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15.1.4 Linear and non-linear force–extension

Graph shape distinguishes linear behaviour

Definition

Limit of proportionality

The point beyond which force and extension are no longer directly proportional.

  1. A linear force-extension relationship produces a straight line, while a non-linear relationship produces a curve.
  2. Direct proportionality requires a straight line through the origin, not merely any straight line.
  3. Below the limit of proportionality, F=kxF=kxF=kx and the gradient of a force against extension graph is the constant kkk.
  4. Beyond this limit, extension no longer increases in direct proportion to force and the gradient changes.

Loading and unloading reveal permanent change

  1. If unloading returns the graph to the origin, the object has recovered its original length.
  2. If the unloading path finishes at a non-zero extension, the object has undergone inelastic distortion.
  3. Rubber bands commonly give curved force-extension graphs even when they return to their original length, so non-linear does not automatically mean inelastic.
Common Mistake

Do not confuse the limit of proportionality with the point where permanent deformation begins; they are not necessarily the same point.

Practical

Investigating a spring

  • Apparatus: clamp stand, boss and clamp, spring, mass hanger and slotted masses, metre rule, pointer, set square and eye protection.
  • Set-up: clamp the stand securely, hang the spring beside a vertical metre rule and attach a horizontal pointer to the lower end of the spring.
  • Method:
    • record the unstretched spring length L0L_0L0​ at eye level, using a set square to align the pointer with the scale.
    • add masses in equal steps, allow oscillations to stop, record the new length LLL and calculate extension using x=L−L0x=L-L_0x=L−L0​.
    • calculate the applied force from F=mgF=mgF=mg, using the total hanging mass in kilograms and g=10 N kg−1g=10\,\text{N kg}^{-1}g=10N kg−1.
    • take at least six force-extension pairs without exceeding the spring's safe load, then remove the masses in the same steps to obtain unloading readings.
    • repeat each reading, identify anomalous values and calculate a mean extension for each force.
    • plot FFF on the vertical axis against xxx on the horizontal axis, draw a best-fit line or curve and use a large gradient triangle in the linear region to find k=ΔF/Δxk=\Delta F/\Delta xk=ΔF/Δx.
    • determine the area beneath the force-extension graph; use E=12kx2E=\dfrac{1}{2}kx^2E=21​kx2 only for the straight-line region.
  • Variables: change the applied force, measure extension, and keep the same spring, starting length, ruler position and temperature.
  • Errors: avoid parallax by reading at eye level, clamp the ruler, use a pointer and wait for the spring to stop moving.
  • Safety: wear eye protection, keep feet clear of falling masses, secure the stand and do not overload the spring.
Example

Using experimental data

  • A best-fit line rises from (0.010 m,2.0 N)(0.010\,\text{m},2.0\,\text{N})(0.010m,2.0N) to (0.040 m,8.0 N)(0.040\,\text{m},8.0\,\text{N})(0.040m,8.0N).
  • k=8.0−2.00.040−0.010=200 N m−1k=\dfrac{8.0-2.0}{0.040-0.010}=200\,\text{N m}^{-1}k=0.040−0.0108.0−2.0​=200N m−1.
  • At x=0.040 mx=0.040\,\text{m}x=0.040m, E=12×200×(0.040)2=0.16 JE=\dfrac{1}{2}\times200\times(0.040)^2=0.16\,\text{J}E=21​×200×(0.040)2=0.16J.
Self review
  • How does a linear relationship differ from a directly proportional relationship?
  • What is the limit of proportionality?
  • How is extension obtained in the spring practical?
  • How is spring constant found from the graph?
  • How is work done found from a non-linear graph?
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15.1.4 Linear and non-linear force–extension Revision Guide

  1. GCSE
  2. /Physics
  3. /15.1.4 Linear and non-linear force–extension

Revision notes for Edexcel GCSE Physics 15.1.4 Linear and non-linear force–extension: explanations and worked examples.

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