Classical-Mechanics Β· Unit 7 Β· Video 1 Β· Interactive Practice

Hooke's Law: The Force Law of the Spring

IKey Formulas

FormulaNameWhat it tells you
Fx=βˆ’kxF_x = -kxHooke's LawLinear restoring force
∣F∣=kβ€‰βˆ£x∣|F| = k\,|x|Force magnitudeProportional to displacement
k=βˆ’(slope)k = -(\text{slope})Spring constantRead off the FxF_x-vs-xx graph
∣a∣=kβ€‰βˆ£Ξ”x∣m|a| = \dfrac{k\,|\Delta x|}{m}Predicted accelerationForce law + Newton's 2nd law

Key Insight: The minus sign in Fx=βˆ’kxF_x = -kx is the whole story β€” the force always drives the block back toward x=0x = 0, so it is a restoring force.

IIVisualization 1 β€” The Restoring Force

A spring force Fx=βˆ’kxF_x = -kx always points back toward equilibrium, and grows with the displacement.

IIIVisualization 2 β€” The Force–Displacement Graph

The spring's force–displacement graph is a straight line through the origin whose slope is exactly βˆ’k-k.

πŸ’‘ Challenge: make this spring twice as stiff as the dashed reference (k=2k = 2) β€” its line should be twice as steep.

IVVisualization 3 β€” Predict, Then Measure

The force law forecasts the block's acceleration ∣a∣=kβ€‰βˆ£Ξ”x∣/m|a| = k\,|\Delta x|/m with no measurement of it.

πŸ’‘ The reckoning: if a real measurement of ∣a∣|a| 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/mk = 50\ \text{N/m} is stretched so the block sits at x=+0.2Β mx = +0.2\ \text{m}. Find the spring force FxF_x.

βœ… Correct! The force is βˆ’10Β N-10\ \text{N} β€” negative, pointing back toward x=0x = 0.
❌ Check the sign. For a stretch (x>0x > 0) the restoring force points in the βˆ’x-x direction, so FxF_x is negative.
❌ Not quite. Multiply, don't divide: Fx=βˆ’kx=βˆ’(50)(0.2)F_x = -kx = -(50)(0.2).
Show solution

Apply Hooke's Law directly with k=50Β N/mk = 50\ \text{N/m} and x=+0.2Β mx = +0.2\ \text{m}:

Fx=βˆ’kx=βˆ’(50)(0.2)=βˆ’10Β NF_x = -kx = -(50)(0.2) = -10\ \text{N}

The negative sign means the force points in the βˆ’x-x 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/mk = 40\ \text{N/m} is compressed so the block sits at x=βˆ’0.3Β mx = -0.3\ \text{m}. Find FxF_x. ⚠️ Watch the double negative!

βœ… Correct! The compressed spring pushes the block in the +x+x direction, back toward equilibrium.
❌ Close β€” mind the signs. Two negatives multiply to a positive: βˆ’kβ‹…(βˆ’0.3)=+-k\cdot(-0.3) = +.
❌ Not quite. Keep the decimal: (40)(0.3)=12(40)(0.3) = 12, not 120120.
Show solution

With k=40Β N/mk = 40\ \text{N/m} and x=βˆ’0.3Β mx = -0.3\ \text{m}:

Fx=βˆ’kx=βˆ’(40)(βˆ’0.3)=+12Β NF_x = -kx = -(40)(-0.3) = +12\ \text{N}

The two minus signs combine to a plus. A compressed spring pushes outward in the +x+x direction β€” again pointing back toward x=0x = 0.

Problem 3 Β· Predict the Acceleration

Given: a spring with k=60Β N/mk = 60\ \text{N/m} holds a block of mass m=3Β kgm = 3\ \text{kg}, stretched by Ξ”x=0.5Β m\Delta x = 0.5\ \text{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 ∣F∣|F|?

What is the acceleration ∣a∣|a|?

βœ… Correct! You forecast ∣a∣=10Β m/s2|a| = 10\ \text{m/s}^2 from the law alone β€” no acceleration measured.
❌ Check the force. Use both factors: ∣F∣=kβ€‰βˆ£Ξ”x∣=(60)(0.5)|F| = k\,|\Delta x| = (60)(0.5).
❌ Check the acceleration. Newton's 2nd law divides by mass: ∣a∣=∣F∣/m|a| = |F|/m.
Show solution

Step 1 β€” Force from the law (no acceleration measured):

∣F∣=kβ€‰βˆ£Ξ”x∣=(60)(0.5)=30Β N|F| = k\,|\Delta x| = (60)(0.5) = 30\ \text{N}

Step 2 β€” Acceleration from Newton's 2nd law:

∣a∣=∣F∣m=303=10 m/s2|a| = \frac{|F|}{m} = \frac{30}{3} = 10\ \text{m/s}^2

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 F0=4Β NF_0 = 4\ \text{N} before it begins to stretch, so for x>0x > 0 the law becomes Fx=βˆ’F0βˆ’kxF_x = -F_0 - kx. With k=20Β N/mk = 20\ \text{N/m}, find FxF_x at x=+0.5Β mx = +0.5\ \text{m}.

βœ… Excellent! The pre-tension adds a constant 4Β N4\ \text{N} on top of the usual βˆ’kx=βˆ’10Β N-kx = -10\ \text{N}.
❌ Don't drop the pre-tension. For a stretch the law is Fx=βˆ’F0βˆ’kxF_x = -F_0 - kx, not just βˆ’kx-kx.
❌ Not quite. Keep both terms and both minus signs: βˆ’(4)βˆ’(20)(0.5)-(4) - (20)(0.5).
Show solution

For a stretch (x>0x > 0) the pre-tensioned law adds the threshold F0F_0:

Fx=βˆ’F0βˆ’kx=βˆ’(4)βˆ’(20)(0.5)=βˆ’4βˆ’10=βˆ’14Β NF_x = -F_0 - kx = -(4) - (20)(0.5) = -4 - 10 = -14\ \text{N}

The pre-tension F0F_0 shifts the ordinary βˆ’kx-kx line downward by a constant β€” the graph no longer passes through the origin. Both F0F_0 and kk are pinned down by experiment.

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