Friction in Physics: Static & Kinetic Friction Easy Notes for NEET
Basic idea of forces on a body
- A body of mass m is kept on a horizontal table.
- Two vertical forces act on it:
- Weight = mg (downward)
- Normal reaction = N (upward)
- These two forces cancel each other.
- So, net vertical force = 0 → no vertical motion.
When horizontal force is applied
- Now a horizontal force F is applied on the body.
- We expect the body to move.
- But sometimes it does not move immediately.
Why the body may not move
- If only force F acted, acceleration would be:
- a = F/m
- But body stays at rest → contradiction.
- So, another force must be acting opposite to F.
Introduction of friction
- A force appears between surfaces in contact.
- This force opposes motion.
- It acts parallel to surface.
- This force is called frictional force (f).
Types of friction
- Static friction (fₛ): when body is not moving.
- Kinetic friction (fₖ): when body is moving.
Static friction (fₛ)
Meaning
- Acts when body is at rest.
- Opposes impending motion (motion that is about to happen).
Important points
- Static friction exists only when force is applied.
- If no force is applied → fₛ = 0
- It increases as applied force increases.
- It always adjusts itself to balance applied force.
Condition
- Until a limit:
- fₛ = F (equal and opposite)
- So net force = 0 → body remains at rest.
Limiting static friction
- Maximum value of static friction is called limiting friction.
- Formula:
- (fₛ)max = μₛ N
- Where:
- μₛ = coefficient of static friction
- depends on nature of surfaces
- N = normal reaction
Law of static friction
- fₛ ≤ μₛ N
- Means static friction can vary from 0 to maximum value.
Kinetic friction (fₖ)
Meaning
- Acts when body is already moving.
- Opposes actual motion.
Important points
- Always acts opposite to motion.
- Independent of contact area.
- Almost independent of speed.
Formula
- fₖ = μₖ N
- Where:
- μₖ = coefficient of kinetic friction
Key comparison
- μₖ < μₛ
- So kinetic friction is less than maximum static friction.
Motion after overcoming friction
-
If applied force F > (fₛ)max → body starts moving.
-
During motion:
- Net force = F − fₖ
- Acceleration = (F − fₖ)/m
If force is removed
- Only kinetic friction acts opposite motion.
- Acceleration becomes negative:
- a = −fₖ/m
- Body slows down and eventually stops.
Nature of friction laws
- These laws are not fundamental laws.
- They are experimental (empirical).
- They are approximate but very useful in physics problems.
Important concept
- Friction acts on contact surfaces.
- It is a component of contact force parallel to surface.
- It opposes relative motion, not absolute motion.
Real-life example: Train and box
- A train accelerates forward.
- A box is kept inside it.
Without friction:
- Box would stay at rest (due to inertia).
- Train would move ahead.
- Box would hit back wall.
With friction:
- Static friction acts on box.
- It pulls box forward with train.
- So box accelerates with train.
- Hence, box stays at rest relative to train.
Final NEET summary
- Friction is a contact force opposing relative motion.
- Two types:
- Static friction (before motion)
- Kinetic friction (during motion)
- Key formulas:
- fₛ ≤ μₛ N
- fₖ = μₖ N
- Always: μₖ < μₛ
Internal Links
Newton's Laws of Motion Explained
Contact and Non-Contact Forces
Free Body Diagrams in Physics
Force and Acceleration Relationship
Circular Motion Fundamentals
Work, Energy and Power
Applications of Newton's Second Law
Momentum and Impulse
Laws of Motion Class 11 Notes
Coefficient of Friction Numerical Problems
Friction - Mind Map (NEET Level)
FRICTION
|
|-- Definition
| |-- Force opposing relative motion between surfaces
| |-- Acts parallel to surface of contact
|
|-- Types of Friction
| |
| |-- 1. Static Friction (fs)
| | |-- Acts when body is at rest
| | |-- Opposes impending motion
| | |-- Adjusts with applied force
| | |-- Range: 0 ≤ fs ≤ μs N
| |
| |-- 2. Kinetic Friction (fk)
| |-- Acts when body is in motion
| |-- Opposes actual motion
| |-- fk = μk N
| |-- μk < μs
|
|-- Laws of Friction
| |-- Independent of area of contact
| |-- Depends on nature of surfaces
| |-- Proportional to normal reaction (N)
|
|-- Coefficients
| |-- μs → coefficient of static friction
| |-- μk → coefficient of kinetic friction
|
|-- Limiting Friction
| |-- Maximum static friction
| |-- (fs)max = μs N
|
|-- Motion Cases
| |
| |-- F ≤ (fs)max → body at rest
| |
| |-- F > (fs)max → motion starts
| | |-- Acceleration = (F - fk)/m
| |
| |-- Force removed
| |-- Retarding force = fk
| |-- Body stops eventually
|
|-- Important Concept
| |-- Friction opposes relative motion, not absolute motion
|
|-- Example: Train and Box
|-- Train accelerates
|-- Box moves due to static friction
|-- Without friction → box slips backward
Friction — Complete Question Bank
Class 11 Physics (CBSE / NEET Level)
✅ 1. Very Short Answer Questions (1 Mark)
✅ 2. Short Answer Questions (2–3 Marks)
- Interlocking of surface irregularities: No surface is perfectly smooth; microscopic hills and valleys interlock when surfaces press together.
- Molecular Adhesion: Highly localized chemical bonding/attractive forces established at the actual contact points between the molecules of the two surfaces.
- Static friction operates when the body is at rest relative to the surface; Kinetic friction operates when the body is in relative motion.
- Static friction is a self-adjusting variable force (0 ≤ fs} ≤ fs(max)), whereas kinetic friction is nearly constant for a given pair of surfaces.
- The coefficient of static friction (μs) is always greater than the coefficient of kinetic friction (μk).
- The magnitude of limiting friction depends entirely on the nature and roughness of the surfaces in contact.
- It acts tangentially and opposite to the direction of impending motion.
- The magnitude of limiting friction is directly proportional to the normal reaction (fs(max) ∝ R).
- It is independent of the apparent area of contact between the surfaces, as long as the normal reaction remains constant.
✅ 3. Long Answer Questions (5 Marks)
When an external force is applied to a body resting on a rough surface, the static friction increases linearly with the applied force to balance it (f = Fapplied). This continues up to a threshold limit called limiting friction.
Once the applied force crosses this threshold value, the molecular bonds break, the interlocking is partially overcome, and the body begins to slide. At this point, the friction drops slightly below the limiting value to a steady value called kinetic friction. Further increase in the applied force does not change the kinetic friction value.
(Graph Note: A plot of Friction Force vs. Applied Force shows a straight line at 45° representing the static region, peaks at the limiting friction value, takes a minor downward dip, and transitions into a flat horizontal line representing constant kinetic friction.)
By experimental observation, the limiting friction force (fs(max)) is found directly proportional to the normal reaction force (R) pressing the surfaces together.
Mathematically:
fs(max) ∝ R
To eliminate the proportionality sign, we introduce a constant:
fs(max) = μs · R
Where μs is the dimensionless constant called the coefficient of static friction. It depends purely on the materials, temperature, and roughness conditions of the touching surfaces.
When the train accelerates forward with an acceleration a, an observer inside the non-inertial frame views a pseudo force acting on the box in the backward direction. Relative to the floor of the train, the box has a tendency to slide backward due to inertia.
Because of this impending backward relative motion, a static frictional force acts on the box in the forward direction (tangential to the floor). If this static friction is large enough (fs = ma) and does not exceed the maximum limiting value (μsmg), it prevents relative slipping. Therefore, static friction acts as the accelerating force that moves the box forward alongside the train.
✅ 4. Multiple Choice Questions (1 Mark Each)
✅ 5. Assertion and Reason Questions
Directions: Choose Option (A) if both Assertion and Reason are true and Reason is correct explanation; Option (B) if both are true but Reason is not correct explanation; Option (C) if Assertion is true but Reason is false; Option (D) if Assertion is false but Reason is false.
Assertion (A): Static friction is a self-adjusting force.
Reason (R): It changes its magnitude and direction according to the applied external force up to its maximum threshold limit.
Assertion (A): Kinetic friction is greater than static friction.
Reason (R): Mechanical interlocking between surface irregularities increases once the relative motion starts.
Assertion (A): Friction always opposes the relative motion between surfaces.
Reason (R): Friction always acts opposite to the absolute velocity vector of the body.
✅ 6. Fill in the Blanks
✅ 7. Match the Column
| Column A | Column B |
|---|---|
| (1) Static friction | (A) Ratio of limiting friction to normal reaction |
| (2) Kinetic friction | (B) Force perpendicular to contact plane |
| (3) μs | (C) Operates under relative motion conditions |
| (4) μk | (D) Operates under relative rest conditions |
| (5) N (or R) | (E) Ratio of sliding friction to normal reaction |
(2) → C
(3) → A
(4) → E
(5) → B
✅ 8. Case Study Based Question
✅ 9. Statement Based Questions
Statement I: Frictional force depends heavily on the visible apparent area of contact.
Statement II: This area dependency law holds true for all macroscopically rigid engineering surfaces.
Statement I: Friction is a necessary evil that allows humans to walk safely on ground platforms.
Statement II: Without any friction force components acting, walking on a surface is completely impossible.

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