Newton's Laws of Motion
Misconceptions
| Misconception | Correction |
|---|---|
| "Objects need force to keep moving" | Objects in motion stay in motion without force (1st Law) |
| "Heavier objects need more force to start moving" | Mass determines acceleration for a given force: a = F/m |
| "Action-reaction forces cancel out" | Action-reaction pairs act on DIFFERENT objects, so they don't cancel |
| "No motion means no forces" | Objects at rest can have many forces that sum to zero (equilibrium) |
| "Force causes velocity" | Force causes acceleration (change in velocity), not velocity itself |
Key Concepts
Newton's First Law (Law of Inertia)
An object at rest stays at rest, and an object in motion stays in motion at constant velocity, unless acted upon by a net external force.
Key insight: Inertia is the tendency to resist changes in motion. Mass is a measure of inertia.
Newton's Second Law
The acceleration of an object is directly proportional to the net force and inversely proportional to its mass.
ΣF = ma or a = ΣF/m
- •ΣF = net force (vector sum of all forces)
- •m = mass (scalar, in kg)
- •a = acceleration (vector, in m/s²)
Newton's Third Law
For every action, there is an equal and opposite reaction.
Key insight: Forces always come in pairs acting on different objects.
- •If A pushes B with force F, then B pushes A with force -F
- •These forces are equal in magnitude, opposite in direction
Free Body Diagrams (FBD)
A diagram showing ALL forces acting on a SINGLE object:
- •Draw the object as a point or simple shape
- •Draw arrows for each force, starting from the object
- •Label each force (W, N, T, f, F_applied, etc.)
- •Arrow length should indicate relative magnitude
Common Forces
- •Weight (W or Fg): W = mg, always points down
- •Normal force (N): Perpendicular to surface, pushes away from surface
- •Tension (T): Along rope/string, pulls away from object
- •Friction (f): Parallel to surface, opposes motion or tendency to move
- •Applied force (F): Any external push or pull
Equations
[1] ΣF = ma (Newton's Second Law) [2] W = mg (Weight) [3] ΣFx = max (x-component) [4] ΣFy = may (y-component) [5] For equilibrium: ΣF = 0 (or ΣFx = 0 and ΣFy = 0)
Worked Examples
Example 1: Horizontal Push
Problem: A 10 kg box is pushed with a force of 50 N on a frictionless surface. What is its acceleration?
Solution:
- •Draw FBD: Weight (W) down, Normal (N) up, Applied force (F) horizontal
- •Apply Newton's 2nd Law in x-direction:
- •ΣFx = ma
- •50 = 10 × a
- •a = 5.0 m/s²
Example 2: Elevator Problem
Problem: A 70 kg person stands on a scale in an elevator accelerating upward at 2 m/s². What does the scale read?
Solution:
- •Draw FBD: Weight (W = mg) down, Normal force (N = scale reading) up
- •Choose up as positive
- •Apply Newton's 2nd Law:
- •ΣF = ma
- •N - mg = ma
- •N = m(g + a) = 70(9.8 + 2) = 70 × 11.8 = 826 N
Example 3: Two Blocks
Problem: Two blocks (3 kg and 5 kg) are pushed across a frictionless surface by a 24 N force applied to the 3 kg block. Find the force between the blocks.
Solution:
- •Find total acceleration: a = F/(m₁ + m₂) = 24/8 = 3 m/s²
- •For the 5 kg block alone, the only horizontal force is from the 3 kg block:
- •F_contact = m₂ × a = 5 × 3 = 15 N
Explanation Patterns
- •Always draw a Free Body Diagram first - identify all forces on the object
- •Choose a coordinate system - typically x horizontal, y vertical
- •Break forces into components if they're at angles
- •Write ΣF = ma for each direction (x and y separately)
- •Solve the resulting equations - often simultaneous equations
- •Check your answer: units should be N or m/s², sign should make physical sense
Common Problem Types
- •Single object, horizontal forces: Direct application of F = ma
- •Inclined plane (without friction): Break weight into components
- •Connected objects: Use same acceleration, different forces
- •Elevator/vertical acceleration: Scale reads N, not mg
- •Equilibrium: ΣF = 0, solve for unknown force
- •Action-reaction identification: Forces on different objects