Work, Energy and Power
Dot product work, kinetic energy theorem, conservation of mechanical energy, spring energy, power & elastic/inelastic collisions.
Topic 5.1 – 5.3: Scalar Dot Product & Work by Constant / Variable Force
W = F · d = F d cos θ (Scalar, SI unit: Joule)θ < 90°: Positive • θ = 90°: Zero • θ > 90°: NegativeW = ∫ F(x) dx = Area under F–x graph90° (like a suitcase carried horizontally), force and motion are strangers, so cos 90° = 0!A · B = AB cos θ) give a plain number (scalar) — how much one arrow helps the other!- 1Scalar Dot Product Rule: For vectors
A = Axî + Ayĵ + Azk̂andB,A · B = AB cos θ = AxBx + AyBy + AzBz. Perpendicular vectors give0! - 2Constant Force Work:
W = (F cos θ) d. Pushing forward gives positive work; friction pulling backward (θ = 180°) gives negative work (−Fd); centripetal force or gravity on level ground (θ = 90°) does zero work! - 3Variable Force Work: When force stretches or shrinks along
x, chop the path into tiny strips and sum them:W = ∫xᵢxf F(x) dx= shaded area under theFvsxcurve.
[ML2T−2]
5 m across a floor with 20 N rope tilted at 60°.W = F d cos 60° = 20 × 5 × ½ = 50 J!
50 m on a flat railway platform carrying a 30 kg trunk on his head. Work done against gravity is ZERO (θ = 90°, cos 90° = 0), NOT mgh or mgd!Topic 5.4 – 5.6: Kinetic Energy & the Work-Energy Theorem
30 km/h versus 60 km/h. If a stray dog dashes across and you jam the brakes with the exact same braking force, how much farther will the scooter skid at double speed? Not twice as far — FOUR times as far! That quadratic jump comes straight from Kinetic Energy!K = ½mv² = p² / (2m) (Scalar, always ≥ 0)Wnet = ΔK = ½mv² − ½mu²Fbrake · d = ½mu² ⇒ d ∝ u²!K; negative braking work drains K!- 1Formula & Momentum Link:
K = ½mv². Since momentump = mv, we get the super-useful shortcutK = p² / (2m)orp = √(2mK). - 2Work-Energy Theorem Proof Idea: From
v² − u² = 2as, multiply by½m:½mv² − ½mu² = (ma)s = Fnet s = Wnet! Even for curved paths and changing forces,Wnet = Kf − Kiholds universally! - 3Meaning of Signs: If
Wnet > 0, body speeds up; ifWnet < 0(friction/brakes), body slows down; ifWnet = 0, speed stays steady.
2 kg football kicked from rest speeds up to 10 m/s. Net work done by the kick = Kf − 0 = ½ × 2 × 10² = 100 J!
p increases by 100% (doubles), what happens to Kinetic Energy? Since K = p²/(2m), K becomes 4 times (a 300% increase), NOT double! Also remember Wnet sums every force acting (gravity + friction + push).Topic 5.7 – 5.8: Potential Energy & Conservation of Mechanical Energy
10 m high on a Palakkad palm tree. Even though it sits completely still, it holds silent trapped energy! The second the stem snaps, gravity swaps every metre of height into pure falling speed — and just before hitting the ground, all stored energy becomes kinetic energy!V(h) = mgh | General link: F = −dV/dxE = K + V = constant (when only conservative forces act!)V into the Kinetic cup K keeps the total water E = K + V unchanged!h gives the exact same speed v = √(2gh) at the bottom (ignoring friction) — because gravity only cares about height dropped!- 1Conservative vs Non-Conservative Forces: Gravity and spring force are conservative (work depends only on start & end heights; closed-trip work = 0). Friction is non-conservative (drains energy into heat!).
- 2Potential Energy Formula: Stored energy due to position:
V(h) = mgh(strictly, changeΔV = −Wconservative). - 3Conservation of Mechanical Energy: When only conservative forces do work,
Ki + Vi = Kf + Vf. Dropping from rest at heightHgives speed at heighth:v = √[2g(H − h)], and at bottomv = √(2gH)!
1 kg coconut falls from 20 m (take g = 10 m/s²). Initial E = mgh = 200 J. Halfway down (10 m), V = 100 J so K = 100 J; at ground, V = 0 so K = 200 J and v = √(2×10×20) = 20 m/s!
V, never ΔV or speeds.Topic 5.9: Potential Energy of a Spring (Hooke's Force)
Fs = −k x (always opposes displacement x!)V(x) = ½ k x² (Symmetric U-parabola, always ≥ 0!)½ m vmax² = ½ k xm² ⇒ vmax = xm √(k/m)k (measured in N/m), while a soft pen spring has a tiny k!- 1Hooke's Law: Spring restoring force is proportional and opposite to stretch/compression
xfrom natural length:Fs = −kx. - 2Integrating / Triangle Area: Since force grows linearly from
0tokx, work stored by stretching (or compressing!) byxis the triangle area:V(x) = ½kx². - 3Oscillation Energy Trade: At extremes
x = ±xm,K = 0andV = ½kxm². Passing equilibriumx = 0,V = 0andK = ½mvmax² = ½kxm²!
k = 200 N/m is compressed by 0.1 m. Stored potential energy V = ½ × 200 × (0.1)² = 1.0 J. If it launches a 0.5 kg block, speed v = √(2×1.0/0.5) = 2 m/s!
x = −0.1 m) STILL stores POSITIVE potential energy +½kx² because (−x)² = +x²! (2) Work to stretch from x₁ to x₂ is ½k(x₂² − x₁²), NEVER ½k(x₂ − x₁)²!Topic 5.10: Power & Commercial Unit of Energy (kWh)
1 hp motor finishes in 10 minutes while a 0.5 hp motor takes 20 minutes — because the faster motor delivers double the Power!Pav = W / t | P = dW/dt = F · v = Fv cos θ1 Watt = 1 J/s | 1 hp = 746 W1 kWh = 1000 W × 3600 s = 3.6 × 10⁶ J (ENERGY!)1 kWh = 3.6 MJ is your KSEB electricity "1 unit"!mgh), but running takes less time so your Power is much higher!- 1Definition: Power is the time rate of doing work:
Pav = W / t. Instantaneous power uses the dot product:P = F · v = Fv cos θ. Like work and energy, Power is a scalar! - 2Units: SI unit is Watt (W) =
1 J/s(dimensions[ML2T−3]). Mechanical motors use Horsepower:1 hp = 746 W. - 3Commercial Electrical Energy (kWh): Running a
1000 W(1 kW) iron box for1 hour(3600 s) consumes1 kilowatt-hour (1 kWh) = 3.6 × 106 J!
1800 kg load at constant 2 m/s against 4000 N friction (g = 10 m/s²).Motor force
F = mg + f = 18000 + 4000 = 22000 N → Power P = Fv = 22000 × 2 = 44000 W = 44 kW!
kW (power) multiplied by hour (time) equals Energy (3.6 × 10⁶ J). Don't fall for "kW means power so kWh means power"!Topic 5.11: Elastic & Inelastic Collisions in 1D and 2D
pi = pf) & Total Energy in ALL collisions!e = 1): K conserved! Inelastic (e < 1): K lost to heat! Sticky (e = 0): max loss!m₁=m₂, u₂=0) → fly apart at 90° (θ₁ + θ₂ = 90°)!m₁ = m₂, ball 1 takes ball 2's speed and ball 2 takes ball 1's speed!- 11D Elastic Formulas (
u₂ = 0): BothpandKstay conserved, so relative speed of separation equals speed of approach (v₂ − v₁ = u₁ − u₂):
v₁ = m₁ − m₂m₁ + m₂ u₁|v₂ = 2m₁m₁ + m₂ u₁. - 23 Special 1D Elastic Cases: (a) Equal mass (
m₁ = m₂) →v₁ = 0, v₂ = u₁(velocities swap!). (b) Heavy truck hits tiny marble (m₁ ≫ m₂) → truck keeps going (v₁ ≈ u₁), marble rockets at2u₁! (c) Light ball hits massive wall (m₁ ≪ m₂) → ball bounces back at−u₁! - 3Perfectly Inelastic (Sticky,
e = 0): Combined speedv = m₁u₁ + m₂u₂m₁ + m₂. Loss in kinetic energy (whenu₂ = 0):ΔK = 12 m₁m₂m₁ + m₂ u₁²!
e = (v₂ − v₁)/(u₁ − u₂) is 1 for elastic and 0 for sticky collisions.Solved Previous Year Questions (Kerala DHSE & NCERT)
Q1 (Kerala HSE March • 1 Marks): Express 1 kilowatt-hour (kWh) in Joules. Which physical quantity does kWh represent?
1 kWh = 1000 W × 3600 s = 3.6 × 10⁶ J.Q2 (Kerala HSE Say • 2 Marks): Define work done by a constant force. Give one physical example each for positive, zero, and negative work.
W = F · d = F d cos θ.• Positive: Work by gravity on a falling coconut (
θ = 0°).• Zero: Work by centripetal force in uniform circular motion, or coolie walking level against gravity (
θ = 90°).• Negative: Work done by friction on a sliding box (
θ = 180°).Q3 (Kerala HSE March • 3 Marks): State and prove the Work-Energy Theorem for a constant force.
Wnet = Kf − Ki.Proof: Using
v² − u² = 2as, multiply both sides by ½m:½mv² − ½mu² = m a s = F s = W (since F = ma along displacement s). Hence ΔK = W.Q4 (Kerala HSE Model • 3 Marks): Derive an expression for the potential energy of an elastic spring stretched by displacement x, and sketch the variation of V(x) with x.
Fs = −kx. External force to slowly stretch is Fext = +kx.W = ∫0x kx dx = [½kx²]0x = ½kx².This stored work equals spring potential energy
V(x) = ½kx² — an upward-opening parabola symmetric for both compression (x < 0) and extension (x > 0).Q5 (Kerala HSE March • 4 Marks): Prove that the total mechanical energy of a freely falling body of mass m remains constant throughout its fall.
H from rest:1. At top (height H):
v = 0 ⇒ K = 0, V = mgH ⇒ E = mgH.2. At distance x below top (height H − x):
v² = 2gx ⇒ K = ½m(2gx) = mgx; V = mg(H − x). Total E = mgx + mgH − mgx = mgH.3. At ground (height 0):
V = 0, v² = 2gH ⇒ K = mgH; Total E = mgH.Hence
K + V = mgH stays conserved at every point.Q6 (Kerala HSE Say • 2 Marks): An elevator of total mass 1800 kg moves upward at a uniform speed of 2 m/s while a constant frictional force of 4000 N opposes motion. Calculate the minimum power delivered by the motor in Watts and Horsepower (g = 10 m/s²).
F = mg + f = (1800 × 10) + 4000 = 22000 N.Power
P = F v = 22000 × 2 = 44000 W (44 kW).In horsepower:
44000 / 746 ≈ 59 hp.Q7 (Kerala HSE March • 2 Marks): A light body and a heavy body have the same linear momentum. Which one has greater kinetic energy? Justify.
K = p² / (2m), since momentum p is identical, K ∝ 1 / m.Therefore, the light body (smaller mass) has greater kinetic energy!
Q8 (NCERT / HSE Model • 4 Marks): Show that in a perfectly inelastic one-dimensional collision where a mass m₁ moving with speed u₁ sticks to a stationary mass m₂, some kinetic energy is always lost. Find the expression for this loss.
m₁u₁ = (m₁ + m₂)v ⇒ v = m₁u₁ / (m₁ + m₂).Initial KE:
Ki = ½ m₁ u₁².Final KE:
Kf = ½ (m₁ + m₂) v² = ½ m₁² u₁² / (m₁ + m₂).Loss
ΔK = Ki − Kf = ½ m₁ u₁² [1 − m₁/(m₁ + m₂)] = ½ · [m₁m₂ / (m₁ + m₂)] · u₁² > 0.