Electric field due to n charges

In summary, the conversation discusses the existence of a vertical component of the electric field for a given expression and whether it cancels out due to symmetry. The participants also discuss the formula for the electric field produced by multiple charges and how it can be proven that the vertical component cancels out for even numbers of charges. The conversation concludes with a clarification about the correct formula to use and an example calculation for two charges.
  • #1
ChiralSuperfields
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Homework Statement
Please see below.
Relevant Equations
Please see below.
For this problem,
1673581735141.png

The solution is,
1673581774615.png

However, should they be a vertical component of the electric field for the expression circled in red? I do understand that assuming that when the nth charge is added it is placed equal distant for the other charges so that a component of the electric field cancels which would be the y-component from how they defined the coordinate system.

I also note how they could have just used the formula for the E-field produced by a discrete number of charges.
1673581994372.png


Many thanks!
 
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  • #2
I assume that by "vertical" you mean a component in the plane parallel to the plane of the circle. Consider a point on the x-axis. If there were such a component of the field at that location, at what "o' clock" position relative to the circle would it point? To make it easy, assume that there are 12 charges on the circle labeled 1 - 12.
 
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  • #3
kuruman said:
I assume that by "vertical" you mean a component in the plane parallel to the plane of the circle. Consider a point on the x-axis.
Thanks for the reply @kuruman , and sorry for the late reply!

Yep, correct was what I meant by "vertical" :)

If there were such a component of the field at that location, at what "o' clock" position relative to the circle would it point? To make it easy, assume that there are 12 charges on the circle labeled 1 - 12.
If there was a positive charge on the x-axis, then I think there would be a electric field surrounding the charge. If there was a spherical Gaussian surface then then there would be a postive electric flux since there would only be electric field lines leaving the charge. But if there were charges on the circle, I think their vertical component will cancel from symmetry. I think the same is true for an even number of charges.

Is there a way to prove that the vertical component of the electric fields cancels from symmetry?

Many thanks!
 
  • #4
If the unit vector ## \hat{i} ## is supposed to mean the unit vector along the x axis the formula outlined in red is wrong. The field of any individual charge is not along the x axis but at an angle, as shown in the figure. This field does have a component perpendicular to the x axis. Only when you add all contributions the off-axis components cancel out.
 
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  • #5
nasu said:
If the unit vector ## \hat{i} ## is supposed to mean the unit vector along the x axis the formula outlined in red is wrong. The field of any individual charge is not along the x axis but at an angle, as shown in the figure. This field does have a component perpendicular to the x axis. Only when you add all contributions the off-axis components cancel out.
Thanks for you reply @nasu ! So really that formula shown in red for the individual charge n should be,

1673660759511.png

Correct?

However, how do we prove without using intuition that y-component of the radical fields cancel for n > 1 to give a resultant electric field of
1673661091103.png

for n charges?

I think the easiest situation to prove this for is for n = 2.
I'll assume that the two charges are separately symmetrically from each other by a distance 2a.
1673661501615.png

Then,
1673662236214.png

However, this does not give
1673662285870.png
mentioned in the solutions. Do you please know what I did wrong?

Thank you!
 
  • #6
Callumnc1 said:
Then,
View attachment 320343
However, this does not give View attachment 320344 mentioned in the solutions. Do you please know what I did wrong?

Thank you!
If you substitute ##n=2##, it gives exactly that.
 
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  • #7
kuruman said:
If you substitute ##n=2##, it gives exactly that.
Thanks @kuruman, I did not see that!
 

What is an electric field?

An electric field is a physical quantity that describes the strength and direction of the force experienced by a charged particle in an electric field. It is represented by electric field lines and is measured in units of volts per meter (V/m).

How is the electric field due to multiple charges calculated?

The electric field due to multiple charges is calculated by summing up the individual electric fields produced by each charge. This can be done using the principle of superposition, where the total electric field at a point is the vector sum of the individual electric fields at that point.

What is Coulomb's law and how is it related to electric fields?

Coulomb's law states that the force between two point charges is directly proportional to the product of their charges and inversely proportional to the square of the distance between them. This force is also related to the electric field, as the electric field at a point is equal to the force per unit charge experienced by a test charge at that point.

What is the difference between electric field and electric potential?

Electric field and electric potential are related but distinct concepts. Electric field is a vector quantity that describes the force experienced by a charged particle, while electric potential is a scalar quantity that describes the potential energy per unit charge at a point in an electric field. In other words, electric field describes the force, while electric potential describes the potential energy.

How does the electric field due to charges change with distance?

The electric field due to charges decreases with distance according to the inverse square law. This means that as the distance from the charges increases, the electric field strength decreases rapidly. Additionally, the direction of the electric field changes with distance, as it is always directed away from positive charges and towards negative charges.

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