Torque and rotational equilibrium
Torque is the rotational analogue of force, causing angular acceleration, and equilibrium occurs when the net torque on a body is zero.
Why this shows up in the exam
NEET often asks you to analyze situations involving torques, rotational equilibrium, and the principle of moments.
How NEET tests this
Learn the idea
Torque is the vector product τ = r × F; rotational equilibrium means the vector sum of all torques on a body is zero. The key insight is that τ is always perpendicular to both r and F, so any dot product with r or F vanishes.
🧠 Memory hook: Think of a screwdriver: the handle (r) twists the screw (F) only when they are at right angles – that twist is the torque.
Get this one clearly and it pays off every single time it shows up in the paper. 🎯
Formulas & facts to keep ready
- τ = r × F (vector product)
- |τ| = r F sinθ, where θ is the angle between r and F
- Direction of τ given by right‑hand rule
- Rotational equilibrium: Στ = 0 (vector sum)
- Principle of moments: clockwise moments = anticlockwise moments about any axis
- r·τ = 0 and F·τ = 0 always
How to approach it
- 1Identify the pivot (or axis) about which torques are to be taken
- 2Write each torque as τ = r × F or as magnitude r F sinθ with appropriate sign
- 3Add all torques vectorially (or use scalar moments about the chosen axis) and set Στ = 0
- 4Use the perpendicular property (r·τ = 0, F·τ = 0) to simplify calculations
Worked example — watch it click
If F is the force acting on a particle having position vector r and τ is the torque of this force about the origin, then :
- A)r.τ > 0 and F.τ < 0
- ✅r.τ = 0 and F.τ = 0
- C)r.τ = 0 and F.τ ≠ 0
- D)r.τ ≠ 0 and F.τ = 0
The concept behind this problem
The example checks whether you remember that τ = r × F is orthogonal to both r and F, so their dot products must be zero.
Step by step
- 1Torque τ = r × F.
- 2By properties of cross product: r · τ = r · (r × F) = 0 (always perpendicular).
- 3Similarly, F · τ = F · (r × F) = 0.
- 4Both dot products are zero regardless of r and F.
Watch out
Treating τ as a scalar magnitude leads to the mistaken belief that r·τ or F·τ could be non‑zero.
Common slip-ups that cost marks
- •Ignoring the perpendicular distance – use the shortest distance from the line of action to the pivot
- •Mixing up sign convention for clockwise and anticlockwise moments
- •Assuming a force whose line of action passes through the pivot produces torque (it does not)
🌟 That's the whole idea — you've got this. Try the practice set below; every question you attempt makes it stick a little harder.
Practise it
These are real questions from past NEET papers that test this exact idea.
A uniform meter scale balances horizontally on a knife edge placed at 55 cm mark. When a mass of 25 g is supported from one end, then the mass of the scale is
More from Motion of System of Particles and Rigid Body
Conservation of momentum and angular momentum
The total linear and angular momentum of a system remains constant in the absence of external forces or torques, including during collisions and rotational motion.
Moment of inertia and radius of gyration
Moment of inertia quantifies how mass is distributed with respect to an axis of rotation, and the radius of gyration is a measure related to this distribution.
Center of mass: definition and calculation
The center of mass is the point representing the mean position of the mass in a system, and can be calculated for discrete particles or continuous bodies.
Rotational kinematics and dynamics
Rotational kinematics describes the motion of rotating bodies, while dynamics relates torque, angular acceleration, and rotational kinetic energy.
Centre of Mass of Discrete Particles
For discrete particles, the centre-of-mass position is the vector sum of each mass times its position divided by total mass; this point governs translation even when the particles move relative to one another.
Centre-of-Mass Shift and Internal Rearrangement
When external force is zero, total momentum and centre-of-mass velocity remain constant; therefore mass displacements relative to a fixed frame obey the mass-weighted displacement constraint.