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Centre of Mass.

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Presentation on theme: "Centre of Mass."— Presentation transcript:

1 Centre of Mass

2 Announcement All Term1 grades will be finalised tomorrow evening.

3 Goal of the class To understand centre of mass.
To find the centre of mass of irregular shapes. Question of the day: Which way can the centre of mass be found practically without calculation?

4 Centre of Mass (COM/CM)
Sometimes called the centre of gravity, but centre of mass is more correct. Buses and sports cars are designed with a very low centre of mass so they don’t tip over as easy. When you run, you lean forward to shift your centre of mass.

5 Collection of Particles
z y x Let’s define a coordinate system in x,y and z And add on a mass m1 at a displacement r1 from the origin. This has coords x1,y1,z1 Do same with m2 and mN The centre of mass of all the particles will have a single location and will be a point! CM: (Xcm,Ycm,Zcm) Xcm = m1x1+m2x2+…..mNxN/m1+m2+…+mN But m1+m2+…+mN = M So Xcm = 1/M Sum (mixi) Same for Y and Z

6 Four Particles Particle 1: m1 = 1 kg (x1,y1,z1) = (1,0,0) m
Draw on particles Using Xcm = 1/M Sum (mixi) where N=4 M = =6kg Xcm = 1/6 (15) = 2.5m Ycm = 0.5m Zcm = 0m ofcourse (Xcm, Ycm,Zcm) = (2.5,0.5,0)

7 Extended Objects Divide volume into N small pieces z y x
Draw an irregular shape and divide into small pieces Each small piece will have a tiny mass and a tiny volume. Let’s label them dm1, dm2 etc up to dmN Suppose I pick a piece (the ith piece) The displacement vector goes to the centre of this piece ri Masses: dm1,dm2,…dmN have positions (x1,y1,z1),(x2,y2,z2) etc.. We know Xcm is approx 1/M (x1dm1 + x2dm2+…+xNdmN) = 1/M sum xidmi But when we take N to be infinite we get the limit N-> inf Xcm = 1/M integral xdm Where we integrate over the mass and not over x,y or z The force he hits the ball with it isn’t constant. In fact if we draw it like so: When he first hits the ball, at that instant the force is 0. The same when the ball leaves the ball. The time he hits it over t2-t1 = delta t which will be a few milliseconds only. J = F_av delta t Example baseball Δt = 2x10-3 seconds What is the average force on the ball F = Δp/Δt or Δp = FΔt Find Δp = 12kgm/s Find F_av = 6x10-3N

8 Centre of Mass of a Rod Draw a rod on the picture
Total length L and mass M Indicate x->x+dx on pic We know Xcm = 1/M integral xdm The mass per unit length is M/L Therefore dm = M/L dx Xcm = 1/M integral xdm = 1/M integral x M/L dx = L/2

9 Centre of Mass of a Right Triangle
Draw a rod on the picture Total length L and mass M Indicate x->x+dx on pic We know Xcm = 1/M integral xdm The mass per unit length is M/L Therefore dm = M/L dx Xcm = 1/M integral xdm = 1/M integral x M/L dx = L/2

10 Orbiting Bodies Virtual centre of mass - doughnut

11 Problem A uniform rod of mass M and length L is bent into a quarter of a circle. Locate its centre of mass. Dm mass of length R d(theta) = M/LR d(theta) But x = Rcos(theta)


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