work Function Calculation

During an experiment with an unknown metal, a student observes that the emission of electrons stops completely when the frequency of light drops below 5.5 × 10¹⁴ Hz. Calculate the exact work function (Φ) of this metal in electron-volts (eV). (Use h = 4.136 × 10 ⁻¹⁵ eV·s).

Click to Reveal Solutions and Step-by-Step Proofs

Solution to Task 1:
E = hc / λ
E = 1240 / 400 = 3.10 eV.

Solution to Task 2:
K_max = E - Φ
K_max = 3.10 eV - 2.36 eV = 0.74 eV.

Solution to Task 3:
Stopping potential V_0 is numerically equal to the maximum kinetic energy when measured in electron-volts.
V_0 = 0.74 eV / 1 e = 0.74 V. The applied voltage must be set to -0.74 V.

Solution to Task 4:
The Stopping Potential remains exactly the same (-0.74 V) because intensity does not change the energy of individual photons. However, doubling the intensity means twice as many photons hit the metal, meaning the maximum current will double.

Solution to Task 5:
The frequency given is the threshold frequency (f_0), where the photon energy exactly matches the work function.
Φ = h × f_0
Φ = (4.136 × 10 ⁻¹⁵) × (5.5 × 10¹⁴)
Φ = 2.27 eV.