How Forces Affect Motion explains what causes a change in motion. It treats force as a quantity with magnitude and direction, measured in newtons, and shows how several forces combine into a net force. Friction explains why moving things slow down. Newton’s first law covers objects with zero net force, the second law links net force, mass and acceleration through F = ma, and the third law explains walking, rowing and rockets. School exams test the laws in exact wording, net-force reasoning and F = ma numericals built on the kinematic equations.
Key Concepts
1. Force and Its Measurement
A force is a push or a pull. It can make an object move from rest (kicking a ball), change the speed or direction of a moving object (a bat striking a ball), or change the shape of an object (squeezing a lemon).
Every force has a direction. Friction acts opposite to motion, the Earth pulls objects towards itself, and a liquid pushes an object in it upwards (buoyant force). So force is a physical quantity with a magnitude, a direction and a unit, like displacement, velocity and acceleration in Chapter 4. If the magnitude, the direction, or both change, the effect of the force also changes.
The SI unit of force is the newton, symbol N. It is named after Isaac Newton. When a unit is named after a person, its full name starts with a small letter (newton) and its symbol with a capital (N).
A spring balance measures the magnitude of a force. It measures weight (the gravitational force with which the Earth pulls an object), and it also measures any pull applied to its free end.
| Force scale | Size |
|---|---|
| Smallest forces we can directly feel (a light touch) | of the order of millinewtons, 10−3 N |
| Smallest forces measured in specialised experiments (as of 2026) | down to yoctonewtons, 10−24 N |
| Upward force of your palm holding a 100 g mass | around 1 N |
2. Balanced and Unbalanced Forces
Usually more than one force acts on an object. A box being pushed has your push forwards and friction backwards. A ball floating on water has the Earth’s gravitational force downwards and the buoyant force upwards.
In a tug of war, if both teams pull with equal force, the rope does not move. Two forces equal in magnitude but opposite in direction are balanced forces. If one team pulls harder, the forces are unbalanced and the rope moves towards the larger force. A non-zero net force then acts.
| Arrangement | Magnitude of net force | Direction |
|---|---|---|
| Same direction (two people pushing a stalled car) | Sum of the magnitudes | Same as the two forces |
| Opposite directions, unequal | Difference of the magnitudes | Along the larger force |
| Opposite directions, equal | Zero | Balanced |
Worked illustration: three students push a cart eastwards with 40 N, 30 N and 20 N, and friction of 60 N acts westwards. Net force = (40 + 30 + 20) − 60 = 30 N towards the east.
A weightlifter holding a barbell steady is a balanced case: the Earth pulls the barbell down and the lifter pushes it up with an equal force. Multiple forces may act on an object, but its motion depends only on the net force.
Forces acting at an angle, and equal and opposite forces on the two ends of a handlebar or tap that make it turn, are studied in higher classes.
3. The Force of Friction
A heavy box often does not move when pushed gently. The force of friction between the box and the floor acts opposite to your push. The box moves only when your push is larger than friction, so that a net force acts in the direction of motion. Its weight (downwards) and the normal force from the surface (upwards, perpendicular to the surface) are balanced.
Stop pedalling a bicycle and it slows down and stops. A force is needed to keep an object moving only to counter friction; without that force, friction acting against the motion brings the object to rest.
Activity 6.1: a stack of four ₹10 coins is placed against a stretched rubber band, pulled back to a fixed mark and released on a wooden table top, a laminated table top and a polished marble or tiled floor. Before release the forces on the stack are balanced. On release the band’s push is larger than friction, so the net forward force accelerates the stack. Once it leaves the band, only friction acts, its velocity decreases gradually and it stops. The band is stretched equally each time, yet the distance changes with the surface, so friction differs from surface to surface.
Activity 6.2: a wooden block is pulled along each surface with a horizontal spring balance. When the block moves with neither increasing nor decreasing velocity, the net force is zero, so the spring’s pull equals friction. The reading gives an approximate measure of the force of friction.
Conclusion: when friction is smaller, the velocity decreases more slowly and the object travels a larger distance before stopping. In the activity, you expect the smallest friction and the longest slide on the polished floor.
Thought experiment: on a perfectly smooth floor with zero friction, nothing would slow the released object down, so it would keep moving. This idea leads to the first law.
Friction can also help motion. When you walk, friction from the ground pushes your foot forwards. Grooves on shoe soles and treads on tyres increase friction. Wet polished floors, ice and roads covered with water or snow give little friction, so walking or driving on them is risky. Unwanted friction is reduced with lubricants, coatings, surface texturing, streamlining and magnetic levitation.
4. Newton’s First Law of Motion
For ages people believed a force was needed to keep an object moving at constant velocity. In the 17th century Galileo Galilei argued, through thought experiments, that a body moving on a horizontal plane with all impediments removed would continue to move indefinitely.
Newton’s first law of motion: An object at rest remains at rest, and an object in motion continues to move with a constant velocity, unless a net force acts upon the object.
If the net force on an object is zero, it cannot begin to move or change its velocity, so its acceleration is zero. “At rest” means zero velocity. “Constant velocity” means no change in magnitude or direction, so a moving object travels in a straight line at the same speed. Several forces may act and still cancel.
Inertia: Newton used this word for the tendency of objects to resist a change in their state of rest or uniform motion. He presented his three laws in 1687.
With zero friction, a net force is needed only to set a resting object moving, to change its velocity, or to stop it. No force is needed to keep it moving at constant velocity.
| State (zero net force) | Position-time graph | Velocity-time graph |
|---|---|---|
| At rest | Straight line parallel to the time axis | Line along the time axis (v = 0) |
| Constant velocity | Straight line inclined to the time axis | Straight line parallel to the time axis |
A curved position-time graph means the velocity is changing, so a net force acts.
NCERT Example 6.2: a person pushes a moving box forwards with a force equal to the friction on it. The forces are equal and opposite, the net force is zero, and the box keeps moving with constant velocity.
Which situations are possible with zero net force? Staying at rest: possible. Moving with constant velocity: possible. Moving with constant acceleration: not possible.
5. Newton’s Second Law of Motion
A change in velocity is acceleration, so a force produces acceleration. Two classroom demonstrations find the relationship.
Activity 6.3 (mass fixed): a cardboard-box cart on wheels is pulled along a table by a thread that runs over a pipe at the far end and holds a paper cup with coins. The falling cup pulls the cart with a constant force. A slow-motion video gives the time T1 to cover the table. The mass in the cup is doubled and the new time T2 is recorded. The cart starts from rest and covers the same distance s, so s = ½a1T12 = ½a2T22, giving a1/a2 = T22/T12. The larger force gives a shorter time and a larger acceleration.
Activity 6.4 (force fixed): the cup’s mass is kept the same and the cart’s mass is doubled. The cart takes longer, so its acceleration is smaller: acceleration is inversely related to mass.
Ideally, doubling the force doubles the acceleration and doubling the mass halves it. Measured values differ slightly because of measurement errors and friction at the wheels.
Newton’s second law of motion: When a net force acts on an object, the object accelerates in the direction of the net force. The magnitude of the acceleration is proportional to the magnitude of the net force and is inversely proportional to the mass of the object.
a = F / m or F = ma, where F is the net force in N, m the mass in kg, and a the acceleration in m s−2, along the net force.
One newton: with m = 1 kg and a = 1 m s−2, F = 1 kg m s−2 = 1 N. One newton is the force that produces an acceleration of 1 m s−2 on an object of mass 1 kg.
Weight: the acceleration of a falling object due to the Earth’s gravitational force is g. From F = ma, the gravitational force on a mass m is F = mg, with g = 9.8 m s−2 (10 m s−2 for quick estimates). g is nearly constant near the Earth’s surface and does not depend on the mass of the object. A 100 g mass has weight 0.1 × 9.8 = 0.98 N, about 1 N.
| Change | Effect on acceleration |
|---|---|
| Force doubled, mass same | Doubles |
| Mass doubled, force same | Halves |
| Force and mass both doubled | Unchanged |
| Force tripled, mass halved | Becomes 6 times |
Stopping gently: if a moving object is brought to rest over a longer time, its acceleration is smaller, so the force needed is smaller.
- Catching a cricket ball: the fielder pulls the hands back with the ball, increasing the stopping time, reducing the force and the risk of injury.
- Airbags: in a collision the passenger’s head and chest push into a soft cushion instead of the hard steering wheel or dashboard. The longer stopping time means a smaller acceleration and a smaller force on the person, which lowers the risk of serious injury, particularly when a seat belt is also worn.
- Bubble wrap or hay around glass and a landing mat or sand bed in the high jump work the same way.
- Cracking a coconut: it hits a hard surface at high velocity and stops in a very short time, so the ground exerts a very large force that breaks the shell.
Beyond this class: momentum is the product of mass and velocity, in the direction of velocity. The complete second law says the rate of change of momentum is proportional to the net force and takes place in its direction, which also works when mass changes.
6. Newton’s Third Law of Motion
At least two objects must interact for a force to come into play. When you kick a ball, you feel the ball push on your foot.
Activity 6.5: sitting on a wheeled chair with your feet off the floor, push a heavy table away and the chair rolls backwards; pull the table and the chair rolls towards it. Each time, the table pushes you in the opposite direction.
Activity 6.6: two identical spring balances are hooked together on a table, one end fixed, and the other end is pulled. Both readings are always the same, so the forces they exert on each other are equal in magnitude and opposite in direction.
Newton’s third law of motion: 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.
The forces always occur in pairs and act on two different objects, so they do not balance each other. Equal and opposite forces on the same object do balance.
| Feature | Balanced forces | Third-law pair |
|---|---|---|
| Magnitude and direction | Equal, opposite | Equal, opposite |
| Act on | The same object | Two different objects |
| Cancel? | Yes, net force zero | No |
| Example | Equal pulls on a tug-of-war rope | Paddle on water, water on paddle |
- Walking and cycling without pedalling: your foot pushes the ground backwards; the ground pushes you forwards through friction. Without friction the foot would slip back.
- Climbing a coconut tree: the legs push down on the trunk; friction pushes the climber up with an equal force. Smooth trunks are harder to climb.
- Rowing a canoe: the paddle pushes water backwards; the water pushes the paddle and canoe forwards. Pushing harder gives a larger forward force and the canoe’s velocity increases. Drag, currents, the canoe’s mass and rowing style also matter.
- Balloon on a string (Activity 6.7): the stretched balloon pushes air out of its neck, the air pushes the balloon the other way, and it moves along the thread opposite to the escaping air.
- Rocket: the engine expels gas downwards and the gas pushes the rocket upwards. When this force is larger than the rocket’s weight, the net force is upwards and it lifts off. Firing in the direction of motion slows a craft down; the Vikram lander of Chandrayaan-3 did this for a soft landing near the Moon’s south pole.
- Fire hose: the pipe pushes water forwards and the water pushes the pipe backwards.
The third law holds for contact and non-contact forces in everyday mechanical situations: two bar magnets, two similarly charged balloons, and the Earth and a falling fruit all exert equal and opposite forces on each other.
Equal forces, unequal accelerations: the pair of forces is equal, but a = F/m, so the lighter object accelerates more. The Earth’s mass is so large that its acceleration towards a falling fruit cannot be noticed. A light bullet gets a large acceleration while the heavier gun gets a small one.
7. Forces Acting on a System of Objects
Two boxes of masses m1 and m2 on a frictionless horizontal surface are joined by a string, and a force F pulls Box 1 to the right. Box 1 pulls Box 2 through the string, and by the third law Box 2 pulls Box 1 back with an equal force, the tension T. On Box 1, F acts right and T acts left; on Box 2, T acts right.
You could find the net force on each box separately. It is simpler to treat both boxes and the string as one system. Forces between its parts are internal forces (tension) and are ignored. Only external forces from outside matter (here F):
a = F / (m1 + m2)
The system accelerates like one object of mass m1 + m2. The other external forces, total weight (m1 + m2)g downwards and total normal force N1 + N2 upwards, are balanced.
Worked illustration: m1 = 4 kg, m2 = 6 kg, F = 20 N. a = 20 / 10 = 2 m s−2. Check: Box 2 is pulled only by the string, so T = 6 × 2 = 12 N; on Box 1, 20 − 12 = 8 N and 8 / 4 = 2 m s−2, the same.
In the same way your whole body can be treated as one object while walking. Newton’s laws work from everyday objects to planets and stars, and need modification only very close to massive objects, near the speed of light and at atomic scales.
Formula and Reaction Sheet
| Relation | Formula | Units and notes |
|---|---|---|
| Net force, same direction | Fnet = F1 + F2 | N; direction of the two forces |
| Net force, opposite directions | Fnet = F1 − F2 (F1 > F2) | N; direction of the larger force |
| Balanced forces | Fnet = 0, so a = 0 | At rest or constant velocity |
| Second law | a = F / m, so F = ma | a in m s−2, same direction as F |
| Unit of force | 1 N = 1 kg m s−2 | Force giving 1 kg an acceleration of 1 m s−2 |
| Weight | F = mg | g = 9.8 m s−2 (10 for estimates) |
| Third law | FAB = −FBA | Equal magnitude, opposite direction, different objects |
| Accelerations in a third-law pair | a1 / a2 = m2 / m1 | Same force F on both, so the lighter object accelerates more |
| Connected system | a = F / (m1 + m2) | Only external forces count |
| Ratio of accelerations from times (same s, u = 0) | a1 / a2 = T22 / T12 | From s = ½aT2 (Activity 6.3) |
Here FAB means the force exerted by object A on object B. The minus sign only shows the opposite direction.
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Important Definitions
- Force: a push or pull that can make an object move from rest, change the speed or direction of a moving object, or change its shape. It has magnitude and direction.
- Newton (N): the SI unit of force. One newton is the force that produces an acceleration of 1 m s−2 on an object of mass 1 kg.
- Weight: the gravitational force with which the Earth pulls an object, F = mg.
- Balanced forces: forces on an object that are equal in magnitude but opposite in direction, so the net force is zero.
- Net force: the overall force on an object when all the forces on it are combined.
- Force of friction: the force between two surfaces in contact that acts opposite to the direction of motion (or attempted motion). It depends on the nature of the surfaces.
- Normal force: the force exerted by a surface on an object placed on it, acting perpendicular to the surface.
- Inertia: the tendency of objects to resist a change in their state of rest or uniform motion.
- Newton’s first law: An object at rest remains at rest, and an object in motion continues to move with a constant velocity, unless a net force acts upon the object.
- Newton’s second law: When a net force acts on an object, the object accelerates in the direction of the net force. The magnitude of the acceleration is proportional to the magnitude of the net force and is inversely proportional to the mass of the object.
- Newton’s third law: 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.
- Acceleration due to gravity (g): the acceleration of an object due to the gravitational force by the Earth, about 9.8 m s−2 near the surface, independent of the object’s mass.
- Tension: the force transmitted through a string that connects two objects.
- Internal force: a force between parts of a system, such as tension in the connecting string.
- External force: a force that acts on the system from outside it.
Solved Examples (NCERT-Based)
Example 1: Pushing a block against friction (NCERT Example 6.5)
Question: A student pushes a stationary block of 25 kg on a horizontal floor. The maximum force of friction opposing the motion is 50 N. Find the displacement of the block in 2 s if the push is (i) 50 N, (ii) 55 N, in the forward direction.
Solution (i): The push equals the maximum friction, so the forces are balanced and the net force is zero. The block stays stationary: displacement = 0.
Solution (ii): Net force = 55 N − 50 N = 5 N forwards.
a = F/m = 5 N / 25 kg = 0.2 m s−2.
u = 0, t = 2 s. s = ut + ½at2 = 0 + ½ × 0.2 × (2)2 = 0.1 × 4 = 0.4 m in the forward direction.
Example 2: Force on a sports car from its motion (NCERT Example 6.6)
Question: A sports car of mass 1500 kg moves towards the east. From its velocity-time graph: from 0 s to 5 s its velocity rises uniformly from 0 to 10 m s−1; from 5 s to 10 s it stays at 10 m s−1; from 10 s to 15 s it falls uniformly from 10 m s−1 to 0. Find the force on the car in each interval.
(i) 0 s to 5 s: u = 0, v = 10 m s−1, t = 5 s. From v = u + at: 10 = 0 + a × 5, so a = 2 m s−2. F = ma = 1500 × 2 = 3000 N towards the east.
(ii) 5 s to 10 s: the graph is parallel to the time axis, so velocity is constant and a = 0. No net force acts on the car.
(iii) 10 s to 15 s: u = 10 m s−1, v = 0, t = 5 s. 0 = 10 + a × 5, so a = −2 m s−2. F = 1500 × (−2) = −3000 N. The minus sign means the force is opposite to the motion: 3000 N towards the west.
Example 3: Recoil of a gun (NCERT Example 6.8)
Question: When a 0.1 kg bullet is fired from a 5 kg gun with a force of 2 N, the gun recoils. What are the magnitudes of initial accelerations of the bullet and the gun?
Solution: By the third law, the recoil force on the gun is also 2 N.
Acceleration of the gun = force / mass of gun = 2 N / 5 kg = 0.4 m s−2.
Acceleration of the bullet = force / mass of bullet = 2 N / 0.1 kg = 20 m s−2.
The forces are equal, but the accelerations differ because the masses differ. The bullet is 50 times lighter, so its acceleration is 50 times larger.
Example 4: The snake boat race (NCERT Exercise 4)
Question: 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.)
Solution: Forward force = 95 × 200 N = 19000 N. Backward force = 5 × 200 N = 1000 N.
Net force = 19000 N − 1000 N = 18000 N in the forward direction.
Example 5: Stopping a bullet in a wooden block (NCERT Exercise 12)
Question: 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).
Solution: Convert units: m = 50 g = 0.05 kg, s = 50 cm = 0.5 m. u = 100 m s−1, v = 0.
v2 = u2 + 2as gives 0 = (100)2 + 2 × a × 0.5, so 0 = 10000 + a, and a = −10000 m s−2.
F = ma = 0.05 × (−10000) = −500 N. The stopping force is 500 N, opposite to the bullet’s motion.
Example 6: Time of contact in a penalty kick (NCERT Exercise 13)
Question: 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.
Solution: For a penalty the ball starts at rest, so u = 0. Convert the speed: v = 108 × 5/18 = 30 m s−1.
a = F/m = 800 N / 0.4 kg = 2000 m s−2.
v = u + at gives 30 = 0 + 2000 × t, so t = 30/2000 = 0.015 s (15 milliseconds).
Example 7: Object on a rough patch (NCERT Exercise 14)
Question: 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?
Solution: Both forces oppose motion, so the net force = 7 N + 3 N = 10 N against the motion.
a = −10 N / 2 kg = −5 m s−2. u = 10 m s−1, v = 0.
v2 = u2 + 2as gives 0 = 100 + 2 × (−5) × s, so 10s = 100 and s = 10 m.
Example 8: Tractor, harrow and trolley (NCERT Exercise 15)
Question: 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.
Solution: From F = ma: m1 = F/a1 and m2 = F/a2.
The harrow on the trolley moves as one system of mass m1 + m2. So a = F / (m1 + m2) = F / (F/a1 + F/a2).
Cancel F: a = 1 / (1/a1 + 1/a2) = a1a2 / (a1 + a2).
Check: if a1 = a2, the total mass doubles and the formula gives a = a1/2, as expected.
Competency-Based Questions (with answers)
1. Case-based: Pushing a cupboard
Riya pushes a 40 kg cupboard across her room floor. At first she pushes with 60 N and the cupboard does not move. She increases her push to 100 N and it starts moving. While it moves, the force of friction on it is 80 N.
(a) What is the friction on the cupboard while she pushes with 60 N and it stays at rest? (b) What is the acceleration of the cupboard while she pushes with 100 N? (c) What push should she apply to keep it moving at constant velocity?
Answer: (a) The cupboard is at rest, so the net force is zero. Friction balances the push: 60 N, opposite to the push. (b) Net force = 100 − 80 = 20 N; a = 20/40 = 0.5 m s−2 in the direction of the push. (c) Constant velocity needs zero net force, so the push must equal friction: 80 N.
2. Case-based: Airbags and seat belts
In a collision a car stops abruptly. An airbag inflates quickly into a soft, compressible cushion. The passenger’s head and chest push into the bag instead of hitting the hard steering wheel or dashboard.
(a) Which quantity does the airbag increase? (b) Use Newton’s second law to explain how this reduces injury. (c) Name one other everyday use of the same idea.
Answer: (a) The time over which the passenger’s velocity drops to zero. (b) The same change in velocity over a longer time means a smaller acceleration. By F = ma, a smaller acceleration means a smaller force on the person, which lowers the risk of serious injury. (c) A fielder pulling the hands back while catching a fast ball, bubble wrap around glass items, or a landing mat in the high jump.
3. Source-based: Activity 6.3 data
A class pulls a cart over the same distance from rest using a hanging cup. With the first cup mass the cart takes T1 = 2.0 s. With double the cup mass it takes T2 = 1.5 s.
(a) Find the ratio a2/a1. (b) The ideal value is 2. Give two reasons why the measured value differs.
Answer: (a) From s = ½aT2 for the same s, a2/a1 = T12/T22 = 4.0/2.25 ≈ 1.78. (b) Friction between the cart’s wheels and the table, and errors in reading the times from the video.
4. Assertion-Reason
Assertion (A): An object moving with constant velocity on a straight road has no net force acting on it. Reason (R): A net force acting on an object always produces an acceleration in its direction.
(a) Both A and R are true and R is the correct explanation of A. (b) Both A and R are true but R is not the correct explanation of A. (c) A is true but R is false. (d) A is false but R is true.
Answer: (a). Constant velocity means zero acceleration. By R (the second law, a = F/m), any net force would produce an acceleration, so the net force must be zero. R correctly explains A.
5. Assertion-Reason
Assertion (A): The force exerted by a paddle on the water and the force exerted by the water on the paddle cancel each other. Reason (R): The two forces are equal in magnitude and opposite in direction.
Options as in Question 4.
Answer: (d). A is false: the two forces act on different objects (water and paddle), so they cannot cancel. R is true, as stated by the third law.
6. Assertion-Reason
Assertion (A): When a fruit falls, the Earth does not seem to move towards the fruit. Reason (R): The force exerted by the fruit on the Earth is much smaller than the force exerted by the Earth on the fruit.
Options as in Question 4.
Answer: (c). A is true. R is false: the two gravitational forces are equal in magnitude. The Earth’s acceleration (a = F/m) is extremely small because its mass is so large.
7. Reasoning: A spacecraft far from any planet
A spacecraft is moving in a region of space where the gravitational force on it is negligible. (a) If its engines are switched off, how will it move? (b) Suggest how it can change its velocity.
Answer: (a) With no net force it continues with constant velocity, by the first law. (b) It fires its engine to expel gas. To speed up, gas is expelled backwards, so the gas pushes the craft forwards. To slow down, the engine fires in the direction of motion, as the Vikram lander did before landing on the Moon. To change its direction, gas is expelled to one side, and the gas pushes the craft towards the opposite side.
8. Competency MCQ: Hand carts
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.
Answer: (iv). By the third law the forces are equal and opposite. The empty cart, having less mass, gets the larger acceleration.
Important Questions for Exams
1-Mark Questions
- What is the SI unit of force? The newton, symbol N (1 N = 1 kg m s−2).
- An object is moving with a constant velocity. Is there a net force acting upon it? No. Constant velocity means zero acceleration, so the net force is zero.
- A toy car of mass 100 g is moving with a constant velocity of 0.5 m s−1. What is the net force acting on the toy car? Zero, because its velocity is constant.
- When a net force acts on an object, it accelerates: (i) opposite to the force, with acceleration proportional to the force; (ii) opposite to the force, with acceleration proportional to the mass; (iii) in the direction of the force, with acceleration inversely proportional to the force; (iv) in the direction of the force, with acceleration proportional to the force. (iv).
- 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? F, acting opposite to the applied force.
2-Mark Questions
- Distinguish between balanced forces and a third-law action-reaction pair. Both are equal and opposite. Balanced forces act on the same object and cancel, giving zero net force. A third-law pair acts on two different objects, so the forces never cancel each other.
- Two children of different masses are sitting on identical swings. To impart identical initial acceleration, for which child would you require to apply a larger force? Explain why. The heavier child. From F = ma, for the same acceleration the force is proportional to the mass.
- Why does a fielder pull the hands back while catching a fast cricket ball? Pulling back increases the time in which the ball stops. The ball’s acceleration is then smaller, so by F = ma the force on the hands is smaller and injury is less likely.
- Why does a fireperson sometimes struggle when holding the pipe issuing water? The pipe pushes a large amount of water forwards at high speed. By the third law the water pushes the pipe backwards with an equal force, so the fireperson must hold it firmly.
3-Mark Questions
- A sailor jumps out from a small boat to the shore. As the sailor jumps forward, will the boat move? If yes, in which direction and why. Yes, the boat moves backwards, away from the shore. To jump, the sailor pushes the boat backwards with the feet. By the third law the boat pushes the sailor forwards with an equal force. The backward force on the boat, which floats on water, sets it moving backwards.
- Define one newton and find the force needed to give a 1200 kg car an acceleration of 1.5 m s−2. One newton is the force that produces an acceleration of 1 m s−2 on an object of mass 1 kg. F = ma = 1200 × 1.5 = 1800 N.
- A net force of 12 N acts on a 4 kg trolley at rest for 5 s. Find its acceleration, its final velocity and the distance covered. a = 12/4 = 3 m s−2. v = u + at = 0 + 3 × 5 = 15 m s−1. s = ut + ½at2 = 0 + ½ × 3 × 25 = 37.5 m.
- When the pole of a bar magnet is brought close to a magnetic compass, the magnet and the compass needle exert equal and opposite forces on each other. However, the compass needle moves, whereas the bar magnet does not move. Explain why. The forces are equal in magnitude, but equal forces do not produce equal accelerations when the masses differ (a = F/m). The compass needle has a very small mass and turns freely on its pivot, so the force gives it a noticeable acceleration and it swings. The bar magnet has a much larger mass, so the same force gives it only a very small acceleration. It is also usually held in the hand or rests on a table, where the hand or friction balances this small force. So the bar magnet shows no noticeable motion.
5-Mark Questions
- State Newton’s second law of motion. Describe an activity to show that, for a fixed mass, a larger force produces a larger acceleration. Statement: When a net force acts on an object, the object accelerates in the direction of the net force. The magnitude of the acceleration is proportional to the magnitude of the net force and is inversely proportional to the mass of the object. Activity: a wheeled cart is pulled along a table by a thread passing over a pipe at the far end to a hanging paper cup with coins. Measure the time T1 to cover the table from rest using a slow-motion video. Double the mass in the cup and measure T2. Since s = ½aT2 for the same s, a1/a2 = T22/T12. T2 is shorter, so a2 is larger: more force, more acceleration.
- State Newton’s third law of motion. Explain with examples how it accounts for (a) walking, (b) rowing a canoe, (c) the launch of a rocket. Why don’t the two forces cancel? Statement: 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. (a) The foot pushes the ground backwards; friction from the ground pushes the foot forwards. (b) The paddle pushes water backwards; the water pushes the paddle and canoe forwards with an equal force. Pushing harder gives a larger forward force. (c) The engine expels gas downwards; the gas pushes the rocket upwards. When this force exceeds the rocket’s weight, the net force is upwards and it lifts off. The two forces of a pair act on different objects, so they cannot cancel; only forces on the same object can balance.
- A 1000 kg car moving at 20 m s−1 brakes uniformly and stops in 4 s. Find (a) its deceleration, (b) the braking force, (c) the distance it covers while braking. (d) If the car carried extra load so that its mass became 1250 kg, what braking force would stop it in the same time? (a) a = (v − u)/t = (0 − 20)/4 = −5 m s−2, a deceleration of 5 m s−2. (b) F = ma = 1000 × 5 = 5000 N, opposite to the motion. (c) s = ut + ½at2 = 20 × 4 + ½ × (−5) × 16 = 80 − 40 = 40 m. (d) The same deceleration is needed, so F = 1250 × 5 = 6250 N.
Common Mistakes and Examiner Tips
- Mistake: saying a moving object needs a force to keep moving. Fix: a force is needed only to overcome friction or to change velocity. With zero net force, a moving object keeps a constant velocity (first law).
- Mistake: writing “no force acts” when the velocity is constant. Fix: write “no net force acts”. Friction, weight and the normal force may all be acting and cancelling.
- Mistake: adding forces that act in opposite directions. Fix: subtract them and give the direction of the larger force. Add only forces in the same direction.
- Mistake: saying action and reaction cancel. Fix: they act on two different objects, so they never cancel. Only forces on the same object can balance.
- Mistake: thinking the heavier object exerts a larger force in a collision or in gravity. Fix: the forces in a pair are always equal. The lighter object has the larger acceleration because a = F/m.
- Mistake: using the applied force in F = ma when friction also acts. Fix: find the net force first (applied force minus friction), then divide by mass.
- Mistake: forgetting unit conversion. Fix: change g to kg, cm to m and km h−1 to m s−1 (multiply by 5/18) before substituting. 50 g = 0.05 kg; 108 km h−1 = 30 m s−1.
- Mistake: dropping the minus sign of a retarding acceleration and then losing track of direction. Fix: keep the sign in the working, then state the answer as a magnitude with a direction (for example, “3000 N towards the west”).
- Mistake: writing the unit as Newton or n. Fix: the full name is newton (small n) and the symbol is N (capital).
- Mistake: believing g depends on the mass of the object. Fix: g is about 9.8 m s−2 for every object near the Earth’s surface. The weight mg changes with mass; g does not.
- Mistake: including tension when finding the acceleration of connected boxes treated as one system. Fix: tension is internal. Use a = F / (m1 + m2) with external forces only.
- Tip: write the three laws in the exact textbook wording. Key phrases such as “unless a net force acts”, “in the direction of the net force” and “simultaneously” are the parts examiners look for.
Quick Revision Points
- A force can start motion, change speed or direction, or change shape.
- Force has magnitude and direction. SI unit: newton (N). Measured with a spring balance.
- Equal and opposite forces on the same object are balanced: net force zero.
- Same direction: add forces. Opposite directions: subtract, direction of the larger force.
- An object’s motion depends only on the net force.
- Friction acts opposite to motion and depends on the nature of the surfaces.
- Smaller friction: velocity falls more slowly and the object travels farther.
- Galileo: with all impediments removed, a body on a horizontal plane moves indefinitely.
- First law: at rest stays at rest, moving keeps constant velocity, unless a net force acts.
- Inertia: the tendency to resist a change in the state of rest or uniform motion.
- Zero net force: zero acceleration. Position-time graph is a straight line.
- Second law: acceleration is along the net force, proportional to it and inversely proportional to mass.
- a = F/m, F = ma, 1 N = 1 kg m s−2.
- Weight F = mg, g = 9.8 m s−2, independent of mass.
- Longer stopping time means smaller acceleration and smaller force: catching, airbags, mats, bubble wrap.
- Very short stopping time means a very large force: cracking a coconut.
- Third law: forces come in equal and opposite pairs acting on two different objects.
- A third-law pair never cancels.
- Walking, pushing a bicycle along with your feet, tree climbing, rowing, balloons and rockets are third-law examples.
- The third law holds for contact and non-contact forces (magnetic, electrostatic, gravitational).
- Equal forces, unequal accelerations: gun and bullet, Earth and fruit.
- Connected objects: a = F / (m1 + m2); ignore internal forces such as tension.
Weightage and Exam Pattern
Class 9 has no board exam. This chapter is assessed in school exams (periodic tests, half-yearly and annual papers), and the NCERT source gives no fixed mark allocation for it. It combines statements of laws, reasoning about everyday situations and numericals built on F = ma and the kinematic equations of Chapter 4.
| Question type | What this chapter typically supplies |
|---|---|
| MCQ and one-word | SI unit of force, net force at constant velocity, which law applies, equal forces in a collision |
| Assertion-Reason | Balanced forces versus third-law pairs, zero net force and constant velocity, Earth and falling fruit |
| Short answer | Net force from several forces, catching a ball, fire hose, sailor jumping from a boat, choosing the larger force for a heavier object |
| Long answer | Statement of a law with an activity, third-law examples, multi-step numericals using F = ma with v = u + at or v2 = u2 + 2as |
| Case-based | Airbags and seat belts, pushing furniture against friction, rockets and spacecraft, connected boxes |
This chapter is the foundation for Class 10 physics. Finding the net force first, converting units before substituting and naming the direction of every force are habits used in every later chapter on force and motion.
Class 9 Science Β· Chapter 6 β swipe through all 10 cards to understand the whole chapter.
Force has size and direction
A force can start motion, change speed or direction, or change shape.
Change the magnitude or direction of a force and its effect changes.
- Measured with a spring balance
- Weight is the Earth’s pull on an object
- newton with small n, symbol capital N
Balanced and unbalanced forces
Motion depends only on the net force, the combined effect of all forces.
Tug of war with equal pulls: rope does not move.
- Equal and opposite on one object: balanced
- Unequal: moves towards the larger force
- 10 N right and 6 N left gives 4 N right
Always present, always opposing
Friction acts opposite to motion and depends on the surfaces in contact.
Smaller friction: the object slows more slowly and travels farther.
- A box moves only when the push exceeds friction
- Spring balance at steady pull reads friction
- Treads and sole grooves increase friction
No net force, no change
An object at rest remains at rest, and an object in motion continues with constant velocity, unless a net force acts.
Newton used the word inertia for this resistance to change.
- Constant velocity: same speed, same direction
- Zero net force is not the same as zero force
- Galileo’s thought experiments came first
Force produces acceleration
Acceleration is along the net force, proportional to it and inversely proportional to mass.
1 N gives 1 kg an acceleration of 1 m sβ»2.
- Double the force: double the acceleration
- Double the mass: half the acceleration
- Find the net force first, then divide by mass
Gravitational force F = mg
Falling objects accelerate at g due to the Earth’s gravitational force.
g does not depend on the mass of the object.
- Take g = 10 m sβ»2 for quick estimates
- 30 kg barbell weighs 294 N
- Holding it steady needs 294 N upwards
More time, less force
Stretching the stopping time lowers the acceleration and so the force.
A coconut stops very quickly, so the force is large and the shell cracks.
- Fielder pulls hands back with the ball
- Airbags and seat belts protect passengers
- Landing mats, sand beds and bubble wrap
Forces come in pairs
When one object pushes a second, the second pushes back equally and oppositely at the same instant.
The pair acts on two different objects, so it never cancels.
- Walking: foot pushes ground back, ground pushes you forward
- Canoe: paddle pushes water back, water pushes paddle forward
- Rocket: gas pushed down, rocket pushed up
Why the lighter object moves more
Third-law forces are equal, but a = F/m differs when the masses differ.
Holds for contact and non-contact forces alike.
- 2 N on a 0.1 kg bullet gives 20 m sβ»2
- 2 N on a 5 kg gun gives 0.4 m sβ»2
- Earth’s acceleration towards a fruit is too small to notice
Connected objects as one
Treat boxes joined by a string as a single system; only external forces count.
Tension in the string is an internal force.
- Weight and normal force balance vertically
- Same answer as analysing each box separately
- 4 kg + 6 kg pulled by 20 N gives 2 m sβ»2
π Practice How Forces Affect Motion - 10 questions
Concept-check questions Β· with answers & explanations
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Why C: Step 1 (weight is a force): the hanging stone stretches the spring by the gravitational force of the Earth on it, so its weight is 4.9 N, directed downward. Step 2 (F = mg): mass = 4.9 N / 9.8 m sβ»Β² = 0.5 kg.
Why not A: Weight is the Earth’s pull towards its centre, so like every force it has a direction, downward.
Why not B: 4.9 is the weight in newtons; the number on the spring balance is not the mass in kilograms.
Why not D: A spring balance measures force; the reading is precisely the stone’s weight.
Remember: Weight = mg, measured in newtons, always pointing towards the Earth.
Why C: Step 1 (same-direction forces add): forward force = 95 Γ 200 N = 19000 N; backward force = 5 Γ 200 N = 1000 N. Step 2 (opposite forces subtract, direction along the larger): net force = 19000 N – 1000 N = 18000 N in the forward direction.
Why not A: 20000 N adds all 100 forces as if every oarsman pushed forward, ignoring that 5 push the opposite way.
Why not B: 19000 N is only the forward force; the 1000 N backward force must still be subtracted.
Why not D: 1000 N is the backward force alone, and it is much smaller than the forward force, so the net force is forward.
Remember: Group forces by direction, add within a group, subtract between opposite groups.
Why B: Only two horizontal forces act on the block: the pull of the spring and the friction of the table. If the velocity is not changing, the net force is zero, so the pull exactly equals friction. The reading of the spring balance is the pull, and hence equals the magnitude of friction.
Why not A: A spring balance reads force in newtons, not mass.
Why not C: The block rests on the table, which supports its weight; the horizontal pull has nothing to do with the weight.
Why not D: Constant velocity means zero net force, not zero applied force; the spring must still pull to cancel friction.
Remember: Steady sliding means pull = friction, so the balance reads friction.
Why C: The slope of a position-time graph gives velocity. P’s horizontal line means zero velocity: the object is at rest. Q’s straight inclined line means a constant velocity. R’s curve with increasing slope means the velocity is increasing, so R is accelerating, and by Newton’s laws only R must have a net force acting on it.
Why not A: P is at rest, and an object at rest has zero acceleration and zero net force.
Why not B: Q moves with constant velocity, which by the first law needs no net force.
Why not D: Neither rest nor constant velocity requires a net force; only a changing velocity does.
Remember: A straight position-time line (flat or sloping) means no net force; a curve means a net force.
Why A: Step 1 (treat the boxes and string as one system): the tension in the string is an internal force and need not be considered; the only external horizontal force is 10 N. Step 2 (Newton’s second law for the system, a = F/(mβ + mβ)): a = 10 N / (2 kg + 3 kg) = 10/5 = 2 m sβ»Β². Both boxes move together with this acceleration.
Why not B: 5 m sβ»Β² divides 10 N by the 2 kg box alone, ignoring the 3 kg box that the same force must also accelerate.
Why not C: 3.3 m sβ»Β² divides 10 N by the 3 kg box alone, forgetting the 2 kg box it drags.
Why not D: 10 m sβ»Β² divides the force by 1 kg, as if the string carried no mass at all behind it.
Remember: A connected system accelerates like one object of the total mass under the external force only.
Why A: Step 1 (Newton’s third law): the bullet exerts an equal and opposite recoil force of 2 N on the gun. Step 2 (Newton’s second law, a = F/m): bullet a = 2 N / 0.1 kg = 20 m sβ»Β²; gun a = 2 N / 5 kg = 0.4 m sβ»Β². The forces are equal but the accelerations differ because the masses differ.
Why not B: This swaps the two results; the lighter bullet must have the larger acceleration.
Why not C: Equal forces do not give equal accelerations when the masses are different.
Why not D: 2 is the force in newtons, not an acceleration; each force must be divided by the corresponding mass.
Remember: Same force, different masses, different accelerations: a = F/m for each object separately.
Why A: The chapter states that if either the magnitude or the direction, or both, of a force changes, the effect of the force also changes; pushing a box forward and pushing it backward with the same 10 N produce opposite motions. This happens precisely because force is a quantity with direction as well as magnitude, so R correctly explains A.
Why not B: R is not a side fact; the directional nature of force is exactly why a change of direction changes the effect.
Why not C: R is true; force, like velocity and acceleration, needs direction along with magnitude and unit.
Why not D: A is true; the same magnitude in a different direction gives a different result, for example friction opposing rather than aiding motion.
Remember: A force is not fully described until you say how strong it is and which way it points.
Why C: The ball stays at rest, so its motion is not changing, which means the net force on it is zero. The downward gravitational force and the upward buoyant force must therefore be equal in magnitude and opposite in direction, that is, balanced.
Why not A: If the buoyant force were larger there would be a net upward force and the ball would rise, not stay at rest.
Why not B: If gravity were larger the ball would sink; friction is not what holds a floating ball at rest.
Why not D: The Earth’s gravitational pull acts on every object near it, including a floating ball; two forces act, not one.
Remember: At rest means net force zero, so the forces present must balance.
Why D: The push of 50 N forward is opposed by friction of 50 N backward. The two forces are equal and opposite on the same block, so they are balanced and the net force is zero. A stationary block with zero net force stays stationary.
Why not A: The block never starts moving, so it cannot have a constant non-zero velocity.
Why not B: 2 m sβ»Β² comes from dividing the whole 50 N push by 25 kg, forgetting that friction cancels it and the net force is zero.
Why not C: 4 m sβ»Β² would need a net force of 100 N, which would mean adding friction to the push instead of opposing it.
Remember: The block moves only when the push is larger than the friction.
Why B: With zero net force the acceleration is zero, so the velocity cannot change. If the object was at rest, it stays at rest (i). If it was moving, it keeps the same velocity (ii). A constant non-zero acceleration (iii) means the velocity is changing, which needs a net force, so (iii) is impossible.
Why not A: Rest is not the only option; an object already moving keeps moving with constant velocity when no net force acts.
Why not C: (iii) requires a net force by Newton’s second law, so it cannot happen with zero net force.
Why not D: (iii) is the one impossible case, not the only possible one.
Remember: Zero net force allows rest or constant velocity, never acceleration.
Chapter Navigation
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Frequently Asked Questions
Both are equal in magnitude and opposite in direction. Balanced forces act on the same object, so they cancel and the net force on that object is zero. A third-law pair acts on two different objects, such as a paddle and the water, so the two forces never cancel. Each force affects only the object it acts on.
No. By Newton’s first law, an object in motion continues with constant velocity unless a net force acts on it. In daily life we keep pushing a moving box only to counter friction. If friction were zero, a net force would be needed only to start the object moving, to change its velocity, or to stop it.
One newton is the force that produces an acceleration of 1 m sβ»Β² on an object of mass 1 kg. From F = ma, 1 N = 1 kg Γ 1 m sβ»Β² = 1 kg m sβ»Β². The full name is written with a small n (newton) and the symbol with a capital N. Holding a 100 g mass needs an upward force of about 1 N.
Pulling the hands back increases the time in which the ball’s velocity drops to zero. The ball’s acceleration is then smaller, and by F = ma the force needed to stop it is smaller. This reduces the force on the hands and the risk of injury. Airbags, landing mats and bubble wrap work on the same idea.
The forces are equal in magnitude, as the third law says, but acceleration is a = F/m. The Earth’s mass is so large compared with the fruit that its acceleration is extremely small and cannot be noticed. The fruit has a small mass, so the same force gives it a clearly visible acceleration towards the Earth.
The rocket engine expels gas downwards. By Newton’s third law the gas pushes the rocket upwards with an equal and opposite force. When this upward force is larger than the rocket’s weight, the net force is upwards and the rocket lifts off. Firing the engine in the direction of motion slows a craft down, as the Vikram lander did before landing.
Treat the two boxes and the string as one system. The tension in the string is an internal force and is ignored. Only external forces count. On a frictionless surface with a pull F, the acceleration is a = F / (mβ + mβ), the same as for a single object of mass mβ + mβ.