2.8 Spring Forces

Syllabus
2024
Topic
2.8
Level

Learning objectives

An ideal spring pushes back toward equilibrium

Define the ideal model

An ideal spring has negligible mass. Its force is proportional to the change in length Δx\Delta\vec x measured from its relaxed length.

Use Hooke's law

Fs=kΔx\vec F_s=-k\,\Delta\vec x

Read the restoring direction

Spring change Displacement sign Spring-force direction
Stretched to the right Δx>0\Delta x>0 Fs<0F_s<0: left, back toward equilibrium
Compressed to the left Δx<0\Delta x<0 Fs>0F_s>0: right, back toward equilibrium
Relaxed Δx=0\Delta x=0 Fs=0F_s=0

Calculate and interpret

Worked example: take right as positive. A spring with k=200N/mk=200\,\text{N/m} is stretched Δx=+0.030m\Delta x=+0.030\,\text{m}.

Fs=kΔx=(200N/m)(+0.030m)=6.0NF_s=-k\Delta x=-(200\,\text{N/m})(+0.030\,\text{m})=-6.0\,\text{N}.

The spring exerts a 6.0N6.0\,\text{N} force to the left, toward equilibrium.

Separate sign and magnitude

The minus sign gives direction; force magnitude is Fs=kΔx|F_s|=k|\Delta x|. The spring constant kk has units N/m\text{N/m} and measures stiffness. Hooke's law is the ideal linear model: doubling the displacement doubles the force magnitude within that model.