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JEE · NEET Physics

Class 11 · Chapter 5

Work, Energy & Power

Overview, notes, short notes, formula sheet, daily practice problems, previous year questions, and videos for this chapter — all in one place.

Work, Energy & Power Formula Sheet

11 formulas across 4 topics in Work, Energy & Power.

2 min read

Updated 2026-07-03 · v1.0.0

Work Done by a Force

Work is force times displacement along the force. The angle between them decides everything — including whether work is positive, negative, or zero.

W = F s cosθ

Work by a constant force

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Variables used in this formula, with units and dimensions
SymbolMeaningUnitDimension
Wwork doneJ[ML²T⁻²]
Fmagnitude of the forceN[MLT⁻²]
smagnitude of displacementm[L]
θangle between force and displacementrad (or °)[M⁰L⁰T⁰]

Valid when

  • Constant force only — for variable force, integrate

Common mistakes

  • Work by friction is not always negative — on the lower block of a stacked pair, friction does POSITIVE work
  • Normal force and centripetal force do zero work (θ = 90°), no matter how large they are

W = ∫ F dx (area under the F–x graph)

Work by a variable force

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Summing F·dx over infinitesimal displacements

Variables used in this formula, with units and dimensions
SymbolMeaningUnitDimension
Fforce as a function of positionN[MLT⁻²]
dxinfinitesimal displacementm[L]

Valid when

  • Area below the x-axis counts as negative work

Common mistakes

  • Plugging the final x into W = Fx for a variable force — you must integrate or take graph area

Worth remembering

  • Work is a scalar but carries a sign — the sign tells whether energy flows into or out of the body
  • Work depends on the frame of reference: the same force can do different work in different frames

Kinetic Energy & the Work-Energy Theorem

The work-energy theorem is the fastest route in mechanics — it skips time and acceleration entirely and connects force directly to speed.

K = ½mv²

Kinetic energy

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Variables used in this formula, with units and dimensions
SymbolMeaningUnitDimension
Kkinetic energyJ[ML²T⁻²]
mmasskg[M]
vspeedm/s[LT⁻¹]

Valid when

  • Always non-negative
  • Frame-dependent

K = p²/2m, p = √(2mK)

Kinetic energy ↔ momentum relation

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Substituting v = p/m into K = ½mv²

Variables used in this formula, with units and dimensions
SymbolMeaningUnitDimension
plinear momentumkg·m/s[MLT⁻¹]
Kkinetic energyJ[ML²T⁻²]

Common mistakes

  • If momentum doubles, KE becomes FOUR times — students often say two times
  • Two bodies with equal KE do NOT have equal momentum unless masses are equal — the heavier one has more momentum

W(net) = ΔK = K(f) − K(i)

Work-energy theorem

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Integrating F = ma over displacement using a = v dv/dx

Variables used in this formula, with units and dimensions
SymbolMeaningUnitDimension
W(net)work done by ALL forcesJ[ML²T⁻²]
K(f), K(i)final and initial kinetic energiesJ[ML²T⁻²]

Valid when

  • W must include EVERY force: gravity, friction, normal, applied, tension

Common mistakes

  • Using only the applied force's work — the theorem needs the NET work
  • It holds even for variable forces and curved paths — students wrongly restrict it to constant force

Worth remembering

  • Choose the work-energy theorem when the question gives distances and speeds but not time

JEE Advanced applies the theorem on curved and rough paths where F = ma is painful — recognising when to switch tools is the real skill tested.

Potential Energy & Conservation of Mechanical Energy

Potential energy exists only for conservative forces. When only such forces act, K + U stays constant — the most powerful shortcut in mechanics.

U = mgh

Gravitational potential energy (near Earth)

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Variables used in this formula, with units and dimensions
SymbolMeaningUnitDimension
Upotential energy relative to the chosen referenceJ[ML²T⁻²]
hheight above the reference levelm[L]
gacceleration due to gravitym/s²[LT⁻²]

Valid when

  • Valid for h ≪ Earth's radius
  • Only CHANGES in U are physical — the zero level is your free choice

U = ½kx²

Elastic potential energy of a spring

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Work done against the spring force: ∫kx dx from 0 to x

Variables used in this formula, with units and dimensions
SymbolMeaningUnitDimension
kspring constantN/m[MT⁻²]
xextension or compression from natural lengthm[L]

Valid when

  • x is measured from NATURAL length, never from the equilibrium position of a hanging load

Common mistakes

  • Energy stored going from stretch x₁ to x₂ is ½k(x₂² − x₁²), NOT ½k(x₂ − x₁)²

F = −dU/dx

Conservative force from potential energy

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Variables used in this formula, with units and dimensions
SymbolMeaningUnitDimension
Fconservative force along xN[MLT⁻²]
Upotential energy functionJ[ML²T⁻²]

Valid when

  • Equilibrium where dU/dx = 0
  • Stable if U is a minimum (d²U/dx² > 0), unstable if a maximum

Common mistakes

  • Dropping the minus sign — force points from HIGH potential energy toward LOW

K(i) + U(i) = K(f) + U(f)

Conservation of mechanical energy

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Work-energy theorem when only conservative forces act

Variables used in this formula, with units and dimensions
SymbolMeaningUnitDimension
Kkinetic energyJ[ML²T⁻²]
Utotal potential energy (all forms)J[ML²T⁻²]

Valid when

  • ONLY when non-conservative forces (friction, air drag) do zero work
  • With friction: K(i) + U(i) = K(f) + U(f) + heat generated

Common mistakes

  • Applying it across a collision — collisions generally destroy mechanical energy unless stated perfectly elastic

Worth remembering

  • Work by a conservative force over any closed loop is zero — that is the defining test
  • In a vertical circle (string), the √(5gr) result of Laws of Motion comes from combining energy conservation with the top-point condition

Power

Power is the rate of doing work. The F·v form is the exam favourite — it connects engines, pumps, and vehicles to forces directly.

P(avg) = W / t

Average power

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Variables used in this formula, with units and dimensions
SymbolMeaningUnitDimension
P(avg)average powerW[ML²T⁻³]
Wwork doneJ[ML²T⁻²]
ttime takens[T]

P = F v cosθ

Instantaneous power

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P = dW/dt with dW = F·ds

Variables used in this formula, with units and dimensions
SymbolMeaningUnitDimension
Pinstantaneous powerW[ML²T⁻³]
FforceN[MLT⁻²]
vinstantaneous speedm/s[LT⁻¹]
θangle between force and velocityrad (or °)[M⁰L⁰T⁰]

Common mistakes

  • A car at TOP speed has engine force = resistive force, so P = F(resistive) × v(max) — the classic pump/vehicle question
  • Pump problems: P = (dm/dt)gh for lifting, plus ½(dm/dt)v² if the water leaves with speed v

Worth remembering

  • 1 horsepower = 746 W; 1 kWh = 3.6 × 10⁶ J (a unit of ENERGY, not power — NEET one-liner)

NEET repeats the pump-lifting-water calculation almost every alternate year; JEE Main prefers constant-power motion, where v ∝ √t and x ∝ t³ᐟ².

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