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
member 731016
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!
 

FAQ: Electric field due to n charges

What is the principle of superposition in the context of electric fields due to multiple charges?

The principle of superposition states that the total electric field created by multiple charges is the vector sum of the individual electric fields produced by each charge. This means that you calculate the electric field due to each charge separately and then add them up vectorially to find the net electric field at a given point.

How do you calculate the electric field at a point due to multiple charges?

To calculate the electric field at a point due to multiple charges, you first determine the electric field due to each individual charge using Coulomb's law. Then, you add these electric fields as vectors. Mathematically, if you have charges q1, q2, ..., qn located at positions r1, r2, ..., rn, the electric field E at a point r is given by E = k Σ (qi / |r - ri|^2) * (r - ri) / |r - ri|, where k is Coulomb's constant.

What are the units of the electric field in the International System of Units (SI)?

The electric field is measured in newtons per coulomb (N/C) in the International System of Units (SI). It can also be expressed in volts per meter (V/m), since 1 N/C is equivalent to 1 V/m.

How does the distance between charges affect the electric field they produce?

The electric field produced by a charge decreases with the square of the distance from the charge. According to Coulomb's law, the electric field E due to a point charge q at a distance r is given by E = k * q / r^2. Therefore, if the distance between the charge and the point where the field is being measured is doubled, the electric field strength is reduced to one-fourth of its original value.

Can the electric field due to multiple charges be zero at some points in space?

Yes, the electric field due to multiple charges can be zero at certain points in space. This occurs at points where the vector sum of the electric fields due to the individual charges cancels out. These points are often referred to as equilibrium points or null points, and their locations depend on the magnitudes and positions of the charges involved.

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