In simple terms
A friendly intro before the formal notes — no formulas yet.
Energy in simple harmonic motion
Cambridge 9702 Paper 4 — Energy in simple harmonic motion (17.2). Senpai Corner diagram-backed pilot with premium structure and live visuals.
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17.2 Energy in simple harmonic motion.
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During SHM, energy is constant exchanged between KE and PE.
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When one goes up, the other goes down and vice versa.
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E.g., the PE of a pendulum swing is maximum when it is at the top of the swing whereby it momentarily stops (KE=0) and reverse direction.
What this topic covers
The official Cambridge syllabus points this lesson works through.
- 17.2.1
Describe the interchange between kinetic and potential energy during simple harmonic motion
- 17.2.2
Recall and use for the total energy of a system undergoing simple harmonic motion
Explore the concept
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Key formulas
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Tap a symbol — great for exam definitions
Tap a symbol — great for exam definitions
Tap a symbol — great for exam definitions
Tap a symbol — great for exam definitions
Full topic notes
Formal explanation with the rigour you need for the exam.
Energy Interconversion in SHM
Imagine a mass-spring system: as the mass moves, its energy continuously transforms. When it's fastest at the equilibrium position, all energy is kinetic. As it slows down moving towards maximum displacement, kinetic energy converts into potential energy, stored in the stretched or compressed spring. At the very ends of its motion, it momentarily stops, meaning all its energy is now potential, ready to pull or push it back.
17.2 Energy in simple harmonic motion.
During SHM, energy is constant exchanged between KE and PE.
When one goes up, the other goes down and vice versa.
E.g., the PE of a pendulum swing is maximum when it is at the top of the swing whereby it momentarily stops (KE=0) and reverse direction.
The KE is maximum at the point of equilibrium (bottom PE=0).
Speed (v) is max when displacement x = 0. Hence KE is maximum.
Key Energy Formulas
The beauty of SHM lies in its predictable energy variations. We have specific formulas to quantify the kinetic and potential energy at any given displacement, . These equations are derived from the velocity-displacement relationship in SHM and are crucial for understanding how energy distribution shifts throughout an oscillation.
Kinetic Energy (KE):
Potential Energy (PE):
Total Energy (E):
Remember that total energy is constant in ideal SHM. If you know the amplitude, you can calculate the total energy, which simplifies finding KE or PE at any point!
Graphical Representation of Energy in SHM
The relationship between energy and displacement in SHM can be visualized with a graph. The potential energy () is a parabola opening upwards, zero at equilibrium () and maximum at the amplitudes (). The kinetic energy () is an inverted parabola, maximum at equilibrium and zero at the amplitudes. The total energy () is a constant horizontal line, representing the conservation of energy. The points where the KE and PE graphs intersect are where the energy is split equally between kinetic and potential.
Damping: Energy Loss
In the real world, no oscillation lasts forever. Damping is the process where energy is gradually lost from an oscillating system, typically converted into heat or sound. This energy dissipation causes the amplitude of the oscillations to decrease over time. The rate at which energy is removed determines the type of damping, influencing how quickly the system returns to equilibrium.
The physical cause of damping is any force that opposes motion and is non-conservative, such as air resistance or friction within the material of a spring. In a car's suspension system, shock absorbers are designed to provide critical damping, preventing the car from bouncing excessively after hitting a bump. This ensures a smooth ride and maintains tyre contact with the road.
Damping dissipates energy from the system, usually as heat or sound.
It causes the amplitude of oscillations to decrease over time.
Underdamping shows slow amplitude decay over many cycles.
Critical damping returns to equilibrium fastest without oscillation.
Overdamping returns to equilibrium slowly, also without oscillation.
Resonance: Energy Gain
While damping removes energy, forced oscillations involve an external force continuously supplying it. When this external driving force's frequency exactly matches the system's natural frequency, a phenomenon called resonance occurs. This leads to highly efficient energy transfer, causing a dramatic increase in the amplitude of oscillations. Think of pushing a child on a swing at just the right time!
Resonance has many important applications. In radio receivers, tuning circuits are adjusted to resonate at the frequency of a specific radio station, amplifying its signal while ignoring others. Magnetic Resonance Imaging (MRI) uses resonance of atomic nuclei in a magnetic field to create detailed images of body tissues. However, resonance can also be destructive, as famously demonstrated by the collapse of the Tacoma Narrows Bridge in 1940, where wind-induced oscillations matched the bridge's natural frequency.
Forced oscillations involve an external driving force.
Resonance occurs when driving frequency equals natural frequency.
Efficient energy transfer causes a large amplitude increase.
Damping limits the maximum amplitude at resonance.
Increased damping makes the resonance curve broader and lower.
Resonance is often misunderstood! Remember it's about efficient energy transfer, not just any large amplitude. Damping always works against resonance, reducing its peak effect.
Worked examples
See the formulas applied — reveal one step at a time, like the exam.
A 0.2 kg mass oscillates with SHM on a spring. Its angular frequency is 5 rad s.05 m. Calculate the kinetic energy when the displacement from equilibrium is 0.03 m.
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Identify given values: , , , .
A simple pendulum has a bob of mass 0.50 kg and oscillates with a period of 2.0 s. The amplitude of the oscillation is 8.0 cm. Calculate: (a) the total energy of the oscillation, and (b) the displacement at which the kinetic energy is equal to the potential energy.
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Identify given values and convert units: , , .
How it all connects
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Glossary
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Quick check
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Revision flashcards
Flip the card. Test yourself before the exam.
At what point in SHM is potential energy maximized?
Potential energy is maximized when the object is at its maximum displacement (amplitude) from the equilibrium position.
Key takeaways
Review these before you close the topic — retrieval beats re-reading.
- ✓
17.2 Energy in simple harmonic motion.
- ✓
During SHM, energy is constant exchanged between KE and PE.
- ✓
When one goes up, the other goes down and vice versa.
- ✓
E.g., the PE of a pendulum swing is maximum when it is at the top of the swing whereby it momentarily stops (KE=0) and reverse direction.
- ✓
The KE is maximum at the point of equilibrium (bottom PE=0).
- ✓
Speed (v) is max when displacement x = 0. Hence KE is maximum.
Practice — then mark it
The whole point: a real Cambridge question, marked mark-by-mark.
9702/42 · Q5(c)
On Fig. 5.3, sketch the variation with x of the kinetic energy Ek of the sphere.
Extra simulations & links
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Frequently asked
Checkpoint
One marked question is worth ten re-reads — close the loop before you move on.
Reading it isn’t knowing it — prove it.
Before you move on: do 9702/42 · Q5(c) on paper, snap a photo, and get examiner-style feedback on exactly where you win and lose marks.