The centre of mass of a system of particles · Physics Class 11–12 | StemPy Lab
Course 6.1·Lesson 1 of 3
The centre of mass of a system of particles
The centre of mass is the mass-weighted average position of a system: rcm=∑mi∑miri
Lesson 1 of 3Show all lessonsHide
Try the code and the simulations beside the lesson.
One point that stands for the whole
A spinning hammer thrown across a field tumbles in a complicated way, yet one point of it follows a smooth parabola, just like a thrown stone. That point is the centre of mass.
Particles
For particles of mass mi at positions xi, the centre of mass is the mass-weighted average position:
xcm=m1+m2+…m1x1+m2x2+…=M∑mixi
and the same for y and z. Heavier particles pull it toward themselves.
A graph with x and y axes in metres. Three particles are drawn: 1 kilogram at the origin, 2 kilograms at x equals 4 metres on the x axis, and 3 kilograms at y equals 3 metres on the y axis. A red cross marks the centre of mass at x equals 1.33 metres and y equals 1.50 metres, with dotted lines to the two axes.
Move the masses and watch it.
You should find the centre of mass always inside the triangle of the three masses, pulled toward the heaviest. With equal masses it sits at the triangle's centre.
Uniform bodies
For a uniform body with a centre of symmetry (a rod, a ring, a disc, a sphere, a rectangle), the centre of mass is at that centre. A body made of simple pieces can be split: treat each piece as its whole mass at its own centre.
A body with a hole can be treated as the full body plus a negative mass where the hole is.
A uniform disc of radius R in blue, with a circular hole of radius R over 2 cut out on its right side. The hole touches the centre of the disc and reaches the right edge. A red cross on the left of the centre marks the centre of mass of what is left, at a distance of R over 6 from the centre.
Watch out. The centre of mass need not lie inside the material: a ring's is at its empty centre, and a boomerang's lies between its arms.
A worked example
Three children sit on a square raft: 30kg at (0,0), 40kg at (3.0,0) and 50kg at (3.0,4.0), in metres.
Total mass.M=120kg.
x.∑mixi=30kg×0m+40kg×3.0m+50kg×3.0m=270kg m, so xcm=120kg270kg m=2.25m.
y.ycm=120kg50kg×4.0m=1.67m.
Think first. Put the origin on one of the masses: every term with a zero drops out.
Practise with new numbers
Try it in Python
The program finds the centre of mass of the children on the raft.
Remember these
xcm=∑mi∑mixi, and the same for y and z.
Uniform symmetric bodies: the centre of mass is at the centre.
Split complex shapes into pieces; a hole is a negative mass.
Check yourself
Try each one on your own first. If you are stuck, open a hint. Then check with Show the answer.
A 2.0kg ball and a 6.0kg ball are 1.6m apart. How far is the centre of mass from the lighter ball?
Where is the centre of mass of a uniform metre rule?
The Earth is about 81 times as heavy as the Moon, and they are 3.84×105km apart. How far from the Earth's centre is their centre of mass?
Can a body balance on a point that is not under its centre of mass?
Enroll free in Centre of Mass and the Motion of a System
Every lesson is open to read. Enrolling also lets you:
Mark lessons done and carry on where you stopped.
Take the tests of this lesson and its course.
Count the course towards the certificate for its chapter.
. It lies nearer the heavier parts, at the centre of a uniform symmetric body, and possibly where there is no material at all. A body with a piece removed can be handled by treating the hole as a negative mass.
about 25 min1 simulation2 practice questions1 Python program4 questions to check yourself
This lesson is free to read. Enroll free to keep your place and take the tests.