Path of the particle on inclined plane

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The discussion revolves around analyzing the forces acting on a particle on an inclined plane, particularly in static equilibrium. Participants clarify that the particle does not slide down due to the angle θ being set such that tanθ = μ, ensuring friction balances the gravitational component. They explore the relationship between tension in the string, friction, and the particle's motion, emphasizing the need to consider both x and y components of forces. The conversation highlights the importance of accurately resolving forces and understanding the direction of friction, especially when the particle is positioned at different points on the incline. Overall, the analysis aims to derive correct equations governing the particle's behavior under the influence of these forces.
  • #61
TSny said:
The important thing is to find the direction of the friction force just before slipping.

If particle sits at rest in third quadrant i.e when T = 0 , then friction acts up the slope .

TSny said:
If ##\phi## is the angle that the string makes to the (negative) y-axis, try to find the angle between the string and the friction force in terms of ##\phi##.

The angle would be ##\phi## .

TSny said:
Also think about which way the particle is going to move when it slips.

The particle will try to move at an angle ##180° - 2\phi## with the -y axis measured CW .
 

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  • #62
OK, your directions look good. But it seems to me that the arrows you added should be drawn at the particle rather than the hole.
[EDIT: I noticed that you did not draw the direction of ##f## very accurately. Your value of ##180^o - 2\phi## is correct. But if you draw this angle more accurately, I think you will see that ##f## points in a different direction.]

So I think you have the correct angle for the direction of motion of the particle. Let ##r## be the length of the string between the particle and the hole. You want to find the path of the particle. In polar coordinates, this would be ##r## as a function ##\phi##.

Suppose the particle undergoes a small displacement ##ds##. Can you find expressions for ##dr## and ##d\phi## in terms of ##ds##, ##r##, and ##\phi##?
 
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  • #63
TSny said:
Let ##r## be the length of the string between the particle and the hole. You want to find the path of the particle. In polar coordinates, this would be ##r## as a function ##\phi##.

Suppose the particle undergoes a small displacement ##ds##. Can you find expressions for ##dr## and ##d\phi## in terms of ##ds##, ##r##, and ##\phi##?

##d\vec{s} = dr\hat{r} + rd\phi \hat{\phi}##
 
  • #64
Vibhor said:
##d\vec{s} = dr\hat{r} + rd\phi \hat{\phi}##
What if you project this equation onto the direction ##\hat{r}##? onto the direction ##\hat{\phi}##?

This will give you two equations to work with.
 
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  • #65
TSny said:
What if you project this equation onto the direction ##\hat{r}##? onto the direction ##\hat{\phi}##?

You mean I need to take dot product of ##d\vec{s}## with ##\hat{r}## and with ##\hat{\phi}## separately ?
 
  • #66
Yes.
 
  • #67
##d\vec{s} \cdot \hat{r}= dr##

##d\vec{s} \cdot \hat{\phi}= rd\phi##
 
  • #68
Yes, but the left hand sides can be expressed explicitly in terms of the magnitude of the vector ##\vec{ds}## and the angle between ##\vec{ds}## and the unit vectors.

Thus, you will need to know the angle between ##\vec{ds}## and ##\hat{r}##. Use your diagram (drawn carefully).
 
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  • #69
The angle between ##\vec{ds}## and ##\hat{r}## is ##180° - \phi## and that between ##\vec{ds}## and ##\hat{\phi}## is ##270° - \phi## .

Is that right ?
 
  • #70
Vibhor said:
The angle between ##\vec{ds}## and ##\hat{r}## is ##180° - \phi## and that between ##\vec{ds}## and ##\hat{\phi}## is ##270° - \phi## .

Is that right ?
No. Can you show a diagram with the forces acting on the particle and also show the vector ##\vec{ds}##?

Note that in the figure, I made ##\phi## roughly 30o. So, what is the approximate value of ##180 - 2\phi## ? Make sure you draw ##f## approximately in this direction. Then draw ##\vec{ds}## in the appropriate direction.

[EDIT: Sorry, Vibhor, your values for the angles are correct! When I worked through this part of the problem, I did not use the unit vectors ##\hat{r}## and ##\hat{\phi}##. When I read your last thread, I had the vectors pictured in my head in their opposite directions.]
 
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  • #71
So, since you got the angles correct, your diagram hopefully looks something like this:
upload_2016-6-12_23-50-10.png
 
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  • #72
So, using your expressions for the angles between ##\vec{ds}## and the unit vectors, try expressing the left sides of the two equations below in terms of the magnitude of the displacement ##ds## and the angle ##\phi##.

##\vec{ds} \cdot \hat{r} = dr##
##\vec{ds} \cdot \hat{\phi} = rd\phi##
 
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  • #73
TSny said:
[EDIT: Sorry, Vibhor, your values for the angles are correct! When I worked through this part of the problem, I did not use the unit vectors ##\hat{r}## and ##\hat{\phi}##. When I read your last thread, I had the vectors pictured in my head in their opposite directions.]

Ok

I got really discouraged reading your initial reply in #70 . But now I feel better :smile:
 
  • #74
##-dscos\phi = dr ##

##-dssin\phi = rd\phi ##

From this I get ##\frac{dr}{r} = \frac{d\phi}{tan\phi}##
 
  • #75
Vibhor said:
##-dscos\phi = dr ##

##-dssin\phi = rd\phi ##

From this I get ##\frac{dr}{r} = \frac{d\phi}{tan\phi}##
Great! The first two equations above can pretty much be read directly off the diagram. But using the unit vectors is good, too.
 
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  • #76
Integrating I get ##r=Csin\phi ## , where ##C## is a constant .
 
  • #77
Yep.
 
  • #78
Does that mean distance of the particle from the hole is oscillating (alternately increasing and decreasing ) like a sine curve ?
 
  • #79
I don't think so.
Perhaps the curve will be more recognizable when expressed in terms of the Cartesian coordinates of the particle (x, y).
 
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  • #80
TSny said:
Perhaps the curve will be more recognizable when expressed in terms of the Cartesian coordinates of the particle (x, y).

Should I replace r =##\sqrt{x^2+y^2}## and ##\sin\phi = \frac{x}{r}## to express curve in cartesian coordinates ?
 
  • #81
Almost. There's a sign error. (Of course you now know not to believe anything I say, but I really do think there is a sign error.)
 
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  • #82
r =##\sqrt{x^2+y^2}## and ##\sin\phi = -\frac{x}{r}##
 
  • #83
Yes.
 
  • #84
Ok .

This gives ##\left( x + \frac{c}{2} \right)^2 + y^2 = (\frac{c}{2})^2## . This is a circle centered at ##(-\frac{c}{2} , 0)## and radius ##\frac{c}{2}## .
 
  • #85
I believe that's correct.
 
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  • #86
Ok .

In polar coordinates we measure angles anti clockwise from x - axis but in this problem we measured it clockwise from -y axis .Doesn't this make a difference ?

It is a very naive question but I am not too familiar with polar coordinates .
 
  • #87
It doesn't make any difference as long as you make your definitions clear.

Does the particle end up where you expect it would?
 
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  • #88
TSny said:
It doesn't make any difference as long as you make your definitions clear.

Ok . Good point .

TSny said:
Does the particle end up where you expect it would?

I don't know . Even though I have got the equation of the curve , I can't imagine how the particle is actually moving (except it is moving in a circular fashion not centered at the hole) . I am still not sure how to determine constant ##C## .
 
  • #89
Can you relate C to the place where the particle crossed the x-axis in going from quadrant II to quadrant III?
 
  • #90
TSny said:
Can you relate C to the place where the particle crossed the x-axis in going from quadrant II to quadrant III?

But that depends on where the particle was initially ( at rest ) in the second quadrant . As it moves vertically down slope in the second quadrant .
 

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