Darshit Sir Institute

Class 11 Physics · Gujarat Board, CBSE, GUJCET and JEE

Laws of Motion and Friction formulas

Laws of motion turns a described situation into an equation. Almost every mark in this chapter comes from one skill: drawing the free-body diagram correctly before writing anything. Friction, which sits inside this chapter, is the single most searched topic of Class 11 mechanics.

21 formulas, 4 memory hooks, and the 5 mistakes that cost the most marks.

Newton's laws

WhatFormulaSymbols and notes
Second lawF = ma = dp/dtp = mv is linear momentum; the vector form is what the law actually says
ImpulseJ = FΔt = Δpa large force for a short time, or a small force for long, can give the same change
Conservation of momentumm₁u₁ + m₂u₂ = m₁v₁ + m₂v₂holds when the net external force is zero
Recoil of a gunvgun = −(mbullet/mgun)vbulletthe minus sign is the recoil direction

Friction

WhatFormulaSymbols and notes
Static frictionfs ≤ μsNstatic friction is whatever it needs to be, up to this maximum
Limiting frictionfmax = μsNthe value just before sliding starts
Kinetic frictionfk = μkNconstant once sliding, and μk < μs
Angle of frictiontanλ = μsλ is the angle the total contact force makes with the normal
Angle of reposetanα = μsthe incline angle at which a body just begins to slide; numerically equal to the angle of friction
Body on a rough inclinea = g(sinθ − μcosθ)when it slides down; it stays put while tanθ ≤ μ
Stopping distanced = v²/(2μg)independent of mass, which is why a loaded truck does not stop later for this reason

Circular motion

WhatFormulaSymbols and notes
Centripetal forceF = mv²/r = mω²rdirected towards the centre; it is a requirement, not a new force
Flat road, maximum speedvmax = √(μrg)friction alone supplies the centripetal force
Banked road, no frictiontanθ = v²/rgthe ideal speed needs no friction at all
Banked road with frictionvmax = √(rg(μ + tanθ)/(1 − μtanθ))the full result used in entrance papers
Vertical circle, topvtop ≥ √(gr)the minimum speed to keep the string taut
Vertical circle, bottomvbottom ≥ √(5gr)follows from energy conservation between top and bottom

Connected bodies

WhatFormulaSymbols and notes
Two masses over a pulleya = (m₁ − m₂)g/(m₁ + m₂)for an ideal pulley and a light inextensible string
Tension in that stringT = 2m₁m₂g/(m₁ + m₂)the same throughout a light string over a frictionless pulley
Lift going up with acceleration aapparent weight = m(g + a)reading of a weighing machine inside the lift
Lift going down with acceleration aapparent weight = m(g − a)zero in free fall, which is weightlessness
Darshit Bhatt

Taught by Darshit Bhatt, founder and lead faculty at Darshit Sir Institute. Instrumentation and Control engineer, with a master's degree and a chartered degree, teaching in Paldi, Ahmedabad since 2006.

Know the formula but not when to use it? Darshit Sir has taught this in Paldi since 2006, in the classroom and live online.

Memory hooks

How to remember this chapter.

“Draw before you write”

Every laws of motion question

Free-body diagram first: weight down, normal perpendicular to the surface, friction along the surface opposing relative motion, then tension. Most lost marks in this chapter are a missing force, not a wrong formula.

“Static is lazy, kinetic is fixed”

Telling the two frictions apart

Static friction only supplies as much as is needed to prevent sliding, up to μsN. Kinetic friction is a fixed μkN once sliding has begun.

“Repose equals friction”

Angle of repose and angle of friction

Both have tangent equal to μs, so the two angles are numerically the same. One is measured from the incline, the other from the normal.

“Centripetal is a job, not a force”

What supplies the centripetal force

Nothing is labelled centripetal on a free-body diagram. Friction, tension, gravity or the normal does that job. Write which one before using mv²/r.

Where marks go

The mistakes that cost the most.

  • Adding a centrifugal force in an inertial frame. In the ground frame there is no outward force on the body.
  • Using f = μN when the body has not started sliding. Below the limit, friction equals the applied force, not μN.
  • Assuming friction always opposes motion. It opposes relative sliding, which is why friction pushes a car forward.
  • Using the mass of only one block for a connected system. Acceleration is common; write the equation for each block, or for the whole system.
  • Forgetting that the string tension is the same throughout only if the string is light and the pulley frictionless.

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