Conservation of Linear Momentum of Rigid Body

Click For Summary
SUMMARY

The discussion focuses on the conservation of linear momentum in a rigid body system involving three particles (A, B, and C) during an impact scenario. Two methods were employed to analyze the problem: the first method utilized the conservation of linear momentum with vector velocities, resulting in a final velocity of particles A and B as v_f = √(6gh). The second method, which considered the center of gravity (CG) of the rigid body, indicated that the CG's velocity after impact equals its velocity before impact, leading to the same angular speed formula ω = √(6gh)/a. However, discrepancies arose regarding the correct answer, which included a factor of 2, prompting a discussion on the effects of external forces and assumptions about particle C's inertia.

PREREQUISITES
  • Understanding of linear momentum and its conservation principles.
  • Familiarity with vector velocity calculations in physics.
  • Knowledge of angular momentum and its relation to rigid body dynamics.
  • Basic trigonometry, particularly involving angles like 30º and 60º.
NEXT STEPS
  • Study the principles of conservation of linear momentum in multi-body systems.
  • Learn about the effects of external forces on momentum conservation.
  • Explore the relationship between linear and angular momentum in rigid body dynamics.
  • Investigate the implications of negligible moment of inertia in collision problems.
USEFUL FOR

Physics students, mechanical engineers, and anyone studying rigid body dynamics and collision analysis will benefit from this discussion.

Uchida
Messages
22
Reaction score
6
Homework Statement
Consider a determined structure of three particles, each with mass m, interconnected by rigid bars of negligible mass forming an equilateral triangle on the side a.
The structure falls from a height h, as shown in the figure and the particle C hooks on the stop.

The angular velocity of the structure immediately after the impact is:
Relevant Equations
Conservation of Linear Momentum
Imagem 135.jpg


I solved it by two methods:

-----------------------------------------------------

First, by conservation of linear momentum, using the vector velocities of each particle:

In the imminence of the impact, the velocity of all the three particles are the same, \vec v_0 = - \sqrt{2gh} \hat j
After que impact, C will have zero velocity, and particles A and B will have velocities with the same magnitude v_f, in the perpendicular direction of the bars connected to them. Therefore:

\vec v_A = - v_fsin(30º) \hat i - v_fcos(30º) \hat j
\vec v_B = v_fsin(30º) \hat i - v_fcos(30º) \hat j

By conservation of linear momentum:

m_A\vec v_0 + m_B\vec v_0 + m_C\vec v_0 = m_A\vec v_A + m_B\vec v_B + m_B\vec v_C

Considering m_A = m_B = m_C = m and \vec v_C = 0, we have:

3m\vec v_0 = 2m(\vec v_A + \vec v_B)

-3\sqrt{2gh} \hat j = -2v_fcos(30º) \hat j

Which give us: v_f = ||v_A|| = ||v_B|| = \sqrt{6gh}

The angular speed of the rigid body can be calculated as ω = \frac{v_t}{r}. where v_t = v_f and r = a.

Finally:
ω = \frac{\sqrt{6gh}}{a}-----------------------------------------------------

The second method, by conservation of linear momentum of the center of gravity of the rigid body.
This method is more straight forward, and the calculations give the velocity of CG after the impact equal to the velocity in the imminence of the impact. v_{f_{CG}} = v_{0_{CG}} = \sqrt{2gh}

The distance of CG from the particle C is r_{CG} = a\frac{2}{3}{cos(30º)} = \frac{a \sqrt{3}}{3}

The angular speed of the rigid body can be calculated as ω = \frac{v_{f_{CG}}}{r_{CG}}.

Finally:
ω = \frac{\sqrt{6gh}}{a}
The problem is, that the correct answer to the question is:
onde.png


The "correct" answer has a 2 dividing the result I found, and there is no answer key to the result I got.

Can someone please help me find where I am wrong, or validate my methods (which would mean that the answer key to the question must be wrong).
 
  • Like
Likes   Reactions: Delta2
Physics news on Phys.org
The total linear momentum of the 3-particle system is not conserved when particle C collides with the support. The support exerts an external, impulsive force on the system that changes the linear momentum.
 
Last edited:
TSny deals with the first method and the conservation of momentum issue of the second.
Another problem with the second approach is, I think, that you take ##v_{CG}## as the velocity of all the masses immediately prior to impact.
On impact, C stops and A & B do not increase their vertical speed (the only possible forces on them are upwards and sideways.) The vertical speed of the CG must be between that of C (zero) and that of A & B, hence less than ##\sqrt{2gh}##, though that speed may not be relevant if momentum is changed.

The only approach that got me the official answer, was to assume C is small, having negligible moment of inertia and negligible friction with the stop bracket.
 
The angular momentum relative to point C just before colisión Is ##L=2m\sqrt(2gh)a\sin(60)## and it's conserved. Upon collision the sistem rotates around C
##2m\sqrt(2gh)a\sin(60)=2ma^2\omega##
##\omega=\frac{\sqrt(6gh)}{2a}##
 

Similar threads

  • · Replies 11 ·
Replies
11
Views
2K
  • · Replies 7 ·
Replies
7
Views
995
  • · Replies 7 ·
Replies
7
Views
2K
Replies
38
Views
4K
  • · Replies 20 ·
Replies
20
Views
2K
Replies
3
Views
2K
  • · Replies 5 ·
Replies
5
Views
3K
  • · Replies 12 ·
Replies
12
Views
2K
  • · Replies 7 ·
Replies
7
Views
5K
Replies
20
Views
3K