10  Newton’s Laws of Motion

10.1 Syllabus inquiry question

  • How do forces change the motion of objects?
Feynman Insight

From The Feynman Lectures on Physics, Vol I, Chapter 10:

Newton’s laws are not explanations of why motion occurs. They are rules that connect force, mass, and acceleration so that motion can be calculated.

10.2 Learning Objectives

  • State Newton’s three laws in words and symbols.
  • Apply \(F_{net} = ma\) to solve motion problems.
  • Identify action-reaction force pairs.
  • Use free-body diagrams to justify equations.

10.3 Content

10.3.1 Newton’s First Law (Law of Inertia)

If the net force on an object is zero, it remains at rest or moves at constant velocity.

This law describes inertia—the tendency of objects to resist changes in their motion.

Key implications:

  • An object at rest stays at rest unless a net force acts
  • An object in motion continues at constant velocity unless a net force acts
  • “Constant velocity” means constant speed AND direction
Inertia in Action

When a car brakes suddenly, passengers continue forward—they have inertia. Seatbelts provide the force needed to decelerate you with the car.

10.3.2 Interactive: First Law Demonstration

A puck on a frictionless surface maintains constant velocity:

Observation: Equal spacing between positions means constant velocity. Zero net force → zero acceleration.

10.3.3 Newton’s Second Law

The acceleration of an object is proportional to the net force and inversely proportional to its mass.

\[\vec{F}_{net} = m\vec{a}\]

Or equivalently: \(a = \frac{F_{net}}{m}\)

This is the most-used equation in mechanics. It connects:

  • Force (N) - the cause
  • Mass (kg) - the resistance to acceleration
  • Acceleration (m/s²) - the effect

10.3.4 Interactive: Force, Mass, and Acceleration

See how doubling force or doubling mass affects acceleration:

Observation: Increasing spacing between positions indicates acceleration. The velocity arrows grow because \(v = v_0 + at\).

10.3.5 Interactive: Free-Body Diagram with Net Force

A 12 kg crate with 30 N applied force:

With \(F_{net} = 30\) N and \(m = 12\) kg: \[a = \frac{F_{net}}{m} = \frac{30}{12} = 2.5 \text{ m/s}^2\]

10.3.6 Newton’s Third Law

For every action force, there is an equal and opposite reaction force acting on a different object.

Key features of action-reaction pairs:

  • Equal magnitude and opposite direction
  • Act on different objects
  • Same type of force (both gravitational, both contact, etc.)
  • Exist simultaneously
Critical Point

Action-reaction pairs never cancel because they act on different objects. Forces only cancel when they act on the same object.

10.3.7 Interactive: Action-Reaction Pairs

When you push on a wall, the wall pushes back on you:

Important: These forces act on different objects—one on the wall, one on you.

10.3.8 Connecting the Laws

Law Statement Key Equation
First No net force → no acceleration \(\vec{F}_{net} = 0 \Rightarrow \vec{a} = 0\)
Second Net force causes acceleration \(\vec{F}_{net} = m\vec{a}\)
Third Forces come in pairs \(\vec{F}_{AB} = -\vec{F}_{BA}\)

10.4 Worked Examples

10.4.1 Example 1: Acceleration from net force

A 12 kg crate is pushed with a net force of 30 N.

Solution:

  1. Use Newton’s Second Law: \(F_{net} = ma\)

  2. Rearrange for acceleration: \(a = \frac{F_{net}}{m} = \frac{30}{12} = 2.5\) m/s²

  3. Acceleration is in the direction of the net force

10.4.2 Example 2: Net force from acceleration

A 0.80 kg cart accelerates at 4.0 m/s².

Solution:

  1. Use \(F_{net} = ma\)

  2. \(F_{net} = 0.80 \times 4.0 = 3.2\) N

  3. Force acts in the direction of the acceleration

10.4.3 Example 3: Action-reaction pair (Skaters)

Two skaters push apart with equal force. Skater A has mass 50 kg, skater B has mass 70 kg. The push force is 140 N.

Solution:

  1. Both experience 140 N force (Third Law)

  2. Acceleration of A: \(a_A = \frac{F}{m_A} = \frac{140}{50} = 2.8\) m/s²

  3. Acceleration of B: \(a_B = \frac{F}{m_B} = \frac{140}{70} = 2.0\) m/s²

Key insight: Same force, different masses → different accelerations. The lighter skater accelerates more.

10.4.4 Example 4: Connected carts

Two carts (6 kg and 4 kg) connected by a rope are pulled with 30 N on a frictionless surface.

Solution:

  1. Total mass: \(m_{total} = 6 + 4 = 10\) kg

  2. System acceleration: \(a = \frac{F}{m_{total}} = \frac{30}{10} = 3.0\) m/s²

  3. Tension in rope (analyse the 4 kg cart):

    • Only force on 4 kg cart is tension T
    • \(T = m_2 \times a = 4 \times 3.0 = 12\) N

10.5 Common Misconceptions

Common Misconceptions
  • Misconception: Action-reaction pairs cancel. Correction: They act on different objects and cannot cancel. Only forces on the same object can cancel.

  • Misconception: A larger force always means a larger acceleration. Correction: Acceleration depends on both force AND mass: \(a = F/m\)

  • Misconception: An object in motion must have a net force. Correction: An object can move at constant velocity with zero net force (First Law).

  • Misconception: Heavier objects fall faster. Correction: In a vacuum, all objects have the same gravitational acceleration \(g\). Mass cancels in \(a = \frac{mg}{m} = g\).

  • Misconception: The reaction to your weight is the normal force from the floor. Correction: The reaction to Earth pulling you down is you pulling Earth up. The normal force is a separate interaction.

10.6 Practice Questions

10.6.1 Easy (2 marks)

A 5.0 kg object experiences a net force of 15 N. Calculate its acceleration.

  • Use \(a = F/m\) (1)
  • Correct acceleration: \(a = 15/5.0 = 3.0\) m/s² with units (1)

Answer: 3.0 m/s²

10.6.2 Medium (4 marks)

A 20 kg box is pulled along a floor with 50 N while friction is 18 N. Find the acceleration.

  • Net force calculation: \(F_{net} = 50 - 18 = 32\) N (2)
  • Acceleration calculation: \(a = 32/20 = 1.6\) m/s² (2)

Answer: 1.6 m/s² in the direction of the pull

10.6.3 Hard (5 marks)

Two carts are connected by a light rope. The system of 6 kg and 4 kg carts is pulled with 30 N on a frictionless surface. Find the acceleration and the tension in the rope.

  • Total mass and system approach: \(m = 10\) kg (1)
  • Acceleration: \(a = 30/10 = 3.0\) m/s² (1)
  • Isolate one cart for tension analysis (1)
  • Tension calculation: \(T = 4 \times 3.0 = 12\) N (1)
  • Correct units throughout (1)

Solution:

Step 1: Treat system as one object - Total mass = 6 + 4 = 10 kg - \(a = F/m = 30/10 = 3.0\) m/s²

Step 2: Analyse the rear cart (4 kg) - Only horizontal force is tension T - \(T = ma = 4 \times 3.0 = 12\) N

Answer: Acceleration = 3.0 m/s², Tension = 12 N

10.7 Multiple Choice Questions

Test your understanding with these interactive questions:

10.8 Summary

Key Takeaways
  • First Law: Zero net force means zero acceleration (inertia)
  • Second Law: \(\vec{F}_{net} = m\vec{a}\) connects force, mass, and acceleration
  • Third Law: Forces come in equal and opposite pairs on different objects
  • Connected systems can be analysed as a whole or as separate free bodies
  • Action-reaction pairs never cancel (they act on different objects)

10.9 Self-Assessment

Check your understanding:

After studying this section, you should be able to: