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Center of Mass question

2025 · 29 Jan · Shift 2 · Q51
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Center of Mass question

2025 · 29 Jan · Shift 2 · Q51

JEE MainPhysicsCenter of MassMCQ+4 / −1
JEE Main 2025 (Online) 29th January Evening Shift Physics - Center of Mass and Collision Question 7 English Three equal masses mmm are kept at vertices (A,B,C)(A, B, C)(A,B,C) of an equilateral triangle of side a in free space. At t=0t=0t=0, they are given an initial velocity VA→=V0AC→,VB→=V0BA→\overrightarrow{V_A}=V_0 \overrightarrow{A C}, \overrightarrow{V_B}=V_0 \overrightarrow{B A}VA​​=V0​AC,VB​​=V0​BA and VC→=V0CB→\overrightarrow{V_C}=V_0 \overrightarrow{C B}VC​​=V0​CB. Here, AC→,CB→\overrightarrow{A C}, \overrightarrow{C B}AC,CB and BA→\overrightarrow{B A}BA are unit vectors along the edges of the triangle. If the three masses interact gravitationally, then the magnitude of the net angular momentum of the system at the point of collision is :
  1. A
    12\frac{1}{2}21​ a mV0\mathrm{mV}_0mV0​
  2. B
    3 a mV0\mathrm{mV}_0mV0​
  3. C
    32\frac{3}{2}23​ a mV0\mathrm{mV}_0mV0​
  4. D
    32\frac{\sqrt{3}}{2}23​​ a mV0\mathrm{m}V_0mV0​
View written solutionFree

Correct answer: D

  1. Key idea: angular momentum about the center of mass is conserved

Since the masses interact only through internal gravitational forces, the net external torque on the system is zero. Hence, the total angular momentum of the system about the center of mass remains constant.

At the instant of collision, all three particles meet at one point. The angular momentum of the system about that collision point is the same as the angular momentum about the center of mass, because the collision point is the center of mass of the system.

So we only need to calculate the initial angular momentum about the center of mass.


  1. Geometry of the equilateral triangle

Let the center of mass (which is also the centroid for equal masses) be OOO.

For an equilateral triangle of side aaa, the distance from centroid to each vertex is

R=a3.R=\frac{a}{\sqrt{3}}.R=3​a​.

Place the triangle so that the vertices are at angular positions 0∘,120∘,240∘0^\circ,120^\circ,240^\circ0∘,120∘,240∘ around OOO.

Each mass has speed V0V_0V0​, directed along the side:

  • at AAA: along ACACAC
  • at BBB: along BABABA
  • at CCC: along CBCBCB

By symmetry, each velocity makes the same angle with the corresponding radius vector from OOO.


  1. Find the angle between radius vector and velocity

In an equilateral triangle, the line from a vertex to the centroid bisects the 60∘60^\circ60∘ angle there. So the radius vector OA→\overrightarrow{OA}OA makes 30∘30^\circ30∘ with each side through AAA.

But the position vector of mass at AAA relative to the center is OA→\overrightarrow{OA}OA, while its velocity is along ACACAC. Therefore the angle between OA→\overrightarrow{OA}OA and VA→\overrightarrow{V_A}VA​​ is

30∘.30^\circ.30∘.

Similarly for the other two masses.

Hence angular momentum magnitude of each particle about OOO is

L1=mRV0sin⁡30∘=m(a3)V0(12)=amV023.L_1 = mRV_0\sin 30^\circ = m\left(\frac{a}{\sqrt{3}}\right)V_0\left(\frac12\right) = \frac{amV_0}{2\sqrt{3}}.L1​=mRV0​sin30∘=m(3​a​)V0​(21​)=23​amV0​​.
  1. Direction of angular momentum of each mass

Now check whether the three angular momenta add or cancel.

The directions of velocities are cyclic: A→CA\to CA→C, C→BC\to BC→B, B→AB\to AB→A. This corresponds to the same sense of rotation for all three particles about the center. Therefore, all three angular momentum vectors are parallel and add directly.

So total angular momentum is

L=3L1=3⋅amV023=32amV0.L = 3L_1 = 3\cdot \frac{amV_0}{2\sqrt{3}} = \frac{\sqrt{3}}{2}amV_0.L=3L1​=3⋅23​amV0​​=23​​amV0​.
  1. Angular momentum at collision

Since angular momentum is conserved, the magnitude of the net angular momentum at the point of collision is the same:

32amV0\boxed{\frac{\sqrt{3}}{2}amV_0}23​​amV0​​
  1. Option check
  • A: 12amV0\frac12 amV_021​amV0​ ❌
  • B: 3amV03amV_03amV0​ ❌
  • C: 32amV0\frac32 amV_023​amV0​ ❌
  • D: 32amV0\frac{\sqrt{3}}{2}amV_023​​amV0​ ✅

Therefore, the correct answer is Option D.

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