Newtons Law: Determine Friction Forces on a Box at Rest

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The discussion centers on calculating the friction forces acting on a 22kg box at rest on a 45-degree ramp, with static and kinetic friction coefficients provided. Participants explore how to determine the maximum applied force that keeps the box stationary, emphasizing the importance of free body diagrams and the relationship between normal force and friction. They clarify that the normal force is influenced by the gravitational force and the applied force, and that friction acts down the incline when an upward force is applied. Additionally, they discuss the effects of a perpendicular force on the box, concluding that it reduces the normal force and thus the maximum static friction, which could lead to slipping if not properly balanced. The conversation highlights the need for a clear understanding of Newton's laws and the components of forces involved in the scenario.
  • #31
there is not enough frictional force for it to remain stationary thus it is overtaken and the box begins to slip. In other words the weight of the box is now to great for frictional force alone to keep the box from moving
 
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  • #32
No, that is not correct:

1. You do not add any weight to the box at all by applying a perpendicular force to it. You can only add weight to the object by either moving it to another planet with stronger value for g, ior more simply, add mass to the box.

2. Furthermore, even if you did that, the normal force N, that keeps the box from going through the incline would increase correspondingly, meaning that MAXIMAL STATIC FRICTION would also increase.

The proper explanation is the following:
By pulling perpendicular on the box (not pushing!), the normal force from the incline will be reduced, since the force it now has to counteract is no longer mgcos(45), but mgcos(45)-P, where P is the force by which you pull the box.

But this means that the maximal static friction ALSO decreases, since it is proportional to the normal force!

However, in order not to slip, the friction force has to balance gravity's component along the incline, mgsin(45).

Pulling too strongly on the box let's maximal static friction below the critical value mgsin(45), and the box starts slipping.

Did you get that?
 
  • #33
absolutely! if the book only explained things like you did i would be flying through this course.. so let's me see if i understand this..
that means that
Fsmax must be greater than mgsin 45 or it will yeild to gravitational pull along the incline? so do i know calculate at what value of p will cause fsmax to equal mgsin 45?
 
  • #34
Correct!
The simplest way to do this in order to get your signs right, is to split your calculations in two:

First find out the magnitude of normal force necessary to keep the box from slipping (Remember, maximal friction is proportional to the magnitude of the normal force!).
Here, evidently, the critical point is when maximal static force EQUALS the gravitational pull.

Secondly, find out what this means P should be.
 
  • #35
should i be using static friction or kinetic friction for this question?
 
  • #36
Hmm..there is a silliness in the exercise as given I overlooked:
Since the ramp happens to be angled at 45 degrees, the components of gravity along&perpendicular to the ramp are EQUAL.
But this means that with the coefficient of friction as given (less than 1), the box CANNOT be at rest on the ramp without an additional force pushing perpendicularly down on the box. Thus, contrary to what the exercise text said, the box isn't at rest UNLESS you apply a force on it.

Thus, you'll get a minimum push on the block, rather than a minimum pull.
The thinking given above in 32, however, remains correct.


It should be static friction!
 
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  • #37
should it be plus mgcos 45 +p or cos45 -p?
 
  • #38
I'll do this one for you:

If positive P is pulling (i.e, away from the incline), then the box remains at rest if:
\mu(mg\cos(45)-P)=mg\sin(45)
This is Newton's 2.law of motion along the incline when the acceleration is zero, with \mu the coefficient of static friction.
Thus, solving for P, we get:
P=mg\cos(45)-\frac{mg\sin(45)}{\mu}
this will be a negative number, i.e, we really have to push on the box in order to keep it in place.
 
  • #39
cause I am getting +p and it equates to 43 N
 
  • #40
i used downward being positive which gave me +p and its just the opposite sign it still works out to be 43 N is that correct?
 
  • #41
I haven't checked the numerical values; the sign change is because your positive p represents "push", whereas my positive P represents "pull"

(That is if you got -43 from my formula..)
 
  • #42
yes i did.. do you have msn messenger? it would be a lot faster talking over that you can add me if you do.. so that you won't have to give out your email address over the net
 
  • #43
Well, I'd like to keep my conversations here on PF, if you don't mind. But you can certainly use the private mail option here! :smile:

And, no, I haven't got myself MSN messenger yet. I think..
 
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  • #44
never really though of it. are you on often, because i just completed my last lesson and i am moving on to circular motion
i really appreciate the help.. and id prefer to just communicate threw private message, i like the way you teach and I am actually learning and absorbing what your telling me..
 
  • #45
Well, that's nice to hear!
As for me being on often..click on my profile to see how many posts a day I average.
You can PM me whenever you like.

Furthermore, there are a lot of others here at PF who are good at teaching maths&physics. Welcome aboard! :smile:
 

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