Electric Field of x-axis line of charge at the origin.

In summary, the charge at the origin of a non-uniform line of charge on the x-axis from -10cm to 10 cm is zero, and the electric field is also zero due to symmetry. The line of charge can be treated as two separate lines starting at the origin, and the electric field at the origin can be found by integrating Coulomb's law for point charges, taking into account the direction of the unit vector \hat{a_r}.
  • #1
fitzfool
3
0

Homework Statement



Calculate the charge and electric field at the origin of non-uniform line of charge on the x-axis from -10cm to 10 cm on the x-axis. Where linear charge density is given by 2x^4

Homework Equations


dq=lambda dx
de=(k dq)/r^2
E=integral of (Kdq)/r^2 = k integral of (lambda dx/r^2)

The Attempt at a Solution


Charge is easy you just integrate the linear charge density equation from -10 to 10.

For the electric field at the origin I believe it is zero but am not sure how to calculate it.

Every example problem puts the point P at some distance away from the line of charge not at the center or even on the line of charge.

The only thing I can think of is that I need to treat the single line of charge like two separate lines(by a extremely small negligible amount) starting at the origin. Then integrate from -10 to 0 and 0 to 10 adding them together to get the total Electric Field.

However, I am not sure if I am even allowed to do it this way.
 
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  • #2
Hello fitzfool,

Welcome to Physics Forums! :smile:

fitzfool said:

Homework Statement



Calculate the charge and electric field at the origin of non-uniform line of charge on the x-axis from -10cm to 10 cm on the x-axis. Where linear charge density is given by 2x^4

Homework Equations


dq=lambda dx
de=(k dq)/r^2
E=integral of (Kdq)/r^2 = k integral of (lambda dx/r^2)

The Attempt at a Solution


Charge is easy you just integrate the linear charge density equation from -10 to 10.

For the electric field at the origin I believe it is zero but am not sure how to calculate it.

Every example problem puts the point P at some distance away from the line of charge not at the center or even on the line of charge.
Yes, it doesn't make sense to put the "test charge" on top of an actual charge, since the electric field blows up as r → 0.

But it's okay for this problem, since there technically is no charge at the origin. The charge density, λ = 2x4 is 0 when x = 0, so it's okay to put the "test charge" at the origin in this case.

The only thing I can think of is that I need to treat the single line of charge like two separate lines(by a extremely small negligible amount) starting at the origin. Then integrate from -10 to 0 and 0 to 10 adding them together to get the total Electric Field.

However, I am not sure if I am even allowed to do it this way.
Treat the line as an infinite number of infinitesimal point charges. The charge dQ of each infinitesimal point charge is λdx. Integrate Coulombs law for point charges, using that. :smile:

[Edit: you even have the proper equation in your list of relevant equations. Just change r to x.]

[Another edit: And yes, you should find that it goes to zero due to symmetry. You'll need to treat the negative x-axis differently than the positive x-axis, because the unit vector [itex] \hat {a_r} [/itex] is in different directions for each. So yes, treating it as two different lines is the right way to go here. :wink:]

[Still, yet another edit: This problem is a good example of why vector calculus is more tricky than plain old run-of-the-mill calculus. Remember, electric field is a vector, that has magnitude and direction. Coulomb's law states, in differential form,

[tex] \vec {dE} = k \frac{dQ}{r^2} \hat{a_r} [/tex]
And it's those pesky unit vectors, [itex] \hat{a_r} [/itex] that cannot be ignored, and can make things tricky. In this problem, [itex] \hat{a_r} [/itex] is different for points on the negative x-asis than it is for points on the positive x-axis. So you'll need to take that into account. This will not be the last time that the pesky unit vectors make things tricky. You can look forward to more of this in future problems. :smile:]
 
Last edited:
  • #3
Hmm, thank you very much for the reply and all of the edits. They were very helpful.

However, I wasn't even thinking of the unit vectors until you posted your last reply.

Taking into consideration the unit vectors I'm getting,

For the left side K ∫2x4 / x2 from -10 to 0 is K .2/3 x3 from -10 to 0 is -5.9E11 multiply that by cos(0) is -5.9E11
For the right side I get 5.9E11 cos(180) is -5.9E11.
-5.9E11+-5.9E11 is -11.8E11. So I must be messing up a sign somewhere. I'm not sure where. Maybe I could get a hint?
 
  • #4
fitzfool said:
Hmm, thank you very much for the reply and all of the edits. They were very helpful.

However, I wasn't even thinking of the unit vectors until you posted your last reply.

Taking into consideration the unit vectors I'm getting,

For the left side K ∫2x4 / x2 from -10 to 0 is K .2/3 x3 from -10 to 0 is -5.9E11 multiply that by cos(0) is -5.9E11
For the right side I get 5.9E11 cos(180) is -5.9E11.
-5.9E11+-5.9E11 is -11.8E11. So I must be messing up a sign somewhere. I'm not sure where. Maybe I could get a hint?
I think the problem was with the evaluation of the negative x-axis part. Remember that (-10)3 is a negative number, and since that limit is on the bottom part of the integral, that also gets evaluated as negative -- a negative times a negative ...

[tex] \vec E = k \int_{-10}^0 2 x^2 dx \ + \ -k \int_0^{10} 2x^2 dx [/tex]
[tex] = \frac{2}{3}k \left[0^3 - \left(-10 \right)^3 \right] -\frac{2}{3}k \left[ 10^3 - 0^3 \right] [/tex]

You should be able to take it from there. :smile:
 
  • #5
Thank you very much.
Can't believe I missed that 0 - a negative number is a positive number!
 

Related to Electric Field of x-axis line of charge at the origin.

1. What is an electric field?

An electric field is a physical quantity that describes the influence of an electrically charged object on other charged objects in its vicinity. It is a vector quantity that indicates the direction and strength of the force that a charged object would experience if placed in the field.

2. What is the x-axis line of charge at the origin?

The x-axis line of charge at the origin is a hypothetical line of charge that is located on the x-axis and passes through the point (0,0) on a Cartesian coordinate system. It is used as a simplified model to study the electric field of a charged object.

3. How is the electric field of a line of charge calculated?

The electric field of a line of charge is calculated using the equation E = kλ/r, where k is the Coulomb's constant, λ is the linear charge density of the line, and r is the distance from the line to the point where the electric field is being measured. The direction of the electric field is always perpendicular to the line of charge and points away from it if the line is positively charged, and towards it if the line is negatively charged.

4. What is the magnitude of the electric field for a line of charge at the origin?

The magnitude of the electric field for a line of charge at the origin is given by the equation E = kλ/r. As the distance from the line of charge increases, the electric field decreases in magnitude, following an inverse relationship. This means that the electric field is strongest closest to the line of charge and becomes weaker as you move away from it.

5. How does the electric field of a line of charge at the origin affect other charged objects?

The electric field of a line of charge at the origin will exert a force on any other charged object placed in its vicinity. The direction and strength of the force will depend on the charge of the object and the direction and magnitude of the electric field. This is the basis for how electric charges interact with each other and is essential in understanding the behavior of electrically charged objects.

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