What is the Displacement of the Wedge When the Smaller Block Reaches the Bottom?

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Homework Help Overview

The problem involves determining the displacement of a wedge when a smaller block reaches the bottom of the wedge. The context is rooted in dynamics, particularly focusing on forces acting on the block and wedge system, as well as energy conservation principles.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the equations governing the forces on the block and wedge, questioning the validity of certain assumptions, particularly regarding the normal force and the effects of acceleration. There are attempts to derive expressions for acceleration and displacement based on conservation laws.

Discussion Status

The discussion is active, with participants exploring different approaches, including the use of conservation of momentum. Some participants express uncertainty about the correctness of derived expressions and seek confirmation of their results, indicating a collaborative effort to clarify the problem.

Contextual Notes

Participants note discrepancies between their results and those in the solutions manual, suggesting potential flaws in the manual. There is an emphasis on finding the correct displacement rather than acceleration, highlighting the focus on the specific outcome of the problem.

utkarshakash
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Homework Statement


Find the displacement of wedge when the smaller block reaches the bottom of wedge.

Homework Equations



See attached diagram.

The Attempt at a Solution



For the smaller block,
N = mg \cos \theta \\<br /> <br /> mg \sin \theta = m v \dfrac{dv}{dx}

For wedge
N \sin \theta = M v \dfrac{dv}{dx}

Let the smaller block attain velocity v when it reaches the bottom and the velocity of wedge at that instant be v'.
Using conservation of energy,
\dfrac{mv^2}{2} + mgh = \dfrac{Mv&#039; ^2}{2}

Solving the above three equations gives me the displacement of wedge as 2h/cosΘ sinΘ. But unfortunately this is not the correct answer. Can anyone help me figure out the mistake?
 

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Your equation for N is only correct if m has no acceleration in the direction normal to the wedge's surface. Since the wedge accelerates that need not be true.
 
haruspex said:
Your equation for N is only correct if m has no acceleration in the direction normal to the wedge's surface. Since the wedge accelerates that need not be true.

OK. Let's say the wedge has an acceleration a' at any time t. Thus, If I take the wedge as the reference frame, I'd have to include a pseudo force as well towards left. So the equation for smaller block then becomes

N + ma&#039; \sin \theta = mg \cos \theta \\<br /> mg \sin \theta + ma&#039; \cos \theta = m v \dfrac{dv}{dx}

For the wedge, I can write

N \sin \theta = M v&#039; \frac{dv&#039;}{dx}

Since the block has two components of velocity when it reaches bottom viz. v' parallel to X-aixs and v parallel to inclined plane, the net velocity is v_{net} ^2 = v^2 + v&#039; ^2

Now If I use energy conservation

mgh = \dfrac{mv_{net} ^2}{2} + \dfrac{M v&#039; ^2}{2}

Solving the above equations, however, yield x = 0 !. :confused:
 
utkarshakash said:
OK. Let's say the wedge has an acceleration a' at any time t. Thus, If I take the wedge as the reference frame, I'd have to include a pseudo force as well towards left. So the equation for smaller block then becomes

N + ma&#039; \sin \theta = mg \cos \theta \\<br /> mg \sin \theta + ma&#039; \cos \theta = m v \dfrac{dv}{dx}

For the wedge, I can write

N \sin \theta = M v&#039; \frac{dv&#039;}{dx}

These equations are sufficient, I don't see the need of writing a' as v'dv'/dx or a as vdv/dx. Can you solve the above equations to find a and a'?
 
Pranav-Arora said:
These equations are sufficient, I don't see the need of writing a' as v'dv'/dx or a as vdv/dx. Can you solve the above equations to find a and a'?

a&#039; = \dfrac{mg \cos \theta \sin \theta}{M+m \sin ^2 \theta} \\<br /> a = g \sin \theta + \dfrac{mg \cos ^2 \theta \sin \theta}{M + m \sin ^2 \theta}

But I need to find displacement and not acceleration.
 
utkarshakash said:
a&#039; = \dfrac{mg \cos \theta \sin \theta}{M+m \sin ^2 \theta} \\<br /> a = g \sin \theta + \dfrac{mg \cos ^2 \theta \sin \theta}{M + m \sin ^2 \theta}

But I need to find displacement and not acceleration.

I haven't checked if the above expressions are correct.

Now that you have the accelerations, can you find the time it take the block to reach the ground? You have to find the displacement of wedge corresponding to this time.
 
Looks like we missed the easier approach.

The problem can be easily solved by conservation of linear momentum. :)
 
Pranav-Arora said:
I haven't checked if the above expressions are correct.

Now that you have the accelerations, can you find the time it take the block to reach the ground? You have to find the displacement of wedge corresponding to this time.

I get the answer as \dfrac{mh \cot \theta}{M+m}. But the correct answer is \dfrac{mh}{M+m}. In the meantime, I solved this problem using another method and got the same result.(the term that includes cotθ) So, I think there's a flaw in the solutions manual. But it'd be better if you could confirm my result.
 
utkarshakash said:
I get the answer as \dfrac{mh \cot \theta}{M+m}. But the correct answer is \dfrac{mh}{M+m}. In the meantime, I solved this problem using another method and got the same result.(the term that includes cotθ) So, I think there's a flaw in the solutions manual. But it'd be better if you could confirm my result.

I got the same answer as yours by both the methods. (Force and conservation of linear momentum) :)
 

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