Electrostatics balancing gravitational, coulomb forces and tension

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Homework Help Overview

The discussion revolves around a problem in electrostatics involving the balancing of gravitational, Coulomb forces, and tension in a system of charged balls. The original poster is attempting to resolve forces acting on one of the balls and has encountered an unexpected factor of two in their calculations.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • The original poster resolves forces vertically and horizontally, leading to a relationship involving tension and gravitational force. They express confusion regarding an extra factor of two in their final equation.
  • Some participants question the correctness of the trigonometric relationships used, particularly the expression for cosθ, and suggest that the original poster may have skipped steps in their reasoning.
  • Others provide analogies to clarify the misunderstanding regarding units in the expression for cosθ.

Discussion Status

Participants are actively engaging with the original poster's reasoning, offering insights and questioning assumptions. The original poster indicates they have resolved their confusion regarding the factor of two and have adjusted their expression for cosθ accordingly, suggesting a productive direction in the discussion.

Contextual Notes

There appears to be a focus on ensuring that trigonometric functions are correctly defined and that the relationships between the variables are properly established. The discussion highlights the importance of unit consistency in mathematical expressions.

FatPhysicsBoy
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Homework Statement


Hi, I'm on the first part of this question and I've got to the end but I have an extra factor of two which I can't seem to explain! Any insight would be much appreciated, thank you!

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Homework Equations


The Attempt at a Solution



I resolved the forces around one ball and came up with the following:

Resolving vertically: mg = Tcosθ, Resolving horizontally: Tsinθ = F2,1

Then using pythagoras I found sinθ = r/2l and cosθ = √(4l2 - r2)

Putting it all together I get: 2F2,1 = mgr/√(4l2 - r2)

I just don't understand the extra factor of 2. I thought it might be because it's at half the separation but this isn't correct. Any help would be much appreciated. Thank you!
 
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cosθ = √(4l2 - r2)
This bit isn't quite right. It looks like you are trying to skip ahead to the next step before you have written things down properly. Maybe if you go through it again, writing down each step then you will get the right answer.
 
BruceW said:
cosθ = √(4l2 - r2)
This bit isn't quite right. It looks like you are trying to skip ahead to the next step before you have written things down properly. Maybe if you go through it again, writing down each step then you will get the right answer.

I don't understand?

I split the "triangle" up with hypotenuse l and adjacent r/2 and then used pythagoras to get:

a2 = l2 - (r2/4)

a = √(l2 - (r2/4)

Then I just multiplied both terms by 4 under the square root sign to get a = √(4l2 - (r2)
 
FatPhysicsBoy said:
a = √(l2 - (r2/4)

Then I just multiplied both terms by 4 under the square root sign to get a = √(4l2 - (r2)
This like saying you have ##x=\sqrt{1/4}##, and you multiplied by 4 under the square root sign to get ##x=\sqrt{1}=1##.Your expression for the cosine can't be right because it has units of length. The result of taking the cosine of an angle should be unitless.
 
BruceW said:
cosθ = √(4l2 - r2)
This bit isn't quite right. It looks like you are trying to skip ahead to the next step before you have written things down properly. Maybe if you go through it again, writing down each step then you will get the right answer.

vela said:
This like saying you have ##x=\sqrt{1/4}##, and you multiplied by 4 under the square root sign to get ##x=\sqrt{1}=1##.


Your expression for the cosine can't be right because it has units of length. The result of taking the cosine of an angle should be unitless.

Thank you for your help guys, I've figured it out now!

so cosθ= [√(l2-(r2/4))]/l

Then fast forward to 2F= mgr/√(l2-(r2/4)) take the 2 across and rewrite as √4 then push into the √(l2-(r2/4)) term to be left with mgr/√(4l2-(r2))

Thank You!
 

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