How to proof that the centre of gravity of a cone is a quarter of the height
Suppose the cylindrical symmetry of the problem to note that the center of mass must lie along the z axis (x = y = 0). The only issue is how high does it lie. If the uniform density of the cone is ρ , then first compute the mass of the cone. If we slice the cone into circular disks of area pi r^2 and height dz, the mass is given by the integral: M=∫ρdV=ρ∫0hpir2dz However, we know that the radius r starts at a for z = 0, and goes linearly to zero when z = h. This means that r = a(1 -z/h), so that: M=ρ∫0hpia2(1−z/h)2dz=pia2ρ∫0h(1−2z/h+z2/h2)dz=1/3pia2hρ Noe that this is simply indicates that the volume of the cone is given by V=1/3pia2h . To find the height of the center of mass, we then compute: zcm=1/M∫ρzdV=ρ/M∫0hpir2zdz=pia2ρ/M∫0h(1−z/h)2zdz =pia2ρ/M∫0h(z−2z2/h+z3/h)dz=1/12pia2h2rh÷M=1/4h As a result, the center of mass of the cone is along the symmetry axis, one quarter of the way up from the base to the tip
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