Millikan Terminal Drop Charge Balance
An oil drop’s fall and rise speeds reveal its charge, while a holding field makes the force balance visible.
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Millikan Terminal Drop Charge Balance
The Millikan oil drop experiment involves observing tiny oil drops in a chamber where an electric field can be applied. By measuring the terminal speed of a drop falling under gravity and its terminal speed rising under an applied electric field, its charge can be inferred.
worked-example
Consider a dimensionless sphere with viscosity η = 1, density difference times gravity gΔρ = 1, drop radius r = 0.5, and an applied upward electric field E = 1. The charge on the drop is q = 1.
First, calculate the effective weight W:
W = (4/3) * π * r3 = (4/3) * π * (0.5)3 ≈ 0.5235987755982988
Calculate the field-off terminal speed v_(fall), where drag balances weight:
v_fall = -W / (6 * π * r * η) = -0.5235987755982988 / (6 * π * 0.5 * 1) ≈ -0.05555555555555555
Calculate the terminal upward speed v with the electric field on, where electric force, weight, and drag balance:
v = (qE - W) / (6 * π * r * η) = (1 * 1 - 0.5235987755982988) / (6 * π * 0.5 * 1) ≈ 0.050547739839041345
Finally, using the measured speeds to infer the charge:
q = 6 * π * r * η * (v - v_fall) / E = 6 * π * 0.5 * 1 * (0.050547739839041345 - (-0.05555555555555555)) / 1 ≈ 1.0
experiment
Explore the relationship between charge, drop radius, electric field, and terminal velocities in the interactive module:
https://riano.app/module/millikan-terminal-drop-charge-balance
- Set Drop radius to 0.5 and Charge units to 1.
- Set Selected field to 1 and Field mode to "Selected".
- Observe the calculated Terminal upward speed (approx 0.0505) and Inferred charge (1.0).
- Change the Field mode to "Hold if possible". Notice that the Terminal upward speed becomes exactly 0 as the field adjusts to exactly balance gravity.
limitations
This idealized model operates strictly in the Stokes flow regime where drag is proportional to velocity. It explicitly omits complexities found in the real experiment, such as:
- Brownian noise: Small droplets undergo random walks due to thermal collisions with air molecules, which adds noise to real speed measurements.
- Slip correction: When droplets are comparable in size to the mean free path of gas molecules, Stokes' law must be modified (Cunningham correction factor).
- Quantized charge assumption: This module synthetically assumes integer charge units for the simulation; it is a pedagogical model and not a raw data proof of charge quantization.
references
Primary reference for the historical context and original experimental details:
- Robert A. Millikan's Nobel Lecture (1924): "The electron and the light-quant from the experimental point of view", detailing the oil drop method.
Experience it interactively
Adjust parameters, observe in real time, and build deep intuition with Riano’s interactive Millikan Terminal Drop Charge Balance module.
Try Millikan Terminal Drop Charge Balance on Riano →