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Principles of Mechanics

Newton's Laws of Motion

Physics I 288 words Free to read

Newton’s deepest insight is what does not need explaining: steady motion needs no force at all. Forces explain changes in motion. Ask "what net force acts?" and you know the acceleration; ask "what acceleration do I see?" and you know the net force. The second law runs in both directions.

Newton's three laws form the foundation of classical mechanics.

The laws

  1. First law (Inertia): A body remains at rest or in uniform motion unless acted on by a net external force.
  2. Second law: Fnet=ma\vec{F}_{\text{net}} = m\vec{a}
  3. Third law: If body A exerts a force on body B, then B exerts an equal and opposite force on A.

Free-body diagrams — The essential tool for applying Newton's laws:

  1. Isolate the object.
  2. Draw all forces acting on it (weight, normal, tension, friction, etc.).
  3. Choose coordinate axes (often along and perpendicular to the surface).
  4. Apply Fx=max\sum F_x = ma_x and Fy=may\sum F_y = ma_y.

Common forces

ForceFormulaDirection
WeightW=mgW = mgDownward
NormalNNPerpendicular to surface
Kinetic frictionfk=μkNf_k = \mu_k NOpposing motion
Static frictionfsμsNf_s \leq \mu_s NOpposing tendency to slide
TensionTTAlong the string
Key insight: Newton's second law is not F=maF=ma — it is Fnet=ma\vec{F}_{\text{net}}=m\vec{a}. Only the vector sum of all forces determines acceleration.
Common pitfall: Action–reaction pairs never cancel, because they act on different bodies. The book’s weight and the table’s normal force on it are NOT such a pair — both act on the book; its true partner forces act on the Earth and the table.
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Principles of Mechanics