Coulomb's Low And Dirac Delta Functio

AI Thread Summary
To prove Coulomb's law for a single point charge using the Dirac delta function, one must understand the charge density for a point charge, which is represented by the Dirac delta function. The integral form of Coulomb's law involves integrating the volume charge density over space, where the charge density for a point charge can be expressed as ρ(ŕ) = qδ(ŕ - ŕ₀). Familiarity with the properties of the Dirac delta function is essential, as it simplifies the integration process by effectively "picking out" the value at the point charge's location. It is recommended to review resources on the Dirac delta function to grasp its application in this context. Mastering these concepts will facilitate the proof of Coulomb's law.
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I want to prove coulomb's low for a single charge point from the general form of coulomb's low:
E→=1/(4∏€) ∫∫∫ ρv(ŕ) * (r→- ŕ→)/│(r→- ŕ→)│^3 dŕ
using Dirac Delta function
where r→ is the field point vector
ŕ→ is the source point vector
ρv(ŕ) is the volume charge density
I really don't know how to do it . I tried a lot but couldn't do it so can u help me please as soon as possible.Just guide me how to do it.
 
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Hey guys I can use a little help here. Just give me a hint.I really really need ur help
 
The equation looks messed up (try LaTeX), but I guess you mean:

\vec E(\vec r)=\frac{1}{4\pi \epsilon_0}\int_V \frac{\rho(\vec r')}{|\vec r-\vec r'|^3}(\vec r-\vec r')dV'

Show what you have done so far. Ofcourse, you should know what the charge density of a point particle looks like.
 
yes ur guess is right the equation u wrote is the one I meant . yet I didnt reach any thing that make sense. I guess because I don't know the charge density for the point charge and because I don't know a lot about dirac delta function. I know it converts continuous functions into discreete ones Ithink this is the main idea of the solution but yet I don't know how Can u help me please?
 
Ofcourse, you should read up on what the dirac delta function is before using it to solve anything. I`m sure there's a discussion about it in your book.
http://planetmath.org/encyclopedia/DiracDeltaFunction.html
 
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