7.1Oscillations
Defining Simple Harmonic Motion (SHM) — AP PHYSICS 1 Revision Notes & Topical Questions
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Lesson summary
7.1 Defining Simple Harmonic Motion (SHM) — AP PHYSICS 1 notes: Describe simple harmonic motion in terms of a restoring force proportional to displacement.SHM = a special case of periodic motion in which the restoring force is proportional to the displacement from equilibrium and…
- Equilibrium position
- Amplitude A
- Hooke's law
- Newton's second law
- Restoring torque
- Small angles
Section 1 of 9What SHM is
What SHM is
SHM
SHM a special case of periodic motion in which the restoring force is proportional to the displacement from equilibrium and in the opposite direction, F = −kx.
Equilibrium position
- Equilibrium position where the net force is zero, usually labelled x = 0; displacement x is measured from it.
Restoring force
- Restoring force a force opposite to the displacement from equilibrium.
Amplitude A
- Amplitude A maximum displacement.
Systems
- Systems an object–ideal spring system on a frictionless surface and a pendulum with small angular displacement.
Section 2 of 9Derived equation for a spring
Hooke's law
- Fs = −kx with k in N/m.
Newton's second law
- Newton's second law max = −kx.
Result
- Result the acceleration is proportional to the displacement and opposite to it.
Section 3 of 9Pendulum
Restoring torque
- Restoring torque must be proportional to angular displacement and opposite to it.
Small angles
- Small angles only for about 15° or less, where mg sinθ ≈ mgθ.
Large angles
- Large angles periodic but not accurately SHM.
Section 4 of 9Features of SHM
Features of SHM
At extremes (x = ±A)
- At extremes (x = ±A) acceleration is maximum, speed is zero.
At equilibrium
- At equilibrium acceleration is zero, speed is maximum.
Acceleration direction
- Acceleration direction always toward equilibrium.
Period
- Period independent of amplitude.
Vertical spring
- Vertical spring the new equilibrium is at kΔx0 = mg; oscillations about it are SHM with the same k.
Section 5 of 9Is it SHM?
| System | Restoring force | Proportional to −x? | SHM? |
|---|---|---|---|
| Mass on spring | −kx | Yes | Yes, within Hooke's law |
| Simple pendulum | −mg sinθ | Approximately for small θ | Approximately |
| Bouncing ball | mg, constant | No | No |
| Floating block bobbing | Buoyancy change | Yes | Yes |
Section 6 of 9Testing a motion
1
Locate the equilibrium position where the net force is zero.
2
Displace the object by x and find the net force.
3
Check whether the net force is proportional to x.
4
Check that the force points back toward equilibrium.
5
If both hold, the motion is SHM with F = −kx.
Section 7 of 9More from the specification
1Oscillation period and simple harmonic cycle
- Oscillation period and simple harmonic cycle the time taken to complete one full mechanical oscillation cycle remains invariant across varying amplitudes.
2Frequency
- Revolutions per second, f = 1/T.What the symbols mean: T = period, the time for one complete wave (s) · f = frequency (Hz)
Section 8 of 9Key terms
| Term | Meaning |
|---|---|
| Simple harmonic motion | Oscillation where restoring force is proportional to −displacement. |
| Restoring force | F = −kx, toward equilibrium. |
| Equilibrium position | Position where the net force is zero. |
| Amplitude | Maximum displacement. |
| Oscillation | Repeated back-and-forth motion. |
Section 9 of 9Exam technique
1
Treating any periodic motion as SHM.
2
Measuring displacement from the spring's natural length for a vertical spring instead of from the equilibrium.
3
Thinking acceleration is zero at the extremes.
4
Using a large pendulum angle and assuming SHM.
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