How Does Horizontal Acceleration Keep a Block Stationary on a Wedge?

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The discussion revolves around understanding how horizontal acceleration of a wedge can keep a block stationary relative to it. To achieve this, the wedge must accelerate horizontally, allowing the block to maintain its position on the inclined surface without sliding off. The key equations derived include the relationship between the normal force and gravitational force, as well as the requirement that the horizontal acceleration of the block equals that of the wedge. The solution shows that the applied force must account for both the mass of the block and the wedge, leading to the conclusion that the force is proportional to the tangent of the wedge's angle. This illustrates the principles of inertia and acceleration in a frictionless environment.
Rococo
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Homework Statement



A wedge of mass M rests on a horizontal table. A block of mass m rests on the wedge.

http://imgur.com/cS02MvM

(a) What horizontal acceleration, a, must M have relative to the table to keep the block stationary relative to the wedge, assuming no friction?

(b) What horizontal force F must be applied to the system to achieve this result, assuming a frictionless table top?

Homework Equations



F=(m+M)a

The Attempt at a Solution



http://imgur.com/etif1qn

All I have so far is this diagram as I don't understand the concept involved. Its not clear to me why the horizontal acceleration of the wedge could keep the block stationary. Also, I'm not sure whether this acceleration would be to the left or to the right.

Also I have read through other similar threads but still can not understand the problem.
 
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Rococo said:

Homework Statement



A wedge of mass M rests on a horizontal table. A block of mass m rests on the wedge.

cS02MvM.jpg


(a) What horizontal acceleration, a, must M have relative to the table to keep the block stationary relative to the wedge, assuming no friction?

(b) What horizontal force F must be applied to the system to achieve this result, assuming a frictionless table top?

Homework Equations



F=(m+M)a


The Attempt at a Solution



etif1qn.jpg


All I have so far is this diagram as I don't understand the concept involved. Its not clear to me why the horizontal acceleration of the wedge could keep the block stationary. Also, I'm not sure whether this acceleration would be to the left or to the right.

Also I have read through other similar threads but still can not understand the problem.

Start by writing the FBD equations. Note that for mass m to be stationary with respect to the wedge, its vertical acceleration must be zero, and it horizontal acceleration must be equal to that of M.
 
Rococo said:
Its not clear to me why the horizontal acceleration of the wedge could keep the block stationary.
It does not keep the block stationary. It keeps it stationary relative to the wedge.
To get the concept, imagine you have a block of ice on a flat tray. If you pull the tray swiftly to one side the ice block will be left behind. Now make the tray slightly wedge shaped so that the ice has to rise slightly in order to slide off. It will still slide off if you jerk the tray fast enough. So increase the slope a bit more...
 
Start by writing Free body diagrams.Create equations applying
ƩFx=max &
ƩFy=may

This will give all the needed equations.
 
voko said:
Start by writing the FBD equations. Note that for mass m to be stationary with respect to the wedge, its vertical acceleration must be zero, and it horizontal acceleration must be equal to that of M.

Here's what I got:

Ncos30° = mg

Nsin30° = F = (m+M)a

Is this right?
 
haruspex said:
It does not keep the block stationary. It keeps it stationary relative to the wedge.
To get the concept, imagine you have a block of ice on a flat tray. If you pull the tray swiftly to one side the ice block will be left behind. Now make the tray slightly wedge shaped so that the ice has to rise slightly in order to slide off. It will still slide off if you jerk the tray fast enough. So increase the slope a bit more...

What's the reason this happens? Is it just as a result of the inertia of the block?
 
Rococo said:
Here's what I got:

Ncos30° = mg

Nsin30° = F = (m+M)a

Is this right?
The first equation, yes. But is F above the force applied to the wedge, as in the question? Why would that be equal to N sin 30? What body did you study an FBD of to obtain it?
 
Rococo said:
What's the reason this happens? Is it just as a result of the inertia of the block?
Yes. For the block to accelerate as fast as the wedge it needs a sufficient horizontal force. If the slope is too low or the friction inadequate then it won't keep up.
 
haruspex said:
The first equation, yes. But is F above the force applied to the wedge, as in the question? Why would that be equal to N sin 30? What body did you study an FBD of to obtain it?

Yes, F is the force applied to the wedge.

I realize F is not equal to Nsin30° now. The horizontal force acting on the block is Nsin30°. The horiztonal force acting on the wedge is F.

As voko said, the horizontal acceleration of the block must be equal to the horizontal acceleration of the wedge. So, since acceleration is force divided by mass I get this:

(Nsin30°)/m = F/(m+M)
 
  • #10
Rococo said:
Yes, F is the force applied to the wedge.

I realize F is not equal to Nsin30° now. The horizontal force acting on the block is Nsin30°. The horiztonal force acting on the wedge is F.

As voko said, the horizontal acceleration of the block must be equal to the horizontal acceleration of the wedge. So, since acceleration is force divided by mass I get this:

(Nsin30°)/m = F/(m+M)
Yes.
 
  • #11
haruspex said:
Yes.

Using the two equations:

(Nsin30°)/m = F/(m+M)
Ncos30° = mg

I was able to rearrange to get the following:

F/(m+M) = gtan30°
a = gtan30°
F = (m+M)gtan30°
 
  • #12
Rococo said:
Using the two equations:

(Nsin30°)/m = F/(m+M)
Ncos30° = mg

I was able to rearrange to get the following:

F/(m+M) = gtan30°
a = gtan30°
F = (m+M)gtan30°
Looks good.
 

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