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

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SUMMARY

The electric field around an infinitely long wire with an even charge distribution is derived using the formula E = (1/(2πε₀))(λ/r), where λ represents the linear charge density defined as λ = dq/dl. The derivation involves integrating the electric field contribution from each infinitesimal segment of the wire, leading to the conclusion that the field behaves radially outward. The integral is computed from negative to positive infinity, simplifying the expression to the stated formula.

PREREQUISITES
  • Understanding of electric fields and charge distributions
  • Familiarity with calculus, particularly integration techniques
  • Knowledge of electrostatics, specifically Gauss's Law
  • Basic concepts of linear charge density
NEXT STEPS
  • Study the application of Gauss's Law in electrostatics
  • Explore the derivation of electric fields for different charge distributions
  • Learn about the concept of linear charge density in more detail
  • Investigate the implications of electric fields in real-world applications, such as in cables and transmission lines
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Students of physics, electrical engineers, and anyone interested in understanding the principles of electrostatics and electric fields around charged conductors.

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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