A thin bar of length L has a mass per unit length λ , that increases linearly with distance from one end. If…

A thin bar of length L has a mass per unit length λ, that increases linearly with distance from one end. If its total mass is M and its mass per unit length at the lighter end is λ 0 ,  then the distance of the centre of mass from the lighter end is
  1. L 3 + λ 0 L 2 8 M
  2. L 3 + λ 0 L 2 4 M
  3. L 2 - λ 0 L 2 4 M
  4. 2 L 3 - λ 0 L 2 6 M

Solution



λ x

λ = Kx + λ 0

dm = λ dx

X cm = 0 L dm · x 0 L dm = 0 L Kx + λ 0 dx.x  0 L Kx + λ 0 dx

= K · x 3 3 0 L + λ 0 x 2 2 0 L K x 2 2 0 L + λ 0  L

= KL 3 3 + λ 0 L 2 2 KL 2 2 + λ 0 L

= KL 3 + λ 0 2 L 2 KL 2 2 + λ 0 L

Now,  M = 0 L dm

= KL 2 2 + λ 0 L

2 M = KL 2 + 2 λ 0 L

K = 2 M - λ 0 L L 2

Putting the value of K.

X cm = 2 M - λ 0 L 3 L + λ 0 2 L 2 M

= 2 L 2 M - λ 0 L 3 LM + λ 0 L 2 2 M

= 2 ML 3 M - 2 λ 0 L 2 3 M + λ 0 L 2 2 M

= 2 L 3 - λ 0 L 2 6 M

Hence,  2 L 3 - λ 0 L 2 6 M

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