Classical-Mechanics Β· Unit 7 Β· Video 1 Β· Interactive Practice
Hooke's Law: The Force Law of the Spring
IKey Formulas
Formula
Name
What it tells you
Fxβ=βkx
Hooke's Law
Linear restoring force
β£Fβ£=kβ£xβ£
Force magnitude
Proportional to displacement
k=β(slope)
Spring constant
Read off the Fxβ-vs-x graph
β£aβ£=mkβ£Ξxβ£β
Predicted acceleration
Force law + Newton's 2nd law
Key Insight: The minus sign in Fxβ=βkx is the whole story β the force always drives the block back toward x=0, so it is a restoring force.
IIVisualization 1 β The Restoring Force
A spring force Fxβ=βkx always points back toward equilibrium, and grows with the displacement.
IIIVisualization 2 β The ForceβDisplacement Graph
The spring's forceβdisplacement graph is a straight line through the origin whose slope is exactly βk.
π‘ Challenge: make this spring twice as stiff as the dashed reference (k=2) β its line should be twice as steep.
IVVisualization 3 β Predict, Then Measure
The force law forecasts the block's acceleration β£aβ£=kβ£Ξxβ£/m with no measurement of it.
π‘ The reckoning: if a real measurement of β£aβ£ disagreed with this forecast, the force law itself would need revision β that is how models grow.
VQuiz Questions
Problem 1 Β· Apply the Force Law
Given: a spring with k=50Β N/m is stretched so the block sits at x=+0.2Β m. Find the spring force Fxβ.
β Correct! The force is β10Β N β negative, pointing back toward x=0.
β Check the sign. For a stretch (x>0) the restoring force points in the βx direction, so Fxβ is negative.
β Not quite. Multiply, don't divide: Fxβ=βkx=β(50)(0.2).
Show solution
Apply Hooke's Law directly with k=50Β N/m and x=+0.2Β m:
Fxβ=βkx=β(50)(0.2)=β10Β N
The negative sign means the force points in the βx direction β back toward equilibrium. That is what makes it a restoring force.
Problem 2 Β· Compression and Signs
Given: a spring with k=40Β N/m is compressed so the block sits at x=β0.3Β m. FindFxβ. β οΈ Watch the double negative!
β Correct! The compressed spring pushes the block in the +x direction, back toward equilibrium.
β Close β mind the signs. Two negatives multiply to a positive: βkβ (β0.3)=+.
β Not quite. Keep the decimal: (40)(0.3)=12, not 120.
Show solution
With k=40Β N/m and x=β0.3Β m:
Fxβ=βkx=β(40)(β0.3)=+12Β N
The two minus signs combine to a plus. A compressed spring pushes outward in the +x direction β again pointing back toward x=0.
Problem 3 Β· Predict the Acceleration
Given: a spring with k=60Β N/m holds a block of mass m=3Β kg, stretched by Ξx=0.5Β m. Using the force law alone, predict the magnitude of the force and the acceleration at the instant of release.
What is the force magnitude β£Fβ£?
What is the acceleration β£aβ£?
β Correct! You forecast β£aβ£=10Β m/s2 from the law alone β no acceleration measured.
β Check the force. Use both factors: β£Fβ£=kβ£Ξxβ£=(60)(0.5).
β Check the acceleration. Newton's 2nd law divides by mass: β£aβ£=β£Fβ£/m.
Show solution
Step 1 β Force from the law (no acceleration measured):
β£Fβ£=kβ£Ξxβ£=(60)(0.5)=30Β N
Step 2 β Acceleration from Newton's 2nd law:
β£aβ£=mβ£Fβ£β=330β=10Β m/s2
This is the payoff of Newtonian induction: the force law lets us forecast the acceleration before touching the apparatus.
Problem 4 Β· A Pre-Tensioned Spring
Given: a tightly-wound spring needs a threshold force F0β=4Β N before it begins to stretch, so for x>0 the law becomes Fxβ=βF0ββkx. With k=20Β N/m, findFxβ at x=+0.5Β m.
β Excellent! The pre-tension adds a constant 4Β N on top of the usual βkx=β10Β N.
β Don't drop the pre-tension. For a stretch the law is Fxβ=βF0ββkx, not just βkx.
β Not quite. Keep both terms and both minus signs: β(4)β(20)(0.5).
Show solution
For a stretch (x>0) the pre-tensioned law adds the threshold F0β:
Fxβ=βF0ββkx=β(4)β(20)(0.5)=β4β10=β14Β N
The pre-tension F0β shifts the ordinary βkx line downward by a constant β the graph no longer passes through the origin. Both F0β and k are pinned down by experiment.