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Elastic Potential Energy and Springs

Hooke's Law, spring force, and elastic potential energy

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🌀 Elastic Potential Energy and Springs

Hooke's Law

A spring exerts a restoring force proportional to its displacement from equilibrium:

Fs=−kxF_s = -kx

where:

  • FsF_s = spring force (N)
  • kk = spring constant (N/m) - measure of spring's stiffness
  • xx = displacement from equilibrium position (m)
  • Negative sign means force opposes displacement (restoring force)

💡 Hooke's Law: Named after Robert Hooke, this is valid for springs in their elastic region (not stretched/compressed too far).


Understanding the Spring Force

Equilibrium Position

The natural length of the spring - no force exerted (x=0x = 0)

Compression (x<0x < 0)

  • Spring is squeezed
  • Force pushes outward (away from compression)

Extension (x>0x > 0)

  • Spring is stretched
  • Force pulls inward (back toward equilibrium)

Spring Constant kk

  • Large kk: Stiff spring (hard to stretch/compress)
  • Small kk: Soft spring (easy to stretch/compress)
  • Units: N/m (newtons per meter)

Elastic Potential Energy

Energy stored in a compressed or stretched spring:

PEelastic=12kx2PE_{elastic} = \frac{1}{2}kx^2

where:

  • PEelasticPE_{elastic} (or UsU_s) = elastic potential energy (J)
  • kk = spring constant (N/m)
  • xx = displacement from equilibrium (m)

Key Properties

  1. Always positive - x2x^2 is always positive (compressed or stretched)
  2. Quadratic relationship - Double displacement = 4× energy
  3. Minimum at equilibrium - PE = 0 when x=0x = 0
  4. Symmetric - Same energy whether compressed or stretched by ∣x∣|x|

Work Done by/on a Spring

Work done BY spring (spring releases)

Wby spring=−ΔPEelastic=−(12kxf2−12kxi2)W_{by\,spring} = -\Delta PE_{elastic} = -\left(\frac{1}{2}kx_f^2 - \frac{1}{2}kx_i^2\right)

Work done ON spring (you compress/stretch it)

Won spring=ΔPEelastic=12kxf2−12kxi2W_{on\,spring} = \Delta PE_{elastic} = \frac{1}{2}kx_f^2 - \frac{1}{2}kx_i^2

Special case: From equilibrium to xx

W=∫0xF dx=∫0xkx′ dx′=12kx2W = \int_0^x F\,dx = \int_0^x kx'\,dx' = \frac{1}{2}kx^2

This equals the elastic PE stored.


Why Is PE = ½kx², Not kx?

The spring force is variable: F=kxF = kx (increases with displacement).

Average force from 0 to xx: Favg=0+kx2=kx2F_{avg} = \frac{0 + kx}{2} = \frac{kx}{2}

Work = Average force × distance: W=Favg⋅x=kx2⋅x=12kx2W = F_{avg} \cdot x = \frac{kx}{2} \cdot x = \frac{1}{2}kx^2

Alternatively, work is the area under the FF vs. xx graph:

  • Triangle with base xx and height kxkx
  • Area = 12⋅base⋅height=12kx2\frac{1}{2} \cdot base \cdot height = \frac{1}{2}kx^2

Conservation of Energy with Springs

For a mass on a spring (horizontal, no friction):

Etotal=KE+PEelastic=12mv2+12kx2=constantE_{total} = KE + PE_{elastic} = \frac{1}{2}mv^2 + \frac{1}{2}kx^2 = constant

  • At maximum compression/extension: v=0v = 0, all energy is elastic PE
  • At equilibrium: x=0x = 0, all energy is kinetic

Spring Combinations

Springs in Series (end-to-end)

Effective spring constant is smaller:

1keff=1k1+1k2\frac{1}{k_{eff}} = \frac{1}{k_1} + \frac{1}{k_2}

Easier to stretch than individual springs.

Springs in Parallel (side-by-side)

Effective spring constant is larger:

keff=k1+k2k_{eff} = k_1 + k_2

Harder to stretch than individual springs.


⚠️ Common Mistakes

Mistake 1: Forgetting the ½

❌ Wrong: PE=kx2PE = kx^2 ✅ Right: PE=12kx2PE = \frac{1}{2}kx^2

Mistake 2: Using Wrong x

xx is displacement from equilibrium, not from one end of possible motion!

Mistake 3: Thinking PE Can Be Negative

Elastic PE is always ≥ 0 (because of x2x^2)

Mistake 4: Sign in Hooke's Law

F=−kxF = -kx has a negative sign (restoring force), but many problems just use magnitude: ∣F∣=k∣x∣|F| = k|x|


Problem-Solving Strategy

  1. Identify equilibrium position where x=0x = 0
  2. Measure displacement xx from equilibrium
  3. For force: Use F=kxF = kx (magnitude) with direction toward equilibrium
  4. For energy: Use PE=12kx2PE = \frac{1}{2}kx^2
  5. Apply conservation of energy if appropriate

Applications

Vehicle Suspension

Springs absorb bumps, converting KE to elastic PE and back.

Pogo Sticks

Compression of spring stores PE, which launches you upward (converts to gravitational PE and KE).

Trampolines

Springs and elastic mat store PE when compressed, releasing it to bounce you up.

Molecular Bonds

Atoms in molecules act like masses connected by springs (vibrating).


Comparison: Elastic vs. Gravitational PE

PropertyGravitational PEg=mghPE_g = mghElastic PEs=12kx2PE_s = \frac{1}{2}kx^2
Zero pointChoose reference (arbitrary)Equilibrium position (natural)
Can be negative?Yes (below reference)No (always ≥ 0)
ForceConstant (F=mgF = mg)Variable (F=kxF = kx)
ExponentLinear in hhQuadratic in xx
Conservative?YesYes

Key Formulas Summary

ConceptFormulaUnits
Hooke's LawFs=−kxF_s = -kxN
Spring constantkkN/m
Elastic PEPEs=12kx2PE_s = \frac{1}{2}kx^2J
Work by springW=−ΔPEsW = -\Delta PE_sJ
Total energy (horizontal)E=12mv2+12kx2E = \frac{1}{2}mv^2 + \frac{1}{2}kx^2J

📚 Practice Problems

1Problem 1easy

❓ Question:

A spring with spring constant k=200k = 200 N/m is compressed 0.15 m from its equilibrium position. (a) What is the spring force? (b) How much elastic potential energy is stored?

💡 Show Solution

Given Information:

  • Spring constant: k=200k = 200 N/m
  • Compression: x=0.15x = 0.15 m

(a) Find spring force


Use Hooke's Law:

F=kxF = kx

(Using magnitude; direction is toward equilibrium)

F=(200)(0.15)=30 NF = (200)(0.15) = 30 \text{ N}

The force points outward (opposite to compression).


(b) Find elastic potential energy


PEelastic=12kx2PE_{elastic} = \frac{1}{2}kx^2

PEelastic=12(200)(0.15)2PE_{elastic} = \frac{1}{2}(200)(0.15)^2

PEelastic=100(0.0225)PE_{elastic} = 100(0.0225)

PEelastic=2.25 JPE_{elastic} = 2.25 \text{ J}


Answers:

  • (a) Spring force: 30 N (directed outward, opposing compression)
  • (b) Elastic PE stored: 2.25 J

2Problem 2medium

❓ Question:

A 0.5 kg block is attached to a spring with k=100k = 100 N/m on a frictionless horizontal surface. The spring is compressed 0.2 m and released. What is the maximum speed of the block?

💡 Show Solution

Given Information:

  • Mass: m=0.5m = 0.5 kg
  • Spring constant: k=100k = 100 N/m
  • Initial compression: xi=0.2x_i = 0.2 m
  • Frictionless surface

Find: Maximum speed vmaxv_{max}


Analysis:

Maximum speed occurs at equilibrium position (x=0x = 0) where all elastic PE converts to KE.


Step 1: Calculate initial energy (at maximum compression)

At x=0.2x = 0.2 m:

  • KEi=0KE_i = 0 (released from rest)
  • PEi=12kxi2=12(100)(0.2)2=50(0.04)=2PE_i = \frac{1}{2}kx_i^2 = \frac{1}{2}(100)(0.2)^2 = 50(0.04) = 2 J

Total initial energy: Ei=2E_i = 2 J


Step 2: Calculate final energy (at equilibrium)

At x=0x = 0:

  • KEf=12mvmax2KE_f = \frac{1}{2}mv_{max}^2 (unknown)
  • PEf=12k(0)2=0PE_f = \frac{1}{2}k(0)^2 = 0 J

Total final energy: Ef=12mvmax2E_f = \frac{1}{2}mv_{max}^2


Step 3: Apply conservation of energy

Ei=EfE_i = E_f

2=12(0.5)vmax22 = \frac{1}{2}(0.5)v_{max}^2

2=0.25vmax22 = 0.25v_{max}^2

vmax2=8v_{max}^2 = 8

vmax=8=22≈2.83 m/sv_{max} = \sqrt{8} = 2\sqrt{2} \approx 2.83 \text{ m/s}


Alternative formula:

For a spring-mass system released from rest at maximum displacement:

vmax=xmaxkm=0.21000.5=0.2200=0.2(102)=22v_{max} = x_{max}\sqrt{\frac{k}{m}} = 0.2\sqrt{\frac{100}{0.5}} = 0.2\sqrt{200} = 0.2(10\sqrt{2}) = 2\sqrt{2} m/s ✓


Answer: The maximum speed is 222\sqrt{2} m/s or approximately 2.83 m/s.

3Problem 3hard

❓ Question:

A 2 kg block is attached to a vertical spring with k=500k = 500 N/m. The block is pulled down 0.1 m from equilibrium and released. (a) What is the total mechanical energy? (b) How high above the release point does the block rise?

💡 Show Solution

Given Information:

  • Mass: m=2m = 2 kg
  • Spring constant: k=500k = 500 N/m
  • Initial displacement: xi=0.1x_i = 0.1 m (down from equilibrium)
  • Vertical spring

(a) Find total mechanical energy


Step 1: Choose reference for gravitational PE

Let equilibrium position be h=0h = 0 for gravitational PE.


Step 2: Calculate energy at release point

At release (0.1 m below equilibrium):

  • KEi=0KE_i = 0 (released from rest)
  • PEelastic,i=12kxi2=12(500)(0.1)2=250(0.01)=2.5PE_{elastic,i} = \frac{1}{2}kx_i^2 = \frac{1}{2}(500)(0.1)^2 = 250(0.01) = 2.5 J
  • PEgrav,i=mghi=(2)(9.8)(−0.1)=−1.96PE_{grav,i} = mgh_i = (2)(9.8)(-0.1) = -1.96 J (negative because below equilibrium)

Total energy: E=0+2.5+(−1.96)=0.54 JE = 0 + 2.5 + (-1.96) = 0.54 \text{ J}


(b) Find maximum height above release point


Step 3: At maximum height

At highest point, block momentarily stops (v=0v = 0) and spring returns through equilibrium and compresses.

Let's say spring compresses by distance dd above equilibrium.

At this point:

  • KE=0KE = 0
  • PEelastic=12kd2PE_{elastic} = \frac{1}{2}kd^2
  • PEgrav=mg(d)PE_{grav} = mg(d) (height dd above equilibrium, which is d+0.1d + 0.1 above release)

Step 4: Apply conservation of energy

Einitial=EfinalE_{initial} = E_{final}

0.54=0+12kd2+mgd0.54 = 0 + \frac{1}{2}kd^2 + mgd

0.54=250d2+19.6d0.54 = 250d^2 + 19.6d

250d2+19.6d−0.54=0250d^2 + 19.6d - 0.54 = 0


Step 5: Solve quadratic

Using quadratic formula: d=−b±b2−4ac2ad = \frac{-b \pm \sqrt{b^2 - 4ac}}{2a}

d=−19.6±(19.6)2−4(250)(−0.54)2(250)d = \frac{-19.6 \pm \sqrt{(19.6)^2 - 4(250)(-0.54)}}{2(250)}

d=−19.6±384.16+540500d = \frac{-19.6 \pm \sqrt{384.16 + 540}}{500}

d=−19.6±924.16500d = \frac{-19.6 \pm \sqrt{924.16}}{500}

d=−19.6±30.4500d = \frac{-19.6 \pm 30.4}{500}

Taking positive solution: d=10.8500=0.0216 m=2.16 cmd = \frac{10.8}{500} = 0.0216 \text{ m} = 2.16 \text{ cm}

Height above release point: h=d+0.1=0.0216+0.1=0.1216h = d + 0.1 = 0.0216 + 0.1 = 0.1216 m


Simplified approach (if we ignore spring compression at top):

If spring just returns to equilibrium (d=0d = 0):

0.54=0+0+mg(h)0.54 = 0 + 0 + mg(h) h=0.5419.6≈0.0276h = \frac{0.54}{19.6} \approx 0.0276 m

But spring actually compresses slightly, giving total height ≈ 0.122 m.


Answers:

  • (a) Total mechanical energy: 0.54 J
  • (b) Height above release point: approximately 0.122 m or 12.2 cm

Note: This problem is complex because both gravitational and elastic PE change. The spring compresses slightly above equilibrium before the block stops.

Explain using:

📌 Related Topics in Energy

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What is Elastic Potential Energy and Springs?▾
Hooke's Law, spring force, and elastic potential energy
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Start by reading the study notes and working through the examples on this page. Then use the flashcards to test your recall. Practice with the 3 problems provided, checking solutions as you go. Regular review and active practice are key to retention.
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