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Unit I · Laws of motion (lesson 3)
10 min readConcept sheetSection A MCQ (1 mark) and objective (2 marks, two parts); Section B very short answer (2 marks)

Force, inertia and Newton's first law; inertial and non-inertial frames

A body keeps its state of rest or steady straight-line motion until a net external force acts. This resistance to change is inertia, measured by mass.

InertiaThe property of a body by which it resists any change in its state of rest or of uniform motion in a straight line
Measure of inertiaMass (SI unit kg). More mass means more inertia
Newton's first lawA body stays at rest, or keeps moving with uniform velocity in a straight line, unless a net external force acts on it
Inertial frameA frame at rest or moving with constant velocity, in which a body with no net force on it has no acceleration. A frame fixed to the Earth is taken as inertial

What a force can do

  • A force is a push or a pull. It is a vector: it has a size and a direction.
  • We cannot see a force. We see only its effects.
  • A force can change the shape or size of a body, as when you squeeze a balloon.
  • A force can start, stop, speed up, slow down or turn a moving body.
  • A force can rotate a body about an axis, as when you open a door.
  • When several forces act together, add them as vectors. Their single equivalent force is the net force (resultant).

How a net force changes motion

Direction of the net forceEffect on the bodyEveryday example
Along the motionSpeed increasesA mango falling from a tree goes faster and faster
Opposite to the motionSpeed decreasesA bicycle slows down when the brakes are pressed
At right angles to the motionOnly the direction changes; the speed stays the sameA stone whirled round on a string
Zero (forces balance)Velocity does not change; a body at rest stays at restA book lying on a table

From Galileo to the first law

Galileo noticed that a ball speeds up rolling down a slope and slows down rolling up one. On a level, smooth surface it should do neither, so it should keep moving. He also let a ball roll down one slope and up a facing slope. It rose to nearly the same height. As the second slope was made less steep, the ball went farther. If that slope became level, the ball would roll on for ever, with no friction. Newton turned this into his first law of motion. It is also called the law of inertia. Why must we keep pushing a trolley at steady speed? Our push only balances friction, so the net force is zero.

Inertia in daily life

  • Inertia of rest: when a bus starts suddenly, standing passengers fall backward. Their feet move with the bus, but the upper body tends to stay at rest.
  • Inertia of motion: when a moving bus stops suddenly, passengers fall forward. Their bodies tend to keep moving.
  • Inertia of direction: when a bus takes a sharp turn, passengers lean outward. Their bodies tend to keep moving in a straight line.
  • Beat a hanging carpet with a stick: the carpet moves, but the dust stays at rest and falls off.
  • Put a coin on a card over a glass. Flick the card away quickly: the coin stays behind and drops into the glass.

Inertial and non-inertial frames of reference

Inertial frameA frame at rest or moving with constant velocity. The law of inertia holds in it. Examples: the ground, or a train moving at steady speed on a straight track. Newton's laws apply only in such frames.
Non-inertial frameA frame that is accelerating: speeding up, braking or turning. A body with no net force on it seems to accelerate, so the first law seems to fail. To use Newton's second law here, add a pseudo force of size ma, opposite to the frame's acceleration a. In a rotating frame this is the centrifugal force.

A box lies on a railway platform. A person on the platform sees it at rest. A passenger in a train moving at steady velocity v sees it moving at −v, still with no acceleration. A passenger in a train speeding up at a sees it accelerate at −a, although no force acts on it.

Worked example: pseudo force in a bus

Problem

A 60 kg passenger stands in a bus that speeds up at 2 m s⁻². What pseudo force seems to act on the passenger in the bus frame? What force keeps the passenger at rest relative to the bus?

Working
  1. The bus is accelerating, so it is a non-inertial frame.
  2. Pseudo force = ma = 60 kg × 2 m s⁻² = 120 N.
  3. It acts opposite to the bus's acceleration, that is, towards the back of the bus.
  4. To stay at rest in the bus, a real force of 120 N must act forward. This is the friction of the floor on the feet (helped by a hand on the rail).
Answer

Pseudo force 120 N towards the back of the bus; it is balanced by 120 N of friction from the floor acting forward

In real life

Seat belts and airbags in cars and buses work against inertia. In a sudden stop your body keeps moving forward, and the belt supplies the force that stops you safely.

Exam angle

1 marks: “Which physical quantity is a measure of the inertia of a body?” Its mass. A larger mass means a larger inertia.

2 marks: “State Newton's first law of motion. Why does a standing passenger lurch forward when a moving bus brakes hard?” Law: a body remains at rest or in uniform motion in a straight line unless a net external force acts on it. When the bus slows, the feet slow with it, but the upper body keeps moving forward because of its inertia of motion.

2 marks: “What is an inertial frame of reference? Is a car going round a sharp bend at constant speed an inertial frame? Give a reason.” An inertial frame is at rest or moves with constant velocity, and the law of inertia holds in it. No: the car's direction of motion changes, so it is accelerating and is a non-inertial frame.

Remember it

First law = law of inertia: no net force, no change in velocity.