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

In summary, the displacement of the wedge when the smaller block reaches the bottom is given by \dfrac{mh \cot \theta}{M+m} or \dfrac{mh}{M+m} depending on the method used. There may be a flaw in the solutions manual as both methods yield the same result.
  • #1
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,
[itex] N = mg \cos \theta \\

mg \sin \theta = m v \dfrac{dv}{dx} [/itex]

For wedge
[itex] N \sin \theta = M v \dfrac{dv}{dx} [/itex]

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,
[itex] \dfrac{mv^2}{2} + mgh = \dfrac{Mv' ^2}{2} [/itex]

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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  • #2
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.
 
  • #3
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

[itex] N + ma' \sin \theta = mg \cos \theta \\
mg \sin \theta + ma' \cos \theta = m v \dfrac{dv}{dx}[/itex]

For the wedge, I can write

[itex] N \sin \theta = M v' \frac{dv'}{dx} [/itex]

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 [itex]v_{net} ^2 = v^2 + v' ^2 [/itex]

Now If I use energy conservation

[itex] mgh = \dfrac{mv_{net} ^2}{2} + \dfrac{M v' ^2}{2} [/itex]

Solving the above equations, however, yield x = 0 !. :confused:
 
  • #4
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

[itex] N + ma' \sin \theta = mg \cos \theta \\
mg \sin \theta + ma' \cos \theta = m v \dfrac{dv}{dx}[/itex]

For the wedge, I can write

[itex] N \sin \theta = M v' \frac{dv'}{dx} [/itex]

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'?
 
  • #5
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'?

[itex] a' = \dfrac{mg \cos \theta \sin \theta}{M+m \sin ^2 \theta} \\
a = g \sin \theta + \dfrac{mg \cos ^2 \theta \sin \theta}{M + m \sin ^2 \theta} [/itex]

But I need to find displacement and not acceleration.
 
  • #6
utkarshakash said:
[itex] a' = \dfrac{mg \cos \theta \sin \theta}{M+m \sin ^2 \theta} \\
a = g \sin \theta + \dfrac{mg \cos ^2 \theta \sin \theta}{M + m \sin ^2 \theta} [/itex]

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.
 
  • #7
Looks like we missed the easier approach.

The problem can be easily solved by conservation of linear momentum. :)
 
  • #8
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 [itex] \dfrac{mh \cot \theta}{M+m} [/itex]. But the correct answer is [itex] \dfrac{mh}{M+m} [/itex]. 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.
 
  • #9
utkarshakash said:
I get the answer as [itex] \dfrac{mh \cot \theta}{M+m} [/itex]. But the correct answer is [itex] \dfrac{mh}{M+m} [/itex]. 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) :)
 

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

What is the definition of displacement?

Displacement is the distance and direction of an object's change in position from its original starting point.

How is displacement related to wedge?

In the context of wedges, displacement refers to the movement of the wedge as it is used to separate or lift objects.

How is the displacement of a wedge calculated?

The displacement of a wedge can be calculated by measuring the distance between the starting and ending positions of the wedge.

What factors affect the displacement of a wedge?

The displacement of a wedge can be affected by the angle of the wedge, the material it is being used on, and the amount of force being applied.

How does the displacement of a wedge affect its mechanical advantage?

The displacement of a wedge is directly related to its mechanical advantage. The larger the displacement, the greater the mechanical advantage of the wedge.

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