Pe Spring

8 MCQs2 revision cards9-step worked example
Source: NCERT Work, Energy and PowerPYQ coverage: NEET 2021, 2022, 2023, 2024, 2025Official key: NTA-verifiedLast reviewed: May 2026

Lesson

The single highest-frequency trap for spring PE questions on NEET is treating the stored energy as proportional to displacement rather than to displacement squared. If a spring stores energy U at stretch x, doubling the stretch does not double the energy — it quadruples it.

An ideal spring obeying Hooke's law exerts a restoring force F = −kx, where k is the spring constant (N/m) and x is the displacement from the natural (unstretched) length. Because this force varies linearly with position, the work done in stretching or compressing the spring by x from its natural length is found by integration:

W = ∫₀ˣ kx′ dx′ = ½kx²

This work gets stored as elastic potential energy: U = ½kx² (NCERT Class 11 Physics Chapter 5, page 10).

Key features to lock in:

  • Quadratic dependence. U ∝ x². Triple the stretch → 9× the energy. This is the core of the NEET scaling trap.
  • Sign-independent. Whether the spring is compressed or extended by the same magnitude, the PE is the same. The x² term wipes out the sign.
  • Zero at natural length. The reference point for spring PE is the natural length itself — no arbitrary reference-level choice (unlike gravitational PE).
  • Valid only in the Hooke's-law regime. Beyond the elastic limit, F is no longer linear in x and this formula breaks down.

NEET questions on spring PE are typically direct-application problems: given U at one displacement, find U at another. The distractor that catches repeaters is the linear-scaling answer. Always compute the ratio of displacements, then square it.


Practice MCQs

Select an option to see the explanation. Wrong answers show why your choice was tempting — and name the exact trap it exploits.

MCQ 1Direct ApplicationPractice

The elastic potential energy stored in a spring compressed by x from its natural length is U. What is the PE when the same spring is compressed by 3x?

MCQ 2Direct ApplicationPractice

A spring of force constant k is first stretched by 2 cm and then further stretched to 6 cm from its natural length. What is the ratio of PE at 6 cm to PE at 2 cm?

MCQ 3Easy RecallPractice

What is the SI unit of the spring constant k?

MCQ 4Easy RecallPractice

Which of the following correctly represents the elastic potential energy stored in a spring?

MCQ 5Direct ApplicationPractice

A spring stores 4.0 J of energy when stretched by 0.10 m from its natural length. What is the spring constant?

MCQ 6Direct ApplicationPractice

A spring of spring constant 200 N/m is compressed by 0.05 m and then released. What is the elastic potential energy stored in the spring just before release?

MCQ 7CalculationPractice

A spring of spring constant k is stretched from displacement x₁ to displacement x₂ (both measured from the natural length, x₂ > x₁ > 0). The work done by the spring force during this process is:

MCQ 8CalculationPractice

The potential energy of a spring at stretch x is U₁, and at stretch 2x is U₂. What is U₂ − U₁ in terms of U₁?

Quick recall before you leave

Worked Example

  1. 1

    Given

    - PE at 2 cm stretch: V - New stretch: 8 cm - Spring obeys Hooke's law (ideal spring)

  2. 2

    Required

    PE at 8 cm stretch, in terms of V.

  3. 3

    Concept

    Spring PE depends quadratically on displacement: U = ½kx². When comparing PE at two different displacements of the same spring, the ratio of PE values equals the square of the ratio of displacements.

  4. 4

    Formula

    U = ½kx² Ratio form: U₂/U₁ = (x₂/x₁)²

  5. 5

    Substitution

    x₁ = 2 cm, x₂ = 8 cm, U₁ = V U₂/V = (8/2)² = 4² = 16

  6. 6

    Calculation

    U₂ = 16V Note on exact values: the numbers 2, 8, and 4 are exact counting/given integers and do not affect significant-figure considerations.

  7. 7

    Final answer

    The potential energy at 8 cm stretch is **16V**.

  8. 8

    Common trap

    The linear-scaling distractor would give 4V (since 8/2 = 4). This is wrong because PE scales as x², not x. If you got 4V, you forgot to square the ratio.

  9. 9

    Similar NEET-style question

    A spring has elastic PE of E when compressed by d. Find the PE when compressed by d/2. (Answer: E/4, since (1/2)² = 1/4.) ---

Before solving, remember these

For an ideal spring with force constant k stretched or compressed by amount x from its natural length, the restoring force is F = -k x and the elastic PE stored is U = ½ k x². Independent of sign of x.

-- NCERT Class 11 Physics, Ch. 5, p. 10

Formulas

10 formulas — click to collapse

Elastic collision — 1D final velocities

Final velocities of two bodies after an elastic head-on (1D) collision — momentum AND kinetic energy are both conserved. Special cases: equal masses exchange velocities; very heavy m2 at rest reflects m1 with reversed velocity.

SymbolQuantitySI Unit
m1, m2Masses of the two bodieskg
u1, u2Initial velocities (signed, before collision)m/s
v1, v2Final velocities (signed, after collision)m/s

Valid when

  • Collision is ELASTIC (kinetic energy conserved)
  • Head-on (1D) — for 2D collisions decompose along/perpendicular to line of impact

Do NOT use when

  • Inelastic collision (KE not conserved; use momentum-only + restitution)
  • Bodies stick together (perfectly inelastic case has its own formula)

Gravitational potential energy (near Earth)

Potential energy of a body of mass m at height h above the chosen reference level, in a region where g is approximately constant.

SymbolQuantitySI Unit
UGravitational PEJ
mMasskg
gGravitational accelerationm/s^2
hHeight above reference levelm

Valid when

  • Region small enough that g is uniform (typically near Earth's surface)
  • Reference level is freely chosen — only DIFFERENCES in U have physical meaning

Do NOT use when

  • Large altitude changes (use U = -GMm/r general form)
  • Below the reference level — h is signed

Kinetic energy

Energy a body possesses by virtue of its motion. Always non-negative. Frame-dependent through v.

SymbolQuantitySI Unit
KKinetic energyJ
mMasskg
vSpeedm/s

Valid when

  • Non-relativistic speeds (v << c)
  • Translational motion only (rotational KE = (1/2) I omega^2 separately)

Conservation of mechanical energy

If only conservative forces do work on a system, the total mechanical energy E = K + U is constant in time.

SymbolQuantitySI Unit
K_i, K_fInitial, final kinetic energyJ
U_i, U_fInitial, final potential energyJ

Valid when

  • Only CONSERVATIVE forces do work (gravity, spring, electrostatic — not friction or drag)
  • Closed system; no energy exchange with surroundings

Do NOT use when

  • Friction, drag, or other non-conservative forces do work
  • External forces add energy to the system

Perfectly inelastic 1D collision — common final velocity and KE loss

When two bodies stick together after a 1D collision, the common velocity is given by momentum conservation. The KE lost is converted to internal energy (heat, deformation).

SymbolQuantitySI Unit
vCommon final velocitym/s
m1, m2Masseskg
u1, u2Initial velocitiesm/s
Delta_KChange in kinetic energyJ

Valid when

  • Bodies stick together immediately after collision (perfectly inelastic)
  • Net external force = 0 during the brief collision (momentum conservation)

Instantaneous power

Instantaneous power is the time rate of doing work; equivalently, the dot product of the force and velocity. Average power over an interval is W/t.

SymbolQuantitySI Unit
PPower (instantaneous)W
FForceN
vVelocitym/s

Valid when

  • F.v form when force and velocity are both known at the instant

Spring potential energy (Hooke's law regime)

Elastic potential energy stored in an ideal spring of force constant k that has been displaced by x from its natural length. Independent of the sign of x (compression or extension).

SymbolQuantitySI Unit
UElastic PEJ
kSpring constant (force per unit displacement)N/m
xDisplacement from natural lengthm

Valid when

  • Spring obeys Hooke's law (F = -k*x) over the displacement range
  • No internal damping / hysteresis assumed

Do NOT use when

  • Beyond elastic limit (Hooke's law fails)
  • Real springs with finite damping (some elastic PE goes to internal energy)

Work done by a constant force

The work done by a constant force F on an object that undergoes a displacement s is the dot product F.s. Equivalently, W = (magnitude of F) * (magnitude of s) * cos(angle between them). Work is a scalar but has a sign.

SymbolQuantitySI Unit
WWork (scalar, signed)J
FConstant force (vector)N
sDisplacement (vector)m
thetaAngle between F and srad/deg

Valid when

  • Force is CONSTANT in magnitude and direction over the displacement
  • Use the COMPONENT of force along the displacement, not magnitude alone

Do NOT use when

  • Force varies with position (use the variable-force integral)
  • Multiple forces act — apply this to each one separately or use net force

Work-energy theorem

The net work done by all forces on a particle equals the change in its kinetic energy. Holds for both constant and variable forces, in 1D and higher dimensions.

SymbolQuantitySI Unit
W_netNet work done by all forcesJ
Delta_KChange in kinetic energyJ
mMass of particlekg
v, v0Final, initial speedm/s

Valid when

  • W_net is the NET (vector-sum) work, not work of any one force
  • Particle (point-mass) idealisation; for extended bodies handle internal energy separately

Work done by a variable force

When a force varies along the path, the work done is the line integral of force over displacement. In one dimension this is the area under the F-vs-x curve between the start and end positions.

SymbolQuantitySI Unit
WWork doneJ
F(x)Force as a function of positionN
dxInfinitesimal displacementm
x_i, x_fInitial and final positionsm

Valid when

  • Force may depend on position (e.g. spring force F = -k*x)
  • Generalises to W = integral F.dr in higher dimensions

Exam Traps & Common Mistakes

These are the exact patterns that cause wrong answers in NEET. Each trap includes when it triggers and how to avoid it.

12 items — click to collapse

Category: Overthinking

Student assumes proportionality of speed to remaining distance under uniform deceleration. In fact, KE drops linearly with distance (v² is the linear quantity, not v): v² = u² - 2as. Speed-vs-distance is a sqrt-curve, not a line.

When it triggers

Question describes a body decelerating through stages with given speed at one stage; asks for distance to stop or speed at another stage.

How to avoid

Always work with v², not v, when uniform deceleration is in play. The work-energy theorem gives the same answer faster: ½ m v² = work done against constant force over distance.

Category: Sign Convention

Student writes a = g sin θ for a rough incline (which is the smooth-incline answer); forgets to subtract μ g cos θ.

When it triggers

Question contrasts rough vs smooth inclines, or asks for acceleration on a rough incline.

How to avoid

On a rough incline (block sliding down): a = g(sin θ - μ_k cos θ). On a rough incline (block sliding up): a = -g(sin θ + μ_k cos θ). Smooth case (μ = 0): just g sin θ.

Category: Similar Terms

Student uses the elastic-collision velocity formulas (m1-m2)/(m1+m2) when the question explicitly says 'completely inelastic' (bodies stick).

When it triggers

Question says 'inelastic', 'stick together', 'after collision moves with common velocity'.

How to avoid

Perfectly inelastic 1D: v_common = (m₁ u₁ + m₂ u₂)/(m₁ + m₂). KE is NOT conserved; loss = ½ (m₁ m₂)/(m₁+m₂) × (u₁ - u₂)². Don't use elastic formulas.

Category: Overthinking

Student computes P = Mgv (just lifting against gravity) and ignores the friction-opposing-motion term.

When it triggers

Question describes a lift moving at constant speed with explicit friction force on cable or guides.

How to avoid

At constant speed, net force = 0, so cable tension T = Mg + f_friction. Power = T × v = (Mg + f) × v. Always add friction when stated.

Category: Overthinking

Student computes ideal power and forgets the (1 - loss_fraction) or efficiency multiplier.

When it triggers

Question gives turbine, motor, or transformer with stated efficiency or loss percentage.

How to avoid

Always read the question for efficiency η or loss%. Useful power P_useful = η × P_input or P_input × (1 - loss). Don't drop the factor even if the rest of the calc is in the unrelated parts of the problem.

Category: Similar Terms

Student plugs displacement x into P = F·v formula instead of velocity v.

When it triggers

Question gives displacement x(t) explicitly and a constant force; asks for instantaneous power.

How to avoid

P = F · v where v = dx/dt. Compute v first (differentiate x(t) once), THEN plug into F·v. P is NOT F·x.

Category: Overthinking

Student treats spring PE as proportional to displacement (linear) instead of displacement-squared (quadratic). Common error: 'doubling the stretch doubles the PE'. Actual: doubling the stretch gives 4× the PE.

When it triggers

Question gives U at one stretch and asks for U at another. Distractors include linear-scaling answer (×2 instead of ×4 for double stretch).

How to avoid

U = ½ k x² is QUADRATIC. The PE-to-stretch ratio is the SQUARE of the stretch ratio: if stretch goes from x₁ to x₂, U_new / U_old = (x₂/x₁)².

Category: Overthinking

Student uses ½ m v₀² = m g (2L) (energy to reach top) and forgets the additional v_top² ≥ gL constraint for tension.

When it triggers

Question asks for minimum v₀ at lowest point so the bob can complete a full vertical circle.

How to avoid

TWO constraints: (1) energy: v_top² = v₀² - 4gL; (2) tension at top ≥ 0: v_top² ≥ gL. Combined: v₀² ≥ 5gL. Energy alone gives only v₀² ≥ 4gL which is insufficient.

Root cause: concept gap

Correction

Elastic: BOTH momentum and kinetic energy conserved -> use the (m1-m2)/(m1+m2) form. Inelastic: ONLY momentum conserved; KE generally lost to heat. Perfectly inelastic: bodies stick together -> common velocity = (m1*u1 + m2*u2)/(m1+m2). Identify which type from the problem before choosing a formula.

Wrong option pattern

Distractor uses elastic-collision formulas for two bodies that the problem says stick together after impact.

Root cause: formula misuse

Correction

Mechanical-energy conservation requires that ONLY conservative forces do work. When friction or drag is present, use the work-energy theorem directly: K_f - K_i = W_conservative + W_non-conservative, where W_non-conservative is typically negative (energy goes to heat).

Wrong option pattern

Distractor sets m*g*h = (1/2)*m*v^2 for a block sliding down a rough incline.

Root cause: concept gap

Correction

PE is defined up to an additive constant. Only DIFFERENCES in PE have physical meaning (they equal the negative work done by the conservative force between two points). Choosing the ground as zero is a convention, not a derivation.

Wrong option pattern

Distractor offers a numerical PE value where two different reference levels would give different correct numbers.

Past Year Questions

6 questions from NEET 2021, 2022, 2023, 2024, 2025. Answers verified against NTA official keys. — click to collapse

How NEET usually asks this

7 recurring patterns from past papers — click to collapse

Sources

NCERT refs: Class 11 Physics Chapter 5, p.10

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