How to solve for unknown charge position

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Homework Help Overview

The discussion revolves around determining the position of an unknown charge in a system involving Coulomb's Law and the forces exerted by two fixed charges. Participants are exploring the conditions under which the forces acting on the unknown charge can cancel each other out.

Discussion Character

  • Exploratory, Assumption checking, Conceptual clarification

Approaches and Questions Raised

  • Participants discuss the need for the forces to have specific relative directions for cancellation and question how these directions affect the possible locations of the unknown charge. There are attempts to derive relationships between the magnitudes of the forces and considerations about the signs of the forces involved.

Discussion Status

There is ongoing exploration of the problem with various approaches being suggested. Some participants have offered hints and guidance on narrowing down the search for the unknown charge's position, while others are reflecting on the implications of their findings and the need for further clarification on vector directions.

Contextual Notes

Participants note the complexity of the problem due to multiple unknowns and the limitations of having only one equation to work with. There is also mention of the need to review vector concepts to better understand the relationships between the forces.

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Homework Statement


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Homework Equations


Coulomb's Law

43cfd29869833e7377d49cc8b89c101c.png


The Attempt at a Solution


Here are 2 different possibilities I drew that I think will have the x component vectors and y component vectors cancel out, but I think there may be some other positions as well.

baNMyVf.png


rnq0pAd.png


##\textbf{F}_x = k_e [\frac{(1.0 \textrm{ uC} \cdot q3) \cdot cos(\theta_1) \cdot \hat{r}_{13}}{{r_1}^2} + \frac{(-3.0 \textrm{ uC} \cdot q3) \cdot cos(\theta_2) \cdot \hat{r}_{23}}{{r_2}^2}]##

##\textbf{F}_y = k_e [\frac{(1.0 \textrm{ uC} \cdot q3) \cdot sin(\theta_1) \cdot \hat{r}_{13}}{{r_1}^2} + \frac{(-3.0 \textrm{ uC} \cdot q3) \cdot sin(\theta_2) \cdot \hat{r}_{23}}{{r_2}^2}]##

But there are so many unknowns and I only have one equation (Coulomb's) so I'm not sure what to do from here.
 
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You should be able to narrow the search considerably by considering:

1) If two forces are to completely cancel, what must be their relative directions?
2) What are the directions that the electric forces act between the fixed charges and the unknown charges?

In what way do the answers to the above two items constrain the possible location of q3?
 
Hint: For two vectors to be able to cancel each other, what angle must they make with each other?

That should simplify your answer.

Edit: gneill beat me to it!
 
gneill said:
You should be able to narrow the search considerably by considering:

1) If two forces are to completely cancel, what must be their relative directions?
2) What are the directions that the electric forces act between the fixed charges and the unknown charges?

Oh, as I was thinking about answering your questions I just realized I need to completely review vectors...but now I see that the unknown charge has to be somewhere axis along the fixed charges, but since the force is inversely proportional to the distance, it can't be on the right side because the charge on the right would overpower the one on the left.
 
Okay, so the magnitudes of the two forces have to equal each other:

##k_e \cdot \frac{|q_1||q_3|}{{r_1}^2} = k_e \cdot \frac{|q_2||q_3|}{({r_1 + L)}^2}##

Cancel out the constant and unknown charge:

##\frac{|q_1|}{{r_1}^2} = \frac{|q_2|}{({r_1 + L)}^2}##

But here I have a question about the signs of the force. Since we're only working with the magnitude, do I need to add a negative sign somewhere?
 
I suggest that you make another drawing and use it to further narrow down the region of interest. Then you can write expressions for the force magnitudes without any signs involved. For example:

attachment.php?attachmentid=61297&stc=1&d=1377962631.gif


The diagram shows there's only one region that the third charge can be located so that zero net force can occur.

Since all the given values have similar units (μC, cm), you can drop those too when you write the equality.
 

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