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    Center Of Mass Of The Uniform Rod MCQ - Practice Questions with Answers

    Edited By admin | Updated on Sep 25, 2023 25:23 PM | #NEET

    Quick Facts

    • 13 Questions around this concept.

    Solve by difficulty

    Centre of mass of uniform symmetrical body like square, rectangular and circular lamina lies at-

    An object comprises of a uniform ring of radius R and its uniform chord AB (not necessarily made of the same material) as shown in the figure. Which of the following cannot be the centre of mass of the object?

    Concepts Covered - 1

    Center of mass of the uniform rod

    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 = \mu = \frac{M}{L}

     

    Take a small dx length of rod at a distance x from x=0

    So mass of that dx element is =  dm = \mu.dx

    Therefore, x-coordinate of COM of the rod will be 

    x_{cm} = \frac{\int_{0}^{L}x.dm}{\int_{0}^{M}dm}

    x_{cm} = \frac{\int_{0}^{L}x.\mu.dx}{\int_{0}^{M}dm} = \frac{\int_{0}^{L}x.\frac{M}{L}.dx}{\int_{0}^{M}dm}

    x_{cm} = \frac{\frac{M}{L}\int_{0}^{L}xdx}{M} = \frac{1}{L}\int_{0}^{L}x.dx = \frac{L}{2}

    So x coordinate of centre of mass of Uniform rod of length L 

     At a distance  \frac{L}{2}  from one of the ends  of the rod.   

    Similarly  , y_{cm}= \frac{\int ydm}{\int dm}

    And  y-coordinate is zero for all particles of rod

    So,  y_{cm}= 0

    Similarly,  z_{cm}= \frac{\int zdm}{\int dm}

    And  z-coordinate is zero for all particles of rod

    So,  z_{cm}= 0

    So the coordinates of COM of the rod are (\frac{L}{2},0,0) 

    Means it lies at the centre of the rod.

    Position of centre of mass for uniform rectangular, square and circular plate
    1. Rectangular plate

    1. Square plate

    1. Circular plate

     

    1. 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. $t$

     

    1. 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.

    1. 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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    Position of centre of mass for uniform rectangular, square and circular plate

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    Reference Books

    Position of centre of mass for uniform rectangular, square and circular plate

    Physics Part II Textbook for Class XI

    Page No. : 146

    Line : 42

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