Classical Mechanics

Newton's Three Laws of Motion:
The Complete Guide

The foundation of all classical mechanics — inertia, F = ma, and action-reaction pairs explained from physical intuition through mathematical formalism, with 12 worked examples and every common misconception corrected.

Table of Contents
  1. What Are Newton's Laws?
  2. First Law: The Law of Inertia
  3. Second Law: F = ma
  4. Third Law: Action & Reaction
  5. Worked Examples
  6. Common Misconceptions
  7. Practice Problems

What Are Newton's Laws?

In 1687, Isaac Newton published Philosophiæ Naturalis Principia Mathematica — one of the most influential scientific works ever written. In it, he stated three laws of motion that, for more than two centuries, provided a complete description of how everything in the universe moves.

These three laws aren't arbitrary rules memorised for exams. They are precise, experimentally verified descriptions of how objects respond to forces. Understand them deeply and you can predict the trajectory of a thrown ball, the orbit of a satellite, the tension in a bridge cable, and the recoil of a rifle — using the same underlying principles.

Key Insight

Newton's laws apply in inertial reference frames — frames that are not accelerating. In everyday situations on Earth's surface (and ignoring Earth's rotation), this is an excellent approximation.

First Law: The Law of Inertia

NEWTON'S FIRST LAW

An object remains at rest, or in uniform motion in a straight line, unless acted upon by an external net force.

Equivalently: if the net force on an object is zero, its velocity (both magnitude and direction) does not change.

Before Newton, the dominant view (inherited from Aristotle) was that objects naturally come to rest — that motion requires a continuous cause. Newton overturned this completely. The natural state is not rest, but constant velocity (which includes zero velocity as a special case).

The property of matter that resists changes in velocity is called inertia. More massive objects have more inertia — they are harder to accelerate from rest, harder to stop when moving, and harder to redirect.

Everyday Examples

Second Law: F = ma

NEWTON'S SECOND LAW

The net force on an object equals its mass times its acceleration.

In vector form: Fnet = ma

Fnet = ma Net force (N) = mass (kg) × acceleration (m/s²)

This is the most useful of the three laws — it's the equation of motion. Given the forces on an object and its mass, you can compute its acceleration, and from that, predict its entire future trajectory.

Several points are crucial:

a = F/m Acceleration = Net force ÷ Mass
Worked Example 1
Finding Acceleration
A 5 kg block is pushed horizontally with a 20 N force on a frictionless surface. What is its acceleration?
1
Identify the net horizontal force. There is no friction, so F_net = 20 N.
2
Apply Newton's Second Law: a = F/m = 20 N ÷ 5 kg
3
Calculate: a = 4 m/s² in the direction of the applied force.
✓ Answer: a = 4 m/s²
Worked Example 2
With Friction
The same 5 kg block is pushed with 20 N, but now there is a friction force of 8 N opposing motion. What is the acceleration?
1
Identify all horizontal forces. Applied force: +20 N. Friction force: −8 N (opposing direction).
2
Calculate net force: F_net = 20 − 8 = 12 N
3
Apply Newton's Second Law: a = F_net / m = 12 N ÷ 5 kg = 2.4 m/s²
✓ Answer: a = 2.4 m/s²

Third Law: Action and Reaction

NEWTON'S THIRD LAW

For every action there is an equal and opposite reaction.

More precisely: if object A exerts a force on object B, then object B exerts an equal and opposite force on object A. These forces are equal in magnitude, opposite in direction, and act on different objects.

The third law is almost universally misunderstood. The key point is that action-reaction pairs always act on different objects. They can never cancel each other out — forces only cancel when they act on the same object.

Common Misconception

"If every action has an equal and opposite reaction, how does anything ever accelerate?" — Because the paired forces act on different objects. The net force on each individual object is what matters for that object's acceleration.

Examples of Newton's Third Law

More Worked Examples

Worked Example 3
Tension in a String
Two blocks (m₁ = 3 kg, m₂ = 5 kg) are connected by a string on a frictionless surface. A force F = 16 N pulls m₁. What is the acceleration of the system and the tension in the string?
1
Treat the system as one object: total mass = 3 + 5 = 8 kg
2
System acceleration: a = F/m_total = 16/8 = 2 m/s²
3
For m₂ alone, the only horizontal force is tension T. Apply Newton's 2nd: T = m₂ × a = 5 × 2 = 10 N
✓ Acceleration = 2 m/s², Tension = 10 N

Common Misconceptions

Practice Problems

Test your understanding with these problems. Try each one before revealing the answer.

Problem 1
Net Force
A 10 kg object has three forces acting on it: 30 N east, 10 N west, and 20 N north. What is the magnitude and direction of the acceleration?
Reveal Solution ▼
1
Net east-west: 30 − 10 = 20 N east
2
Net north-south: 20 N north
3
Resultant net force: √(20² + 20²) = 20√2 ≈ 28.3 N at 45° NE
4
Acceleration: a = 28.3 / 10 = 2.83 m/s² at 45° NE
✓ a ≈ 2.83 m/s² at 45° north of east
Continue Learning

Now that you understand Newton's laws, the natural next topics are Projectile Motion (applying the laws in 2D) and SUVAT equations (kinematics toolbox built on these laws).