Newtons Law: Determine Friction Forces on a Box at Rest

AI Thread Summary
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.
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Sorry people, not sure where I am going wrong, I am just not sure in which direction to take this question. I don't even know where to start.

A box with mass of 22kg is at rest on a ramp inclined at 45 degrees to the horizontal. The coeffecient of friction between the box and ramp are (Static friction = 0.78, Kinetic Friction = 0.65)

a) determine the magnitude of the largest force that can be applied upward, parallel to the ramp, if the box ix to remain at rest

b) determine the magnitude of the smalled force that can be applied onto the top of the box, perpendicular to the ramp, if the box is to remain at rest
 
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for a start maybe u want to try drawing the free body diagram of the object and resolve the forces into 2 direction...
 
a)
i. Will an applied force parallell to the ramp influence the normal force?
ii. If you apply a "strong" parallell force upwards along the incline, in which direction will the frictional force point? Upwards along the incline or downwards?
 
i am doing this correspondence course and i don't have a teacher helping me so I am not exactly sure where to take this question. i have drawn the free body diagram and i am trying to resolve it into two direction I am just not sure what formulae i am supposed to be using to solve this question. As far as answering those questions you asked i have no idea that's exactly how its phrased in the book. As i said i have nobody else to ask for help
 
Try to answer the questions I gave you, they are perfectly clear. Use your head for example.
 
sorry about that .. i wasnt really paying attention
ai) an applied force will not influence the normal force.. at least i don't think it should
aii) frictional force will point downwards
 
quickslant said:
sorry about that .. i wasnt really paying attention
ai) an applied force will not influence the normal force.. at least i don't think it should
aii) frictional force will point downwards
Correct!

So, according to ai), you should be able to calculate the normal force without knowing what the applied force is. Do so!

As for ii), how is MAXIMAL STATIC FRICTION related to the normal force?
 
Coeffecient of static friction = Static friction max / force normal ??
 
Quite so, meaning that Static friction max=?
 
  • #10
force normal / coeffecient of static friction.

ok so here is what i have so far.. i calculated the force of gravity. 22 (9.8) then to calculate force norm do i do Fg cos 45?
 
  • #11
"force normal / coeffecient of static friction"
TOTALLY WRONG! THINK AGAIN!

Do not insert digits yet, keep the letters!
So, the force of gravity is mg, where m is the mass and g is the acceleration due to gravity.
Furthermore, as you've found out, the normal force N=mgcos(45).

Now, what should you do further?
 
  • #12
its sin 45.. ok.. so what i got so far is that force normal = mass (acceleration) sin 45, which = 22 (9.8) sin 45 which = 152.45 N correct?
now.. i take that and its force normal / coeffecient of static friction
which = 152.45 / 0.78 which i equate to equal 194.87 N correct?
 
  • #13
its force normal / coeffecient of static friction

THIS IS WRONG!
 
  • #14
sorry about that.. Fsmax = coeffecient of statfriction * Normal Force
 
  • #15
Yes, that's correct. Given the expression for the normal force in post 11, what is Fsmax?
 
  • #16
mgcos 45 * coeffecient Fs
 
  • #17
Correct!

Now, set up Newton's 2.law PARALLELL to the incline, knowing that the box is at rest, and that the applied force is called A.
 
  • #18
mgcos45 * coeffecient of Fs
 
  • #19
quickslant said:
mgcos45 * coeffecient of Fs
Eeh, is this Newton's 2.law of motion??
 
  • #20
ok done.. let me take a crack at this one more time :
force normal = mass (acceleration)cos 45, which = 22 (9.8) sin 45 which = 152.45 N correct?
now.. Fsmax = force normal * coeffecient of static friction
which = 152.45 * 0.78 which equals 118.9 N correct? when i did the diagram it only makes sense that the applied force can not exceed the normal force * coeffecient of static friction .. am i headed on the right track?
 
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  • #21
First of all, STOP PUTTING IN THOSE MEANINGLESS DIGITS YET!
Secondly: The normal force is mgcos(45). That it should be the cosine should be evident since when the inclination angle is 0, then the normal force equals mg, not 0 as would be the case using the sine function.

Thirdly, remember that the force of gravity also has a component along the incline.
Set up Newton's 2.law of motion along the incline!
 
  • #22
ok.. the book that i am using is absolutely worthless.. what it very vauge and i don't know how the expect people to teach themselves with it. what it has is a triangular block (wedge like) and it has Mg, Fn, Fsmax, and theta labelled. along the incline we have mgsin0 and that's all it shows
 
  • #23
all i get is that Fapp > Fsmax if it is to result in acceleration
 
  • #24
What is gravity's component along the incline, knowing that the inclination is (theta), or in this case, 45 degrees?
 
  • #25
i am so confused. I am sooo sorry I am just not getting it..
mgsin45?
 
  • #26
CORRECT!

Now, before continuing, let us recoup what we know about the forces along the incline:

1. Frictional force Ff: We have found that this equals Ff=(mu)mgcos(45), where (mu) is the coefficient of static friction.
Further, as you have stated, Ff works downwards along the incline.

2. Gravity's component: mgsin(45), this also works downwards along the incline.

3. Applied force A: This works UPWARDS along the incline as given in the exercise.


Now, relate these quantities together in Newton's 2.law along the incline, knowing that the box is at rest!
 
  • #27
ok.. so this is what my paper looks like

Fapp or A must not exceed ((mu)mg cos45 + mg sin 45) or the box will no longer be at rest according to Newtons 2nd law. am i in the right direction?
 
  • #28
That is correct!
And you're finished with a) now..:smile:

(OR, now you can put in the numbers if you like..)
 
  • #29
oh thank god.. now where do i start with b.. and again i thank you soooo much you don't know what this means to me!
 
  • #30
Okay, about b).

Before doing any maths at all, WHY would the box start sliding if you applied a too strong perpendicular force on it?
 
  • #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
 
  • #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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