Understanding the Electric Field Equation in Electromagnetism

In summary, the conversation discusses deriving the electric field using the formula $$\nabla \frac{1}{|x-x'|} = - \frac{x-x'}{|x-x'|^3}$$ and the necessary condition for this to be valid, which is $$\nabla |x-x'| = \frac{x-x'}{|x-x'|}$$ in spherical coordinates. It also addresses a mistake in using the formula and corrects it.
  • #1
davidge
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I was reading a book on Electromagnetism and it's said on deriving the electric field that $$\nabla \frac{1}{|x-x'|} = - \frac{x-x'}{|x-x'|^3}$$ where ##|x-x'|## is the magnitude of the distance between two point charges. I've tried to derive this result and I found that $$\nabla |x-x'| = \frac{x-x'}{|x-x'|}$$ must be true for the first identity to be valid. Is this right?
 
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  • #2
Yes, it essentially boils down to ##\nabla r = \vec e_r## in spherical coordinates.
 
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  • #3
Orodruin said:
Yes, it essentially boils down to ∇r=⃗er∇r=e→r\nabla r = \vec e_r in spherical coordinates.
Thanks. Can you point out where I'm wrong?

I'm assuming a Minkowskian metric, so vectors- and covectors- components are equal. So we have ##|x-x'| = \sum_i(x^i - x'^{\ i})^2##. I guess we need some formalism to express ##x-x'##, because it's a vector. Let's say an arbitrary vector can be written as ##V = V^i \partial_i##. Then ##x - x' = (x^i - x'^{\ i})\partial_i ##. We have then $$ \nabla |x-x'| = \frac{x-x'}{|x-x'|} = \sum_i\partial_i[(x^i-x'^{\ i})^2] = \sum_i\frac{(x^i - x'^{\ i})\partial_i}{(x^i - x'^{\ i})^2}$$
If we apply the derivative on the far right-hand-side on ##|x-x'|##, we get a bad result, namely ##(x^i - x'^{\ i}) = 1##. I guess this can't be right..
 
  • #4
Why are you using ##|\vec x| = x^i x^i##?? This does not even make sense dimensionally. You are missing some square roots ...
 
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Orodruin said:
Why are you using |⃗x|=xixi|x→|=xixi|\vec x| = x^i x^i?? This does not even make sense dimensionally. You are missing some square roots ...
Oh yea. I got the correct result now. Thank you.
 

FAQ: Understanding the Electric Field Equation in Electromagnetism

What is the electric field equation?

The electric field equation, also known as Coulomb's law, describes the relationship between the electric field, the distance between two charged particles, and the magnitude of the charges. It can be written as F = k(q1q2)/r^2, where F is the force between the particles, k is the Coulomb's constant, q1 and q2 are the charges, and r is the distance between them.

How is the electric field equation derived?

The electric field equation is derived from the principle of superposition, which states that the net force on a particle due to multiple charges is equal to the vector sum of the individual forces from each charge. By applying this principle to a single point charge, the electric field equation can be derived.

What are the units of the electric field equation?

The units of the electric field equation depend on the unit system being used. In the SI system, the units are newtons per coulomb (N/C), while in the CGS system, the units are dynes per statcoulomb (dyn/esu).

How does the electric field equation relate to electric potential?

The electric field equation can be used to calculate the electric potential at a point in space, as the electric potential is the work done per unit charge by an electric field in moving a charge from one point to another. The relationship is given by V = kq/r, where V is the electric potential, k is the Coulomb's constant, q is the charge, and r is the distance from the charge.

Can the electric field equation be applied to non-point charges?

Yes, the electric field equation can be applied to non-point charges by breaking them down into smaller point charges and using the principle of superposition to find the net electric field. It can also be applied to continuous charge distributions by using integration to sum up the contributions from infinitesimal charge elements.

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