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Question: Two particles of masses \[100g\] and \[300g\] at a given time have positions \[2\vec i + 5\vec j + 1...

Two particles of masses 100g100g and 300g300g at a given time have positions 2i+5j+13k2\vec i + 5\vec j + 13\vec k and 6i+4j2k - 6\vec i + 4\vec j - 2\vec k m respectively and velocities 10i7j3k10\vec i - 7\vec j - 3\vec k and 7i9j+6k7\vec i - 9\vec j + 6\vec k m/s respectively. Determine the instantaneous position and velocity of C.M

Explanation

Solution

The center of mass is the point at which the whole mass of the body is concentrated is called the center of mass. For a system center of mass is the point that can be used to define the motion of the system. So we need to use the formula for the position of the center of mass and velocity of the center mass and need to substitute the given values in the formula.
Formula used:
rcom=i=1nmirii=1nmi{\vec r_{com}} = \dfrac{{\sum\limits_{i = 1}^n {{m_i}{{\vec r}_i}} }}{{\sum\limits_{i = 1}^n {{m_i}} }}
vcom=i=1nmivii=1nmi{\vec v_{com}} = \dfrac{{\sum\limits_{i = 1}^n {{m_i}{{\vec v}_i}} }}{{\sum\limits_{i = 1}^n {{m_i}} }}

Complete answer:
Given two position vectors, let them be named as r1{\vec r_1} and r2{\vec r_2}. Also given that two velocity vectors, let them be named as v1{\vec v_1} and v2{\vec v_2}.
Given
r1=2i+5j+13k{\vec r_1} = 2\vec i + 5\vec j + 13\vec k and 6i+4j2k - 6\vec i + 4\vec j - 2\vec k. Also v1=10i7j3k{\vec v_1} = 10\vec i - 7\vec j - 3\vec k and v2=7i9j+6k{\vec v_2} = 7\vec i - 9\vec j + 6\vec k.
Now first we will find the instantaneous position of the center of mass. The formula for the instantaneous position of the center of mass is given as,
rcom=i=1nmirii=1nmi{\vec r_{com}} = \dfrac{{\sum\limits_{i = 1}^n {{m_i}{{\vec r}_i}} }}{{\sum\limits_{i = 1}^n {{m_i}} }}
rcom=m1r1+m2r2m1+m2\Rightarrow {\vec r_{com}} = \dfrac{{{m_1}{{\vec r}_1} + {m_2}{{\vec r}_2}}}{{{m_1} + {m_2}}}
Given two masses as m1{m_1} and m2{m_2} which is equal to 100g100g and 300g300g.
Substituting all the known values in the above formula we will get,
\Rightarrow {\vec r_{com}} = \dfrac{{100(2\vec i + 5\vec j + 13\vec k) + 300( - 6\vec i + 4\vec j - 2\vec k)}}{{100 + 300}}$$$$\dfrac{{gm.m}}{{gm}}
rcom=100(2i+5j+13k)+300(6i+4j2k)400m\Rightarrow {\vec r_{com}} = \dfrac{{100(2\vec i + 5\vec j + 13\vec k) + 300( - 6\vec i + 4\vec j - 2\vec k)}}{{400}}m
rcom=14(2i+5j+13k18i+12j6k)m\Rightarrow {\vec r_{com}} = \dfrac{1}{4}(2\vec i + 5\vec j + 13\vec k - 18\vec i + 12\vec j - 6\vec k)m
rcom=14(16i+17j+7k)\Rightarrow {\vec r_{com}} = \dfrac{1}{4}( - 16\vec i + 17\vec j + 7\vec k)
This is the required position of the center of mass.
Now we need to find the velocity of the center of mass. The formula for the instantaneous velocity of the center of mass is given by,
vcom=i=1nmivii=1nmi{\vec v_{com}} = \dfrac{{\sum\limits_{i = 1}^n {{m_i}{{\vec v}_i}} }}{{\sum\limits_{i = 1}^n {{m_i}} }}
vcom=m1v1+m2v2m1+m2\Rightarrow {\vec v_{com}} = \dfrac{{{m_1}{{\vec v}_1} + {m_2}{{\vec v}_2}}}{{{m_1} + {m_2}}}
Now substituting all the known values in the above formula we will get as,
vcom=100(10i7j3k)+300(7i9j+6k)100+300gm.m/sgm{\vec v_{com}} = \dfrac{{100(10\vec i - 7\vec j - 3\vec k) + 300(7\vec i - 9\vec j + 6\vec k)}}{{100 + 300}}\dfrac{{gm.m/s}}{{gm}}
vcom=100(10i7j3k)+300(7i9j+6k)100+300m/s\Rightarrow {\vec v_{com}} = \dfrac{{100(10\vec i - 7\vec j - 3\vec k) + 300(7\vec i - 9\vec j + 6\vec k)}}{{100 + 300}}m/s
vcom=14(10i7j3k+21i27j+18k)m/s\Rightarrow {\vec v_{com}} = \dfrac{1}{4}(10\vec i - 7\vec j - 3\vec k + 21\vec i - 27\vec j + 18\vec k)m/s
vcom=14(31i34j+15k)m/s\Rightarrow {\vec v_{com}} = \dfrac{1}{4}(31\vec i - 34\vec j + 15\vec k)m/s
Therefore this is the required velocity of the center of mass.

Note:
We should always note that the center of mass is a point that is hypothetical and it may either lie inside of the system or outside of the system. It is not necessary that there must be some material particle at the center of mass of the system. But in a homogeneous body that is the body that is having a uniform distribution of mass the center of mass will always coincide with the geometrical center of the body.