A rod of length L is placed along the x-axis between x=0 and x=L. The linear mass density is lambda such that lambda=a+bx. Find the mass of the rod.
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linear mass density of the rod is given by
\lambda = \alpha + \beta xλ=α+βx
now we have
\frac{dm}{dx} = \alpha + \beta x
dx
dm
=α+βx
integrate both sides
\int dm = \int \alpha + \beta x dx∫dm=∫α+βxdx
M = \alpha L+\frac{ \beta L^2}{2}M=αL+
2
βL
2
so above is the total mass of rod
now by the formula of center of mass
r_{cm} = \frac{1}{M}\int xdmr
cm
=
M
1
∫xdm
r_{cm} = \frac{1}{M} \int x*(\alpha + \beta x) dxr
cm
=
M
1
∫x∗(α+βx)dx
r_{cm} = \frac{1}{M} (\alpha*\frac{L^2}{2} + \beta*\frac{L^3}{3})r
cm
=
M
1
(α∗
2
L
2
+β∗
3
L
3
)
now plug in value of mass of rod
r_{cm} = \frac{(\alpha*\frac{L^2}{2} + \beta*\frac{L^3}{3})}{( \alpha L+\frac{ \beta L^2}{2})}r
cm
=
(αL+
2
βL
2
)
(α∗
2
L
2
+β∗
3
L
3
)
so above is the position of center of mass of rod
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