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Physics 16 Online
OpenStudy (anonymous):

A small mass m is set on the surface of a sphere, the figure. If the coefficient of static friction is 0.75, at what angle ϕ would the mass start sliding?

OpenStudy (anonymous):

This is the figure: http://session.masteringphysics.com/problemAsset/1057220/4/GIANCOLI.ch05.p087.jpg

OpenStudy (anonymous):

This is my free-body diagram.

OpenStudy (anonymous):

I wanted to make sure that I got my angles on here right. I think I know how to solve it, but the cosine and sine always through me off. =/

OpenStudy (anonymous):

its better to resolve mg, along the directions of friction and Normal..

OpenStudy (anonymous):

So tilt the axis?

OpenStudy (anonymous):

yup yup.. i think you can do it this way.. but then u need to resolve friction as well.. we ll try this method later but m sure if u just resolve mg, like u said tilting the axis.. u ll get the answer pretty soon

OpenStudy (anonymous):

Okay, let me try that then.

OpenStudy (anonymous):

So, I kind of flipped the picture I drew in my notes so that the block was on top of the sphere so the normal force is opposite mg and not out at an angle. Is this right?

OpenStudy (anonymous):

no need to flip the pic.. just consider the flipped axis.. :P

OpenStudy (anonymous):

Oh, dang, I see what you mean.

OpenStudy (anonymous):

Let me use the power of paint to see if I got this right.

OpenStudy (anonymous):

ok.. i did it too.. u try.. and then i ll upload mine!

OpenStudy (anonymous):

Here is what I think it is supposed to look like.

OpenStudy (anonymous):

no thats wrong.. and when i say wrong.. i mean horribly wrong why are you resolving normal force? its already along your chosen y direction, and friction along your negative x direction, the only thing you have to resolve is Mg.. concentrate bro/sis !!

OpenStudy (anonymous):

1. Not appreciating the sarcasm as I am just as frustrated as you. 2. You said that I needed to resolve the normal force in your first response.

OpenStudy (anonymous):

lol m not frustrated :D.. sorry about that.. i have a habit of doing that.. :-/.. and no.. read again. i did mention resolve mg..!!

OpenStudy (anonymous):

@Hagopian13 can you try once again?!

OpenStudy (anonymous):

I am in the process of working on it.

OpenStudy (anonymous):

good good good.. ll wait..

OpenStudy (anonymous):

Okay, makes enough sense.

OpenStudy (anonymous):

as long as you get it :P

OpenStudy (anonymous):

so did you get the answer @Hagopian13

OpenStudy (anonymous):

Both angles are wrong.

OpenStudy (anonymous):

So lets stick to the free body diagram shall we? come on finish that.. you can do it ;-)

OpenStudy (anonymous):

I worked out the whole thing longhand and got 53.1 degrees off the y-axis for slide to begin. Does that sound right?

OpenStudy (anonymous):

I used the equations and drawing from this link: http://hyperphysics.phy-astr.gsu.edu/hbase/mincl2.html#c1

OpenStudy (anonymous):

If you use the above link, remember that it is measuring the theta angle from the x-axis and that was 36.9 degrees off the x-axis

OpenStudy (theeric):

Hi!! Look at my attachment - hopefully I didn't make any mistakes in setting the diagram up. I got the opposite of @biire, where I got \(36.9^\circ\) from the \(y\)-axis.

OpenStudy (theeric):

This is a neat physics trick. Pretty much, you want to examine the case where friction force is less than the gravitational force that will make it slide. So, I split up the forces in the picture. I saw that you did similarly. Anyway, \(\left| F_f\right|\lt \left|mg\sin\phi\right|\) We know what \(F_f\) is. \(F_f=F_N\ \mu\) And we know what \(F_N\) is. \(F_N=mg\cos\phi\) Going through those substitutions, \(F_f=F_N\ \mu\) \(F_f=mg\cos\phi\ \mu\) \(\left| mg\cos\phi\ \mu\right|\lt \left|mg\sin\phi\right|\) We can divide by \(\left| mg\right|\) to get \(\left| \cos\phi\ \mu\right|\lt \left|\sin\phi\right|\) Hmm.... \(\phi\) in two places... So... We fix that. \(\sin\) and \(\cos\) have a bunch of fun relations. One is \(\dfrac{\sin\theta}{\cos\theta}=\tan\theta\). So we divide by \(\left|\cos\phi\right|\) so we wind up with \(\phi\) in only one spot. Take a minute and look at that cool trick, if you want. So \(\left|\mu\right|\lt\dfrac{\sin\phi}{\cos\phi}\) \(\left|\mu\right|\lt\tan\phi\) And then we take the inverse tangent of both sides. I honestly don't know how this effects the inequality. Sometimes things like this will create more inequalities. But we'll find out for this problem by common sense in the context. We are looking for the angle where gravity is more than friction. \(\arctan\left|\mu\right|\ \ ?\ \ \phi\) \(\arctan(0.75)=36.869 ....^\circ=36.9^\circ=\phi\) So, if phi is less than this, normal force is greater (look at the diagram). So friction force will be greater than gravity. At that angle we found, the friction and gravity are equal (as if we went through with equalities rather than inequalities). So, when the angle is any greater than that... Which is pretty much just that angle... We see that the box will slide. Feel free to ask questions for me or whoever is on! Take care!

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