Equilibrium of a rigid body · Physics Class 11–12 | StemPy Lab
Course 6.3·Lesson 2 of 3
Equilibrium of a rigid body
A rigid body is in equilibrium when the net external force is zero (no acceleration of the centre of mass) and the net torque about every point is zero (no angular acceleration). In practice: balance the forces along two axes, and take torques about a well-chosen point, often where an unknown force acts. A couple, two equal and opposite forces not along one line, has zero net force but a torque.
about 25 min1 simulation2 practice questions
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Two conditions
A rigid body stays at rest (or moves steadily without changing its spin) only if both of these hold:
∑Fext=0and∑τ=0
The first stops the centre of mass accelerating. The second stops the turning from changing. Neither is enough alone: two equal and opposite forces that are not along one line, a couple, give zero net force, but they still turn a body.
Choosing the pivot
The torque condition holds about every point. So choose a point where an unknown force acts: that force has no torque about it and drops out.
Two drawings. On the left, a seesaw on a pivot in balance: a 30 kilogram block is 2.0 metres to the left of the pivot, and a 20 kilogram block is 3.0 metres to the right, and 30 times 2.0 is equal to 20 times 3.0. On the right, a beam rests on two supports with the reactions R one and R two pushing up, a load pushing down on the left part and the weight of the beam pushing down at its middle.
Slide a load along a plank and watch the supports share it.
You should find the two pushes always adding up to the total weight, and the support nearer the load always carrying more.
A ladder
A ladder against a smooth wall has three forces from outside besides its weight: the wall's push (horizontal, since the wall is smooth), and the ground's push and friction at its foot.
A ladder of length 5 metres leans on a smooth vertical wall, with its foot 3 metres from the wall and its top 4 metres up the wall. Four forces are drawn: the weight W downward at the middle of the ladder, the push N two of the wall horizontally at the top, the push N one of the floor upward at the foot, and the friction f of the floor, horizontal at the foot and pointing toward the wall.
Take torques about the foot to find the wall's push; then friction must balance it.
Watch out. The weight of a uniform body acts at its middle, not at an end. Its moment arm is measured to that point.
A worked example
A 12kg uniform board 2.4m long rests on two trestles at its ends. A 30kg tin of paint sits 0.60m from the left end.
Torques about the left end.RB×2.4m=117.6N×1.2m+294N×0.60m, so RB=2.4m141.1Nm+176.4Nm=132.3N.
Forces.RA=117.6N+294N−132.3N=279.3N.
Check about the right end.279.3N×2.4m=117.6N×1.2m+294N×1.8m: 670Nm=670Nm.
Think first. Draw every force, mark where each acts, then pick the pivot that removes the most unknowns.
Practise with new numbers
Try it in Python
The program moves the tin of paint along the board and finds how the trestles share the load.
Remember these
Equilibrium: ∑F=0 and ∑τ=0 about any point.
Take torques about a point where an unknown force acts.
A couple: zero net force, torque = force × distance between the lines.
Check yourself
Try each one on your own first. If you are stuck, open a hint. Then check with Show the answer.
A 30kg child sits 2.0m from a seesaw's pivot. Where must a 40kg child sit to balance?
Two forces of 10N, equal and opposite, act on a ruler at points 0.30m apart, at right angles to it. What is their net force? Their torque?
Why is a ladder more likely to slip when it leans at a shallow angle?
A uniform 2.0m shelf of 6.0kg rests on brackets at its two ends. What does each bracket carry? (g=9.8m/s2.)
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