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Work is the integral of force along displacement, not necessarily final force times total distance.
Worked example 1
A spring has constant k=10mN. Find the work in joules to stretch it from 0 to 0.2m beyond equilibrium.
F(x)=10x
W=∫051≈0.210xdx=[210x2]051≈0.2
W=210(51≈0.22−02)=51≈0.2
Answer:51≈0.2
Worked example 2
A spring has constant k=20mN. Find the work in joules to stretch it from .1 to 0.3m beyond equilibrium.
F(x)=20x
W=∫0.10.320xdx=[220x2]0.10.3
W=220(0.32−0.12)=54≈0.8
Answer:54≈0.8
Idea 2 of 3
Lifting against gravity
With constant weight, work is weight times height. Use consistent force and distance units.
Worked example 1
A 2 kg object is raised 1m at constant speed. Use g=9.8 m/s2. Find the work in joules.
F= mg =2⋅9.8=598≈19.6N
W= Fh =598≈19.6⋅1J=598≈19.6
Answer:598≈19.6
Worked example 2
A 4 kg object is raised 2m at constant speed. Use g=9.8 m/s2. Find the work in joules.
F= mg =4⋅9.8=39.2N
W= Fh =39.2⋅2J=5392≈78.4
Answer:5392≈78.4
Idea 3 of 3
Spring equilibrium and bounds
Stretch is measured from equilibrium. Changing the starting stretch changes the lower integral bound.
Worked example 1
A spring has constant k=10mN. Find the work in joules to stretch it from 0 to 0.2m beyond equilibrium.
F(x)=10x
W=∫051≈0.210xdx=[210x2]051≈0.2
W=210(51≈0.22−02)=51≈0.2
Answer:51≈0.2
Worked example 2
A spring has constant k=20mN. Find the work in joules to stretch it from .1 to 0.3m beyond equilibrium.
F(x)=20x
W=∫0.10.320xdx=[220x2]0.10.3
W=220(0.32−0.12)=54≈0.8
Answer:54≈0.8
Resource alignment: Larson & Edwards, Calculus of a Single Variable, Tenth Edition, §7.5,p. 477. Explanations, diagrams and numerical practice variants are original MathLab content aligned to this section.