Wait, What? If the speed changes while you change radius, you are no longer testing radius.
Circular-motion practicals are easy to contaminate because force, speed and radius are tightly coupled. A student may move a marker outward, spin faster without noticing, and then attribute the larger force to radius alone. The experiment therefore lives or dies on variable control.
The model
For uniform circular motion:
F = mv²/r
or, using angular speed ω:
F = mω²r
These forms show why the independent variable must be chosen explicitly. Testing F against v² requires m and r to stay constant. Testing F against r at constant ω requires m and ω to stay constant.
Timing many revolutions
One revolution is usually too fast for reliable hand timing. Time 10, 20 or more revolutions, then divide by the count to obtain the period T.
Speed can then be estimated from:
v = 2πr/T
Reaction-time uncertainty becomes a smaller fraction of the total interval when many cycles are timed.
Radius must be measured to the centre of mass path
The relevant radius is the distance from the axis of rotation to the path of the rotating mass’s centre. Measuring to a string knot or outer edge can introduce a fixed geometry error.
A marker on the string helps maintain a chosen radius, but the marker itself is not necessarily the centre-of-mass location.
Using a hanging mass to set force
In one common design, a hanging mass provides string tension. If the hanging mass remains approximately stationary while the rotating mass moves in a horizontal circle, the string tension is close to the hanging weight:
F ≈ mhg
If the hanger bobs up and down, the tension is not simply constant weight. The apparatus itself is telling you that the intended force condition has failed.
Quantitative window
A 0.050 kg rotating mass moves in a circle of radius 0.40 m. Twenty revolutions take 16.0 s.
T = 16.0/20 = 0.800 s
v = 2π(0.40)/0.800 ≈ 3.14 m s⁻¹
F = mv²/r ≈ 0.050(3.14²)/0.40 ≈ 1.23 N
This corresponds to a hanging mass of about 0.125 kg if the simple tension model holds.
Graph methods
At fixed m and r, plot F against v². The model predicts a straight line with gradient m/r.
At fixed m and ω, plot F against r. The model predicts a straight line with gradient mω².
Choosing the wrong graph can hide whether the experiment actually tests the intended proportionality.
Observation versus inference
Observation: “At r = 0.40 m, 20 revolutions took 16.0 s while the hanger remained approximately stationary.”
Inference: “The rotating mass moved with approximately steady speed and experienced inward force near 1.23 N under the model assumptions.”
Failure modes
- Changing radius and speed together.
- Timing too few revolutions.
- Measuring radius from the wrong geometric point.
- Hanging mass oscillating instead of remaining steady.
- Circle tilted out of the intended plane.
- String stretching with force.
- Assuming constant speed from one average timing result.
Unfamiliar transfer: banked motion
A car on a banked curve still needs inward acceleration, but the inward force can come from components of normal reaction and friction rather than string tension. The transferable skill is to identify the radial direction and determine which real forces contribute to the net inward force.
Secondary → JC → deeper Physics
Secondary: connect circular motion to inward acceleration and measure period reliably.
JC: test F ∝ v² and F ∝ r under controlled conditions, use graphs and analyse tension assumptions.
Deeper Physics: extend to rotating frames, angular momentum, rigid-body dynamics and non-uniform circular motion.
Checkpoint
A student doubles the radius and notices the required hanging mass also doubles, but the revolution time changes too. Has F ∝ r been demonstrated?
Answer key and WHY reasoning
Not cleanly. The F ∝ r form assumes angular speed is constant. If the period changed, ω changed too, so two variables influenced the force.
How to study this practical
Before each run write three quantities in a triangle: force, radius, speed. Circle the one you are changing and cross-check that the other two are truly controlled or explicitly measured.
Evidence boundaries
A school circular-motion experiment tests the radial-force model under approximately uniform speed and controlled geometry. It does not prove that string tension is perfectly constant or that the motion is exactly circular at every instant.
Authoritative next steps
Teaching Guide
Give students two datasets: one with radius varied at constant period and one with radius varied while period drifts. Ask which can test F ∝ r. This makes control-variable reasoning visible rather than implicit.
