Flashcards — Chapter 7 🃏
Work and Energy — the bridge between forces and transformations! Master work, kinetic energy, potential energy, and power with these cards. ⚡
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- 🎴 Study Mode — Cards one at a time. Think, then see the answer.
- ⚡ Quick Quiz — 10 questions in 20 seconds. Score, streak, and competition!
📋 Card deck: Key terms & formulas
Section §7.1 — Work by constant force
- Work (W) — force applied in direction of motion × distance; \( W = \mathbf{F} \cdot \mathbf{d} = Fd\cos\theta \) (joule, J)
- Dot product — \( \mathbf{A} \cdot \mathbf{B} = AB\cos\phi \); commutative, distributive
- Unit of work — joule (J) = newton·meter (N·m) = kg·m²/s²
- Positive work — force has component in direction of motion; \( \theta < 90° \)
- Negative work — force opposes motion; \( \theta > 90° \)
- Zero work — force is perpendicular to displacement; \( \theta = 90° \)
Section §7.2 — Kinetic energy & work–energy theorem
- Kinetic energy (KE) — energy of motion; \( KE = \frac{1}{2}mv^2 \) (joule, J)
- Work–energy theorem — net work equals change in kinetic energy; \( W_{\text{net}} = \Delta KE = KE_f - KE_i \)
- Stopping distance — proportional to \( v^2 \); doubling speed quadruples stopping distance
- Total work — sum of work by all forces; \( W_{\text{total}} = W_1 + W_2 + \cdots \)
Section §7.3 — Variable forces & springs
- Hooke's law — restoring force in a spring; \( F = -kx \) (spring constant \( k \) in N/m)
- Elastic potential energy (spring) — \( PE_{\text{spring}} = \frac{1}{2}kx^2 \) (joule)
- Work by variable force — \( W = \int F \, dx \) (area under \( F \)–\( x \) graph)
- Spring constant \( k \) — stiff spring has large \( k \); stretching or compressing by same \( |x| \) gives same energy
Section §7.4 — Gravitational potential energy & conservative forces
- Gravitational PE (near Earth) — \( PE_{\text{gravity}} = mgh \) (height \( h \) above reference point)
- Gravitational PE (general) — \( PE = -\frac{GMm}{r} \) (zero at \( r = \infty \); bound objects have negative PE)
- Conservative force — work done is independent of path; potential energy can be defined (e.g., gravity, spring)
- Non-conservative force — work depends on path (e.g., friction, air resistance)
- Potential energy difference — \( \Delta PE = -W_{\text{conservative}} \) (work against the force)
Section §7.5 — Mechanical energy & conservation
- Total mechanical energy — \( E = KE + PE \) (sum of kinetic + potential energy)
- Conservation of mechanical energy — \( E_i = E_f \) (or \( KE_i + PE_i = KE_f + PE_f \)) when no non-conservative forces act
- Friction dissipates energy — \( \Delta E_{\text{mech}} = -W_{\text{friction}} = -f \cdot d \) (lost to heat, sound)
- Non-conservative work — \( W_{\text{non-cons}} = \Delta E = E_f - E_i \) (energy dissipation or input)
Section §7.6 — Power
- Power (P) — rate of energy transfer; \( P = \frac{\Delta E}{\Delta t} \) or \( P = \frac{dE}{dt} \) (watt, W = J/s)
- Instantaneous power — \( P = \mathbf{F} \cdot \mathbf{v} = Fv\cos\theta \) (product of force and velocity components)
📊 Topics covered
- Work — dot product, constant force, positive/negative/zero
- Kinetic energy — \( \frac{1}{2}mv^2 \), work–energy theorem
- Variable forces & springs — Hooke's law, elastic PE, integration
- Gravitational PE — near Earth and general form
- Conservative vs non-conservative — path independence
- Mechanical energy — conservation, dissipation
- Power — rate, average, instantaneous
What's next:
👉 §7.7 — Worked problems (step-by-step examples)
👉 §7.8 — Practice problems (exercises)
👉 §7.9 — Q&A (FAQs on common misconceptions)
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