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Lecture notes

UNIT 4 Physics Oxford IB Diploma Programme

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These are detailed notes of the IBDP Physics course Unit 4: Waves.

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Uploaded on
May 29, 2024
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Written in
2023/2024
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Unit 4 of ibdp physics sl and hl

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Oscillations
Oscillation: the cyclical and periodic variation of the displacement x of an object about an
equilibrium position (x=0).
- "Cyclical”: the motion repeats in cycles,
- "Periodic": the motion occurs at regular intervals




- Displacement (x): distance of a point on the wave from its equilibrium position. As a
vector quantity, it can be positive/negative [m - meters].

- Amplitude (A or 𝑥0): the maximum displacement of an oscillating wave on either
side of the equilibrium position. Depends on initial energy input from primary
oscillator.0

- Wavelength (λ): length of one complete complete oscillation measured from the same
point on two consecutive waves [m - meters].

- > frequency < wavelength




- Period (T): time interval for a point on the wave to undergo a complete repetition [s -
seconds]. Depends on the medium’s properties (e.g mass and spring constant, or length
of a string etc.) not on the energy supplied by primary oscillator or displacement.

- Isochronous: oscillations have a constant period.

- Frequency (f): number of full oscillations per second [Hz - hertz, or s-1]
1
𝑓= 𝑇

,
,Simple Harmonic Motion (SHM)
SHM: a motion arising from a linear restoring force directed to a fixed equilibrium position.

Conditions of SHM:
- Fixed cyclical path

- Isochronous (i.e the motion repeats at equal time intervals)

- Central equilibrium point

- Displacement, velocity and acceleration change continuously

- Linear restoring force directed to equilibrium position and opp. to displacement


Linear Restoring force
- Switch direction every half cycle, becoming 𝐹𝑛𝑒𝑡 = 0 at equilibrium point,

- |𝐹𝑛𝑒𝑡 | not constant, but increases proportionally with displacement.
𝐹𝑛𝑒𝑡 ∝ (− 𝑥)
𝑎 ∝ (− 𝑥)

- Hooke’s Law (spring system): 𝐹𝑛𝑒𝑡 = − 𝑘𝑥, where k is spring’s constant
- > k → > acceleration > frequency, < period, = amplitude

, SHM in pendulum




- 𝑇 − 𝑚𝑔𝑐𝑜𝑠θ = 0, no motion along string
- 𝑚𝑔𝑠𝑖𝑛θ = 𝑚𝑎, tangential motion → 𝑎 = 𝑔𝑠𝑖𝑛θ

SHM in spring




0 1 2 3

Displacement (x) < > < >
- - + +

Acceleration (a) < > < >
+ - + -

Speed (v) >, at < rate <, at > rate >, at < rate <, at > rate
- - + +
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