Welcome to “Ch 6: How Forces Affect Motion Class 9 Question Answer? “
This comprehensive guide provides accurate, step-by-step solutions for all textbook exercises.
Fully aligned with the latest CBSE syllabus and NCERT curriculum, these answers are designed to clear your physics concepts and help you score higher in your school exams.
We have also provided the source of almost all the answers in the official NCERT textbook(Exploration).
Before attempting the chapter-end questions of Revise, Reflect, Refine, learn deeply our short notes on chapter 6, How Forces Affect Motion
Q1
Using a horizontal force F, a table is moved across the floor at a constant velocity.
How much is the frictional force exerted by the floor on the table?
Answer:
The frictional force = F (equal in magnitude to applied force, opposite in direction).
The table moves at constant velocity. By Newton’s 1st Law, constant velocity means zero net force.
Two horizontal forces act on the table — applied force F (forward) and friction (backwards). For the net force to be zero, these must be exactly equal and opposite. Therefore, friction = F.
Constant velocity always means zero net force.
Page 100 and Page 101, Example 6.2
Q2
For a ball moving on a smooth frictionless surface, choose the appropriate option that will make the following statements physically correct.
(i) If no net force is applied on the ball, the velocity of the ball will remain the same/increase/decrease.
(ii) If a net force is applied on the ball in the direction of its motion,
The magnitude of the velocity of the ball will remain the same/ increase/decrease.
(iii) If a net force is applied on the ball in a direction opposite to the
direction of its motion, the magnitude of the velocity of the ball will remain the same/increase/decrease.
Answers:
| Part | Situation | Answer | Reason |
|---|---|---|---|
| (i) | No net force applied | Velocity will remain the same | Newton’s 1st Law — zero net force means no change in velocity. |
| (ii) | Net force in direction of motion | Velocity magnitude will increase | Force produces acceleration in the same direction — speed increases. |
| (iii) | Net force opposite to motion | Velocity magnitude will decrease | Force produces deceleration — speed decreases, like friction slowing an object. |
(i) Page – 100
(ii)Page – 103
(iii)Page – 97 – 98
Q3
Two blocks P and Q on a smooth horizontal surface are shown in Fig. 6.36a and Fig. 6.36b. Two forces of magnitudes 4 N and 5 N are acting in opposite directions on block P, while block Q is moving with a constant velocity.
Which of the following statements is correct?
(i) P experiences a net force, and Q does not experience a net force.
(ii) P does not experience a net force, and Q experiences a net force.
(iii) Both P and Q experience a net force.
(iv) Neither P nor Q experiences a net force.
Answer:
Option (i) — P experiences a net force; Q does not.
| Block | Forces | Net Force | Reason |
|---|---|---|---|
| P | 5 N and 4 N in opposite directions | Yes — 5 − 4 = 1 N (rightward) | “When forces are opposite in direction but unequal in magnitude, net force = difference.” |
| Q | Moving at constant velocity | No — net force = 0 | Constant velocity → zero net force by Newton’s 1st Law. |
Block P- page 96
Block Q – Page 100
“Multiple forces may act on an object, but its motion depends only on the net force.“Page 97, Note box
Q4
While practising for the snake boat race (Vallum kalli in Kerala),100 oarsmen are rowing a boat together. Out of these, 95 row backwards to propel the boat forward. But by mistake, 5 oarsmen row in the opposite direction. If each oarsman applies a horizontal force of 200 N, what is the net force on the snake boat? (Ignore drag forces, air friction, etc.)
Answer:
Step-by-step calculation:
- Forward force (95 oarsmen): 95 × 200 = 19,000 N
- Backward force (5 oarsmen): 5 × 200 = 1,000 N
Net Force = 19,000 − 1,000 = 18,000 N in the forward direction. Ans
Method: “When forces act in opposite directions, net force = difference between them.”
Page – 96, Second paragraph and Example 6.2
Q5
When a net force acts on an object, we observe that the object accelerates:
(i) opposite to the direction of force, with acceleration proportional
to the force acting on the object.
(ii) opposite to the direction of force, with acceleration proportional
to the mass of the object.
(iii) in the direction of force, with acceleration inversely proportional
to the force acting on the object.
(iv) in the direction of force, with acceleration proportional to the
force acting on the object.
Answers:
Option (iv) — in the direction of force, with acceleration proportional to the force acting on the object.
| Option | Correct? | Why |
|---|---|---|
| (i) Opposite direction, proportional to force | No | Direction is wrong — acceleration is in the same direction as force |
| (ii) Opposite direction, proportional to mass | No | Both direction and relationship are wrong |
| (iii) Same direction, inversely proportional to force | No | Acceleration is proportional to force, not inversely |
| (iv) Same direction, proportional to force | Yes | Matches F = ma exactly. |
Newton’s 2nd Law: “The magnitude of the acceleration is proportional to the magnitude of the net force.”
(iv) Page – 104, Equation- 6.2
Page – 100 Example – 6.5
Q6
The position-time graph for four objects A, B, C and D moving along a straight line are given in Fig. 6.37.
A net force acts on:
(i) Object A
(ii) Object B
(iii) Object C
(iv) Object D
Answers:
Answer: Net force acts on Object C and Object D.
The key principle: if net force = 0, the position-time graph is either flat (at rest) or a straight inclined line (constant velocity).
| Object | Graph shape | Net Force? | Reason |
|---|---|---|---|
| A | Straight inclined line | No | Constant velocity → net force = 0 |
| B | Horizontal flat line | No | Object at rest → velocity = 0 → net force = 0 |
| C | Upward curve | Yes | Changing slope = changing velocity = acceleration → net force exists |
| D | Downward curve | Yes | Changing slope = deceleration → net force acts |
A. Page – 101, Fig 6.16a
B. Page 101, Fig. 6 .15a
Quick rule:
- Straight line (flat or inclined) on position-time graph → No net force
- Curve (upward or downward) on the position-time graph → Net force is present
Q7
A sailor jumps out from a small boat to the shore (Fig. 6.38). As the sailor jumps forward, will the boat move? If yes, in which direction and why?
Answers:
Answer: Yes — the boat moves in the direction opposite to the sailor’s jump (away from shore).
Newton’s 3rd Law: when the sailor pushes off the boat to jump forward, the boat simultaneously receives an equal and opposite force, pushing it backwards.
Flow:
Sailor pushes boat backwards → Boat pushes sailor forward (equal force) → Sailor goes to shore, boat moves away
The two forces are equal in magnitude, opposite in direction, but act on two different objects (sailor and boat) — so they do not cancel each other.
This works on the same principle as rowing a canoe: “When the canoeist pushes water backwards, water pushes the paddle forward with an equal force.”
Page 108, topic 6.6 – Newton’s Third Law of Motion
Page 108 – Note Box
Q8
During a high jump event, a landing mat or sand bed is placed for the athlete to fall upon (Fig. 6.39). Explain the reason behind it.
Answers:
A soft landing mat increases the time of impact, which reduces the force on the athlete and lowers the risk of injury.
| Surface | Time to stop | Force experienced | Injury risk |
|---|---|---|---|
| Hard floor | Very short | Very large | High |
| Soft mat / sand | Longer | Much smaller | Low |
Explanation:
By Newton’s 2nd Law (F = ma), to bring the athlete from high velocity to rest, if this happens over a longer time, the deceleration (acceleration) is smaller, so the force is smaller.
The same principle applies to:
- A cricket fielder pulling hands back while catching — “the time duration is increased during which the high velocity reduces to zero.”
- Airbags in vehicles — the passenger’s head pushes into the soft bag over a longer time, reducing force.
Page – 104–105, Topic 6.5-Newton’s Second Law of Motion
Q9
A hand cart loaded with vegetables collides with an identical but empty
hand cart. During the collision:
(i) The loaded cart exerts a force of larger magnitude on the empty cart.
(ii) the empty cart exerts a force of larger magnitude on the loaded cart.
(iii) neither cart exerts a force on the other.
(iv) the loaded cart and the empty cart, both exert an equal magnitude
of force on each other.
Answers:
Option (iv) — Both carts exert equal magnitude forces on each other.
Newton’s 3rd Law states: “Whenever one object is exerting a force on a second object, the second object is simultaneously exerting an equal and opposite force on the first object.”
This applies to all interactions regardless of mass or speed.
Important distinction:
| Cart Type | Force | Acceleration |
|---|---|---|
| Loaded cart (more mass) | = F | Smaller (a = F/m, large m) |
| Empty cart (less mass) | = F | Larger (a = F/m, small m) |
“Even though the forces acting on the two interacting objects are always equal in magnitude, they do not, in general, produce equal acceleration. This is because the masses of the objects may be different.”
Page – 108, Topic 6.6 – Newton’s Third Law of Motion
Page – 110, Note box
Q10
The acceleration-mass graph for the acceleration produced by a force on objects of different masses is plotted in Fig. 6.40. Plot the force-mass graph for this case.
Answers:
The force-mass graph is a horizontal straight line — force is constant.
Using F = ma, we can calculate F for each point on the graph (Fig. 6.40):
| Mass (kg) | Acceleration from the graph (m/s²) | Force = m × a (N) |
|---|---|---|
| 1 | 10.0 | 10 |
| 2 | 5.0 | 10 |
| 4 | 2.5 | 10 |
Force = 10 N at every mass value — it is constant throughout.
The force-mass graph is therefore a horizontal straight line at F = 10 N, parallel to the mass axis.
Page – 103 – 104
Method from Activity 6.4
Q11
The velocity-time graph of an object of mass 10 kg moving along a straight line is shown in Fig. 6.41. Calculate the force acting on the object by using the graph
Answers:
Step 1 — Find acceleration:
a = (v − u) / t = (30 − 0) / 8 = 3.75 m/s²
Step 2 — Apply Newton’s 2nd Law:
F = ma = 10 × 3.75 = 37.5 N
The force acting on the object = 37.5 N in the direction of motion.
A straight line on a velocity-time graph means constant acceleration — use a = (v−u)/t, then F = ma.
Page 106, Example 6.6
Q12
A bullet of mass 50 g moving with a speed of 100 m s–1 enters a heavy, stationary wooden block and stops after penetrating a distance of 50 cm. Estimate the stopping force acting on the bullet (assume that the bullet undergoes constant acceleration within the block).
Answer:
Given: m = 0.05 kg; u = 100 m/s; v = 0 m/s; s = 0.5 m
Step 1 — Find deceleration using v² = u² + 2as:
0 = (100)² + 2 × a × 0.5
0 = 10,000 + a
a = −10,000 m/s²
Step 2 — Apply Newton’s 2nd Law:
F = ma = 0.05 × 10,000 = 500 N
The stopping force = 500 N (acting opposite to the bullet’s direction of motion).
Q13
An ace footballer converted a penalty shot by kicking the football with a speed of 108 km h–1. The estimated force they imparted was 800 N. The mass of the football was 0.4 kg. Calculate the time of contact between their foot and the ball.
Answer:
Step 1 — Convert speed:
108 km/h = 108 × (1000/3600) = 30 m/s
Step 2 — Find acceleration:
a = F/m = 800 / 0.4 = 2,000 m/s²
Step 3 — Find time (ball starts from rest, u = 0):
v = u + at → 30 = 0 + 2000 × t → t = 30/2000 = 0.015 s
Time of contact = 0.015 seconds (15 milliseconds) — extremely brief!
Q14
An object of mass 2 kg moving with a constant velocity of 10 m s–1 encounters a rough patch where the force of friction on the object is 7 N. At the same time, an additional constant force of 3 N opposing the motion is applied on the object. After entering the rough patch, how much distance does the object travel before coming to rest?
Answer:
Given: m = 2 kg; u = 10 m/s; v = 0; friction = 7 N; additional force = 3 N (both opposing)
Step 1 — Total opposing force:
7 + 3 = 10 N
Step 2 — Deceleration:
a = F/m = 10/2 = 5 m/s² (deceleration)
Step 3 — Distance using v² = u² + 2as:
0 = (10)² + 2 × (−5) × s
0 = 100 − 10s
s = 10 metres
The object travels 10 metres before stopping.
Q15
A tractor pulls a harrow (a ploughing tool) of mass m1 with a net force F resulting in an acceleration of a1. The same tractor pulls a trolley of mass m2 with a force F producing an acceleration of a2. If the tractor now pulls the trolley with the harrow placed on it (with the same force F ), then obtain an expression for the resulting acceleration in terms of a1 and a2. Ignore friction.
Answers:
Step 1 — Express masses using F = ma:
m₁ = F/a₁ and m₂ = F/a₂
Step 2 — Total mass:
m₁ + m₂ = F/a₁ + F/a₂ = F(a₁ + a₂) / (a₁ × a₂)
Step 3 — New acceleration:
a = F / (m₁ + m₂) = F / [F(a₁ + a₂)/(a₁ × a₂)]
a = (a₁ × a₂) / (a₁ + a₂)
The resulting acceleration = (a₁ × a₂) / (a₁ + a₂)
Note: the combined acceleration is always less than either a₁ or a₂ alone — the same force now moves a greater combined mass.
Page 111
Topic 6.7 – Forces Acting on a System of Objects
Q16
When the pole of a bar magnet is brought close to a magnetic compass, the bar magnet and the compass needle (which is also a magnet) exert a magnetic force on each other. As per Newton’s third law of motion, both the forces are equal in magnitude and opposite in direction. However, the compass needle moves, whereas the bar magnet does not move (Fig. 6.42). Explain why.
Answers:
The forces are equal — but the masses are very different. The compass needle has far less mass, so it accelerates much more.
Newton’s 2nd Law: a = F/m. Same force, different masses → different accelerations.
| Object | Force | Mass | Acceleration (a = F/m) | Observed motion |
|---|---|---|---|---|
| Compass needle | = F | Very small | Very large | Visibly moves |
| Bar magnet | = F | Much larger | Very small | Appears stationary |
This is the same reasoning as why the Earth does not visibly move toward a falling fruit: “The mass of the Earth is so large that the acceleration caused by the force is extremely small… too small to be noticed.”
Page 104, Eq. 6.1
Page 110, Example 6.7
End of solutions: Revise, Reflect, Refine Chapter 6 “How Forces Affect Motion”
Common Mistakes to Avoid
| Mistake | Correct Understanding | Source |
|---|---|---|
| Newton’s 3rd Law forces cancel out | They act on two DIFFERENT objects — they never cancel | p.108, Note |
| Constant velocity needs a continuous force | Constant velocity needs ZERO net force | p.100 |
| Equal forces always mean equal accelerations | Equal forces on different masses → different accelerations | p.110, Note |
| Friction always opposes motion | Friction can enable motion (walking, tree climbing, rowing) | p.107 |
All Important Formulas
| Formula | What it means |
|---|---|
| F = ma | Force = mass × acceleration |
| a = F/m | Acceleration = force ÷ mass |
| F = mg | Weight = mass × gravitational acceleration (g = 9.8 m/s²) |
| v = u + at | Velocity after time t |
| v² = u² + 2as | Velocity after distance s |
| Net F (same direction) = F₁ + F₂ | Forces add up when in the same direction |
| Net F (opposite directions) = F₁ − F₂ | Subtract when opposite; direction follows the larger force |
FAQs Ch 6: How Forces Affect Motion Class 9 Question Answer
What are Newton’s three laws of motion in simple words for Class 9?
Newton’s three laws explain what happens to an object when forces act on it — or don’t.
Law 1 (The Lazy Law): An object does not change what it is doing on its own. If it is sitting still, it stays still. If it is moving, it keeps moving at the same speed in the same direction. Something has to push or pull it to change that. This “something” is a net force.
Law 2 (The Push Law): When a net force acts, the object speeds up, slows down, or changes direction — that is, it accelerates. The bigger the force, the bigger the acceleration. The heavier the object, the smaller the acceleration for the same force. This gives us the most important formula in mechanics:
F = ma (Force = mass × acceleration)
Law 3 (The Comeback Law): Forces never come alone. When you push something, it pushes back on you — equally hard, in the opposite direction. This always happens with two different objects.
| Law | One-line version | Real-world example |
|---|---|---|
| 1st | No net force = no change in motion | A book stays on a table; a rolling ball keeps rolling |
| 2nd | Net force → acceleration; F = ma | Kicking a lighter ball sends it faster than a heavier one |
| 3rd | Every action has an equal and opposite reaction | A rocket pushes gas down; gas pushes rocket up |
What is the difference between balanced and unbalanced forces? Give examples.
Balanced forces produce no change in motion. Unbalanced forces cause acceleration.
When two or more forces act on an object, what matters is their combined effect — the net force.
Balanced Forces
When forces cancel each other out, the net force is zero. The object either stays at rest or continues moving at constant velocity.
Examples:
➽ A book resting on a table — gravity pulls it down, the table’s normal force pushes it up. Net force = zero. Book stays still.
➽ A weightlifter holding a barbell steady — upward force from arms equals downward gravitational force. Net force = zero.
➽ A tug of war where both teams pull equally — the rope does not move.
Unbalanced Forces
When forces do not cancel, a net force remains. This net force causes acceleration in its direction.
Examples:
➽ In tug of war, if one team pulls harder, the rope moves toward that team.
➽ A box being pushed across the floor when the push is greater than the friction — the box accelerates forward.
| Situation | Net Force | Result |
|---|---|---|
| Book on table | Zero | Stays at rest |
| Tug of war, equal teams | Zero | Rope stationary |
| Tug of war, unequal teams | Non-zero | Rope moves toward stronger team |
| Ball kicked harder than friction | Non-zero | Ball accelerates |
Quick formula:
- Forces in same direction → Net force = F₁ + F₂
- Forces in opposite directions → Net force = F₁ − F₂ (direction follows the larger)
Why does friction slow a moving object down — and can friction ever help motion?
Friction opposes the relative motion between surfaces. But in many situations, friction is what enables motion in the first place.
Why friction slows things down
When an object moves across a surface, friction acts on it in the direction opposite to its motion. Once you stop applying a push, only friction remains — and it decelerates the object until it stops. This is why a rolling ball eventually stops, a bicycle slows when you stop pedalling, and a sliding box comes to rest.
The smoother the surface, the smaller the friction force, and the longer the object travels before stopping. This was shown directly in Activity 6.1 of the chapter — a stack of coins travels farther on a polished marble floor than on a wooden table top, because the friction force is smaller.
When friction helps motion
Friction is not always the enemy of motion. Consider:
➽ Walking: You push the ground backwards with your foot. Friction from the ground pushes you forward. Without friction, your foot would slip and you would fall.
➽ Rowing a canoe: The paddle pushes water backwards; water pushes the paddle forward. The forward motion comes from this interaction, which involves friction-like resistance.
➽ Climbing a tree: The climber’s legs push down and back against the trunk; friction pushes the climber upward.
➽ Vehicle tyres: Tyre treads increase friction between the tyre and road, which is what allows the vehicle to move forward and stop safely.
| Situation | Role of friction |
|---|---|
| Rolling ball slowing down | Opposes motion — slows object |
| Walking | Enables motion — pushes you forward |
| Driving on wet road | Reduced friction = dangerous (skidding) |
| Shoe soles with grooves | Increased friction = better grip |
How does Newton’s Second Law explain real-life safety features like airbags, landing mats, and a fielder pulling hands back while catching?
All three work by increasing the time over which a fast-moving object is brought to rest, which reduces the force experienced and therefore reduces injury.
The logic flows directly from F = ma:
➽ The change in velocity (from fast to zero) is fixed — that cannot be changed.
➽ But the time taken to achieve that change can be controlled.
➽ Longer time → smaller acceleration → smaller force on the body.
Airbags in vehicles
When a car collides and stops suddenly, a passenger’s body continues moving forward at high speed (Newton’s 1st Law). Without an airbag, the head hits the hard steering wheel or dashboard in a very short time, meaning a huge force on the skull.
An airbag inflates instantly into a soft cushion. The passenger’s head pushes into the bag over a longer time. The deceleration is reduced, and so is the force — significantly lowering the risk of serious head injury.
Landing mats in high jump
The athlete falls from a height with high velocity and must be brought to zero velocity on landing. A hard floor does this in a very short time, producing a very large force. A thick soft mat extends the time of stopping, reducing the force on the athlete’s body.
A fielder catching a cricket ball
A fast-moving ball carries high velocity. If the fielder keeps their hands rigid, the ball stops in a very short time — large force, and possible injury. By pulling hands backwards with the ball, the fielder increases the stopping time, reducing the force needed and avoiding injury.
| Safety feature | How it works | Benefit |
|---|---|---|
| Airbag | Soft cushion increases time of impact | Reduces force on head and chest |
| Landing mat | Extends time to bring athlete to rest | Reduces force on body |
| Pulling hands back while catching | Increases time ball takes to stop | Reduces force on hands |
| Crumple zones in cars | Car body deforms slowly in a crash | Absorbs impact over a longer time |
The underlying formula in all cases:
F = m × (v − u) / t
Keep m and (v − u) fixed. Increase t. Force F drops.
What is Newton’s Third Law, and why do the two forces not cancel each other out?
Newton’s 3rd Law forces are always equal and opposite — but they act on two different objects. Forces can only cancel when they act on the same object.
The Law
Whenever one object exerts a force on a second object, the second object simultaneously exerts an equal and opposite force on the first.
This is not a special situation — it happens in every single force interaction, every time, without exception.
Why do they not cancel
Cancellation of forces only happens when two forces act on the same object. Newton’s 3rd Law pairs always involve two objects — one force on each. They cannot cancel each other because they are not acting on the same thing.
| Scenario | Force A | Force B | Do they cancel? |
|---|---|---|---|
| Book on table | Table pushes book up | Book pushes table down | No — different objects |
| Rocket launch | Rocket pushes gas down | Gas pushes rocket up | No — different objects |
| You push a wall | You push wall forward | Wall pushes you backward | No — different objects |
| Balanced forces on one object | Weight of book downward | Normal force upward (on same book) | Yes — same object, net = zero |
The critical rule to remember:
Same object + equal and opposite forces = balanced forces (net force zero, no acceleration).
Different objects + equal and opposite forces = Newton’s 3rd Law pair (each object accelerates according to its own mass).




