Derive spring period and distinguish frequency measures
One cycle returns the oscillator to the same position and direction of motion. The period T is time per cycle; frequency f=1/T counts cycles per second. Angular frequency ω=2πf measures phase advance in radians per second. Confusing f and ω introduces a factor of 2π, even though both describe the same repetition.
Learning outcome: Choose two masses at one stiffness; predict the period ratio before capture. Then change stiffness to keep m/k fixed. Record T, f and ω separately, including their units. Explain which amplitude claim follows from the model rather than a measured spring.
Starting recap
Review Newton’s second law, radians, sine/cosine graphs, energy and momentum boundaries, and bounded measurement errors.
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Try
For m=1 kg and k=20 N/m, ω=√20≈4.472 rad/s, T≈1.405 s and f≈0.712 Hz. Replacing the mass by 4 kg with the same spring doubles T to about 2.810 s. Doubling amplitude within the linear range leaves these periods unchanged.
Open the experimentPredict
If both mass and stiffness double, does the period change?
Experiment
Choose two masses at one stiffness; predict the period ratio before capture. Then change stiffness to keep m/k fixed. Record T, f and ω separately, including their units. Explain which amplitude claim follows from the model rather than a measured spring.
Predict period from inertia and stiffness
Worked teaching model · synthetic values · Ideal massless Hooke-law spring and point mass, no drag or friction. Motion remains within the linear spring range; amplitude is not a period control.
Reset keeps your prediction, captures and practice history.
| Quantity | Value | Unit |
|---|---|---|
| Angular frequency | 4.47214 | rad/s |
| Period | 1.40496 | s |
| Frequency | 0.71176 | Hz |
| Period squared | 1.97392 | s² |
Accessible plot coordinates
| coordinate | value |
|---|
Period grows with square root of mass and falls with square root of stiffness.
From ma=−kx and a=−ω²x, ω²=k/m and T=2π√(m/k). Amplitude cancels only for the ideal linear model, not for arbitrary oscillators.
Period grows with square root of mass and falls with square root of stiffness.
From ma=−kx and a=−ω²x, ω²=k/m and T=2π√(m/k). Amplitude cancels only for the ideal linear model, not for arbitrary oscillators.
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Public practice checks a specific claim. It does not establish independent mastery.
What additional evidence would separate a moving-spring-mass effect from a timing offset in a nonzero T² intercept?
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