# Block on a moving inclined plane

1. Sep 30, 2008

### M4573R

1. The problem statement, all variables and given/known data
A block of mass M is on a plane with an incline of Theta. What horizontal force must the ramp be pushed so that the block does not move relative to the ramp.

This is to be solved generally.

2. Relevant equations
Force of gravity on block: m*g*sin(theta)
Normal force: -m*g*cos(theta)

3. The attempt at a solution
I have no idea where I should start.
I the normal force needs to counteract the force of gravity on the block, but I don't know how the horizontal force on the ramp factors into the normal force.

2. Sep 30, 2008

### LowlyPion

Welcome to PF.

You have 2 forces acting on the block.
Gravity acting vertically and the force of the ramp pushing horizontally against the block.
To keep the block from moving then the components acting along the plane of the incline must cancel.
The forces normal to the incline aren't useful for your purposes.

3. Sep 30, 2008

### M4573R

Is the force that the ramp is exerting on the block all in the normal force? And the normal force has a vertical and horizontal component?

After doing some trig I came to the answer that the ramp must push horizontally at m*g. Which happens to be the vertical force on the block. Is this correct? The normal Force keeps throwing me off.

4. Sep 30, 2008

### LowlyPion

No.

The m*g is acting along the incline with m*g*sinθ .

The force that the incline is exerting on the block is as the incline accelerates horizontally.
This translates into an m*a component up the ramp as a function of θ .

5. Sep 30, 2008

### M4573R

I'm just not sure what forces I have to cancel here. I've got a force down the slope, I've got a force of gravity pointing down, a normal force pointing perpendicular to the slope, and a force pushing horizontally on the block.

6. Sep 30, 2008

### LowlyPion

Gravity acts downward.

It results in 2 components. Normal to the incline and parallel along the plane of the incline. That force is determined by the angle as Sinθ.

You're done with gravity.

Now the incline is accelerating at some rate if it is to exert a force. That force resolves itself into two components as well. The acceleration needed to keep the block steady creates an m*a*???θ that must equal the m*g*sinθ .

7. Sep 30, 2008

### M4573R

The accelerating ramp produces the horizontal force and the normal force of mg*cos(theta). Do I just need the normal force to equal the force down the slope?

8. Sep 30, 2008

### LowlyPion

No. I've already pointed out that the normal force component of gravity does not matter. m*g*cosθ is not useful.

"a" is the acceleration of the incline. It is the component of "a"*m that is parallel to the incline that you use.

9. Sep 30, 2008

### M4573R

I'm sorry that I'm not getting this yet. Soon or later its going to click. All my common sense tells me that the ramps horizontal force is acting along the normal of the block and that I need it to solve the problem.

If I have the force of the ramp as m*a:
Fblock = m*a, I can solve for a = Fblock / m.

You're saying this acceleration as the equal the acceleration of the block perpendicular to the ramp (g*sin(theta))?

As in
Fblock / m = g*sin(theta)
so the Force of the ramp = mg*sin(theta)?

Edit: Force on the ramp must = (mass of the ramp) * sin(theta)?

Edit2: Another try:
acceleration of the block = g*sin(theta)
horizontal acceleration of ramp = (Force of ramp / mass of ramp)
cos(theta) = ramps acceleration parallel to block's / horizontal acceleration of ramp
since acceleration parallel to block's must = g*sin(theta),
cos(theta) = g*sin(theta) / accel of ramp
Force of ramp = (mass of ramp * g * sin(theta)) / cos(theta)

Force on ramp = mass of ramp * g * tan(theta)

I don't know what else to try.

Last edited: Sep 30, 2008
10. Sep 30, 2008

### LowlyPion

That's just about it. I think the question wants it in terms of M. (The mass of the ramp/inclined plane is not given.)

It's probably easier to think in terms of the ramp accelerating, to determine the angle, because the actual force on the block balances when it is being accelerated in this fashion. That then makes the overall force on the ramp = to the acceleration of the ramp (is it massless, the problem doesn't say) and the acceleration imparted to the block of mass M.