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This lesson covers finding the centre of mass of a system of discrete particles. The centre of mass (also called the centre of gravity in a uniform gravitational field) is the single point at which the entire mass of the system can be considered to act.
For n particles with masses m1,m2,…,mn at positions (x1,y1),(x2,y2),…,(xn,yn):
xˉ=∑mi∑mixi,yˉ=∑mi∑miyiIn vector form:
rˉ=∑mi∑miri=M∑miriwhere M=∑mi is the total mass.
Masses 3 kg at x=2 and 5 kg at x=6. Find xˉ.
Solution
xˉ=3+53(2)+5(6)=86+30=836=4.5
The centre of mass is at x=4.5, closer to the heavier mass.
Masses: 2 kg at (1,3), 4 kg at (5,1), 6 kg at (3,5).
Solution
M=2+4+6=12 kg.
xˉ=122(1)+4(5)+6(3)=122+20+18=1240=310≈3.33
yˉ=122(3)+4(1)+6(5)=126+4+30=1240=310≈3.33
Centre of mass: (10/3,10/3).
Three particles of masses 1 kg, 2 kg, and 3 kg are placed at the vertices (0,0), (6,0), and (3,4) respectively.
Solution
M=6 kg.
xˉ=61(0)+2(6)+3(3)=60+12+9=621=3.5
yˉ=61(0)+2(0)+3(4)=612=2
Centre of mass: (3.5,2).
For particles attached to a rod (or along a line), the problem reduces to one dimension.
A light rod AB has length 2 m. Masses of 4 kg and 6 kg are attached at A and B respectively. Find the distance of the centre of mass from A.
Solution
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