Physics Lab
Class XI/Chapter 5: Laws of Motion/Inertia and Newton's First Law

Inertia and Newton's First Law

Aristotle believed bodies need a continuous push to keep moving. Galileo and Newton corrected this profoundly: a body left alone keeps doing whatever it was already doing. This tendency to resist change in motion is called inertia, and Newton's first law puts it into a precise statement.

Concept

Newton's First Law (Law of Inertia): Every body continues in its state of rest or of uniform motion in a straight line unless compelled by a net external force to change that state.

Mathematically, if the net external force is zero,

Fnet=0v=constant\vec{F}_{\text{net}} = 0 \quad \Longrightarrow \quad \vec{v} = \text{constant}

This includes the special case v=0\vec{v}=0 (rest).

Inertia is a property of mass. The greater the mass of an object, the more inertia it has, and the harder it is to change its motion.

Three kinds of inertia:

  • Inertia of rest — a body at rest tends to remain at rest. A book on a table doesn't move on its own.
  • Inertia of motion — a body in uniform motion tends to keep moving uniformly. A passenger lurches forward when a moving bus stops suddenly.
  • Inertia of direction — a body in motion tends to move in a straight line. Mud flies off a spinning bicycle tyre tangentially.

The first law also defines an inertial frame: a frame in which a force-free body moves with constant velocity. Newton's laws hold in inertial frames.

Derivation

The first law is not derived from the second; rather, it identifies the class of frames in which Newton's mechanics applies. Still, the second law contains the first as a special case:

Fnet=ma=mdvdt\vec{F}_{\text{net}} = m\vec{a} = m\frac{d\vec{v}}{dt}

If Fnet=0\vec{F}_{\text{net}} = 0, then

dvdt=0v=constant\frac{d\vec{v}}{dt} = 0 \quad \Longrightarrow \quad \vec{v} = \text{constant}

So a body with no net force experiences no acceleration and moves with constant velocity, exactly as the first law states.

Worked Example

A 5 kg block sits at rest on a frictionless horizontal surface. Two horizontal forces act on it: 12 N east and 12 N west. Describe the subsequent motion.

Solution:

Net force in the east direction:

Fnet=1212=0NF_{\text{net}} = 12 - 12 = 0 \, \text{N}

Since Fnet=0\vec{F}_{\text{net}} = 0, by Newton's first law the block remains at rest. Even though forces are present, they cancel, and the body keeps its state of motion (here, rest).

If instead the block had been moving east at 3 m/s with the same two forces acting, it would have continued moving east at 3 m/s forever — uniform motion in a straight line.

Common Confusions

  • "No motion means no force." Wrong — a book on a table has gravity pulling down and normal force pushing up. The forces balance; the net is zero, so it stays at rest.
  • "Heavy objects need more force to keep them moving." On a frictionless surface, no force is needed to maintain motion, only to change it. Heavy objects need more force only because friction usually acts.
  • Inertia is not a force. Inertia is a property of a body, not something that pushes back.
  • Frames matter. Inside an accelerating bus, a free coin appears to accelerate — but that's because the bus frame is non-inertial. Newton's laws need an inertial frame.

Key Takeaways

  • A body's natural state is uniform motion (including rest); a net force is required to change it.
  • Inertia is the resistance to change of motion, and is measured by mass.
  • The three kinds of inertia — rest, motion, direction — are everyday manifestations of the first law.
  • The first law defines inertial frames, where F=ma\vec{F}=m\vec{a} holds.
  • Balanced forces produce zero acceleration, indistinguishable from no force at all.

AI Summary

Summarize this page in your favorite LLM