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Oct 19 at 10:10 history edited LPZ CC BY-SA 4.0
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Jul 1 at 11:36 history edited LPZ CC BY-SA 4.0
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Oct 26, 2023 at 19:05 history edited LPZ CC BY-SA 4.0
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Sep 25, 2023 at 23:00 comment added Ján Lalinský > "Essentially, it shows that an isolated wire is not physical, and they always come in pairs of opposing currents like in waveguides (this is a form of confinement). " Isolated wire certainly is physical, and they do not always come in pairs. Infinite wire, isolated or not, is unphysical.
Sep 25, 2023 at 22:20 history edited LPZ CC BY-SA 4.0
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Sep 25, 2023 at 20:26 history edited LPZ CC BY-SA 4.0
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Aug 24, 2023 at 4:41 comment added LPZ No, with an oscillating current, the magnetic field will be oscillating as well. Even the OP’s solution shows oscillations, as usual, the electric and magnetic field are merely in quadrature.
Aug 24, 2023 at 4:37 history edited LPZ CC BY-SA 4.0
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Aug 24, 2023 at 0:03 comment added Ján Lalinský @LPZ displacement current is vital here: if we assume it vanishes, magnetic field is restricted to be a linear function of time, and OP assumes oscillating current, which will have oscillating magnetic field.
Aug 23, 2023 at 23:23 history edited LPZ CC BY-SA 4.0
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Aug 23, 2023 at 23:19 comment added LPZ The OP used the quasistatic approximation, so I just focused on its consistencies. Taking into account the displacement current is not always necessary.
Aug 23, 2023 at 23:17 history edited LPZ CC BY-SA 4.0
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Aug 23, 2023 at 18:50 comment added Ján Lalinský The electric field obeys $\nabla \times \mathbf E = - \frac{\partial \mathbf B}{\partial t}$, but this equation is not enough to find the fields, we need the other equation $\nabla \times \mathbf B = \mu_0 \mathbf j + \mu_0\epsilon_0 \frac{\partial \mathbf E}{\partial t}$ too. I think it makes no sense to seek solutions to only $\nabla \times \mathbf E = 0$ here, the magnetic term is important.
Aug 23, 2023 at 18:45 comment added Diger I see, anyway. I think Jan's answer is more what I was actually looking for, but I wouldn't mind if you elaborate specifically on the last point about the log-divergence and how it arises and cancels with two wires?
Aug 23, 2023 at 18:42 comment added Ján Lalinský The relevance is that electric field with zero curl is wrong for the assumed situation - the correct field has to have non-zero curl in general (that can be zero only at special position and time).
Aug 23, 2023 at 18:00 comment added LPZ @Diger It’s rather an “option. The formalism allows you to add a uniform charge distribution (since you are looking at $z$ invariant solutions). If you set $c_1=0$, then there will be no charge.
Aug 23, 2023 at 17:58 comment added LPZ @JánLalinský yes for the second charge density commentary, it was just a bad copy paste. For your first comment, I don’t see how it’s relevant. I’m just looking at the homogeneous solutions, the discussion is purely mathematical.
Aug 23, 2023 at 17:56 history edited LPZ CC BY-SA 4.0
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Aug 23, 2023 at 17:18 comment added Diger Just wondering, if I have a current along the $z$-axis, does it necessarily represent a charge distribution as well? I mean, this is how I interpret this answer, because I was actually only considering a current, not a charge.
Aug 23, 2023 at 17:15 comment added Ján Lalinský Circulation of $\mathbf E$ has nothing to do with charge distribution on the z axis. For field $\frac{c_2}{2\pi r} \mathbf e_{\varphi}$, circulation is non-zero but does not depend on radius, so curl of such field vanishes except on the z axis.
Aug 23, 2023 at 17:09 comment added Ján Lalinský $\nabla \times \mathbf E = 0$ does not hold except in static case where $\mathbf B = const.$, or specific instants when $\partial \mathbf B/\partial t = 0$.
Aug 23, 2023 at 16:43 history answered LPZ CC BY-SA 4.0