Understanding the Wedge Problem in Conservation of Momentum and Energy

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Homework Help Overview

The discussion revolves around a wedge problem involving conservation of momentum and energy, where a block of mass m rests on a wedge of mass M. The system starts at rest, and the goal is to find the velocity of the wedge when the block touches the table after falling a height h.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants discuss the conservation equations for momentum and energy, with attempts to derive the velocities of the wedge and block. Questions arise regarding the correct application of these equations and the relationships between the velocities of the block and the wedge.

Discussion Status

Some participants have offered guidance on correcting the momentum equation, while others express uncertainty about the accuracy of their conservation equations. There is an ongoing exploration of the relationships between the components of velocity and the implications for both the momentum and energy equations.

Contextual Notes

Participants note the challenge of interpreting the problem without visual aids and the potential confusion arising from different variable definitions. The discussion reflects a collaborative effort to clarify assumptions and refine the approach to the problem.

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Homework Statement



Attached in the files, scan from Resnick and Halliday. Also the answers (notice that I use a different meaning for [tex]u[/tex], but it shouldn't matter.

Homework Equations



Conservation of momentum, and conservation of energy.

The Attempt at a Solution



Initial Energy of the system is [tex]mgh[/tex], initial momentum is 0.
I'll call the velocity of the wedge [tex]u[/tex] and the velocity of the block [tex]v[/tex].
The equations:
[tex]2mgh = mv^2 + Mu^2[/tex] - all potential energy goes to the velocities of both objects.
[tex]Mu = -mv \cos \alpha[/tex] - conservation of momentum - only the horizontal component of [tex]v[/tex] is taken into consideration.

I end up having this as an answer:
[tex]u = \sqrt{\frac{2gh}{M^2 + Mm \cos ^2 \alpha}}m \cos \alpha[/tex]
Which is, not correct according to the answer.
What did I do wrong?
 

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I can't see the pictures pending approval, so I guessed at what the question is asking. I assumed that you are looking for the speed of the wedge and I got the same answer as you. What is the answer in the back of the book?
 
I'll type it in:
A block of mass m rests on a wedge of mass M which, in turn, rests on a horizontal table, as shown in Fig. All surfaces are frictionless. If the system starts at rest with point P of the block a distance h above the table, find the velocity of the wedge the instant point P touches the table.

Answer is:
[tex](\frac{u \cos \alpha}{\sqrt{1-u \cos ^2 \alpha}})\sqrt{2gh}[/tex]

[tex]u = \frac{m}{m+M}[/tex]

It has some similarities to my answer, so I guess the general idea I had in mind was correct. My guess is my conservation equations are not accurate (because I don't feel sure about them).
 
The problem with your expression is that the x component of the block's velocity is vblock*cosα relative to the wedge, not relative to the table. Relative to the table it is vblock*cosα - Vwedge.
 
so I need to replace it only in the momenton equation? What about the energy equation?
 
manenbu said:
so I need to replace it only in the momenton equation? What about the energy equation?
You'll need to modify both equations.
 
Meaning in the energy equation the vertical component of the block's velocity stays the same while the horizontal is relative?
I'll try.
 
So here is yet another attempt.
I'm out of ideas.
Where did I go wrong?
 

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I haven't had a chance to look at your attempt in detail (I will a bit later), but at first glance:
(1) Your energy equation is OK.
(2) Correct your momentum equation: The velocity of the wedge is -u (u is positive).
 
  • #10
It works. You should correct your momentum equation as Doc Al has suggested. From the momentum equation you should get

[tex]v cos\alpha = \frac{M+m}{m}u[/tex]

In order not to confuse your u with the book's u, let

[tex]\frac{M+m}{m} = \frac{1}{\beta}[/tex] so that

[tex]v cos\alpha = \frac{u}{\beta}[/tex]

Put that in your energy equation and it should come out.
 
  • #11
Ok, I got it. Thanks!
 

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