Defining Simple Harmonic Motion (College Board AP® Physics 1: Algebra-Based)

Study Guide

Test yourself
Dan Mitchell-Garnett

Written by: Dan Mitchell-Garnett

Reviewed by: Caroline Carroll

Defining simple harmonic motion

What is simple harmonic motion?

  • Simple harmonic motion (SHM) is a special case of periodic motion

  • In SHM, an object oscillates regularly around an equilibrium position:

An equilibrium position is a location at which the net force exerted on an object is zero

  • This is where displacement x is defined as zero so the equilibrium position will often be labeled with x space equals space 0

  • Examples of systems that exhibit SHM:

    • An object attached to a spring oscillating horizontally across a frictionless surface (often called an object-ideal spring system)

    • A pendulum (object suspended from a string) with a small angular displacement

Systems in simple harmonic motion

Two diagrams illustrate a mass spring system and a pendulum. The mass spring system shows a mass moving horizontally. The pendulum diagram shows a bob swinging.
Different systems can undergo SHM. A pendulum and object-ideal spring system are just two examples.

Conditions for simple harmonic motion

  • A restoring force is required for SHM:

A restoring force always acts in a direction opposite to the object’s displacement from an equilibrium position

  • The condition for SHM is that the restoring force is proportional to the displacement of the object from the equilibrium position but in the opposite direction

Conditions for a pendulum in SHM

  • A linear system, such as an object-ideal spring system, requires a restoring force in the opposite direction to linear displacement

  • A pendulum, however, is better described as moving through angular displacement

  • This means that, for a pendulum to undergo SHM, a restoring torque must be proportional to angular displacement but act in the opposite direction

    • These quantities are only proportional for small angular displacements

    • A pendulum can only be modeled as SHM when the angle is small

SHM in a pendulum

A pendulum with the angle to the vertical labelled as θ and the torque acting towards the equilibrium position marked as τ.
Angular displacement and torque are proportional for a pendulum, provided that angular displacement is small.

Derived equation

  • Simple harmonic motion of an object-ideal spring system can be characterized by the equation:

m a subscript x space equals space minus k straight capital delta x

  • This shows that the acceleration of the object is proportional to the displacement and acts in the opposite direction

Object-ideal spring system

A horizontal spring is connected to an object of mass m. The object is at a displacement Δx from equilibrium, with a restoring force F acting back towards equilbrium.
The restoring force acts in the opposite direction to displacement and always towards the equilibrium position. In this system, the restoring force comes from the spring.

Derivation

Step 1: Identify the fundamental equations

stack F subscript s with rightwards arrow on top space equals space minus k straight capital delta x with rightwards arrow on top

  • Where:

    • F with rightwards arrow on top subscript s = spring's force measured in straight N

    • k = spring constant of the spring, measured in straight N divided by straight m

    • straight capital delta x with rightwards arrow on top = displacement of the object from the equilibrium position, measured in straight m

  • This describes the restoring force, as it acts in the opposite direction to the displacement vector

  • Recall Newton's second law, which relates the force on an object with its mass and acceleration:

F with rightwards arrow on top subscript n e t end subscript space equals space m a with rightwards arrow on top

  • Where:

    • F with rightwards arrow on top subscript n e t end subscript = net force on the mass, measured in straight N

    • m = the object's mass, measured in kg

    • a with rightwards arrow on top = the object's acceleration, measured in straight m divided by straight s squared

Step 2: Apply the specific conditions

  • The spring's restoring force is the only force that acts, therefore:

F subscript n e t end subscript space equals space F subscript s

  • Additionally, all forces act in the x direction so Hooke's law and Newton's second law can be rewritten as:

F subscript s space equals space minus k straight capital delta x

F subscript n e t end subscript space equals space m a subscript x

  • Where:

    • a subscript x is the acceleration in the x direction, measured in straight m divided by straight s squared

  • Substituting Hooke's law and Newton's second law into the above gives:

m a subscript x space equals space minus k straight capital delta x

  • This is the derived equation and does not appear on the equation sheet

Examiner Tips and Tricks

The derived equation applies specifically to the system described. To derive a similar equation for a different system you must identify the restoring force, apply the conditions for simple harmonic motion and combine these with Newton's second law.

Last updated:

You've read 0 of your 10 free study guides

Unlock more, it's free!

Join the 100,000+ Students that ❤️ Save My Exams

the (exam) results speak for themselves:

Did this page help you?

Dan Mitchell-Garnett

Author: Dan Mitchell-Garnett

Expertise: Physics Content Creator

Dan graduated with a First-class Masters degree in Physics at Durham University, specialising in cell membrane biophysics. After being awarded an Institute of Physics Teacher Training Scholarship, Dan taught physics in secondary schools in the North of England before moving to Save My Exams. Here, he carries on his passion for writing challenging physics questions and helping young people learn to love physics.

Caroline Carroll

Author: Caroline Carroll

Expertise: Physics Subject Lead

Caroline graduated from the University of Nottingham with a degree in Chemistry and Molecular Physics. She spent several years working as an Industrial Chemist in the automotive industry before retraining to teach. Caroline has over 12 years of experience teaching GCSE and A-level chemistry and physics. She is passionate about creating high-quality resources to help students achieve their full potential.