Improper integral help: coloumb's law

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Homework Help Overview

The discussion revolves around deriving the electric field due to an infinite line of charge using Coulomb's law, specifically focusing on an improper integral that arises in the process. Participants are examining the integral expression for the electric field and the challenges associated with evaluating it.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the use of trigonometric substitution and the application of L'Hôpital's rule to evaluate the limit of the integral. There are questions about the correctness of the approach and the limits of integration.

Discussion Status

Some participants have offered alternative methods for evaluating the integral, suggesting changes to the limits of integration and different substitution techniques. There is ongoing exploration of the problem, with no explicit consensus reached on the best approach.

Contextual Notes

Participants note potential typos and the importance of correctly applying limits and substitutions in the integration process. The discussion reflects a collaborative effort to clarify the mathematical reasoning behind the integral evaluation.

Edwardo_Elric
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Homework Statement


i was deriving an infinite line of charge formula by coloumb's law:
so i got stuck with this integral (since it is in the maths forum)
\vec{E}_{\rho} = \int_{-\infty}^{\infty} \frac{\rho_L \rho dz}{4\pi\epsilon_o ({\rho}^2 + z^2)^{\frac{3}{2}}}

Homework Equations


where
{\rho}_L = linear charge density
{\rho} = direction perpendicular to z axis in cylindrical coordinates

The Attempt at a Solution


so when integrating (using trigo substitution):
\vec{E}_{\rho} = \frac{\rho_L\rho}{4\pi\epsilon_o} (\frac{1}{{\rho}^2} \frac{z}{p^2 + z^2})_{-\infty}^{\infty}
this is where i got stuck
no matter how i use lhopitals rule in this equation:
\lim_{z \infty} \frac{z}{({\rho}^2 + z^2)^{\frac{1}{2}}
it keeps going back

because the infinite is supposed to add to equate to 2
the answer which is
\vec{E}_{\rho} = \frac{\rho_L}{2\pi\epsilon_o\rho}
 
Last edited:
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Edwardo_Elric said:

Homework Statement


i was deriving an infinite line of charge formula by coloumb's law:
so i got stuck with this integral (since it is in the maths forum)
\vec{E}_{\rho} = \int_{-\infty}^{\infty} \frac{\rho_L \rho dz}{4\pi\epsilon_o ({\rho}^2 + z^2)^{\frac{3}{2}}}


Homework Equations


where
{\rho}_L = linear charge density
{\rho} = direction perpendicular to z axis in cylindrical coordinates


The Attempt at a Solution


so when integrating (using trigo substitution):
\vec{E}_{\rho} \frac{\rho_L\rho}{4\pi\epsilon_o} (\frac{1}{{\rho}^2} \frac{z}{p^2 + z^2})_{-\infty}^{\infty}
this is where i got stuck
I think you need to show your work here. This is not at all what I got.

no matter how i use lhopitals rule in this equation:
You don't need to use L'Hopital's rule- just divide numberator and denominator by z2. Of course, then the limits are both 0 which is not what you want.

\lim_{z \infty} \frac{z}{({\rho}^2 + z^2)^{\frac{1}{2}}
it keeps going back
\lim_{z \to \infty} \frac{z}{({\rho}^2 + z^2)^{\frac{1}{2}}

because the infinite is supposed to add to equate to 2
the answer which is
\vec{E}_{\rho} = \frac{\rho_L}{2\pi\epsilon_o\rho}
I would prefer to change the limits of integration with each substitution.
 
yeah typo:
(\frac{z}{\sqrt{p^2 + z^2}})_{-\infty}^{\infty}

the problem is differentiating \sqrt{p^2 + z^2} when i keep using LHR it
keeps on going back

edit:
wait did you mean this?
\frac{\frac{z}{z}}{\frac{\frac{\sqrt{p^2+z^2}}{z^2}}}}
i tihink i get it now

just divide both sides by z
the denominator you divide by sqrt(z^2)

thx a lot halls
 
Last edited:
You say you used a trig substitution so why worry about the integral as a function of z at all? Change the limits of integration as you change the variable.

When I did it, my first substitution was \rho tan(\theta)= z. z will go to -\infty and \infty as \theta goes from -\pi/2 to \pi/2. I then integrated the resulting trig function by letting u= sin(\theta). While theta goes from -\pi/2 to \pi/2, u goes from -1 to 1 so I only had to evaluate the "u" formula between -1 and 1 without having to go back to the original variable.
 

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