Work, Energy and Power
🟢 Lite — Quick Review
Rapid summary for last-minute revision before your exam.
Work, Energy and Power — Key Facts for BUET Work: W = F·d = Fd cos θ (θ = angle between F and d); unit: joule (J) Kinetic Energy: KE = ½mv²; gravitational PE: PE = mgh Work-Energy theorem: net work done = change in KE = ΔKE Conservation of mechanical energy: total energy (KE + PE) is conserved in absence of non-conservative forces ⚡ Exam tip: BUET frequently tests work-energy conservation — if only conservative forces act, KE₁ + PE₁ = KE₂ + PE₂!
🟡 Standard — Core Study
Standard content for students with a few days to months.
Work, Energy and Power — BUET Study Guide
Work:
- W = F·d = Fd cos θ
- Only component of force along displacement does work
- Negative work when force opposes displacement (friction, gravity on upward motion)
- Unit: joule (J) = N·m
Energy types:
- Kinetic Energy (KE): KE = ½mv² (motion)
- Gravitational Potential Energy: PE = mgh (height h above reference)
- Elastic Potential Energy: PE = ½kx² (spring with stiffness k)
- Work done by variable force: W = ∫ F·dx
Work-Energy theorem: Net work done by all forces = change in KE W_net = ½mv₂² − ½mv₁²
Conservation of mechanical energy: In absence of non-conservative forces (friction, air resistance): KE₁ + PE₁ = KE₂ + PE₂
Power:
- Average power = work/time = energy/time
- Instantaneous power = F·v
- Unit: watt (W) = J/s
- 1 horsepower = 746 W
Conservative vs non-conservative forces:
- Conservative: gravity, spring force — path independent, PE definable
- Non-conservative: friction, air resistance — energy lost as heat
Spring potential energy: PE = ½kx² where k = spring constant (stiffness) x = displacement from equilibrium
Gravitational PE: PE = mgh; depends on height h above chosen zero level
Kinetic energy formula derivation: For constant force F = ma, using v² = u² + 2as: W = Fs = mas = ½m(v² − u²) = ½mv² − ½mu² = ΔKE ✓
- Key formula: W = Fd cos θ; KE = ½mv²; PE = mgh; energy conservation: KE₁ + PE₁ = KE₂ + PE₂
- Common trap: Work done by gravity going up is negative (−mgh); PE increases while KE decreases
- Exam weight: 2–3 questions per exam (8–12 marks); frequently combined with motion problems
🔴 Extended — Deep Dive
Comprehensive coverage for students on a longer study timeline.
Work, Energy and Power — Comprehensive BUET Notes
Variable force work: W = ∫_{x₁}^{x₂} F(x) dx For spring: W = ∫₀ˣ kx dx = ½kx²
Power and velocity: P = F·v = Fv cos θ For motion along line: P = Fv (if F and v in same direction)
Elastic collision: Both momentum and kinetic energy conserved For two masses m₁, m₂ with velocities u₁, u₂: v₁ = [(m₁ − m₂)u₁ + 2m₂u₂]/(m₁ + m₂) v₂ = [(m₂ − m₁)u₂ + 2m₁u₁]/(m₁ + m₂)
Inelastic collision: Only momentum conserved; KE lost = ½μv_rel² where μ = m₁m₂/(m₁+m₂)
Vertical circular motion energy: At top of circle (radius R): minimum speed v = √(gR) Total energy at top = ½m(gR) + mg(2R) = ½mgR + 2mgR = 2.5mgR At bottom: minimum KE needed = 2mgR (to reach top with v = √(gR))
Simple pendulum: PE = mgL(1 − cos θ) KE = ½m(Lθ̇)² Total E = mgL(1 − cos θ) + ½mL²θ̇² = constant
Mass-spring system: x = A cos(ωt + φ) where ω = √(k/m) KE = ½mω²A² sin²(ωt + φ) PE = ½kA² cos²(ωt + φ) Total = ½kA² (constant)
Reduced mass: For two-body system: μ = m₁m₂/(m₁ + m₂) Replaces two-body problem with single body of mass μ
Conservative force and potential: F = −dU/dx (one dimension) In 3D: F = −∇U For gravity: U = mgh; F = −dU/dh = −mg (downward) For spring: U = ½kx²; F = −dU/dx = −kx (restoring)
Non-conservative forces: Work done by friction = −f_k × distance This energy becomes heat (not recoverable as mechanical energy)
Gravitational potential: For large distances (not near Earth’s surface): U = −GMm/r (negative, since zero at infinity) For Earth’s surface: g = GM/R², so U = mgR at surface
Orbital energy: Kinetic: KE = ½mv² = GMm/(2r) Potential: PE = −GMm/r Total: E = KE + PE = −GMm/(2r) (negative, bound orbit) Escape velocity: v_esc = √(2GM/R) = √(2gR)
Time-varying force and energy: For any force: W = ΔKE (work-energy theorem, always valid) Only for conservative forces: W = −ΔPE
Power and efficiency: Efficiency η = useful output/total input For machine: η = (work output)/(work input) × 100%
Circular motion and energy: For satellite in circular orbit: v = √(GM/r) KE = GMm/(2r); PE = −GMm/r; E = −GMm/(2r)
Energy method for velocity: For conservative system: ½mv² + mgh + ½kx² = constant Use to find speed at any position without solving differential equation
- Remember: W = ∫ F·dx = ΔKE; for conservative forces: KE + PE = constant; spring PE = ½kx²; escape velocity v_esc = √(2gR)
- Previous years: “Block slides down from height h. Find speed at bottom” [2023 BUET]; “Spring with k=100 N/m compressed 0.1m. Find max speed of 2kg block” [2024 BUET]; “Find power needed to lift 100kg at 2m/s” [2024 BUET]
📊 BUET Admission Exam Essentials
| Detail | Value |
|---|---|
| Questions | Varies by year (~40-50 MCQ) |
| Time | Usually 2–3 hours |
| Marks | Varies by section |
| Subjects | Mathematics (highest weight), Physics, Chemistry |
| Negative | Usually no negative marking in BUET |
| Mode | Written + MCQ depending on year |
🎯 High-Yield Topics for BUET Physics
- Mechanics (Laws of Motion, Work-Energy, Rotational) — very high weight
- Electrostatics and Current Electricity — very high weight
- Modern Physics (Photoelectric effect, Atoms) — high weight
- Heat and Thermodynamics — medium-high weight
- Optics (Reflection, Refraction) — medium weight
📝 Previous Year Question Patterns
- Work, Energy, Power: 2–3 questions per exam, 8–12 marks
- Common patterns: energy conservation, spring PE, power calculations, collision KE
- Weight: very high — frequently combines with motion and circular motion
💡 Pro Tips
- Work-energy theorem is always valid, even with friction: W_net = ΔKE
- Only conservative forces allow mechanical energy conservation
- For springs: PE = ½kx² regardless of whether compressing or extending
- Gravitational PE = mgh only valid when g is constant; for large heights, use U = −GMm/r
- When solving energy problems, always choose reference level for PE clearly
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