What does Laws of Motion cover for NEET Physics?

16 lessons: Centripetal Force, Conservation Linear Momentum, Dynamics UCM, Equilibrium Concurrent Forces, Force and Inertia, Impulse, Kinetic Friction, Laws of Friction, Momentum, Newton 1, Newton 2, Newton 3, Rolling Friction, Static Friction, Vehicle Banked Road and Vehicle Level Road.

How often has Laws of Motion come up in NEET past papers?

Our set of verified past papers has 13 questions from this unit, from NEET 2020, 2021, 2022, 2023, 2024, 2025 and 2026. Each is answered against the official NTA key.

Is the Laws of Motion material free?

Yes. All 16 lessons and 128 practice questions are free, with no login needed.

Laws of Motion

16 lessons

Topic index in NCERT order

16 of 16 lessons by the NCERT chapter they teach from, in book order. The page is the first printed page of your NCERT book the lesson cites; PYQs are the past NEET questions on that topic.

Class 11 Physics, Chapter 3

Dynamics UCMp. 420 PYQs

Class 11 Physics, Chapter 4

Force and Inertiap. 500 PYQs
Newton 1p. 500 PYQs
Equilibrium Concurrent Forcesp. 521 PYQ
Newton 3p. 520 PYQs
Momentump. 541 PYQ
Newton 2p. 543 PYQs
Impulsep. 552 PYQs
Conservation Linear Momentump. 571 PYQ
Kinetic Frictionp. 600 PYQs
Laws of Frictionp. 600 PYQs
Rolling Frictionp. 600 PYQs
Static Frictionp. 602 PYQs
Centripetal Forcep. 630 PYQs
Vehicle Level Roadp. 630 PYQs
Vehicle Banked Roadp. 641 PYQ

Centripetal Force

8 MCQs5 revision cardsWorked example

Direct Application (3)Easy Recall (3)Concept Trap (1)Calculation (1)

Conservation Linear Momentum

8 MCQs1 PYQs4 revision cardsWorked example

Direct Application (3)Easy Recall (2)Calculation (2)Concept Trap (1)

Dynamics UCM

8 MCQs9 revision cardsWorked example

Easy Recall (3)Direct Application (3)Concept Trap (1)Calculation (1)

Equilibrium Concurrent Forces

8 MCQs1 PYQs3 revision cardsWorked example

Direct Application (3)Calculation (2)Easy Recall (2)Concept Trap (1)

Force and Inertia

8 MCQs2 revision cardsWorked example

Easy Recall (3)Concept Trap (1)Direct Application (3)Calculation (1)

Impulse

8 MCQs2 PYQs5 revision cardsWorked example

Easy Recall (3)Direct Application (3)Calculation (1)Concept Trap (1)

Kinetic Friction

8 MCQs6 revision cardsWorked example

Easy Recall (3)Direct Application (3)Calculation (1)Concept Trap (1)

Laws of Friction

8 MCQs3 revision cardsWorked example

Direct Application (5)Easy Recall (1)Concept Trap (1)Calculation (1)

Momentum

8 MCQs1 PYQs6 revision cardsWorked example

Easy Recall (3)Direct Application (3)Calculation (1)Concept Trap (1)

Newton 1

8 MCQsWorked example

Easy Recall (5)Concept Trap (1)Direct Application (2)

Newton 2

8 MCQs3 PYQs2 revision cardsWorked example

Concept Trap (1)Direct Application (3)Easy Recall (3)Calculation (1)

Newton 3

8 MCQs3 revision cardsWorked example

Easy Recall (3)Concept Trap (1)Direct Application (3)Calculation (1)

Rolling Friction

8 MCQs4 revision cardsWorked example

Easy Recall (3)Direct Application (3)Calculation (1)Concept Trap (1)

Static Friction

8 MCQs2 PYQs2 revision cardsWorked example

Calculation (2)Direct Application (3)Easy Recall (3)

Vehicle Banked Road

8 MCQs1 PYQs4 revision cardsWorked example

Easy Recall (3)Direct Application (3)Concept Trap (1)Calculation (1)

Vehicle Level Road

8 MCQs6 revision cardsWorked example

Direct Application (4)Easy Recall (2)Concept Trap (2)

Past-paper questions from this unit

13 questions from NEET 2020, 2021, 2022, 2023, 2024, 2025, 2026. Answers verified against NTA official keys.

By year in our set: 2020 (1) · 2021 (1) · 2022 (2) · 2023 (2) · 2024 (2) · 2025 (3) · 2026 (2)

Lesson: Momentum

NEET 2026

A frictionless circular wire of unit radius is fixed on the horizontal plane. Two point particles of unit mass start moving simultaneously from point A (θ = π/2) with identical uniform angular speeds in opposite directions, and meet again at point B (θ = −π/2). During this time, which of the following figures schematically represent the magnitude of the total linear momentum P of the system, as a function of θ ?

NTA Answer: Option 3(final)

Report an error · Every fix is public: corrections log

Lesson: Vehicle Banked Road

NEET 2026

A car travels on a circular racetrack of radius 50 m, which is banked at an angle θ. If the car travels at a speed 10 ms⁻¹, then the wear and tear on its tyres is minimum. Taking the acceleration due to gravity to be 10 ms⁻², the value of θ is :

1tan⁻¹(1/5)

2tan⁻¹(2/5)

3tan⁻¹(√3/2)

4tan⁻¹(2√3)

NTA Answer: Option 1(final)

Report an error · Every fix is public: corrections log

Lesson: Static Friction

NEET 2025

There are two inclined surfaces of equal length (L) and same angle of inclination 45° with the horizontal. One of them is rough and the other is perfectly smooth. A given body takes 2 times as much time to slide down on rough surface than on the smooth surface. The coefficient of kinetic friction (µ k) between the object and the rough surface is close to

10.75

20.25

30.40

40.5

NTA Answer: Option 1(final)

Report an error · Every fix is public: corrections log

Lesson: Impulse

NEET 2025

A ball of mass 0.5 kg is dropped from a height of 40 m. The ball hits the ground and rises to a height of 10 m. The impulse imparted to the ball during its collision with the ground is (Take g = 9.8 m/s2)

184 NS

221 NS

37 NS

NTA Answer: Option 2(final)

Report an error · Every fix is public: corrections log

Lesson: Equilibrium Concurrent Forces

NEET 2025

A uniform rod of mass 20 kg and length 5 m leans against a smooth vertical wall making an angle of 60° with it. The other end rests on a rough horizontal floor. The friction force that the floor exerts on the rod is (Take g = 10 m/s2)

1200 3N

2100 N

3100 3N

4200 N

NTA Answer: Option 3(final)

Report an error · Every fix is public: corrections log

Lesson: Newton 2

NEET 2024Revised key

A horizontal force 10 N is applied to a block A as shown in figure. The mass of blocks A and B are 2 kg and 3 kg respectively. The blocks slide over a frictionless surface. The force exerted by block A on block B is :

1Zero

24 N

36 N

410 N

NTA Answer: Option 3(revised_final)

Report an error · Every fix is public: corrections log

NEET 2024Revised key

A particle moving with uniform speed in a circular path maintains:

1Constant velocity

2Constant acceleration

3Constant velocity but varying acceleration

4Varying velocity and varying acceleration

NTA Answer: Option 4(revised_final)

Report an error · Every fix is public: corrections log

Lesson: Newton 2

NEET 2023

A football player is moving southward and suddenly turns eastward with the same speed to avoid an opponent. The force that acts on the player while turning is

1Along northward

2Along north-east

3Along south-west

4Along eastward

NTA Answer: Option 2(final)

Report an error · Every fix is public: corrections log

Lesson: Static Friction

NEET 2023

Calculate the maximum acceleration of a moving car so that a body lying on the floor of the car remains stationary. The coefficient of static friction between the body and the floor is 0.15 (g = 10 m s⁻²).

1150 m s⁻²

21.5 m s⁻²

350 m s⁻²

41.2 m s⁻²

NTA Answer: Option 2(final)

Report an error · Every fix is public: corrections log

NEET 2022

An electric lift with a maximum load of 2000 kg (lift + passengers) is moving up with a constant speed of 1.5 ms–1. The frictional force opposing the motion is 3000 N. The minimum power delivered by the motor to the lift in watts is : (g = 10 m s⁻²)

123500

223000

320000

434500

NTA Answer: Option 4(final)

Report an error · Every fix is public: corrections log

Lesson: Conservation Linear Momentum

NEET 2022

A shell of mass m is at rest initially. It explodes into three fragments having mass in the ratio 2 : 2 : 1. If the fragments having equal mass fly off along mutually perpendicular directions with speed v, the speed of the third (lighter) fragment is

132v

32v

422v

NTA Answer: Option 4(final)

Report an error · Every fix is public: corrections log

Lesson: Impulse

NEET 2021

A ball of mass 0.15 kg is dropped from a height 10 m, strikes the ground and rebounds to the same height. The magnitude of impulse imparted to the m/s2) ball is (g = 10 nearly

11.4 kg m/s

20 kg m/s

34.2 kg m/s

42.1 kg m/s

NTA Answer: Option 3(final)

Report an error · Every fix is public: corrections log

Lesson: Newton 2

NEET 2020

Two bodies of mass 4 kg and 6 kg are tied to the ends of a massless string. The string passes over a pulley which is frictionless (see figure). The acceleration of the system in terms of acceleration due to gravity (g) is :

1g/10

3g/2

4g/5

NTA Answer: Option 4(final)

Report an error · Every fix is public: corrections log

Exam traps and common mistakes in this unit

Lesson: Conservation Linear Momentum

Trap

Momentum vector vs scalar in explosions

Category: Sign Convention

Student adds magnitudes of momenta of fragments instead of vectors; ignores cancellation when fragments fly perpendicular or in opposite directions.

When it triggers

Question describes a body at rest exploding into multiple fragments with given mass ratios and partial velocity info.

How to avoid

Total momentum is a VECTOR. Initial p = 0; therefore Σ m_i v_i = 0 as a vector equation. Decompose along chosen axes (often natural symmetry axes); sum = 0 in each.

Lesson: Equilibrium Concurrent Forces

Trap

Ladder problem: pivot choice for torque equation

Category: Overthinking

Student takes torque about the centre of mass (introducing all 4 forces with non-zero moment arms) instead of about the floor contact (where 2 forces have zero moment arm and the equation simplifies).

When it triggers

Question gives a uniform rod or ladder leaning against a wall; asks for friction coefficient or limiting condition.

How to avoid

Pick the pivot to ELIMINATE unknown forces from the torque equation. Floor-contact pivot: normal force and friction at floor contribute zero torque; only weight (mid-length) and wall normal (top) appear. Result: μ_min = 1 / (2 tan θ).

Lesson: Equilibrium Concurrent Forces

Trap

Treating Atwood pulley as single mass instead of two F=ma equations

Category: Overthinking

Student tries to apply F=ma to the system as a whole (using net force = (m1-m2)g and total mass m1+m2) but loses track of the tension. The correct approach writes Newton's Second Law SEPARATELY for each mass and treats T as an unknown in two simultaneous equations.

When it triggers

Question contains a frictionless pulley with two unequal masses tied to a string. Asks for tension T or acceleration a (or both).

How to avoid

Draw a free-body diagram for EACH mass. Write F=ma per body, treating T as the same magnitude on both sides of the string. Solve simultaneously: a = (m1 - m2) g / (m1 + m2); T = 2 m1 m2 g / (m1 + m2).

Lesson: Equilibrium Concurrent Forces

Trap

Atwood pulley: T and a sub-formulas

Category: Negative Marking

Multi-mass pulley problem requires computing acceleration first, then tension. T = 2 m1 m2 g/(m1+m2). Sign errors in m1−m2 propagate.

When it triggers

Atwood machine or pulley system with multiple masses.

How to avoid

Compute a = (m1-m2)g/(m1+m2) first with m1 the heavier mass and downward as positive. Then T from F=ma on either mass. Always re-check by plugging back into both Newton's 2nd Law equations.

Lesson: Impulse

Trap

Impulse on bounce: direction reversal in velocity

Category: Sign Convention

Student forgets that velocity DIRECTION reverses on bounce; computes |v₁ - v₂| instead of |v₁ + v₂|.

When it triggers

Question describes ball dropped from height h₁, rebounding to height h₂; asks for impulse on ball.

How to avoid

Impulse J = Δp = m(v_after - v_before). Take down as positive: v_before = +v₁, v_after = -v₂. So J = m(-v₂ - v₁) = -m(v₁ + v₂); magnitude = m(v₁ + v₂).

Lesson: Kinetic Friction

Trap

Incline-with-friction: missing μ cos θ term

Category: Sign Convention

Student writes a = g sin θ for a rough incline (which is the smooth-incline answer); forgets to subtract μ g cos θ.

When it triggers

Question contrasts rough vs smooth inclines, or asks for acceleration on a rough incline.

How to avoid

On a rough incline (block sliding down): a = g(sin θ - μ_k cos θ). On a rough incline (block sliding up): a = -g(sin θ + μ_k cos θ). Smooth case (μ = 0): just g sin θ.

Lesson: Momentum

Trap

Force direction: Δp vs v

Category: Sign Convention

Student picks the direction of MOTION as the direction of the net force, instead of the direction of the change in momentum (Δp). When velocity changes direction at constant speed, the force is perpendicular to BOTH the initial and final velocity vectors (in the limit) — it's the direction of Δv.

When it triggers

Question describes a body changing direction (e.g. turning) and asks for the force direction or the direction of Δp.

How to avoid

F ∝ Δp = m Δv = m (v_f − v_i). Always draw v_i and v_f as vectors and subtract; the result (v_f − v_i) is the direction of net force.

Lesson: Newton 2

Trap

Friction force vs friction-limited acceleration

Category: Unit Conversion

Student computes μmg (friction FORCE in Newtons) when asked for the friction-limited ACCELERATION. The two differ by a factor of m: a = μg, F = μmg.

When it triggers

Question gives μ, g, and a body's mass and asks for the maximum acceleration of the supporting surface OR the friction force on the body.

How to avoid

Read carefully: 'maximum acceleration of the vehicle so the body stays still' = μg (no mass). 'Friction force on the body' = μmg (mass present). Units expose the error: N for force, m/s² for acceleration.

Lesson: Newton 2

Trap

Two-block contact-force confusion

Category: Overthinking

Student applies the full external force F to a single block instead of recognising the system needs to be analysed for the contact (internal) force.

When it triggers

Question gives horizontal force F on block A which pushes block B; asks for contact force between A and B or acceleration.

How to avoid

System acceleration: a = F / (m_A + m_B). Contact force on B from A = m_B × a. The full F acts on the system, not on each block independently.

Lesson: Newton 2

Trap

Lift-power: friction term overlooked

Category: Overthinking

Student computes P = Mgv (just lifting against gravity) and ignores the friction-opposing-motion term.

When it triggers

Question describes a lift moving at constant speed with explicit friction force on cable or guides.

How to avoid

At constant speed, net force = 0, so cable tension T = Mg + f_friction. Power = T × v = (Mg + f) × v. Always add friction when stated.

Unit-wide

Trap

Uniform circular motion: velocity vs speed constancy

Category: Similar Terms

Student claims velocity is constant in uniform circular motion (it's not — direction changes).

When it triggers

Question asks 'in uniform circular motion at constant speed, which is also constant?'

How to avoid

In UCM: SPEED constant; KE constant. VELOCITY (vector) NOT constant. ACCELERATION (centripetal, magnitude v²/r) constant in MAGNITUDE but NOT in direction.

Lesson: Centripetal Force

Mistake

Student adds 'centripetal force' as a separate, additional force on the free-body diagram of a body in circular motion (instead of recognising it as the NET inward radial force already supplied by tension/friction/gravity etc.).

Root cause: concept gap

Correction

Centripetal force is NOT a new fundamental force. It is the NET inward radial component of the real forces (tension, friction, normal, gravity, etc.). On a free-body diagram, draw only the real forces; their net inward component must equal m*v^2/r.

Wrong option pattern

Distractor sums tension + 'centripetal force' as separate inward forces.

Lesson: Conservation Linear Momentum

Mistake

Student applies 'conservation of linear momentum' to a system over a time interval during which a significant external force (gravity, normal reaction with non-zero net) acts.

Root cause: concept gap

Correction

Linear momentum is conserved only when the net EXTERNAL force is zero. Gravity over a finite time changes momentum. For collision problems we use conservation because the collision happens over a brief time interval where external impulses are negligible compared to internal collision forces.

Wrong option pattern

Distractor sets initial momentum = final momentum for a free-fall problem where gravity has acted for several seconds.

Lesson: Equilibrium Concurrent Forces

Mistake

Student identifies the weight of a book and the normal force from the table on the book as a Newton's-third-law action-reaction pair (they are not — both act on the SAME body, the book).

Root cause: concept gap

Correction

Action-reaction pairs ALWAYS act on DIFFERENT bodies. The pair to the book's weight is the gravitational pull the book exerts on the Earth. The pair to the normal force from table on book is the force the book exerts on the table. Equal-and-opposite forces on the SAME body are an equilibrium statement, not third-law statement.

Wrong option pattern

Distractor labels two forces on the same body as a Newton's-third-law pair.

Lesson: Impulse

Mistake

Student equates impulse with force (units N = kgm/s^2 versus impulse Ns = kg*m/s).

Root cause: unit error

Correction

Impulse J has dimensions of momentum (kg*m/s) and equals F*Delta_t. Force has dimensions kg*m/s^2. Confusing them inflates or deflates an answer by a factor of seconds. Always check units before declaring an answer.

Wrong option pattern

Distractor reports an answer in newtons where the correct answer is in N*s (or vice versa).

Lesson: Laws of Friction

Mistake

Student uses f_s = mu_s * N for static friction whenever surfaces are in contact, even when applied tangential force is small. (mu_s * N is the MAXIMUM static friction, not the actual value.)

Root cause: formula misuse

Correction

Static friction is SELF-ADJUSTING: f_s exactly cancels the applied tangential force up to a ceiling f_s_max = mu_s * N. Below the ceiling, f_s = applied force. At the ceiling, motion is impending. Substituting mu_s * N too early over-estimates the friction.

Wrong option pattern

Distractor uses mu_s * N for the static friction force in a no-slip scenario where the applied force is well below threshold.

Formulas in this unit

Lesson: Centripetal Force

Maximum safe speed on a banked road (with friction)

v_\max = \sqrt{\tfrac{gr(\mu_s + \tan\theta)}{1 - \mu_s \tan\theta}}

On a road banked at angle theta from horizontal with tyre-road friction coefficient mu_s, this is the maximum speed for safe negotiation of a curve of radius r.

Symbol	Quantity	SI Unit
v_max	Maximum safe speed	m/s
g	Gravitational acceleration	m/s^2
r	Radius of the curve	m
mu_s	Coefficient of static friction	(dimensionless)
theta	Banking angle	rad/deg

Valid when

Banked turn at angle theta (theta = 0 reduces to level-road formula)
1 - mu_s*tan_theta > 0 (formula breaks down for very steep banks at high friction)
Optimum/no-friction speed v_o = sqrt(g*r*tan_theta) is a SPECIAL CASE

Do NOT use when

Banked angle so steep that 1 - mu_s*tan_theta <= 0 (use centripetal limit form)
Friction direction reversed (very low speed on a steep bank — vehicle slides inward)

Lesson: Centripetal Force

Centripetal force in uniform circular motion

F_{c} = \frac{m v ^{2}}{r} = m ω^{2} r

The net inward force required to keep a body of mass m moving in a circle of radius r at speed v is m*v^2/r. This 'centripetal' force is NOT a new fundamental force — it is whichever real force (tension, friction, gravity, etc.) provides the inward acceleration.

Symbol	Quantity	SI Unit
F_c	Centripetal force	N
m	Mass of the body	kg
v	Tangential speed	m/s
r	Radius of the circle	m
omega	Angular speed	rad/s

Valid when

Speed is uniform (a_t = 0, only radial acceleration matters)
Identify the real force that provides F_c (tension, friction, normal component, etc.)

Lesson: Centripetal Force

Maximum safe speed on a level circular road

v_\max = \sqrt{\mu_s g r}

Static friction is the only force available to provide centripetal acceleration on a level road. Setting mu_s*N = m*v^2/r and N = m*g gives this maximum-safe speed bound.

Symbol	Quantity	SI Unit
v_max	Maximum safe speed (no skid)	m/s
mu_s	Coefficient of static friction (tyre vs road)	(dimensionless)
g	Gravitational acceleration	m/s^2
r	Radius of the circular path	m

Valid when

Road is level (no banking)
Tyres do not slide (static friction regime)
Driver maintains uniform speed on the curve

Do NOT use when

Banked road (use the banked-road formula)
Slippery / wet road where mu_s is reduced

Lesson: Conservation Linear Momentum

Conservation of linear momentum

\sum F_{ext} = 0 \Rightarrow i \sum m_{i} v_{i} = const.

If the net external force on a system of particles is zero, the total linear momentum of the system is conserved (vector equality of total p before and after any internal interaction). Basis of all collision and recoil analysis.

Symbol	Quantity	SI Unit
F_ext	Net external force on system	N
p_total	Sum of m_i*v_i over all particles	kg*m/s

Valid when

Net EXTERNAL force is zero (internal forces always cancel by Newton's 3rd law)
Conservation is vector — apply componentwise (x and y separately)
Holds independent of whether collisions are elastic or inelastic

Do NOT use when

External impulses present (gravity over a long time, friction)

Lesson: Dynamics UCM

Centripetal acceleration in uniform circular motion

a_{c} = \frac{v ^{2}}{r} = ω^{2} r

An object moving in a circle of radius r at constant speed v has acceleration of magnitude v^2/r (or equivalently omega^2 * r) directed toward the centre. This is centripetal (radially inward), not tangential.

Symbol	Quantity	SI Unit
a_c	Centripetal acceleration	m/s^2
v	Tangential speed	m/s
r	Radius of circle	m
omega	Angular speed	rad/s

Valid when

Speed v is constant (uniform circular motion)
r and the centre are well-defined (instantaneous radius of curvature for general curved motion)

Do NOT use when

Non-uniform circular motion (then there is also a tangential acceleration component)

Lesson: Equilibrium Concurrent Forces

Newton's Second Law of Motion

F = m a (or) F = \frac{d p}{d t}

The net external force on a body equals the rate of change of its linear momentum. For a body of constant mass, this reduces to F = m*a — net force equals mass times acceleration. Both F and a are vectors; the acceleration is in the direction of the net force.

Symbol	Quantity	SI Unit
F	Net external (vector) force	N
m	Mass of the body	kg
a	Acceleration (vector)	m/s^2
p	Linear momentum (= m*v)	kg*m/s
t	Time	s

Valid when

F is the resultant (net) of all external forces, not any single force
Mass is constant for the form F = m*a (use F = dp/dt for variable mass)
Inertial reference frame (no pseudo-forces); add inertial corrections in non-inertial frames

Do NOT use when

Frame is non-inertial (need pseudo-forces)
Mass is varying significantly (use F = dp/dt)
Quantum / relativistic regimes (Newtonian mechanics breaks down)

Lesson: Impulse

Impulse of a force

J = F Δ t = Δ p

Impulse equals the product of force and the time interval over which it acts. By Newton's Second Law, impulse equals the change in linear momentum during that interval.

Symbol	Quantity	SI Unit
J	Impulse (vector)	Ns = kgm/s
F	Force (treated as average)	N
Delta_t	Time interval	s
Delta_p	Change in momentum	kg*m/s

Valid when

Useful when forces are large but act briefly (collisions, bat-on-ball, kicks)
Direction of impulse is the direction of average force

Lesson: Kinetic Friction

Kinetic friction

f_{k} = μ_{k} N

When two surfaces slide relative to each other, kinetic friction opposes the motion with magnitude proportional to the normal force.

Symbol	Quantity	SI Unit
f_k	Kinetic friction force	N
mu_k	Coefficient of kinetic friction	(dimensionless)
N	Normal force	N

Valid when

Surfaces ARE sliding
Direction: opposite to instantaneous relative velocity of one surface vs the other

Lesson: Laws of Friction

Maximum static friction

f_{s, m a x} = μ_{s} N

The maximum value of static friction between two surfaces in contact equals the coefficient of static friction times the normal force. Below f_s_max, static friction self-adjusts to whatever value is needed to prevent relative motion.

Symbol	Quantity	SI Unit
f_s_max	Maximum static friction	N
mu_s	Coefficient of static friction	(dimensionless)
N	Normal force	N

Valid when

Surfaces in contact, no relative motion (impending motion limit)
Below f_s_max, actual static friction = applied tangential load (self-adjusting)
f_s_max is independent of the apparent area of contact (Coulomb-Amontons assumption)

Do NOT use when

Surfaces are sliding (use kinetic friction f_k = mu_k * N instead)
Lubricated / fluid-friction conditions

NEET question patterns in this unit

Lesson: Conservation Linear Momentum

A body at rest explodes into 3 fragments; mass ratios given; some fragments' velocities given; find velocity of remaining fragment. Apply vector momentum conservation: Σ m_i v_i = 0 (since initial p = 0). Common shape: 2:2:1 mass ratio, two equal-mass fragments fly perpendicular with given speed; third fragment recoils.

Multi StepMedium

Common distractors

scalar sum of momenta

Treating momentum as scalar; ignores vector cancellation

Lesson: Dynamics UCM

Particle in uniform circular motion at constant speed; identify which of speed / velocity / acceleration / kinetic energy is constant. Speed and KE constant; velocity (vector) and acceleration (centripetal) are NOT constant — direction changes.

InterpretationEasy

Common distractors

treats velocity as scalar

Conflates speed (scalar) with velocity (vector)

Lesson: Equilibrium Concurrent Forces

Uniform rod / ladder of mass M and length L leans against a smooth vertical wall at angle θ; floor is rough with friction coefficient μ. Find limiting condition for static equilibrium. Apply ΣF = 0 (3 equations: horizontal, vertical, torque about base). Wall provides only horizontal reaction (smooth); floor provides normal + friction. μ_min = 1 / (2 tan θ).

Multi StepHard

Common distractors

torque about wrong pivot

Default pivot at center of mass adds complexity

Lesson: Equilibrium Concurrent Forces

Atwood-style pulley with two unequal masses connected by an inextensible massless string over a frictionless pulley. Apply F = ma to each mass separately along the string direction. The tension is the same throughout the string; the magnitudes of acceleration are equal but oriented oppositely. Solve simultaneous equations for tension T and acceleration a. Common shape: given two masses m1, m2 and asked for a or T, with options testing common confusions (g vs a in equations, treating the system as one body).

Multi StepMedium

Common distractors

uses g where a belongs

Forgetting that the system accelerates, so weight is balanced by net force minus T

confuses tension with weight

Treating T = m·g for one of the masses (which is true only when a=0)

Lesson: Impulse

Ball of mass m dropped from height h₁; rebounds to height h₂ (≤ h₁); find impulse on ball from ground. Use v² = 2gh to get speeds at impact and rebound; impulse J = m(v₂ - (-v₁)) = m(v₁ + v₂) where v₁ = √(2g h₁) and v₂ = √(2g h₂). Sign of velocity flips on rebound.

Multi StepEasy

Common distractors

subtracts v2 from v1 instead of adding

Forgetting velocity DIRECTION reversal at bounce

Lesson: Kinetic Friction

Two inclines of equal length L and same angle θ (e.g. 45°); one rough (with μ), one smooth. Compare time-of-descent or final velocity at bottom. Smooth: a = g sin θ. Rough: a = g(sin θ - μ cos θ). Use L = ½ a t² or v² = 2aL.

Multi StepMedium

Common distractors

ignores mu cos theta term

Forgetting the friction-along-incline component

Lesson: Laws of Friction

A body rests on the floor of an accelerating vehicle; find the maximum vehicle acceleration before the body slides. Static friction provides the horizontal force on the body; max accel = μ_s g. Above this, body slides backward relative to the vehicle. Common shape: μ_s, g given; find a_max.

Direct ApplicationEasy

Common distractors

uses mu times g times mass

Confusing force (μ·N = μmg) with acceleration

Lesson: Momentum

A body moving in one direction suddenly changes velocity direction (same or different speed); find the direction of the net force. Force direction = direction of momentum CHANGE (Δp = p_f − p_i), NOT direction of motion. Common shape: 'moving south, suddenly turning east at same speed' → Δp vector points north-east.

InterpretationEasy

Common distractors

force along final velocity

Default to thinking force points in direction of motion

force along initial velocity

Newton-1 misread: object 'wants' to keep moving in original direction

Lesson: Newton 2

Horizontal force F applied to block A (mass m_A); A pushes B (mass m_B) in front. Find acceleration of system AND contact force between A and B. System: a = F/(m_A + m_B); contact force on B from A = m_B × a = m_B F / (m_A + m_B).

Multi StepEasy

Common distractors

treats each block with full F

Forgetting Newton's 3rd law internal force decomposition

Lesson: Newton 2

Lift moving up at constant speed v with total mass M; friction force f opposes motion. Power required from cable = (Mg + f) × v. Common shape: M = 2000 kg, v = 1.5 m/s, f given; find motor power.

Multi StepEasy

Common distractors

forgets friction term

Ignoring opposing force

Questions about this unit

What does Laws of Motion cover for NEET Physics?: 16 lessons: Centripetal Force, Conservation Linear Momentum, Dynamics UCM, Equilibrium Concurrent Forces, Force and Inertia, Impulse, Kinetic Friction, Laws of Friction, Momentum, Newton 1, Newton 2, Newton 3, Rolling Friction, Static Friction, Vehicle Banked Road and Vehicle Level Road.
How often has Laws of Motion come up in NEET past papers?: Our set of verified past papers has 13 questions from this unit, from NEET 2020, 2021, 2022, 2023, 2024, 2025 and 2026. Each is answered against the official NTA key.
Is the Laws of Motion material free?: Yes. All 16 lessons and 128 practice questions are free, with no login needed.