Simple harmonic oscillations

Section: Oscillations  |  Syllabus: Cambridge A Level Physics (9702)

Describing Oscillations

An oscillation is a type of periodic motion that repeats regularly (e.g., up and down, back and forward). The equilibrium position is the position where an object returns when oscillation stops; the resultant force at this position is zero.

Key Terms:

ω = 2π f = (2π/T)

Defining Simple Harmonic Motion (SHM)

Simple harmonic motion occurs when the restoring force (and thus acceleration) is proportional to the displacement and acts in the opposite direction.

a = -ω^2 x

The negative sign indicates that acceleration a and displacement x are always in opposite directions (acceleration is always directed towards the equilibrium position).

Figure 17.1: Simple Harmonic Motion Graphs

Graphs showing the relationship between displacement, velocity, and acceleration over time. Displacement as a sine curve, velocity as a cosine curve, and acceleration as a negative sine curve.

Equations of Motion

The displacement x depends on the starting position of the oscillation:

Velocity (v) and Acceleration (a) are derived from these:

v = v_0cos(ω t) (where v_0 = ω x_0 is the max velocity)

v = ± ω √(x_0^2 - x^2)

a = -ω^2 x = -ω^2 x_0sin(ω t)

Worked Examples

Worked Example: Ball in a Curved Bowl

Question: A ball oscillates in a curved bowl starting at the center (displacement zero). Amplitude is 5.0 cm and period is 860 ms. Calculate the displacement at t = 250 ms.

Solution

1. ω = 2π / T = 2π / 0.86 = 7.31 rad s^-1.

2. Since it starts at equilibrium, x = x_0sin(ω t).

3. x = 0.050 × sin(7.31 × 0.25) = 0.048 m (or 4.8 cm).

Note: Ensure your calculator is in RADIANS mode.

Worked Example: Floating Test Tube

Question: A test tube is lifted up by 2 cm and released. It oscillates with period 0.80 s. Sketch the displacement-time graph for two cycles.

Solution Sketch

Since the motion starts at max displacement (x = +2 at t = 0), the graph is a cosine curve starting at +2. Period is 0.8 s, so two cycles end at 1.6 s.

Figure 17.2: Test Tube Oscillation Graph

A cosine graph for x vs t. Y-axis: +2 to -2 cm. X-axis: Mark 0.4, 0.8, 1.2, 1.6 s.

The Vertical Mass-Spring System

A mass m on a spring with constant k obeys F = -kx. By Newton's Second Law (F=ma):

ma = -kx a = -(k/m)x

Since a = -ω^2 x, then ω^2 = (k/m).

T = 2π√(m/k)

Note: The period is independent of gravity (g) and the amplitude.

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