Solving Inclined Plane Problems

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Homework Help Overview

The discussion revolves around a physics problem involving a block on an inclined plane, where participants are tasked with finding the frictional force and the horizontal force acting on the block. The scenario includes a mass of 100kg, a ramp inclined at 20 degrees, and a coefficient of friction of 0.7.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants explore the breakdown of forces acting on the block, including gravitational forces and applied forces. There are attempts to derive equations for net forces in both the vertical and horizontal directions. Some participants express uncertainty about the role of friction and the correct application of Newton's laws.

Discussion Status

The discussion is ongoing, with participants providing insights and corrections to each other's reasoning. Some have suggested re-evaluating the definitions of net forces and the conditions under which the block is moving or at rest. There is a focus on deriving simultaneous equations to solve for unknowns, but no consensus has been reached on the correctness of the approaches taken.

Contextual Notes

Participants are working under the assumption that the force P is just sufficient to initiate movement or maintain constant velocity, leading to discussions about static versus dynamic friction. There is also mention of confusion regarding the terminology used, particularly the term "net force."

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Homework Statement



A block with a mass of 100kg is being pulled with a force P in and effort to move it down the ramp. The ramp makes a 20 degree with the horizontal ground. The coefficient of the friction between the ramp and the block is 0.7.

Find the frictional force and the horizontal force.

ppSDyCA.jpg


Assume g=10m/s^2

Homework Equations



Inclined plane equations

The Attempt at a Solution



Let
F(y) = vertical force due to gravity.

F(py) = vertical force due to applied force.

F(x) = horizontal force due to gravity

F(px) = horizontal force due to applied force P.

F(yNet)
= Total vertical net force
= F(y) - F(py)
= mg(cos(theta)) - P(sin(theta))
= 1000cos20 - Psin20

F(xNet)
= Total horizontal net force
= F(x) + F(py)
= mg(sin(theta)) - P(cos(theta))
= 1000sin20 - Pcos20

Am I doing it right above?

Let
F(N) be the normal force.

My rationale is that since the horizontal force P lifts the mass upwards, it's force acting downwards will be reduced.

Am I right to say that,
F(N) = F(yNet)
Normal force = The net force acting vertically downware to the ramp.

Am I getting the concept right or wrong?

I am now stuck at this part because I have so many unknown. I still can't find P. Can someone correct my understanding? Thank you all.
 
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What happened to the friction?
 
Sorry let me re edit again for F(xNet)

Let F(f) = Frictional Force

F(xNet)
= Total horizontal net force
= F(x) + F(px) - F(f)
= mg(sin(theta)) + P(cos(theta)) - F(f)
= 1000sin20 + Pcos20 - F(f)

I still can't figure how to find the frictional force.

I know
F(f)
= F(N) * mu
= F(yNet) * 0.7
= 700cos 20 - 0.7Psin20

Did I make anymore mistakes? How do I move on from here?
 
Last edited:
I haven't gone through all your work. Your use of the word "net" is what is confusing me.

Assume for this problem that the force P is just large enough to get the block moving, but no more than that. If you prefer, you may think of the block sitting at rest on the ramp, but just almost enough to start moving. Or alternately, if it is moving, it is moving down the ramp at a constant velocity. My point is that it is not accelerating.

Given the lack of acceleration, what does Newton's second law of motion tell you about the net force on the block?

The next step is to break of the force equations into their x- and y- components. That will give you two simultaneous equations (one for the horizontal and another for the vertical). Two equations, two unknowns. :wink:
 
I have broken down the forces and I am not sure if I am right. I will re-edit my working again.

CVvO6ZI.jpg


(Note: Force P is parallel to the horizontal ground.)

F(gx) = Force parallel to the inclined due to gravity.

F(gy) = Force perpedicular to the inclined due to gravity.

F(px) = Force parallel to the inclined due to Force P.

F(py) = Force perpedicular to the inclined due to Force P.

Using Newton's second law, I will attempt to find the value P that allows it to move from rest. Net force = 0N

F(N) = The normal force perpendicular to the inclined.

F(f) = Frictional Force

For net force parallel to the ramp = 0N,
F(f) = F(gx) + F(px)
F(N)*mu = 1000sin20 + Pcos20
0.7(F(N)) = 1000sin20 + Pcos20
[Equation 1]

For net force perpendicular to the ramp = 0N,

F(N) = F(gy) - F(py)
F(N) = 1000cos20 - Psin20
[Equation 2]

Substitute equation 2 into equation 1.
0.7(1000cos20-Psin20) = 1000sin20+Pcos20

Eventually I get
P=267.80N approximately.

F(f)= F(N) * mu
F(f)
= 1000cos20-267.80sin20
= 848.10N

I get Force P=267.80N
Frictional Force = 848.10N

Both answers are still wrong. What am I doing wrongly?
 
Last edited:
Something goes wrong during your 'Eventually'. Please post the detailed working.
 

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