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Introduction

NEET > Physics > Laws of Motion > Friction > Introduction

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NEET Physics — Friction

Introduction to Friction – Complete Notes, Revision, Important Questions & Downloads

Introduction to Friction begins with the Friction Force Definition — friction is the force that opposes the relative motion or tendency of motion between two surfaces in contact, acts parallel to the surface and opposite to intended motion, and arises from microscopic bonding at the contact interface. This defintion underpins all three types of friction covered here. NEET tests: (1) identifying the correct type of friction in a given situation — static friction (self-adjusting, f = P as long as no motion), limiting friction (maximum static friction, f_l = μ_s N at the point of motion), and kinetic friction (f_k = μ_k N once motion begins); (2) applying the laws of limiting and kinetic friction: friction force is proportional to normal reaction N, depends on surface materials (μ), and is INDEPENDENT of apparent contact area and velocity; (3) the inequality μ_k < μ_s — kinetic friction coefficient is always less than static friction coefficient — explaining why more force is needed to start motion than to sustain it. Mastery of the Friction Force Definition and these distinctions with the two friction laws (f = μN for limiting and kinetic cases) forms the complete foundation of the Friction chapter for NEET.

⬇ Download Notes PDFView Important Questions →
Static, Limiting, and Kinetic FrictionFriction Ch.5f = μN
Expected QuestionsQ
1–2
Friction is a high-yield NEET topic. The Introduction establishes all foundational laws tested across the entire chapter. NEET regularly tests: identifying the type of friction in a scenario; applying f = μN; the fact that friction is independent of contact area; the μ_k < μ_s inequality; and 'self-adjusting' static friction. Friction as a chapter contributes 1–3 questions in most NEET papers.
Time Required⏱
40 min
15 min to master the three friction types (static, limiting, kinetic) with clear examples and the self-adjusting nature of static friction. 10 min for the two friction laws: f_l = μ_s N and f_k = μ_k N, the properties of μ, and what μ does/doesn't depend on. 15 min for NEET practice MCQs on all three types, applied force vs friction force graphs, and the μ_k < μ_s inequality.
Difficulty⚡
Easy
The Introduction to Friction is conceptually clear — three types, two laws, and a few key properties (contact area independence, velocity independence of kinetic friction). NEET tests this material at a direct application level. The main errors are confusing static vs limiting vs kinetic friction, and forgetting that static friction is self-adjusting (equals applied force until it reaches the limiting value).
NRI USA Curriculum GapUS
Low
AP Physics 1 covers static and kinetic friction extensively at a similar level. The distinction between static friction (self-adjusting) and kinetic friction (constant μ_k N) is well-covered in US high school physics. The term 'limiting friction' is specific to Indian physics education — US courses call it 'maximum static friction'. The physics is identical; only the terminology differs slightly.
1Subtopics
4+Practice Questions
4Free Downloads
40 minPrep Time
⬇ Get Free Downloads

NEET Weightage — Introduction to Friction

Friction (Chapter 5)
NEET YearQuestions from this TopicBarMarks
20241
 
1 Q
4
20232
 
2 Q
8
20221
 
1 Q
4
20212
 
2 Q
8
20201
 
1 Q
4
20191
 
1 Q
4
6-Year Total (2019–2024)6–9 24–36
Static friction is self-adjusting: f_s = P (applied force) as long as P ≤ f_l (limiting friction). It adjusts to exactly oppose the tendency of motion. If no force is applied: f_s = 0. Static friction increases with P up to the maximum value f_l = μ_s N.
Limiting friction f_l = μ_s N: the maximum value of static friction. Once P exceeds f_l, the object starts moving. The body is at the 'verge of motion' (impending motion) when P = f_l. For a horizontal surface: N = mg (normal reaction equals weight for horizontal surface with no vertical applied force).

Kinetic friction f_k = μ_k N (once in motion): constant magnitude regardless of velocity. Important properties: (a) independent of velocity of motion; (b) independent of apparent area of contact; (c) depends on μ_k (material and surface condition); (d) always LESS than limiting friction: μ_k < μ_s. Typical values: μ_s (wood on wood) ≈ 0.3–0.5; μ_s (rubber on concrete) ≈ 0.6–0.8; μ_s (steel on steel, dry) ≈ 0.6–0.7.
📊
1.3
Avg Questions / Year
🎯
32
Total Marks (6 yrs)
📈
Direct
Pattern
⚠️
Easy
Difficulty

How to Prepare Introduction to Friction for NEET

1

Know the three friction types and their exact conditions Static friction: acts when body is at REST but a force is applied. Self-adjusting: f_s = P (where P = applied force), increases with P, until P = f_l = μ_s N (limiting value). At P > f_l: body starts moving. Kinetic friction: acts when body is IN MOTION. Constant at f_k = μ_k N (independent of velocity and area). Limiting friction: the boundary case, maximum static friction, at impending motion. NEET distinguisher: if the question says 'body is on the verge of moving' or 'just about to slip' → use f_l = μ_s N. If 'body is moving at constant velocity' → use f_k = μ_k N. If 'body is at rest with some force applied' and no 'verge of motion' → f_s = P (not μ_s N).

2

Memorise the laws of friction and what they DON'T depend on Laws of friction: (1) f ∝ N (friction proportional to normal reaction); (2) f = μN (limiting and kinetic cases); (3) friction is INDEPENDENT of apparent area of contact (famously counter-intuitive — a wider tire doesn't have more friction than a narrow tire on the same road, kinetically); (4) kinetic friction is INDEPENDENT of velocity. NEET loves testing the 'friction is independent of area' as a True/False or MCQ option. The μ_k < μ_s inequality is also frequently tested — 'coefficient of static friction is always greater than coefficient of kinetic friction'.

3

Draw the applied force vs friction force graph The f_friction vs P_applied graph is the pre-eminent NEET figure for friction: (1) from P = 0 to P = f_l: the static friction region — a straight line at 45° since f_s = P (friction = applied force); (2) at P = f_l: the peak — limiting friction, highest point on the graph; (3) at P > f_l: body is in motion — friction drops suddenly to f_k = μ_k N (a lower, constant value); (4) the graph remains at f_k for all higher values of P. The sudden drop at P = f_l is the key visual: kinetic < limiting confirms μ_k < μ_s. NEET frequently tests 'which point represents limiting friction?' on this graph.

Study Materials — Introduction to Friction

PDF · Cheat Sheet · MCQ Set · PYQ
📘
Full Notes
Friction definition (force opposing relative motion/tendency of motion). Three types: static (self-adjusting), limiting (maximum static), kinetic (constant while moving). Laws: f = μN; independence from area and velocity; μ_k < μ_s. Applied force vs friction graph. Derivation of F from Newton's laws.
Single topic2 pagesLaws + Properties
Download Notes
📗
Formula Sheet
f_s ≤ μ_s N (static, self-adjusting up to max); f_l = μ_s N (limiting); f_k = μ_k N (kinetic); μ_k < μ_s; f independent of contact area and velocity. All formulas with units and dimensions: μ is dimensionless.
5 formulas1 pageQuick reference
Download Sheet
📙
MCQ Practice
10 MCQs: identify friction type, calculate friction from μ and N, applied-force-vs-friction graph interpretation, area/velocity independence, μ_k vs μ_s comparison.
10 MCQsAll variantsSolved
Download MCQs
📒
PYQ
Year-tagged NEET questions on friction definitions, laws of friction, graph interpretation, and friction type identification.
4+ year-tagged Qs2015–2024Solved
Download PYQs

2-Column Table
Column AColumn B
Friction Force Definition↗

Rapid Revision — Introduction to Friction

Concept → Trap → Example

1) Friction Force Definition — What is Friction and How Does It Arise?

Friction Force Definition

Friction is the force that opposes the relative motion or tendency of motion between two surfaces in contact. When a body slides or attempts to slide over a surface, the contact between the surfaces involves microscopic interlocking of irregularities (asperities) and adhesive bonding between atoms at the interface. This bonding resists relative motion. The net effect of all these microscopic contact forces is represented as a single macroscopic force — the friction force — acting parallel to the surface and opposite to the direction of intended motion (or actual motion). Friction is a contact force; it can only exist where two surfaces are in contact. Friction is NOT a fundamental force — it arises from electromagnetic (intermolecular) bonding at the contact surface.

  • The force of friction is PARALLEL to the surface and OPPOSITE to the direction of intended or actual motion. Note 'intended' — static friction opposes the TENDENCY of motion, not actual motion (since the body is still at rest). Kinetic friction opposes ACTUAL motion velocity direction. NEET trap: if the block is on a surface and no force is applied, friction = 0 (no tendency of motion, nothing to oppose). Friction doesn't spontaneously appear — it requires an applied force or a tendency of relative motion.
  • Molecular origin: surfaces that appear smooth are microscopically rough. At the atomic scale, contact points (asperities) weld together due to adhesive forces. When one surface tries to slide over the other, these welds must be broken. The force required to break them is the friction force. On polished surfaces: fewer and smaller contact asperities → lower friction. On rough surfaces: more and larger contact asperities → higher friction. The coefficient μ quantifies the extent of surface bonding and interlocking.
  • Friction is NOT always undesirable: (a) Walking requires friction — without friction, feet would slip back instead of pushing the body forward. The forward motion of walking depends entirely on static friction between foot and ground. (b) Tyres grip the road via friction. (c) Writing on paper requires friction between pen/pencil and paper. (d) Brakes work via kinetic friction. Friction is undesirable in machines (energy loss, heat generation) but essential for locomotion, gripping, and many mechanical operations.
Example (NEET-style)A book rests on a table. No force is applied. What is the friction on the book? ZERO. Friction is zero because there is no applied force and no tendency of motion. Now, 2 N is applied horizontally. The book remains at rest. Friction force = 2 N (static, equals applied force). Now, 5 N is applied. Still at rest. Friction = 5 N. Now, 8 N applied, and the book just starts to move. Limiting friction = 8 N = μ_s × N = μ_s × mg. After the book starts moving at 10 N: kinetic friction = μ_k × N = 6 N (assuming μ_k < μ_s gives 6 N < 8 N). The sequence 0 → 2 → 5 → 8 (limiting) → 6 (kinetic) demonstrates all three friction regimes.

2) Three Types of Friction: Static, Limiting, Kinetic

High Priority

Three distinct regimes of friction: (1) STATIC FRICTION (f_s): when the body is at REST but a force P is applied. The body remains at rest because static friction exactly matches P. f_s = P (self-adjusting). Range: 0 ≤ f_s ≤ f_l (maximum static = limiting). (2) LIMITING FRICTION (f_l): the MAXIMUM value of static friction, reached when the body is just about to move (impending motion). f_l = μ_s × N, where μ_s is the coefficient of static friction. The body transitions from rest to motion at P = f_l. (3) KINETIC FRICTION (f_k): the friction once the body IS MOVING. f_k = μ_k × N, where μ_k is the coefficient of kinetic friction. f_k < f_l always (μ_k < μ_s). Kinetic friction is constant — independent of velocity and contact area.

  • Self-adjusting nature of static friction makes it unique: (a) If P = 0: f_s = 0 (no applied force, no friction). (b) If P = 3 N and the body stays at rest: f_s = 3 N. (c) If P = 7 N and just at the brink of motion: f_s = f_l = 7 N = μ_s N. The static friction adjusts itself to EXACTLY cancel the applied force component — it is 'lazy' but infinitely responsive within 0 to f_l. This is different from kinetic friction which is a fixed value f_k = μ_k N regardless of the applied force (as long as there is motion).
  • μ_k < μ_s: why? Once motion starts, the contact asperities have less time to form adhesive bonds (there's relative sliding motion between the surfaces) — the bonds are constantly being broken faster than new ones form. Thus the resistance (kinetic friction) is less than the maximum static resistance (limiting friction) where the bonds were fully formed and steady. Qualitatively: it is harder to 'initiate' (start) sliding than to 'maintain' sliding. This is why it takes a strong push to start a heavy furniture sliding, but it moves more easily once going.
  • Friction on the applied force vs friction graph: The f_s vs P graph is a 45° straight line (f_s = P) from origin to the peak at P = f_l. At the peak: P = f_l = μ_s N. For P > f_l: the body moves; friction drops to f_k = μ_k N (a constant, lower value). The graph shows a linear rise, a peak (limiting friction), then a sudden drop to a constant value (kinetic friction). This graph is one of the most frequently tested NEET figures in the friction chapter. Key points: maximum is limiting friction; constant lower value is kinetic; slope of rising portion = 1 (f_s = P).
Example (NEET-style)A block of mass 5 kg on a horizontal surface. μ_s = 0.4, μ_k = 0.3, g = 10 m/s². Normal N = mg = 50 N. Limiting friction f_l = μ_s N = 0.4 × 50 = 20 N. Kinetic friction f_k = μ_k N = 0.3 × 50 = 15 N. Case A: P = 10 N applied. Body at rest (P < f_l = 20 N). Static friction f_s = 10 N (equals applied force). Net force = 0. Case B: P = 20 N applied. Body at verge of motion. f_s = f_l = 20 N. Net force = 0. Case C: P = 25 N applied. Body in motion. Kinetic friction f_k = 15 N. Net force = P − f_k = 25 − 15 = 10 N. Acceleration = 10/5 = 2 m/s². Note: as soon as P > 20 N, friction drops to 15 N (from 20 N to 15 N at the moment motion starts).

3) Laws of Friction and Properties of μ

Laws & Properties

Laws of Friction (empirical, not derived from first principles): (1) The friction force is directly proportional to the normal reaction force N: f = μN. (2) The friction force is independent of the apparent area of contact between the surfaces. (3) Static friction is self-adjusting (0 ≤ f_s ≤ μ_s N). (4) Kinetic friction is independent of the velocity of the sliding body. (5) Kinetic friction < Limiting friction: μ_k < μ_s. These are the 'Laws of Limiting Friction' and 'Laws of Kinetic Friction'. The coefficient μ (dimensionless, no units, dimensions M⁰L⁰T⁰) depends on: the materials of the two surfaces; the surface conditions (wet, dry, polished, rough). μ does NOT depend on: velocity, contact area, mass of the object.

  • Why friction is independent of contact area (Law 2)? Intuitive puzzle: a wider tire and narrower tire on the same road — kinetic friction is the same? YES. Explanation: when contact area increases, the pressure (force/area) at each contact point decreases proportionally. The total friction = (friction per contact point) × (number of contact points). More contact area → more contact points BUT less pressure per point → less friction per point. These effects cancel exactly: total friction = μN regardless of area. This is why a flat tire and an inflated tire have the same traction (kinetically). NEET loves this as a conceptual option.
  • Why kinetic friction is independent of velocity (Law 4)? Over the range of typical velocities in mechanics problems (not molecular scale velocities), the bonding and breaking mechanism of asperities doesn't change significantly with sliding speed. The kinetic friction coefficient μ_k remains approximately constant. Note: at very high velocities, heat generation softens surfaces and can change μ_k (brake fade). At atomic/quantum velocities, different models apply. For NEET: kinetic friction is velocity-independent over all tested speed ranges.
  • Dimensions and units of μ: μ = f/N = (force)/(force) = dimensionless. Unit: none. Dimension: [M⁰L⁰T⁰]. μ can technically be > 1 (e.g., rubber on rubber μ_s can be > 1). μ = 0 means perfectly frictionless (ice → 0.01–0.05; well-oiled surfaces → 0.05–0.1). Typical NEET values: μ_s (wood on wood, dry) = 0.25–0.5 (use 0.4 if not given); μ_s (rubber on concrete) = 0.6–0.8; μ_k is always 20–30% lower than μ_s for the same pair.
Example (NEET-style)A block of mass 10 kg has μ_s = 0.5 and μ_k = 0.4. (g = 10 m/s²). N = 100 N. f_l = 0.5×100 = 50 N (maximum static). f_k = 0.4×100 = 40 N (kinetic). Question: 'If the contact area is halved (same mass, same surfaces), what is the new limiting friction?' Answer: SAME, 50 N. Friction is independent of contact area (f = μN; N = mg = 100 N unchanged; f_l = 50 N unchanged). NEET answer: friction does not depend on contact area — only μ and N matter. Question: 'If the block slides at 2 m/s vs 4 m/s, is kinetic friction different?' Answer: NO — f_k = 40 N at both speeds. Kinetic friction is velocity-independent.

US Curriculum Gaps — Introduction to Friction

Topics in this section are tested in NEET but organised differently in standard US physics courses.

Term 'Limiting Friction' vs 'Maximum Static Friction' (Terminology Gap)

NEET uses the term 'limiting friction' for the maximum value of static friction, achieved at the onset of motion. US physics (AP Physics 1, university physics) calls this 'maximum static friction' (f_s,max = μ_s N). The concept is identical; only the terminology differs. US students may not recognise 'limiting friction' as a term, but the physics is the same. NEET also formally lists three types (static, limiting, kinetic) while US courses typically mention only two (static, kinetic) with the maximum static friction as a property of static friction rather than a third named type.

  • NEET: three named types — static, limiting, kinetic (limiting = maximum static friction)
  • AP Physics 1: two types — static and kinetic; maximum static friction = μ_s N at boundary
  • Physics is identical; NEET terminology 'limiting friction' = US terminology 'maximum static friction'

Self-Adjusting Nature of Static Friction (Conceptual Emphasis Gap)

While AP Physics 1 does cover static friction, the NEET curriculum places special emphasis on the 'self-adjusting' property of static friction — that f_s = P (equals the applied force) and varies from 0 to f_l. NEET explicitly tests whether students understand that static friction = 0 when no force is applied, and increases proportionally with P up to μ_s N. AP Physics 1 teaches the same concept but may not frame it as explicitly as 'static friction is self-adjusting'. The friction force vs applied force graph (showing the 45° line, the peak, and the drop to kinetic) is a standard NEET figure that may be less prominent in AP Physics 1 instruction.

  • NEET: static friction is explicitly 'self-adjusting' — f_s = P from 0 to f_l = μ_s N
  • NEET: friction vs applied force graph (45° rise, peak at f_l, drop to f_k) is frequently tested
  • AP Physics 1: same physics taught but less emphasis on the self-adjusting language and the comparative graph

NEET-Style Practice Questions — Introduction to Friction

4 Questions
1A block of mass 10 kg is placed on a horizontal surface. The coefficient of static friction is 0.4 and kinetic friction is 0.3. A horizontal force of 30 N is applied. What is the friction force on the block? (g = 10 m/s²)Static vs Kinetic
30 N
40 N
30 N (static)
30 N (kinetic)
Normal N = mg = 10×10 = 100 N. Limiting friction f_l = μ_s × N = 0.4×100 = 40 N. Applied force P = 30 N < f_l = 40 N. The block DOES NOT MOVE (P < f_l). Therefore friction is STATIC and self-adjusting: f_s = P = 30 N. Static friction exactly cancels the applied force. The friction is 30 N (static), NOT 40 N (that would be limiting — the block is not yet at the verge of motion). Common mistake: applying f = μN here gives 40 N — but μN gives limiting friction, not the actual static friction when P < f_l.
2Which of the following is NOT a property of kinetic friction?Properties of Kinetic Friction
It depends on the velocity of the sliding body
It depends on the nature of the surfaces in contact
It depends on the normal reaction
It is less than limiting friction
Kinetic friction f_k = μ_k N. Properties: (a) depends on μ_k (material/surface nature) ✓; (b) proportional to normal reaction N ✓; (c) INDEPENDENT of velocity (i.e., 'kinetic friction depends on velocity' is FALSE ✓ — this is the NOT property); (d) f_k < f_l always ✓. The correct answer is Option A: 'depends on velocity' is NOT a property of kinetic friction. Kinetic friction is velocity-independent over the entire range of practical velocities tested in NEET.
3The ratio of limiting friction to normal reaction is:Coefficient of Friction
Coefficient of kinetic friction
Coefficient of static friction
Coefficient of rolling friction
Angle of friction
By definition: coefficient of static friction μ_s = f_l / N = (limiting friction) / (normal reaction). This is the ratio of the MAXIMUM static friction (limiting friction f_l) to the normal reaction N. Note: μ_k = f_k/N (coefficient of kinetic friction = kinetic friction / normal reaction). μ_s ≠ μ_k in general (μ_k < μ_s). The ratio of limiting friction to N is specifically μ_s (static friction coefficient), not kinetic.
4The graph of friction force vs applied force for a body initially at rest on a horizontal surface shows:Friction Graph
A straight horizontal line throughout
A linear increase (slope = 1) until limiting friction, then a constant lower value
A linear increase until kinetic friction, then constant
A constant value equal to μ_s N throughout
The friction vs applied force graph has three regions: (1) From P = 0 to P = f_l: friction is static and self-adjusting → f = P (straight line, slope = 1 at 45°). (2) At P = f_l = μ_s N: peak of the graph — this is LIMITING friction. (3) For P > f_l: body is in motion; friction = f_k = μ_k N (constant, lower than f_l — because μ_k < μ_s). The graph rises linearly, peaks at f_l, then drops to the constant f_k level. Option B correctly describes this: 'Linear increase (slope = 1) until limiting friction, then a constant lower value.' The drop at P = f_l represents the transition from static to kinetic friction ← most commonly tested feature.

Practice Problems — Introduction to Friction

Click "Reveal Answer" after attempting
1A 5 kg block rests on a horizontal surface with μ_s = 0.5 and μ_k = 0.35. (g = 10 m/s²). Find: (a) the minimum force needed to start the block moving; (b) if the force in (a) is maintained, what is the block's acceleration?
(a) 25 N; (b) 3 m/s²
(a) 17.5 N; (b) 0 m/s²
(a) 25 N; (b) 1.5 m/s²
(a) 17.5 N; (b) 1.5 m/s²
👁 Reveal Answer
(a) The minimum force to start moving = limiting friction = f_l = μ_s N = μ_s mg = 0.5×5×10 = 25 N. (b) Once motion starts with P = 25 N, kinetic friction applies: f_k = μ_k mg = 0.35×5×10 = 17.5 N. Net force = P − f_k = 25 − 17.5 = 7.5 N. Acceleration a = F_net/m = 7.5/5 = 1.5 m/s². Note: at the instant motion starts (P = 25 N just overcomes f_l = 25 N), friction drops from 25 N to 17.5 N — a net force of 7.5 N accelerates the block at 1.5 m/s².
2A 10 kg block on a horizontal surface (μ_s = 0.4, μ_k = 0.3) is pushed by a 45 N horizontal force. (g = 10 m/s²). (a) Does the block move? (b) If yes, find acceleration. (c) What would be the minimum μ_s such that the block does NOT move under 45 N?
(a) Yes; (b) 1.5 m/s²; (c) μ_s = 0.45
(a) No; (b) N/A; (c) μ_s = 0.45
(a) Yes; (b) 1.5 m/s²; (c) μ_s = 0.5
(a) Yes; (b) 3 m/s²; (c) μ_s = 0.45
👁 Reveal Answer
(a) N = mg = 100 N. f_l = μ_s N = 0.4×100 = 40 N. Applied force = 45 N > 40 N = f_l. YES, the block moves. (b) f_k = μ_k N = 0.3×100 = 30 N. Net force = 45 − 30 = 15 N. a = 15/10 = 1.5 m/s². (c) For block NOT to move: f_l ≥ P → μ_s N ≥ 45 → μ_s ≥ 45/100 = 0.45. Minimum μ_s = 0.45 to keep the block stationary under 45 N. Answers: (a) Yes, (b) 1.5 m/s², (c) μ_s = 0.45.
3A horizontal force of 15 N is applied to a 4 kg block on a horizontal surface (μ_s = 0.5, μ_k = 0.4, g = 10 m/s²). Find the friction force and state of motion of the block.
f = 20 N (limiting); block on verge of motion
f = 15 N (static); block at rest
f = 16 N (kinetic); block moving
f = 20 N (kinetic); block moving
👁 Reveal Answer
N = mg = 4×10 = 40 N. f_l = μ_s N = 0.5×40 = 20 N. Applied P = 15 N < f_l = 20 N. Block does NOT move. Static friction (self-adjusting) f_s = P = 15 N. State: block at rest; friction = 15 N (static). Not on verge of motion (that would require P = 20 N). Not kinetic (block not moving). The friction is LESS than μ_s N = 20 N because the applied force is less than the limiting value.
4The coefficient of static friction between two surfaces is 0.6 and kinetic friction is 0.4. A 2 kg block is on a horizontal surface. A horizontal force is gradually increased from zero. At what force does the block start to slide, and what is the friction when P = 18 N (after sliding)? (g = 10 m/s²)
Starts at 12 N; kinetic friction after = 8 N
Starts at 8 N; kinetic friction after = 8 N
Starts at 12 N; kinetic friction after = 12 N
Starts at 8 N; kinetic friction after = 12 N
👁 Reveal Answer
N = mg = 2×10 = 20 N. Limiting friction f_l = μ_s N = 0.6×20 = 12 N. Block starts sliding when P = 12 N. When P = 18 N (block is sliding): kinetic friction f_k = μ_k N = 0.4×20 = 8 N. Net force = 18 − 8 = 10 N. Acceleration = 10/2 = 5 m/s². Answers: starts at P = 12 N; kinetic friction after sliding = 8 N. Note: f_k = 8 N is constant regardless of whether P = 12 N or P = 18 N or P = 50 N (as long as the block is moving, f_k = μ_k N = 8 N always).

Physics — Friction Revision Checklist

Check off chapters as you revise

Use this section for quick chapter tracking before mocks, part tests, and final NEET revision.

Tip: Mark a chapter complete only after revising formulas, solving PYQs, and reviewing your error log for that chapter.

FAQ — Introduction to Friction

Notes · Downloads · Revision · Important Questions
What is the difference between static friction, limiting friction, and kinetic friction?
Static friction is the friction force when the body is AT REST with an applied force (but not yet moving). It is self-adjusting: f_s = P (equals the applied force) up to a maximum. Limiting friction is the MAXIMUM value of static friction — the value at which the body is on the verge of moving. Formula: f_l = μ_s N. This is the 'threshold' — once P > f_l, the body starts moving. Kinetic friction (also called dynamic friction) is the friction force when the body IS MOVING. Formula: f_k = μ_k N. It is constant (independent of velocity and P). Relationship: f_k < f_l (μ_k < μ_s). Summary: static (adjusting, body at rest) → limiting (maximum static, at onset) → kinetic (constant, while moving).
Why does friction decrease when the body starts moving?
When the body is at rest (static regime), microscopic adhesive welds form at the contact asperities. To START moving, all these welds must be broken simultaneously — this requires maximum force f_l = μ_s N. Once motion begins, the surfaces slide relative to each other. The asperities no longer have time to completely rebond — they are being broken and reformed continuously as the surfaces slide. The AVERAGE resistance during sliding is less than the peak static resistance. Result: f_k < f_l. This is why it is harder to start a heavy object sliding than to keep it sliding — the 'activation energy' to break all static bonds is higher than the steady-state sliding friction.
If contact area doesn't matter, why do racing car tyres have wider tyres?
Excellent question — this is a famous apparent paradox. Kinetic and static friction are indeed independent of contact area for rigid bodies in simple sliding friction (Coulomb friction model). However, racing tyres (made of soft rubber) work differently: (a) Deformational effects: soft rubber deforms into the road texture, creating a much larger effective contact area at a molecular level than a rigid tyre — the rubber interlocks with road surface irregularities deeply; (b) Hysteresis: energy is dissipated in cyclic deformation of soft rubber; (c) Chemical adhesion: rubber-road contact involves van der Waals adhesion forces that DO scale with real contact area; (d) Heat distribution: wider tyres distribute heat better, keeping rubber in optimal temperature range for maximum friction. For NEET (rigid body, Coulomb friction): friction is independent of area. In real-world soft-rubber tyre physics: multiple mechanisms cause area-dependence.
What is the unit and dimension of the coefficient of friction?
μ is dimensionless. It is a ratio: μ = f/N = (force)/(force) — the forces cancel, leaving a dimensionless number. Unit: none. Dimension: [M⁰L⁰T⁰]. Value range: 0 (perfectly frictionless) to > 1 (possible for high-adhesion surfaces like rubber on rubber). Typical NEET values: μ_s ≈ 0.3–0.7 (dry surfaces). NEET may test: 'The coefficient of friction has units of...' → answer: no units (dimensionless).
Does kinetic friction depend on the speed of sliding?
No — kinetic friction is independent of the velocity of sliding in the classical (Coulomb) friction model. f_k = μ_k N regardless of whether the block slides at 1 m/s or 10 m/s. This is one of the four empirical laws of kinetic friction. Physically: at the atomic scale, the bonding/breaking rate between asperities adjusts to the sliding speed, but the NET friction force remains approximately constant over the range of speeds relevant to NEET mechanics problems. NEET answer: 'kinetic friction does not depend on the velocity of the body' — TRUE for all NEET problems.
What does 'self-adjusting force' mean for static friction?
'Self-adjusting' means static friction automatically adjusts its magnitude to exactly cancel the applied force, within its range 0 to f_l. If P = 5 N (body at rest): f_s automatically becomes 5 N. If P increases to 12 N (still at rest): f_s automatically becomes 12 N. No calculation needed — static friction equals the applied force as long as P ≤ f_l. At P = f_l = μ_s N: f_s has reached its maximum (cannot increase further). At P > f_l: body moves (kinetic friction takes over at the lower value μ_k N). Other self-adjusting forces: normal force (adjusts to balance perpendicular forces), tension in strings that are not fully extended. Static friction is 'self-adjusting' because it is a REACTIVE force — it responds to applied force to maintain the no-slip condition.
Can the coefficient of friction be greater than 1?
Yes, μ can be greater than 1. This means the friction force exceeds the normal force. Example: rubber on rubber (μ_s ≈ 1.0–1.4), silicon carbide surfaces, or surfaces with high adhesion. μ > 1 simply means the friction force F = μN > N — the surfaces are very 'grippy'. The laws of friction still apply: F = μN, μ is constant for given surfaces. Common misconception: students sometimes assume μ < 1 always, perhaps confusing it with sinθ or cosθ (which are ≤ 1). There is no physical constraint preventing μ > 1 — friction force can exceed normal force for high-adhesion surfaces.
Is friction always a resistance? Can it ever drive motion?
Friction can drive useful motion. Walking: when you push your foot backward, friction from the ground pushes you FORWARD (Newton's third law). Without friction, you cannot walk. Driving a car: the engine torque spins the tyres; friction between tyre and road propels the car forward. Braking: kinetic friction converts KE to heat, decelerating the car. Climbing: friction between shoes and the surface provides grip upward. In all these cases, friction is the driving force for locomotion/propulsion. Friction is 'resistance' only in the sense that it opposes relative sliding motion between two surfaces — in the case of walking, the 'relative motion' would be the foot slipping backward, and friction prevents this, effectively propelling the body forward. NEET may test: 'A car can be accelerated because of...' → friction between tyre and road.
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Friction Force Definition

Kinetic friction depends upon the normal reaction

Static friction

Limiting friction

Kinetic or dynamic friction

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Friction Force Definition

Kinetic friction depends upon the normal reaction

Static friction

Limiting friction

Kinetic or dynamic friction

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