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Chapter 04 · Part I · Mechanics
Revised on ____________________
Chapter 04 · Newton's Laws of Motion

Draw the body, name every force, then write ΣF = ma

2 sheets
2 diagrams
25 results

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

I

The three laws, and the diagram

NO FBD, NO MARKS
I.First law  ΣF = 0v constant defines an inertial frame
II.Second law  ΣF = m a = dpdt one equation per axis
III.Third law  FAB = − FBA different bodies — they never cancel
IV.Weight  W = m g always toward the centre of the Earth
V.Normal force  N ⊥ to the surface, N ≥ 0 contact is lost when N = 0
VI.Tension  same throughout a light, ideal string a massive string does not qualify
Only three kinds of force appear in mechanics: field forces (mg), contact forces (N, f, T) and, in an accelerating frame, the pseudo-force. If a fourth appears in your diagram, it is a mistake.
mgweightNnormalTtensionFspring F=−kxvffriction
II

Systems, pulleys and constraints

THE STRING FIXES THE ACCELERATIONS
I.Blocks in contact  a = Fm1 + m2 contact force N = m₂a
II.Atwood machine  a = (m1 − m2) gm1 + m2
III.Its tension  T = 2 m1 m2 gm1 + m2 T < both weights
IV.String constraint  Σ (length along each segment) = constant differentiate twice for a
V.Movable pulley  apulley = a1 + a22
VI.Wedge constraint  the block stays on the wedge face relative a along the face
III

Friction

STATIC IS A RANGE, KINETIC IS A VALUE
I.Static  fs ≤ μs N it takes whatever value equilibrium needs
II.Kinetic  fk = μk N opposes relative sliding
III.Down an incline  a = g(sin θ − μk cos θ)
IV.Stopping distance  d = 2 μk g
V.Minimum pull at angle α  F = μ m gcos α + μ sin α least at tan α = μ
VI.Block on block  check the friction limit at each surface
applied force Ffriction fμₛNμₖNμₛNstatic: f = Fkinetic: f = μₖN
IV

Accelerating frames

ADD −ma, THEN WORK AS IF AT REST
I.Pseudo-force  Fps = − m aframe no reaction pair; it is not a real force
II.Lift going up with a  N = m(g + a) apparent weight
III.Effective gravity  geff = gaframe
IV.Pendulum in a car  tan θ = ag hangs along geff
V

Springs and equilibrium

THE LAST FEW RESULTS
I.Hooke's law  F = − k x x from the natural length
II.In series  1keq = 1k1 + 1k2
III.In parallel  keq = k1 + k2
Where marks are lost in this chapter
1“Friction opposes motion.” It opposes relative sliding — walking and pedalling are driven by it.
2Writing fs = μsN always. That is the limit: push a stuck block with 10 N and friction is 10 N.
3Taking N = mg. True only on the level with no other vertical force — on an incline N = mg cos θ.
4Confusing apparent with true weight. The scale reads N; in a lift accelerating up that is m(g + a).