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Chapter 3 · Class 11 Physics

Laws of Motion — Important Questions

34 questions With answers CBSE format

SUMMARY: This chapter focuses on the fundamental principles governing the motion of objects and the forces acting upon them, as formulated by Newton.
KEY TOPICS: Newton's First Law, Newton's Second Law, Newton's Third Law, inertia, momentum, equilibrium of a particle, common forces in mechanics, friction, circular motion, dynamics of uniform circular motion.

Q1 1 Mark

Newton's first law of motion is also known as:

ALaw of acceleration
BLaw of inertia
CLaw of conservation
DLaw of universal gravitation
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Correct answer: Option 2 — Law of inertia
Q2 1 Mark

The SI unit of impulse is:

AN s
BN/s
CN m
Dkg/s
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Correct answer: Option 1 — N s
Q3 1 Mark

Newton's second law gives the formula:

AF = ma
BF = mv
CF = m/a
DF = a/m
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Correct answer: Option 1 — F = ma
Q4 1 Mark

The momentum of an isolated system is:

AAlways increasing
BAlways decreasing
CConserved
DZero
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Correct answer: Option 3 — Conserved
Q5 1 Mark

A body moving in a horizontal circle at constant speed has a force called:

AFrictional force
BCentripetal force
CCentrifugal force
DCoriolis force
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Correct answer: Option 2 — Centripetal force
Q6 3 Marks

State Newton's three laws of motion.

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First law (inertia): a body remains at rest or in uniform motion unless acted upon by an external force. Second law: F = dp/dt = ma — net force equals rate of change of momentum. Third law: for every action there is an equal and opposite reaction.
Q7 3 Marks

Define impulse and write its relation with change in momentum.

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Impulse = force × time of action = F · Δt (for constant force). It equals the change in momentum: F · Δt = Δp = m(v − u). SI unit: N·s = kg·m/s. A large force acting for a short time (e.g. a hammer hit) gives the same impulse as a small force over a long time.
Q8 3 Marks

State the law of conservation of linear momentum.

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In an isolated system (no external force) the total linear momentum is conserved. Σ p_initial = Σ p_final. Follows from Newton's third law: in any internal interaction the equal-and-opposite forces produce equal-and-opposite changes in momentum which cancel.
Q9 3 Marks

A force of 10 N acts on a body of mass 2 kg for 5 s. Find the change in momentum and the resulting velocity if the body started from rest.

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Impulse = F · t = 10 × 5 = 50 N·s. Change in momentum = 50 kg·m/s. Final velocity v: m·v − m·u = 50; with u = 0 m = 2: 2v = 50 ⇒ v = 25 m/s.
Q10 3 Marks

What is friction? Distinguish between static and kinetic friction.

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Friction is the resisting force at the interface between two surfaces in contact. Static friction (f_s ≤ μ_s N) prevents an object from starting to move; can take any value up to μ_s N. Kinetic friction (f_k = μ_k N) acts on an already-moving object; usually μ_k < μ_s. Friction enables walking but causes wear and inefficiency in machines.
Q11 6 Marks

State Newton's second law of motion and derive F = ma from it.

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Newton's second law: the rate of change of momentum is proportional to the net external force and is in the direction of that force. Mathematically: F ∝ dp/dt. Choosing units to make the constant of proportionality equal to 1: F = dp/dt. For a particle of constant mass m: p = mv ⇒ dp/dt = m dv/dt = ma. Therefore F = ma. The general form F = dp/dt is more fundamental — it applies even when mass changes (rocket motion).
Q12 6 Marks

A 2 kg block on a horizontal surface is pulled by a horizontal force of 10 N. The coefficient of friction is 0.2. Find the acceleration of the block. (g = 10 m/s²)

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Normal force N = mg = 2(10) = 20 N. Friction force f = μN = 0.2(20) = 4 N opposing motion. Net force = 10 − 4 = 6 N. Acceleration a = F_net/m = 6/2 = 3 m/s² in the direction of pulling.
Q13 6 Marks

Two bodies of masses m₁ = 5 kg and m₂ = 3 kg connected by a light inextensible string pass over a frictionless pulley (Atwood machine). Find the acceleration of the system and the tension in the string. (g = 10 m/s²)

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Heavier (m₁) descends; lighter (m₂) rises with same acceleration a. For m₁: m₁g − T = m₁a. For m₂: T − m₂g = m₂a. Adding: (m₁ − m₂)g = (m₁ + m₂)a ⇒ a = (m₁ − m₂)g / (m₁ + m₂) = (5 − 3)(10)/8 = 20/8 = 2.5 m/s². Tension: T = m₂(g + a) = 3(10 + 2.5) = 37.5 N. Check with m₁: 5(10 − 2.5) = 37.5 N ✓.
Q14 6 Marks

Derive an expression for the maximum speed at which a vehicle can take a turn on a banked road of radius r and banking angle θ. Friction is absent.

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On a banked road without friction the horizontal component of the normal force provides the centripetal force. Let N = normal force angle θ with vertical. Vertical equilibrium: N cos θ = mg. Horizontal (centripetal): N sin θ = mv²/r. Dividing: tan θ = v²/(rg) ⇒ v² = rg tan θ. Maximum (also called design) speed: v_max = √(rg tan θ). At this speed the vehicle stays on track without needing friction. Faster: needs additional friction inward; slower: needs friction outward to prevent skidding.
Q15 6 Marks

A 50 g bullet moving at 200 m/s strikes a 5 kg block at rest and embeds in it. Find their common velocity after collision.

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Mass of bullet m₁ = 0.05 kg; velocity u₁ = 200 m/s. Mass of block m₂ = 5 kg; u₂ = 0. After collision they move together with velocity v. Conservation of momentum: m₁u₁ + m₂u₂ = (m₁ + m₂)v. 0.05(200) + 0 = 5.05(v). 10 = 5.05 v ⇒ v ≈ 1.98 m/s.
Q16 6 Marks

Compare mass and weight with the help of a table on five points.

Q17 1 Mark

Assertion (A): A body in motion continues in motion unless acted upon by an external force.

Reason (R): This is Newton's first law of motion (law of inertia).

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Correct answer: Option 1 — Both A and R are true, and R is the correct explanation of A.
Q18 1 Mark

Assertion (A): Action and reaction never cancel each other.

Reason (R): Newton's third law forces act on different bodies — to cancel forces they must act on the same body.

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Correct answer: Option 1 — Both A and R are true, and R is the correct explanation of A.
Q19 1 Mark

Assertion (A): The total momentum of an isolated system is conserved.

Reason (R): Internal forces (action-reaction pairs) cancel and external forces are absent in an isolated system.

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Correct answer: Option 1 — Both A and R are true, and R is the correct explanation of A.
Q20 1 Mark

Assertion (A): Static friction is generally greater than kinetic friction.

Reason (R): Once motion starts molecular bonds at the interface break and re-form less effectively — μ_k < μ_s.

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Correct answer: Option 1 — Both A and R are true, and R is the correct explanation of A.
Q21 1 Mark

Assertion (A): A long follow-through reduces the force needed to change momentum by a given amount.

Reason (R): Impulse = F × Δt; for the same change in momentum a longer Δt needs a smaller F.

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Correct answer: Option 1 — Both A and R are true, and R is the correct explanation of A.
Q22 1 Mark

Statement 1: Mass is a measure of inertia.

Statement 2: A body with greater mass is harder to accelerate.

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Correct answer: Option 1 — Both statements are true.
Q23 1 Mark

Statement 1: The SI unit of force is the newton.

Statement 2: 1 N is the force needed to give a 1 kg mass an acceleration of 1 m/s².

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Correct answer: Option 1 — Both statements are true.
Q24 1 Mark

Statement 1: Action and reaction forces are equal in magnitude and opposite in direction.

Statement 2: Action and reaction forces act on different bodies.

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Correct answer: Option 1 — Both statements are true.
Q25 1 Mark

Statement 1: Friction depends on the nature of surfaces in contact.

Statement 2: Friction does not depend significantly on the area of contact.

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Correct answer: Option 1 — Both statements are true.
Q26 1 Mark

Statement 1: A body in uniform circular motion has a centripetal force directed toward the centre.

Statement 2: The centripetal force is the net force in the radial direction.

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Correct answer: Option 1 — Both statements are true.
Q27 3 Marks
A passenger sitting on a chair in a moving bus suddenly leans forward when the bus brakes. The driver wonders why this happens — was the passenger pushed forward by some force or does the explanation lie in Newton's first law of motion?
  1. The passenger leans forward due to:
    AA backward force
    BInertia of rest
    CInertia of motion
    DFriction
  2. The phenomenon is best explained by:
    ANewton's first law
    BNewton's second law
    CNewton's third law
    DLaw of conservation
  3. Why is wearing a seat belt important during sudden braking?
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1. Option 3 — Inertia of motion
2. Option 1 — Newton's first law
3. Newton's first law (law of inertia): a body in motion continues in motion with the same velocity unless acted on by an external force. The passenger was moving forward with the bus. When the bus brakes (decelerates) the passenger's body — having no external retarding force on it — tries to continue forward. This is inertia of motion. Seat belts apply the necessary backward force to keep the passenger from continuing forward into the windshield.
Q28 3 Marks
A rocket of total mass 1000 kg burns fuel at the rate of 5 kg/s expelling exhaust gases at 2000 m/s relative to the rocket. The mission engineer wants to determine the thrust force the initial acceleration and to verify that the principle is Newton's third law in action.
  1. The thrust on the rocket is:
    A5000 N
    B10000 N
    C20000 N
    D400000 N
  2. The principle behind rocket propulsion is:
    ANewton's first law
    BNewton's second law
    CNewton's third law
    DConservation of mass
  3. Why does the rocket's acceleration increase as fuel burns?
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1. Option 2 — 10000 N
2. Option 3 — Newton's third law
3. Thrust F = (dm/dt) × v_exhaust = 5 × 2000 = 10000 N. Initial acceleration (assuming weight is negligible compared to thrust for now): a = F/M = 10000/1000 = 10 m/s². Including gravity: a_net = (F − Mg)/M = (10000 − 9800)/1000 = 0.2 m/s² (just barely lifting off). As fuel burns M decreases so a increases. Newton's third law: rocket pushes gases backward gases push rocket forward — equal and opposite forces.
Q29 3 Marks
In an Atwood machine two masses m₁ = 6 kg and m₂ = 4 kg are connected by a light inextensible string passing over a frictionless pulley. The student wants to compute the acceleration of the system the tension in the string and to identify which mass moves up. Use g = 10 m/s².
  1. The acceleration of the system equals:
    A1 m/s²
    B2 m/s²
    C4 m/s²
    D5 m/s²
  2. The tension in the string equals:
    A40 N
    B48 N
    C60 N
    D72 N
  3. If both masses were equal what would the acceleration be?
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1. Option 2 — 2 m/s²
2. Option 2 — 48 N
3. For Atwood machine with m₁ > m₂: heavier descends and lighter rises with common acceleration a. From Newton's 2nd law: m₁g − T = m₁a (descending) and T − m₂g = m₂a (ascending). Adding: (m₁ − m₂)g = (m₁ + m₂)a ⇒ a = (6 − 4)(10)/10 = 2 m/s². Tension: T = m₂(g + a) = 4(12) = 48 N. Verification: m₁(g − a) = 6 × 8 = 48 N ✓.
Q30 3 Marks

Study Newton's three laws of motion:

LawStatement
1st (Inertia)A body remains at rest or in uniform motion unless acted on by a net external force.
2ndF = dp/dt = ma — net force produces acceleration in its direction.
3rdFor every action there is an equal and opposite reaction.
  1. The law of inertia is:
    A1st
    B2nd
    C3rd
    DAll three
  2. The 2nd law gives the formula:
    AF = ma
    BAction-reaction
    CConservation of momentum
    DBanking
  3. Give one practical example of each of Newton's three laws.
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1. Option 1 — 1st
2. Option 1 — F = ma
3. Newton's three laws underpin all of classical mechanics. 1st law defines a force as something that changes state of motion (introduces inertia). 2nd law quantifies the effect of force as proportional to rate of change of momentum. 3rd law states that forces always act in pairs — explains rocket propulsion walking and recoil. Together they predict motion in all situations from atomic scale to planetary scale.
Q31 3 Marks

Study the friction coefficients on different surfaces:

Surface pairμ_s (static)μ_k (kinetic)
Glass on glass0.940.40
Steel on steel0.740.57
Rubber on dry concrete1.00.8
Rubber on wet concrete0.70.5
Teflon on Teflon0.040.04
  1. Which surface gives the maximum static friction coefficient?
    AGlass on glass
    BSteel on steel
    CRubber on dry concrete
    DTeflon on Teflon
  2. Generally:
    Aμ_s > μ_k
    Bμ_s < μ_k
    Cμ_s = μ_k
    DCannot decide
  3. Why is the kinetic friction coefficient generally less than the static one?
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1. Option 3 — Rubber on dry concrete
2. Option 1 — μ_s > μ_k
3. Static friction (μ_s) is generally greater than kinetic friction (μ_k) — once an object starts moving the molecular bonds at the interface break and reform less effectively making it easier to keep moving than to start. Rubber-on-dry-concrete has very high μ — explains why car tyres grip well (and why wet roads are dangerous). Teflon famously has very low μ — used in non-stick cookware and bearings.
Q32 6 Marks

Two masses 4 kg and 6 kg are connected by a string over a frictionless pulley (Atwood machine). Compute (i) the acceleration of the system, (ii) the tension in the string. (g = 10 m/s²)

MassValue (kg)
m₁ (heavier)6
m₂ (lighter)4
Q33 6 Marks

A 5 kg block on a horizontal surface is pulled by a horizontal force of 25 N. The coefficient of kinetic friction between block and surface is μ_k = 0.2. Compute (i) the friction force, (ii) the net force, (iii) the acceleration. (g = 10 m/s²)

QuantityValue
Mass5 kg
Applied force25 N
μ_k0.2
g10 m/s²
Q34 3 Marks

Study the free body diagram of a block on an inclined plane and answer:

Laws of Motion figure
  1. The component of weight perpendicular to the incline (= normal force N) is:
    Amg sin θ
    Bmg cos θ
    Cmg tan θ
    Dmg
  2. The block remains stationary on the incline if:
    Aμ_s ≥ tan θ
    Bμ_s ≤ tan θ
    Cμ_s = sin θ
    Dμ_s = cos θ
  3. Explain when the block remains in equilibrium on the incline.
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1. Option 2 — mg cos θ
2. Option 1 — μ_s ≥ tan θ
3. Resolve weight W = mg into two components: along the incline (downward, mg sin θ) and perpendicular to the incline (mg cos θ). Normal force balances perpendicular component: N = mg cos θ. Maximum static friction available: f_s,max = μ_s N = μ_s mg cos θ. The block is on the verge of sliding when f_s,max = mg sin θ ⇒ μ_s = tan θ. So if μ_s ≥ tan θ the block is stationary; if μ_s < tan θ it slides down with acceleration a = g(sin θ − μ_k cos θ).

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