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Simple harmonic motion IB DP Physics Study Notes

Simple harmonic oscillations IB DP Physics Study Notes

Simple harmonic oscillations IB DP Physics Study Notes at  IITian Academy  focus on  specific topic and type of questions asked in actual exam. Study Notes focus on IB Physics syllabus with Students should understand

  • conditions that lead to simple harmonic motion
  • A particle undergoing simple harmonic motion can be described using the time period \( T \), frequency \( ƒ \),
    angular frequency \( \omega \), amplitude, equilibrium position, and displacement

  • The time period in terms of frequency of oscillation is given by:
    \(T = \frac{1}{ƒ}\)

  • The time period in terms of angular frequency is given by:
    \(T = \frac{2\pi}{\omega}\)

Standard level and higher level: 3 hours
Additional higher level: 4 hours

IB DP Physics 2025 -Study Notes -All Topics

Oscillations

  • Oscillations are vibrations which repeat themselves.
  • EXAMPLE: Oscillations can be driven externally, like a pendulum in a gravitational field.
  •  
  • EXAMPLE: Oscillations can be driven internally, like a mass on a spring.
    FYI ∙In all oscillations, v = 0 at the extremes and v = vmax in the middle of the motion.
  •  
  • EXAMPLE: Oscillations can be very rapid vibrations such as in a plucked guitar string or a tuning fork.

Time period, amplitude and displacement

  • Consider a mass on a spring that is displaced 4 meters to the right and then released.
  • We call the maximum displacement x0 the amplitude. In this example x0 = 4 m.
  • We call the point of zero displacement the equilibrium position. Displacement x is measured from equilibrium.
  • The period T (measured in s) is the time it takes for the mass to make one full oscillation or cycle.
  • For this particular oscillation, the period T is about 24 seconds (per cycle).

Time period and frequency 

  • The frequency $f$ (measured in Hz or $\frac{\text{cycles}}{\text{s}}$) is defined as how many cycles (oscillations, repetitions) occur each second.
  • Since period $T$ is seconds per cycle, frequency must be $\frac{1}{T}$. Therefore, the relation between $T$ and $f$ is:

EXAMPLE: The cycle of the previous example repeated each 24 s. What are the period and the frequency of the oscillation?

SOLUTION:

 The period is $T = 24$ s.

The frequency is $f = \frac{1}{T} = \frac{1}{24} \approx 0.042$ Hz.

Angular speed ω

  • Since 2π rad = 360° = 1 rev it should be clear that the angular speed ω is just: $\frac{2\pi}{T}$. This means $T = \frac{2\pi}{\omega}$.
  • And since $f = \frac{1}{T}$ it should also be clear that ω = 2πf.

EXAMPLE: Find the angular frequency (angular speed) of the second hand on a clock.

SOLUTION:

Since the second hand turns one circle each 60 s, it has an angular speed of:

ω = $\frac{2\pi}{T}$ = $\frac{2\pi}{60}$ = 0.105 rad s⁻¹

Phase difference

  • We can pull the mass to the right and then release it to begin its motion:
  •  
  • Or we could push it to the left and release it:
  • Both motions would have the same values for T and f.
  • However, the resulting motion will have a phase difference of half a cycle.

Two identical mass-spring systems are started in two different ways. What is their phase difference?

The phase difference is one-quarter of a cycle.
The phase difference is three-quarter of a cycle.

Conditions for simple harmonic motion

  • If we place a pen on the oscillating mass, and pull a piece of paper at a constant speed past the pen, we trace out the displacement vs. time graph of SHM.
  • SHM traces out perfect sinusoidal waveforms.
  •  

  • Note that the period can be found from the graph: Just look for repeating cycles.

Conditions for simple harmonic motion

  • A very special kind of oscillation that shows up often in the physical world is called simple harmonic motion.
  • In simple harmonic motion (SHM), a and x are related in a very precise way: Namely, a ∝ -x.
  • The minus sign in Hooke’s law, F = -kx, tells us that if the displacement x is positive (right), the spring force F is negative (left).
  • It also tells us that if the displacement x is negative (left), the spring force F is positive (right).
  • Any force that is proportional to the opposite of a displacement is called a restoring force.
  • For any restoring force F ∝ -x.
  • Since F = ma we see that ma ∝ -x, or a ∝ -x.
  • All restoring forces can drive simple harmonic motion (SHM).
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