Three charges attached to the vertices of a triangle

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SUMMARY

The discussion centers on the existence of equilibrium points for three equal charges positioned at the vertices of a triangle. Participants conclude that there are at least two saddle points for a test ion, regardless of its charge polarity. The geometry of the setup guarantees these points, particularly near the midpoint between like charges. The conversation emphasizes the necessity of mathematical proof to establish the locations of these points, rather than relying on numerical methods.

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Homework Statement
Two positive ions and one negative ion are fixed at the vertices of
an equilateral triangle. Where can a fourth ion be placed, along the
symmetry axis of the setup, so that the force on it will be zero? Is
there more than one such place? You will need to solve something
numerically.
Relevant Equations
Coulomb's Law would be enough.
Actually we find the two position in the axis very easily, but, what am trying to find is if exist such position (Being the charge of the ions equal) away from the symmetry axis, but i really don't want to try find it numerically, it would be a disaster.
The only conclusion i got is, if such position exist, it should be somewhere in the red region of the figure:
1598718243200.png

The blue charge is negative
The red positive.

There is a way to prove if exist or not this position? Without the math would arise?
 
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You will need to use math.

Solving a similar example problem, with the algebra and trig being performed on symbols (saving the numerical substitution for the last step), may provide you with the insight you need for this homework problem.

See this solution, and don't just read it. Instead work it out on paper.
https://www.ux1.eiu.edu/~cfadd/1360/23EFields/Ch23Hmwk/23.17.html
 
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I sketched the field lines. It seems to me there can only be the two saddle points.
 
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Note that the question does not specify the sign of the "test" ion. It simply calls it "a fourth ion". It also doesn't ask for how many null force points exist, only if there is more than one.

Presumably, given the geometry of the setup, there must be at least one such point for a given test ion. So if there are two choices of charge polarity for the test ion, there must be at least two such points...
 
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gneill said:
Note that the question does not specify the sign of the "test" ion. It simply calls it "a fourth ion". It also doesn't ask for how many null force points exist, only if there is more than one.

Presumably, given the geometry of the setup, there must be at least one such point for a given test ion. So if there are two choices of charge polarity for the test ion, there must be at least two such points...
I don't see how the polarity of the test ion matters. A zero field is a zero field.

Assuming all three charges have the same magnitude, there will will always be a saddle point in the potential near the midpoint between the two like charges, just a little further away than that from the third charge, and another on the far side of that third charge, roughly twice as far from the like charges as from the third charge.

For each of the combinations of of one charge and one saddle point, there is a unique field line connecting them. Using the diagram layout, there is a field line from the lower left charge to each saddle point, and a straight field line from each of those to the top charge. Together, these lines bound roughly a semicircle. Inside that, all field lines run from the lower left charge to the top charge. This leaves no possibility of another saddle point in that region.
Etc.
 
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The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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