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Chapter 05 · Part I · Mechanics
Revised on ____________________
Chapter 05 · Work, Energy and Power

Forces you can integrate away

2 sheets
2 diagrams
26 results

Formulas and conditions only — no derivations, no solved numbers. The diagrams are the reader's own.

I

Work

A DOT PRODUCT, WITH A SIGN
I.Constant force  W = F·d = F d cos θ
II.Variable force  W = ∫ F·dr area under an F–x graph
III.Gravity  W = − m g Δh path-independent
IV.Spring  W = 12 k xi² − 12 k xf²
V.Kinetic friction  W = − fk s s is the path length, not displacement
VI.Normal force  W = 0 whenever it is ⊥ to the motion
VII.Zero-work forces  tension on a fixed pulley, centripetal force, static friction on a rolling wheel
VIII.Sign  θ < 90° adds energy, θ > 90° removes it
Friction is the one force here whose work depends on the route. Everything else on this sheet can be replaced by a difference of potential energies.
θmgNfdgravity +W · normal 0 · friction −W
II

The work–energy theorem and power

TRUE FOR ANY FORCE, ANY PATH
I.Kinetic energy  K = 12 m v² = 2m
II.The theorem  Wnet = ΔK = Kf − Ki
III.Average power  ⟨P⟩ = Wt
IV.Instantaneous power  P = F·v = F v cos θ
V.Constant-power motion  v = √( 2 P tm ) from rest; x ∝ t3/2
VI.Efficiency  η = PoutPin
III

Potential energy

ONLY CONSERVATIVE FORCES HAVE ONE
I.Definition  ΔU = − Wcons the reference is yours to choose
II.Near-Earth gravity  U = m g h
III.Spring  U = 12 k x² x from the natural length
IV.General gravity  U = − G M mr zero at infinity
V.Force from U  Fx = − dUdx the slope of the landscape
VI.Conservative test  W around any closed loop is zero
VII.Equilibrium  dUdx = 0 stable if U″ > 0
stableU″ > 0unstableU″ < 0neutralU″ = 0
IV

Conservation of energy

WHERE THE ACCOUNTING IS DONE
I.No friction  K + U = constant
II.With friction  ΔK + ΔU = − fk s the deficit is heat
III.General  Wext = ΔK + ΔU + ΔEint
IV.Speed at the bottom  v = √(2 g h) any smooth track, any shape
V.Vertical circle, lowest point  v ≥ √(5 g L) for a string to complete the loop
Joule
1 J = 1 N m
Electron-volt
1 eV = 1.6×10−19 J
Calorie
1 cal = 4.186 J
Kilowatt-hour
1 kWh = 3.6×106 J
Horsepower
1 hp = 746 W
g h per metre
9.8 J kg−1
V

The energy landscape

READ THE GRAPH, SKIP THE ALGEBRA
Turning points  Where E = U(x). The particle stops and reverses; K = E − U is never negative, so regions with U > E are forbidden.
Bound and free  A well with E below the barrier top traps the particle between two turning points. Raise E above the barrier and the motion becomes unbounded.
Where marks are lost in this chapter
1W = F d cos θ uses the displacement of the point of application — friction's work uses the path length.
2“The normal force never does work.” Only while the surface is still: a moving wedge or a lift floor does.
3Setting the work of one force equal to ΔK. The theorem sums the work of every force.
4Using energy to find a time. Energy relates speeds to positions; time enters only through kinematics.