Work,energy COM and linear momentum conservation

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Homework Help Overview

The problem involves a wagon with mass M moving on a frictionless surface, with an ideal pendulum attached. Initially at rest, the pendulum makes an angle x with the vertical, and the question seeks to determine the wagon's velocity when the pendulum makes an angle y with the vertical. The context relates to concepts of work, energy, and conservation of momentum.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the conservation of linear momentum and energy within the system. There are attempts to formulate equations relating the velocities of the wagon and the pendulum bob, with some questioning the reference frame and the nature of the forces involved.

Discussion Status

The discussion is active, with participants providing insights into the conservation principles applicable to the problem. Some guidance has been offered regarding the equations that relate the components of velocity, but there is no explicit consensus on the formulations or the reference frame to be used.

Contextual Notes

Participants are navigating the complexities of the problem, including the implications of choosing different reference frames and the associated fictitious forces. There is an acknowledgment of the need to clarify the relationships between the various components of motion.

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Homework Statement


A wagon with mass M can move on frictionless surface. A mathematical/ideal pendulum is fastened on the wagon. At the initial moment the wagon and the pendulum were at rest and the pendulum makes an angle of x with the vertical. What will be the velocity of the wagon when the pendulum makes an angle of y with the vertical?


Homework Equations


I guess its a linear momentum question but I don't know the equation.


The Attempt at a Solution

 
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Hi,

1 - You nearly got the 1st thing right. Since friction is neglected, the system wagon-pendulum experiences no horizontal force, and thus its horizontal component of linear momentum is conserved. From this, you have the 1st equation relating the horizontal components of the velocities of the wagon and the bob [tex]v_{h(wagon)}[/tex] and [tex]v_{h(bob)}[/tex] respectively.

2 - The 2nd conserved thing is the total energy of the system, which comprises of the potential energy of the bob and the kinetic energies of the wagon and the bob. This is the 2nd equation, which relates [tex]v_{h(wagon)}[/tex] , [tex]v_{h(bob)}[/tex] , [tex]v_{v(bob)}[/tex] - the vertical component of the bob's velocity and the angles x, y.

3 - The 3rd condition is that in the reference frame of the wagon, the velocity of the bob is perpendicular to the string. You should deduce the 3rd equation relating [tex]v_{h(wagon)}[/tex] , [tex]v_{h(bob)}[/tex] , [tex]v_{v(bob)}[/tex] and the angle y.

Try to write down the equations :smile:
 
well i m not sure of the first equation.
is it mv(bob)= - Mv(wagon)??
 
It's [tex]mv_{h(bob)} = - Mv_{h(wagon)}[/tex]. (horizontal component!)
 
but the velocity of bob is it relative to the ground??
 
Yes. If you choose the reference frame of the wagon from the start, you have to take into account the fictitious force, which is unnecessarily complicated.
 

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