Understanding the Wedge Problem in Conservation of Momentum and Energy

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The discussion focuses on solving a physics problem involving the conservation of momentum and energy for a block on a wedge. The initial energy is expressed as mgh, and the momentum equations are analyzed, leading to an incorrect expression for the wedge's velocity. Participants clarify that the horizontal component of the block's velocity must be adjusted to account for the wedge's motion, impacting both momentum and energy equations. Ultimately, the correct relationships are established, guiding the user toward a solution. The conversation emphasizes the importance of accurately applying conservation principles in this context.
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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 u, 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 mgh, initial momentum is 0.
I'll call the velocity of the wedge u and the velocity of the block v.
The equations:
2mgh = mv^2 + Mu^2 - all potential energy goes to the velocities of both objects.
Mu = -mv \cos \alpha - conservation of momentum - only the horizontal component of v is taken into consideration.

I end up having this as an answer:
u = \sqrt{\frac{2gh}{M^2 + Mm \cos ^2 \alpha}}m \cos \alpha
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:
(\frac{u \cos \alpha}{\sqrt{1-u \cos ^2 \alpha}})\sqrt{2gh}

u = \frac{m}{m+M}

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

v cos\alpha = \frac{M+m}{m}u

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

\frac{M+m}{m} = \frac{1}{\beta} so that

v cos\alpha = \frac{u}{\beta}

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