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12 Questions around this concept.
Centre of mass of uniform symmetrical body like square, rectangular and circular lamina lies at-
Suppose a rod of mass M and length L is lying along the x-axis with its one end at x = 0 and the other at x = L
Mass per unit length of the rod =
Take a small dx length of rod at a distance x from x=0
So mass of that dx element is =
Therefore, x-coordinate of COM of the rod will be
So x coordinate of centre of mass of Uniform rod of length L
At a distance from one of the ends of the rod.
Similarly ,
And y-coordinate is zero for all particles of rod
So,
Similarly,
And z-coordinate is zero for all particles of rod
So,
So the coordinates of COM of the rod are
Means it lies at the centre of the rod.
Rectangular plate
Square plate
Circular plate
For a 2-dimensional body with uniform negligible thickness formulae for finding the position of centre of mass can be rewritten as
$$
r_{c m}=\frac{m_1 \vec{r}_1+m_2 \vec{r}_2 \ldots}{m_1+m_2 \ldots}=\frac{\rho A_1 t \vec{r}_1+\rho A_2 t \vec{r}_2 \ldots}{\rho A_1 t+\rho A_2 t \ldots}=\frac{A_1 \vec{r}_1+A_2 \vec{r}_2 \ldots}{A_1+A_2 \ldots}
$$
Where, $m=\rho$.A. $t$
Centre of mass when some mass is added to the body
$$
\vec{r}_{c m}=\frac{m_1 \vec{r}_1+m_2 \vec{r}_2}{m_1+m_2}
$$
Where $m_{1 \&}, \overrightarrow{r_1}$ are mass and position of the centre of mass for the whole body. $m_2 \& \overrightarrow{r_2}$ are mass and position of the centre of mass of added mass.
Position of centre of mass when some mass is removed
$$
\vec{r}_{c m}=\frac{m_1 \overrightarrow{r_1}-m_2 \vec{r}_2}{m_1-m_2}
$$
Where $m_{1 i s}$ the value of the whole mass and $\overrightarrow{r_1}$ is the position of the centre of mass for whole mass. Similarly $m_2 \& \overrightarrow{r_2}$ are values for mass which has been removed.
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