Inclined Plane with block of mass

In summary, the conversation discusses a block on an inclined plane and finding its acceleration based on known forces. The conversation also includes a diagram and calculations for various forces acting on the block. Ultimately, the solution is found by considering the effect of the pulley on the normal force and adjusting the calculated friction force accordingly.
  • #1
danago
Gold Member
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[SOLVED] Inclined Plane

A block of mass m sits on an inclined plane. The coefficient of kinetic friction is known. If the tension in the rope is T, and at the instant shown the block is moving down the slope, what is the blocks acceleration up the slope?

http://img374.imageshack.us/img374/2218/36905063xh5.gif

I started by drawing a free body diagram of the block.

http://img111.imageshack.us/img111/8047/96925869yv4.jpg

Where W is the force due to the weight of the block, P is the force from the pulley, F is the friction force and N is the normal force.

I can easily calculate the weight force and resolve it into components down the slope and perpendicular to the slope to find the normal force and the force down the slope. I can then use the normal force to find the frictional force.

What i am having trouble with is finding the force due to the pulley. I tried drawing a FBD of it, but I am not really sure how the tension in the rope applies a force to the pulley. Do i assume the force to be applied to the point where the rope first contacts each side of the pulley?
 
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  • #2
I came up with the following forces acting on the block:

[tex]
\begin{array}{l}
\overrightarrow W = \left( {\begin{array}{*{20}c}
{mg\sin \theta } \\
{ - mg\cos \theta } \\
\end{array}} \right) \\
\overrightarrow N = - \overrightarrow {W_y } = \left( {\begin{array}{*{20}c}
0 \\
{mg\cos \theta } \\
\end{array}} \right) \\
\overrightarrow F = - \mu _k \left| {\overrightarrow N } \right|\widehat{\underline i } = \left( {\begin{array}{*{20}c}
{ - \mu _k mg\cos \theta } \\
0 \\
\end{array}} \right) \\
\end{array}
[/tex]

The notation i am using for my vectors is as follows:

[tex]
\left( {\begin{array}{*{20}c}
a \\
b \\
\end{array}} \right) = a\widehat{\underline i } + b\widehat{\underline j }
[/tex]

Where i is a unit vector down the slope and j is a unit vector normal to the surface of the slope.
 
  • #3
assume the angle between ropes constant and the tension on rope is T.

P = T + T Cos (alpha)
(P is the force you show above)

N = mg Cos (alpha) - T Sin (alpha)
 
  • #4
Oh yep i see what i did wrong now. I forgot to consider the effect of the pulley on the normal force, which affected the friction force i calculated.

Thanks for the help :smile:
 

FAQ: Inclined Plane with block of mass

What is an inclined plane?

An inclined plane is a flat surface that is tilted at an angle to the horizontal. It is used to make it easier to lift heavy objects by reducing the amount of force needed.

How does an inclined plane work?

An inclined plane works by increasing the distance over which a force is applied in order to move an object. This decreases the amount of force needed to lift the object by spreading it out over a longer distance.

What is the formula for calculating the force needed to push an object up an inclined plane?

The formula for calculating the force needed to push an object up an inclined plane is F = mg sinθ, where F is the force, m is the mass of the object, g is the acceleration due to gravity, and θ is the angle of the incline.

How does the mass of the block affect the required force on an inclined plane?

The mass of the block affects the required force on an inclined plane because a heavier object will require more force to lift it up the same height on the inclined plane compared to a lighter object.

How does the angle of the inclined plane affect the force needed to lift the block?

The angle of the inclined plane affects the force needed to lift the block because a steeper angle will require more force to lift the block compared to a shallower angle. This is because the steeper angle increases the height that the block needs to be lifted, requiring more force to overcome the gravitational force acting on the block.

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