A spring exerts a restoring force proportional to its displacement from equilibrium:
Fsโ=โkx
where:
F = spring force (N)
๐ Practice Problems
1Problem 1easy
โ Question:
A spring with spring constant k=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?
Hooke's Law, spring force, and elastic potential energy
How can I study Elastic Potential Energy and Springs effectively?โพ
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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What course covers Elastic Potential Energy and Springs?โพ
Elastic Potential Energy and Springs is part of the AP Physics 1 course on Study Mondo, specifically in the Energy section. You can explore the full course for more related topics and practice resources.
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sโ
k = spring constant (N/m) - measure of spring's stiffness
x = displacement from equilibrium position (m)
Negative sign means force opposes displacement (restoring force)
๐ก 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=0)
Compression (x<0)
Spring is squeezed
Force pushes outward (away from compression)
Extension (x>0)
Spring is stretched
Force pulls inward (back toward equilibrium)
Spring Constant k
Large k: Stiff spring (hard to stretch/compress)
Small k: Soft spring (easy to stretch/compress)
Units: N/m (newtons per meter)
Elastic Potential Energy
Energy stored in a compressed or stretched spring:
PEelasticโ=21โkx2
where:
PEelasticโ (or Usโ) = elastic potential energy (J)
k = spring constant (N/m)
x = displacement from equilibrium (m)
Key Properties
Always positive - x2 is always positive (compressed or stretched)
Quadratic relationship - Double displacement = 4ร energy
Minimum at equilibrium - PE = 0 when x=0
Symmetric - Same energy whether compressed or stretched by โฃxโฃ
At maximum compression/extension: v=0, all energy is elastic PE
At equilibrium: x=0, all energy is kinetic
Spring Combinations
Springs in Series (end-to-end)
Effective spring constant is smaller:
keffโ1โ=k1โ1โ+k2โ1โ
Easier to stretch than individual springs.
Springs in Parallel (side-by-side)
Effective spring constant is larger:
keffโ=k1โ+k2โ
Harder to stretch than individual springs.
โ ๏ธ Common Mistakes
Mistake 1: Forgetting the ยฝ
โ Wrong: PE=kx2
โ Right: PE=21โkx2
Mistake 2: Using Wrong x
x is displacement from equilibrium, not from one end of possible motion!
Mistake 3: Thinking PE Can Be Negative
Elastic PE is always โฅ 0 (because of x2)
Mistake 4: Sign in Hooke's Law
F=โkx has a negative sign (restoring force), but many problems just use magnitude: โฃFโฃ=kโฃxโฃ
Problem-Solving Strategy
Identify equilibrium position where x=0
Measure displacementx from equilibrium
For force: Use F=kx (magnitude) with direction toward equilibrium
For energy: Use PE=21โkx2
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
Property
Gravitational PEgโ=mgh
Elastic PEsโ=21โkx2
Zero point
Choose reference (arbitrary)
Equilibrium position (natural)
Can be negative?
Yes (below reference)
No (always โฅ 0)
Force
Constant (F=mg)
Variable (F=)
Key Formulas Summary
Concept
Formula
Units
Hooke's Law
Fsโ=โkx
N
Spring constant
k
N/m
Elastic PE
PEsโ=21โkx
Work by spring
W=โฮPEsโ
J
Total energy (horizontal)
E=21โmv2+
k=200
Compression: x=0.15 m
(a) Find spring force
Use Hooke's Law:
F=kx
(Using magnitude; direction is toward equilibrium)
F=(200)(0.15)=30ย N
The force points outward (opposite to compression).
(b) Find elastic potential energy
PEelasticโ=21โkx2
PEelasticโ=21โ(200)(0.15)2
PEelasticโ=100(0.0225)
PEelasticโ=2.25ย J
Answers:
(a) Spring force: 30 N (directed outward, opposing compression)
(b) Elastic PE stored: 2.25 J
2Problem 2medium
โ Question:
A 0.5 kg block is attached to a spring with k=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?
๐ก Show Solution
Given Information:
Mass: m=0.5 kg
Spring constant: k=100 N/m
Initial compression: xiโ=0.2 m
Frictionless surface
Find: Maximum speed vmaxโ
Analysis:
Maximum speed occurs at equilibrium position (x=0) where all elastic PE converts to KE.
Step 1: Calculate initial energy (at maximum compression)
At x=0.2 m:
KEiโ=0 (released from rest)
PE J
Total initial energy: Eiโ=2 J
Step 2: Calculate final energy (at equilibrium)
At x=0:
KEfโ=21โmv (unknown)
Total final energy: Efโ=21โmv
Step 3: Apply conservation of energy
Eiโ=Efโ
2=21โ(0.5)vmax2โ
2=0.25vmax2โ
vmax2โ=8
vmaxโ=8โ
Alternative formula:
For a spring-mass system released from rest at maximum displacement:
vmaxโ=xmaxโ m/s โ
Answer: The maximum speed is 22โ m/s or approximately 2.83 m/s.
3Problem 3hard
โ Question:
A 2 kg block is attached to a vertical spring with k=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?
๐ก Show Solution
Given Information:
Mass: m=2 kg
Spring constant: k=500 N/m
Initial displacement: xiโ=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=0 for gravitational PE.
Step 2: Calculate energy at release point
At release (0.1 m below equilibrium):
KEiโ=0 (released from rest)
J
Total energy:
E=0+2.5+(โ1.96)=0.54ย J
(b) Find maximum height above release point
Step 3: At maximum height
At highest point, block momentarily stops (v=0) and spring returns through equilibrium and compresses.
Let's say spring compresses by distance d above equilibrium.
At this point:
KE=0
PEelasticโ=
Step 4: Apply conservation of energy
Einitialโ=Efinalโ
0.54=0+21โkd2+
0.54=250d2+19.6d
250d2+19.6dโ0.54=0
Step 5: Solve quadratic
Using quadratic formula: d=2aโbยฑb2โ4a
d=2(250)โ19.6ยฑ(19.6)
d=500โ19.6ยฑ384.16+540
d=500โ19.6ยฑ924.16โ
d=500โ19.6ยฑ30.4โ
Taking positive solution:
d=50010.8โ=0.0216ย m=2.16ย cm
Height above release point: h=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=0):
0.54=0+0+mg(h)h=19.6 m
But spring actually compresses slightly, giving total height โ 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.
โพ
Yes, this page includes 3 practice problems with detailed solutions. Each problem includes a step-by-step explanation to help you understand the approach.
1
โ
k
xi2โ
)
kx
Exponent
Linear in h
Quadratic in x
Conservative?
Yes
Yes
2
J
21โ
k
x2
J
iโ
=
21โkxi2โ=
21โ(100)(0.2)2=
50(0.04)=
2
max2โ
PEfโ=21โk(0)2=0 J
max
2
โ
=
22โโ
2.83ย m/s
mkโโ
=
0.20.5100โโ=
0.2200โ=
0.2(102โ)=
22โ
P
Eelastic,iโ
=
21โkxi2โ=
21โ(500)(0.1)2=
250(0.01)=
2.5
PEgrav,iโ=mghiโ=(2)(9.8)(โ0.1)=โ1.96 J (negative because below equilibrium)
21โkd2
PEgravโ=mg(d) (height d above equilibrium, which is d+0.1 above release)