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Apr 15, 2022 at 9:35 comment added jensen paull Coulombs law can be derived from maxwells equations using only gauss law and assumptions. It can also be directly derived from maxwells equations and a charge density of $Q\delta^3(r)$
Apr 15, 2022 at 9:33 comment added jensen paull In the context of electrodynamics, ( and technically electrostatics): We CAN also feel the fields from an electron in andromeda, otherwise we wouldn't be able to see the light from there.
Apr 15, 2022 at 9:31 comment added jensen paull Please note $E = 0, R= \infty$ doesnt have to be the case when considering electrodynamics. Background EM solutions can exist that are non zero, that are not limited to constant solutions, but inherend wave like solutions "tagged onto" the fields 'produced' by charged. These fields are determined by initial conditions of the universe and not the location of charges and currents.
Apr 15, 2022 at 9:14 history edited Urb CC BY-SA 4.0
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Mar 12, 2015 at 16:24 vote accept CommunityBot
Mar 12, 2015 at 3:50 history edited Ali Moh CC BY-SA 3.0
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Mar 12, 2015 at 3:38 comment added user70720 Let us continue this discussion in chat.
Mar 12, 2015 at 3:38 comment added user70720 Lets take this discussion to chat. Thank you very much for answering my inquiries.
Mar 12, 2015 at 3:37 comment added user70720 Okay. So common sense has to be used along with Maxwell's equations to derive the Coloumb law. Does that mean that Coloumb's law isn't fully contained within Maxwell's equations and Lorentz's equation, but also with the fact that a small charge cannot produce an infinit energy?
Mar 12, 2015 at 3:34 comment added Ali Moh No. It has to do with common sense and everyday experience, that a small charge cannot produce an infinite energy that permeates the entire universe.
Mar 12, 2015 at 3:33 comment added user70720 So $E$ has to vanish at $r→∞$ because otherwise conservation of energy will be violated? In other word, is the boundary condition $E→0$ as $r→∞$ motivated by the physical principle of conservation of energy?
Mar 12, 2015 at 3:26 comment added Ali Moh A situation where $E\neq 0$ at $r\rightarrow\infty$ is the hypothetical problem you see in electrostatics where you have an "infinite" uniformly charged wire. Or an "infinite" uniformly charged sheet.
Mar 12, 2015 at 3:25 comment added Ali Moh To be precise it has to vanish at least as fast as $1/r$, because: 1- because otherwise this would imply that you can feel an electron in Andromeda. 2 - This would imply that the electric energy stored in the electromagnetic field of a small charge to be infinite (forgetting now about the energy exactly near the point charge).
Mar 12, 2015 at 3:18 comment added user70720 Thanks for the re-edit. Why does $E→0$ as $r→∞$? Do there exist situations where $E$ is not zero at $r = ∞$, or am I missing something obvious?
Mar 12, 2015 at 3:17 comment added Ali Moh The justification for spherical symmetry when deriving coulombs law using Gauss's law is inevitable, because if a spherically symmetric charge resulted in an asymmetric electric field this would be a very nontrivial statement about the electric permittivity of the vacuum.
Mar 12, 2015 at 3:13 history edited Ali Moh CC BY-SA 3.0
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Mar 12, 2015 at 3:01 review Low quality answers
Mar 12, 2015 at 3:16
Mar 12, 2015 at 2:59 history edited Ali Moh CC BY-SA 3.0
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Mar 12, 2015 at 2:59 comment added Ali Moh My answer was misleading, i'll edit it.
Mar 12, 2015 at 2:55 comment added user70720 Also, would it make sense for a different boundary condition to be chosen such that $F(x)$ is a nonconstant function?
Mar 12, 2015 at 2:46 comment added user70720 Thanks for the response. How can coloumb's law be derived from Maxwell's law and Lorentz's law without resorting to ambiguities or assumptions? Is there a link? Most texbooks include a proof using the integral form of Maxwell's equations, but the spherical symmetry of the electric field is assumed, without justification.
Mar 12, 2015 at 2:42 history answered Ali Moh CC BY-SA 3.0