Moments and centres of mass of discrete massesEdexcel A-Level Further Maths: Revision notes
Section 1
Moment of a force
The moment of a force about a point is the force multiplied by the perpendicular distance from the point to the line of action of the force: It is measured in N m and has a sense, clockwise or anticlockwise. A body is in equilibrium when (1) the resultant force is zero and (2) the sum of the moments about any point is zero. The weight of a body acts at its centre of mass. For a uniform rod this is the midpoint. Example: a force of 20 N acts at a perpendicular distance of 0.3 m from a pivot, so its moment is N m.
Using the distance along the rod instead of the perpendicular distance when the force is not at right angles to the rod.
Take moments about the point where an unknown force acts. That force then has zero moment and drops out.
Section 2
Centre of mass of particles on a line
The centre of mass of a system is the single point at which its total weight can be taken to act. For particles of masses at positions on a line, the moment of the total weight about the origin equals the sum of the moments of the separate weights: , so Example: masses 2 kg, 3 kg, 5 kg at give m. The centre of mass is nearer to the heavier particles, not at the mean of the positions. Adding or removing a particle: include (or leave out) its and in both sums. A 10 kg particle added at gives m.
Dividing by the number of particles. Divide by the total mass.
Section 3
Centre of mass in two dimensions
Treat the and coordinates separately with the same formula: Example: 1 kg, 2 kg, 3 kg, 4 kg at , , , . Then , and , so the centre of mass is . Distances from the centre of mass to a particle use Pythagoras. The distance to the 2 kg particle is m.
Make a table with columns , , , , and add each column. It prevents sign slips with negative coordinates.
Section 4
Changing the system
Problems often add or remove a particle, or give the centre of mass and ask for an unknown mass or position.
- Unknown mass: write as an expression in and solve. If and the total mass is , then gives , so .
- Removing a particle: subtract its , and from the totals.
- Condition on the centre of mass: for example it lies on . Write and in terms of the unknown, then equate. Example: remove the particle at (leaving , , ) and add kg at . On : , so .
Forgetting that removing a particle also removes its mass from the denominator.
Section 5
Rods on supports and tilting
A uniform rod of mass and length has its weight at its midpoint. If it rests horizontally on two supports, take moments to find the reactions, then resolve vertically to check. Example: a rod of length 6 m and mass 12 kg rests on supports and with m and m. Moments about : , so N and N. A rod is about to tilt about a support when the reaction at the other support becomes zero. With a particle of mass at and , moments about give , so .
State the point you take moments about, and which way you take positive, before writing the equation.
That's the notes covered.
Carry on to the next subtopic.
Exam questions on Moments and centres of mass of discrete masses
- Three particles of masses 2 kg, 3 kg and 5 kg are placed on a straight line at the points m, m and m respectively, where is the distance from a fixed origin on the line. Take m s⁻².Find the total moment of the weights of the three particles about .2 marks
- Four particles of masses 1 kg, 2 kg, 3 kg and 4 kg are placed at the points with coordinates , , and respectively, where distances are in metres.Find the distance between the centre of mass and the 2 kg particle.2 marks
- A uniform rod has length 6 m and mass 12 kg. It rests horizontally on two smooth supports at and , where m and m. Take m s⁻².Find the magnitudes of the reactions at and .3 marks
Written by the Exaim team, led by Shaun Daswani (Head of Upper Secondary, Improve ME Institute; MSc Financial Mathematics, Imperial College London; BSc, UCL) and Jason Daswani (operational lead, Improve ME Institute; LSE).