If the linear mass density of a rod of length 2m varies as λ=a+bxkg/m, where x is the distance (in metres) from its one end, then its centre of mass (in metres) is given by
A
xcom=4(a+b)(9a+4b)
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B
xcom=3a+4b3(a+b)
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C
xcom=2(3a+4b)3
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D
xcom=(4a+12b)3
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Solution
The correct option is Bxcom=3a+4b3(a+b)
Since the rod is lying along x− axis, as shown in figure, its COM will have only x−coordinate. ∴ycom=0&zcom=0 Consider an element of the rod of length dx at a distance x from the origin (O) ⇒dm=λdx ∴dm=(a+bx)dx From the equation: xcom=∫xdm∫dm Putting limits of x=0→x=2 xcom=∫20x(a+bx)dx∫20(a+bx)dx xcom=a[x22]20+b[x33]20a[x]20+b[x22]20 xcom=2a+8b32a+2b