How can I find the critical mu of friction?

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To find the critical coefficient of static friction (μ) for a box being pushed at an angle θ, the correct formula is μ = 1/tan(θ). The initial equations derived by the student included terms for the applied force (F) and gravitational force (mg), leading to confusion. As the pushing force increases, the influence of gravity diminishes, simplifying the relationship to μ ≤ (1/tanθ). The discussion emphasizes the importance of understanding the limits of μ as the applied force approaches infinity, confirming that if μ exceeds 1/tan(θ), the box cannot be moved. The final consensus is that the textbook's answer is indeed correct.
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Homework Statement



A lady pushes a box with mass (m) with force (F) at a horizontal angle of θ. There is a static friction (μ)

Homework Equations



ƩFy = Fn - m*g - F*sinθ = 0

ƩFx = F*cosθ - μFn = 0, where μFn is the force of friction.

The Attempt at a Solution



F*cosθ - μ*Fn = 0

μ*Fn = F*cosθ; and Fn = m*g + F*sinθ

So, μ(m*g + F*sinθ) = F*cosθ

μ = (F*cosθ)/(m*g + F*sinθ)

But the textbook's answer is μ = 1/tanθ. Is it wrong? I almost get their answer except for the m*g. And when I use dummy values I don't get the same answer as the book, so I am pretty sure that my problem is from not simplifying the equation enough.
 
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The answer must have F in it somewhere! So yeah, the book answer is wrong. I believe.
My answer has tan(theta) in it, but it also has mg and F.
(Ooh, can't wait to be corrected on this one by some smart ME! :smile: )
 
rude man said:
The answer must have F in it somewhere! So yeah, the book answer is wrong. I believe.
My answer has tan(theta) in it, but it also has mg and F.
(Ooh, can't wait to be corrected on this one by some smart ME! :smile: )

Is your answer equivalent to mine?
 
student34 said:
Is your answer equivalent to mine?

'Fraid not.

Don't even bother to write separate equations in x and y.

The lady has to overcome two forces as she's pushing the mass uphill. What are those two forces (along the ramp)?
 
student34 said:
A lady pushes a box with mass (m) with force (F) at a horizontal angle of θ. There is a static friction (μ)
Is she pushing down at angle theta or up at that angle? I'll guess it's up.
You haven't said what the question asks. I'll guess again: it asks for the angle which minimises F.
 
haruspex said:
Is she pushing down at angle theta or up at that angle? I'll guess it's up.
You haven't said what the question asks. I'll guess again: it asks for the angle which minimises F.

She pushes down at an angle θ below the horizontal.
 
You're still not saying what the book actually asks. Pls post the whole question verbatim.
 
haruspex said:
You're still not saying what the book actually asks. Pls post the whole question verbatim.

I am not sure if I have to do this, but I am going to reference the question just in case I am not committing some kind of plagiarism. So just ignore the reference.

"A large crate with mass m rests on a horizontal floor. The coefficients of friction between the crate and the floor are μ(static) and μ(kinetic). A woman pushes downward at an angle θ below the horizontal on the crate with force F. If μ(static) is greater than some critical value, the woman cannot start the crate moving no matter how hard she pushes. Calculate this critical value of μ(static)" (P167).

Referenced from Sears and Zemansky's University Physics (Young and Freedman 13th Edition)
 
student34 said:
I am not sure if I have to do this, but I am going to reference the question just in case I am not committing some kind of plagiarism. So just ignore the reference.

"A large crate with mass m rests on a horizontal floor. The coefficients of friction between the crate and the floor are μ(static) and μ(kinetic). A woman pushes downward at an angle θ below the horizontal on the crate with force F. If μ(static) is greater than some critical value, the woman cannot start the crate moving no matter how hard she pushes. Calculate this critical value of μ(static)" (P167).

Referenced from Sears and Zemansky's University Physics (Young and Freedman 13th Edition)

Showing the complete problem does help very much.

Start by drawing a free body diagram for the crate.
 
  • #10
student34 said:
no matter how hard she pushes.
That's the piece of information that was missing. You obtained this equation correctly (rude man seems to have misread the set-up as being a ramp):
μ = (F*cosθ)/(m*g + F*sinθ)​
With the understanding that F is not a specific value and is unlimited in magnitude, can you now derive the desired result from your equation?
 
  • #11
haruspex said:
That's the piece of information that was missing. You obtained this equation correctly (rude man seems to have misread the set-up as being a ramp):
μ = (F*cosθ)/(m*g + F*sinθ)​
With the understanding that F is not a specific value and is unlimited in magnitude, can you now derive the desired result from your equation?

The only way that I can get rid of F is by using ƩFy = Fn - m*g - F*sinθ, where Fn = (F*cosθ)/μ. Then I isolate F which equals (μ*m*g)/(cosθ - μ*sinθ), and substitute this equation in for F from our answer μ = (F*cosθ)/(m*g + F*sinθ). But it turns into a massive mess that I can't simplify to 1/tanθ, and these questions never expect us to do that kind of math. So I know that I must be missing a way that is much more simple.
 
  • #12
student34 said:
The only way that I can get rid of F is by using ƩFy = Fn - m*g - F*sinθ, where Fn = (F*cosθ)/μ.

You're not grasping the implication of "no matter how hard she pushes".
Consider your equation μ = (F*cosθ)/(m*g + F*sinθ) as defining μ as a function of F. What happens to μ as F increases?
 
  • #13
SammyS said:
Start by drawing a free body diagram for the crate.

A free body diagram should help you get an expression for the normal force -- which does depend upon F .
 
  • #14
haruspex said:
You're not grasping the implication of "no matter how hard she pushes".
Consider your equation μ = (F*cosθ)/(m*g + F*sinθ) as defining μ as a function of F. What happens to μ as F increases?

After trying some values of F, I noticed that μ increases less and less as F increases. So, now I do understand how F increases so does μ therefore so does friction pushing against her push. But I can't make the connection as to how they get μ = 1/tanθ.

It all makes good sense except for how they get μ = 1/tanθ.
 
  • #15
SammyS said:
A free body diagram should help you get an expression for the normal force -- which does depend upon F .

I have made a FBD. In it Fn = m*g + F*cosθ, and Fn = (F*cosθ)/μ. I can't find anymore useful relationships to Fn.
 
  • #16
the woman cannot start the crate moving no matter how hard she pushes.

for maximum force F applied toslide depends on angle θ. for critical value of coefficient of friction dF/dθ must be equal to zero for some angle θ.
 
Last edited:
  • #17
What equation do you get from the horizontal component of force?
 
  • #18
SammyS said:
What equation do you get from the horizontal component of force?

ƩFx = F*cosθ - μFn = 0, where μFn is the force of friction, and Fn = m*g + F*cosθ, and Fn = (F*cosθ)/μ
 
  • #19
student34 said:
I have made a FBD. In it Fn = m*g + F*cosθ, and Fn = (F*cosθ)/μ. I can't find anymore useful relationships to Fn.

That should be Fn = mg + F sin(θ) .
student34 said:
ƩFx = F*cosθ - μFn = 0, where μFn is the force of friction, and Fn = m*g + F*cosθ, and Fn = (F*cosθ)/μ

Put those together.
 
  • #20
student34 said:
After trying some values of F, I noticed that μ increases less and less as F increases. So, now I do understand how F increases so does μ therefore so does friction pushing against her push. But I can't make the connection as to how they get μ = 1/tanθ.

It all makes good sense except for how they get μ = 1/tanθ.
What you might also notice is that μ does not go on increasing without limit. What value does it tend to as F tends to infinity?
 
  • #21
SammyS said:
That should be Fn = mg + F sin(θ) .



Put those together.

Ok but when I do, I just get my original answer of μ = (F*cosθ)/(m*g + F*sinθ). The answer in the textbook is μ = 1/tanθ.
 
  • #22
Isolate F.

ehild
 
  • #23
haruspex said:
What you might also notice is that μ does not go on increasing without limit. What value does it tend to as F tends to infinity?

I will go out on a limb and make the derivative of μ equal zero, but I don't think that they expect us to do this yet. So μ' = 0 = (-F*sinθ)/(m*g + F*sinθ) + (F*cosθ)/-(m*g + F*sinθ)^2, and when F is isolated, its value should be a derivative of zero.
 
  • #24
Isolate F instead of mu from μ = (F*cosθ)/(m*g + F*sinθ). You know that F must be positive, being the magnitude of the applied force.

ehild
 
  • #25
ehild said:
Isolate F.

ehild

Ok, F = (μ*m*g)/(cosθ - μ*sinθ), but I am not sure why I want to do this.
 
  • #26
Because F can not be negative. What dos it mean for (cosθ - μ*sinθ)?

ehild
 
  • #27
ehild said:
Because F can not be negative. What dos it mean for (cosθ - μ*sinθ)?

ehild

I see; cosθ ≥ μ*sinθ. But that is so beyond any kind of critical thinking that the textbook has ever expected in any other questions. This is very humbling.
 
  • #28
student34 said:
I will go out on a limb and make the derivative of μ equal zero, but I don't think that they expect us to do this yet. So μ' = 0 = (-F*sinθ)/(m*g + F*sinθ) + (F*cosθ)/-(m*g + F*sinθ)^2,
You seem to have got confused between differentiating wrt F and wrt θ. Wrt F will give you F=∞, which is correct. I.e., μ will always increase as F increases. But that isn't what I asked - the question is whether there is a limit to the value of μ. For that, let F tend to infinity in your equation for μ. This will make the mg term so small in comparison that it can be ignored. What does that leave you with?
 
  • #29
Code:
I see; cosθ ≥ μ*sinθ. But that is so beyond any kind of critical thinking that the textbook has ever expected in any other questions. This is very humbling.

cosθ ≥ μ*sinθ
or μ*sinθ ≤ cosθ
or μ ≤ (1/tanθ)

this means that 1/tanθ is the critical value for μ. if μ is greater than this value the force required to move the block is infinite i.e.can not be moved.
 
  • #30
student34 said:
Ok but when I do, I just get my original answer of μ = (F*cosθ)/(m*g + F*sinθ). The answer in the textbook is μ = 1/tanθ.
Write your expression for μ as

\displaystyle \ \mu=\frac{1}{\displaystyle\frac{mg}{F\cos(\theta)}+\frac{F\sin(\theta)}{F\cos(\theta)}}
\displaystyle=\frac{1}{\displaystyle\frac{mg}{F\cos(\theta)}+\tan( \theta)}\ .​
Then follow haruspex's advice in post #20.
 
  • #31
student34 said:
I see; cosθ ≥ μ*sinθ. But that is so beyond any kind of critical thinking that the textbook has ever expected in any other questions. This is very humbling.

You just have to read a problem text carefully.

The problem said
If μ(static) is greater than some critical value, the woman cannot start the crate moving no matter how hard she pushes. Calculate this critical value of μ(static)

Assume that μ is given. The woman can just set the cart moving if her force is

F = (μ*m*g)/(cosθ - μ*sinθ).

If μ=1/tan(θ) the required force becomes infinite, the women can not exert infinite force no matter how hard she pushes. If μ is greater than that the equation can not be fulfilled by a positive F.

ehild
 
  • #32
The answer is as follows: as the woman pushes harder and harder, the effect of gravity becomes less important overall, in proportion to her pushing, in deciding what happens to the box. As we approach this extreme point, or the limit, since mg <<< Fsinø, You can essentially take mg+Fsinø = Fsinø. Now reducing becomes simple algebra.

In other words, in the case that she is pushing infinitely hard, or somewhere near there, if mu_s is cotø, the box will not budge.
 
  • #33
PhysicsLord said:
mg+Fsinø = Fsinø
I assume that is not what you meant.
Anyway, the student seems to have arrived at the answer in post #27, three years ago.
 
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