Electric field within solenoid

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Discussion Overview

The discussion revolves around the presence or absence of a radial electric field within a solenoid and around a current-carrying wire. Participants explore concepts from electromagnetism, including Gauss's law and Maxwell's equations, while addressing both theoretical and practical implications of electric and magnetic fields in these contexts.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant questions why a radial electric field cannot exist within a solenoid, expressing confusion over the application of Gauss's law and Faraday's law.
  • Another participant inquires about the net charge of a current-carrying wire and whether the magnetic field is changing over time.
  • A participant explains that Gauss's law indicates no radial electric field exists inside a solenoid due to zero enclosed charge, even with a time-varying current.
  • Some participants suggest that a current-carrying wire could be modeled as a line of moving charge, potentially leading to a net charge under certain conditions.
  • There is a discussion about the implications of enclosing a line of current with a Gaussian surface, with some arguing that the net charge remains zero in typical scenarios.
  • One participant proposes that imperfections in symmetry could lead to a small radial component inside the solenoid, while also noting that local surface charges in a current-carrying wire could contribute to a small radial electric field.

Areas of Agreement / Disagreement

Participants express differing views on the existence of a radial electric field within a solenoid and around current-carrying wires. While some argue for the absence of such fields based on symmetry and charge considerations, others suggest that imperfections and local surface charges could introduce small radial components. The discussion remains unresolved with multiple competing views.

Contextual Notes

Participants reference various Maxwell's equations and their implications, but there are limitations in the assumptions made regarding charge distribution and the idealized nature of the solenoid and wire models. The discussion also touches on advanced concepts like the Hall effect without reaching a consensus on their relevance to the main question.

blintaro
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Hello all,

I can't figure out why it is impossible to have a radial electrical field within a solenoid. My gut tells me there would be one. For that matter, I also don't understand why there is no radial component surrounding a current carrying wire. Considering gauss' law has not helped me so far since I can't restrict the radial and longitudinal components of flux. I also tried to consider faraday's law by reasoning that the product (b field) of the curl must be along the axis (z direction) in cylindrical coordinates but that just created more conditions on the components of E.

If anyone can help it would be really appreciated, I might be a little butthurt since I spent the majority of my exam time puzzling over this an consequently ran out of time. Whoops!
 
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Does a current carrying wire have a net charge? Is the magnetic field changing in time?
 
The Maxwell's equations for the electric field ## E ## need to be considered. One is ## \nabla \cdot E=\rho/\epsilon_o ##. With Gauss's law, this becomes in integral form ## \int E \cdot dA=Q/\epsilon_o ##. The current carrying solenoid has radial symmetry and the enclosed ## Q ## is zero. This equation tells us there will be no radial electric field ## E ## inside a solenoid, even for a time-varying current. The other Maxwell equation involving ## E ## is ## \nabla \times E=-dB/dt ## which in integral form using Stokes theorem becomes ## \oint E \cdot dl=-d(BA)/dt ## where ## BA ## is the magnetic flux across the area of the path of the line integral . For the steady state case, this gives ## E=0 ## for the ## \phi ## component, but for a time varying solenoid current, the changing ## B_z ## will result in a ## \phi ## component of ## E ## which is a Faraday EMF inside the solenoid (as well as outside of the solenoid). Perhaps this helps to answer your question. Meanwhile there are no electrical charges to generate any static ## E_z ##. Even for a time-varying current, I believe ## E_z=0 ##, but this last one is a minor detail that can be worked out by considering another of Maxwell's equations ## \nabla \times B=\mu_o J +\mu_o \epsilon_o dE/dt ##.
 
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That's a good question! Since the definition of current is time varying charge I don't see why it can't be modeled as a line of moving charge. Which can be integrated along a line at given moment of time to give some amount of net charge.

In this case the magnetic field in the solenoid was varying because the current around the solenoid was dependent on time.
 
Ah I see! The enclosed charge must be zero! What about when the Gaussian surface encloses a line of current, then there might be enclosed charge right?
 
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blintaro said:
Ah I see! The enclosed charge must be zero! What about when the Gaussian surface encloses a line of current, then there might be enclosed charge right?
Normally a line of current in a conductor is still electrically neutral. The net charge contained in any portion of the conductor is considered to be zero. In some very advanced treatments of the subject, there may be some non-neutral cases considered, e.g. the Hall effect, but for most elementary cases, the current carrying conductor is assumed to be electrically neutral.
 
I think that makes sense in terms of an ionic fluid or free electrons in a metal... So does that mean if a wire connected a charged sphere to an uncharged sphere, say, then there would be quantitatively different behavior?
 
There will be radial component inside the solenoid , though very small, and that is due to imperfection in the symmetry (a solenoid is a helix, a not a series of perfect cyclic currents closely spaced together as we theoretically view it).

There will also be radial component in the case of a straight wire carrying current, and that is because - though the conductor will have zero net charge as a whole- of the local surface charges that are present. But these surface charge densities are small also so the radial component will be very small, practically zero.
 
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