Class 9SCIENCE AT ADVANCED LEVELChapter 3

Chapter 3: Newton's Laws of Motion

Pseudo force, gravitation and orbital motion, variation of g with altitude and depth, and turning forces (torque).

Last updated: 09/10/2026Chapter Notes and Solved Questions

Quick Chapter Information

Class9
SubjectAdvanced Science
Chapter3
DifficultyAdvanced

Limitations of Newton's Laws in Accelerating Frames

Newton's laws work without modification in inertial frames: frames at rest or moving with constant velocity. In an accelerating frame, an observer may introduce a pseudo force to describe apparent motion. It does not arise from a physical interaction.

Fpseudo = −m aframe. The negative sign indicates that the pseudo force acts opposite to the frame's acceleration.

Quick Check 1. In which type of reference frame are Newton's laws valid?

Answer: Newton's laws are valid without modification in an inertial frame of reference.


Quick Check 2. Define pseudo force and write its formula.

Answer: A pseudo force is an apparent force introduced when describing motion from an accelerating frame. Its formula is Fpseudo = −m aframe.


Quick Check 3. A lift accelerates upward at 4.5 m/s². Find the pseudo force on a 60 kg person.

Fpseudo = −ma = −60 × 4.5 = −270 N.

Answer: Magnitude = 270 N downward, opposite to the lift's acceleration.


Quick Check 4. Why does pseudo force disappear in an inertial frame?

Answer: An inertial frame has zero acceleration, so Fpseudo = −m × 0 = 0.


3.2 Gravitation and Orbital Motion

The Sun's gravitational force provides the centripetal force that continuously changes Earth's velocity direction and keeps it in orbit. Earth's tangential velocity and inertia prevent it from falling straight into the Sun.

Why do astronauts appear weightless?

Astronauts and their spacecraft are both in continuous free fall around Earth. They appear weightless because they accelerate together; gravity has not disappeared.


Why do objects fall at the same rate in a vacuum?

In a vacuum there is no air resistance. Since F = mg and a = F/m, a = mg/m = g. The mass cancels, so objects have the same gravitational acceleration at the same location.


Gravity at height h

gh = g [R/(R + h)]². As altitude increases, the distance from Earth's centre increases and g decreases.


Gravity at depth d

For the uniform-density Earth model, gd = g(1 − d/R). In this simplified model, g decreases towards the centre and becomes zero at the centre.


Quick Check 1. Where does g reach its maximum value—on the surface, above, or below Earth?

Answer: In the chapter's simplified model, g is maximum at Earth's surface and decreases above and below it.


Quick Check 2. What happens to g at Earth's centre?

Answer: It becomes zero in the idealised spherical model because the gravitational pulls balance.


Quick Check 3. Calculate g at a height of 400 km if R = 6400 km.

Using g = 9.8 m/s² and gh = g[R/(R+h)]²:

gh = 9.8 × [6400/6800]² ≈ 8.68 m/s².


Quick Check 4. At what depth will g become half of its surface value?

g/2 = g(1 − d/R), so 1/2 = 1 − d/R and d = R/2.

Answer: Half the Earth's radius; for R = 6400 km, 3200 km.


Quick Check 5. Why does gravity decrease both above and below Earth's surface?

Answer: Above Earth, distance from its centre increases. Below the surface, the enclosed mass contributing to the net gravitational pull decreases towards the centre in the uniform-density model.


3.3 Turning Forces (Moment of Force / Torque)

Torque is the turning effect of a force about a pivot.

τ = F × d × sin θ

F is force, d is the distance from pivot to the point of application, and θ is the angle between the force and lever arm. SI unit: N m.

Question 1. Why is a door easier to open at the handle than near the hinges?

Answer: The handle is farther from the hinge, giving a larger lever arm and greater torque for the same perpendicular force.


Question 2. At what angle is torque maximum? What if force is parallel to the wrench?

Answer: Torque is maximum at 90°. If force is parallel or antiparallel to the wrench, sin θ = 0 and torque is zero.


Question 3. Two students push a gate with the same perpendicular force at 20 cm and 80 cm from the hinge. Who produces greater torque?

τ = Fd. The second torque is F × 0.8, while the first is F × 0.2.

Answer: The student pushing at 80 cm produces four times the torque.


Question 4. Can a force act on a body and still produce zero torque?

Answer: Yes. If the line of action passes through the pivot, the perpendicular distance is zero. For example, pushing a door exactly at its hinge produces no turning effect.


Question 5. Two 10 N downward forces act on a rod pivoted at its centre, one 0.5 m to the left and one 0.5 m to the right. Will it rotate?

Each torque has magnitude 10 × 0.5 = 5 N m, but the directions are opposite. Net torque = 5 − 5 = 0 N m.

Answer: The torques balance, so there is no net turning effect.


Question 6. Why can a mechanic loosen a tight bolt with a long spanner?

Answer: A longer spanner increases the lever arm, so it produces greater torque with the same force.


Question 7. A force of 20 N is applied 0.8 m from a door hinge. Find torque at 90°, 60° and 30°.

τ = Fd sin θ = 20 × 0.8 × sin θ = 16 sin θ.

  • 90°: 16 N m
  • 60°: 16 × 0.866 ≈ 13.9 N m
  • 30°: 16 × 0.5 = 8 N m

Formula Summary

  • Pseudo force: Fpseudo = −m aframe
  • Newton's second law: Fnet = ma
  • Gravitational force: F = Gm₁m₂/r²
  • Weight: W = mg
  • Gravity at height: gh = g[R/(R+h)]²
  • Gravity at depth (uniform-density model): gd = g(1 − d/R)
  • Torque: τ = Fd sin θ

Note: The altitude and depth equations are simplified textbook models. Earth's actual density is not uniform.