How Is the Electric Field Around an Infinitely Long Wire Derived?

AI Thread Summary
The electric field around an infinitely long wire with uniform charge distribution is derived using the formula E = (1/2πε₀)(λ/r), where λ is the linear charge density expressed as λ = dq/dl. To derive this, one starts with the general electric field equation E = (1/4πε₀)∫(ρ/r²)âdV, adapting it for a wire by substituting volume with linear charge. The integration is performed from negative to positive infinity, focusing on the radial symmetry of the field. Resources and examples for this derivation can be found through online searches, including educational sites like HyperPhysics. Understanding this derivation is crucial for grasping electric fields in cylindrical symmetry.
Uku
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Homework Statement


I know that around an infinitely long wire with even charge distribution the electric field is expressed as:

E=\frac{1}{2\pi\epsilon_{0}}\frac{\lambda}{r} (1)

Where \lambda can be expressed as \lambda=\frac{dq}{dl}

Right, but I want to know where I get this formula from, I mean the E field.

The Attempt at a Solution



So I know that in general:

E=\frac{1}{4\pi\epsilon_{0}}\int\frac{\rho}{r^{2}}\widehat{r}dV

In my case I don't have volume, I have a thread. I can also forget about the unit vector, since the field is radially pointed outward. The charge is evenly distributed so I can write:

E=\frac{1}{4\pi\epsilon_{0}}\lambda\int\frac{1}{r^{2}}dL

Okay, but now... I can integrate the expression from minus infinity to infinity, but how do I get to that formula (1)
 
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Uku said:
Okay, but now... I can integrate the expression from minus infinity to infinity, but how do I get to that formula (1)

You can find a number of sites that work this out for you. A google search, or even a search here at PF will give you many looks at this problem. Here is one, for example.

http://hyperphysics.phy-astr.gsu.edu/hbase/electric/elelin.html
 
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