Why does my textbook only show magnetostatics when curl of H = 0?

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Discussion Overview

The discussion revolves around the conditions for magnetostatics, particularly the implications of the curl of the magnetic field intensity vector H being zero. Participants explore the definitions and assumptions surrounding magnetostatics, the role of currents, and the relationship between the magnetic field and its behavior in time and space.

Discussion Character

  • Debate/contested
  • Conceptual clarification
  • Technical explanation

Main Points Raised

  • Some participants assert that curl of H = 0 indicates a magnetostatic situation, suggesting that H should be a constant vector field.
  • Others argue that curl of H can be non-zero in the presence of steady currents, which complicates the definition of magnetostatics.
  • It is noted that magnetic fields can only arise when a current is present, leading to questions about the constancy of H and whether this aligns with magnetostatics.
  • Some participants reference Biot-Savart law and Ampere's law to illustrate that a steady current produces a steady magnetic field, even outside the region of the current.
  • A later reply emphasizes that the curl operator relates to spatial changes in H, not temporal behavior, and that magnetostatics is defined by a constant magnetic field over time.
  • Participants discuss the distinction between free currents and bound currents in the context of magnetostatics, questioning the textbook's assertion that magnetostatics only applies when curl of H = 0.
  • One participant challenges the notion that magnetostatics cannot involve electrical coils, suggesting that a constant magnetic field can be established without magnets.

Areas of Agreement / Disagreement

Participants express differing views on the definition of magnetostatics and the implications of curl of H. There is no consensus on whether the conditions outlined in textbooks accurately reflect the complexities of the topic.

Contextual Notes

Some participants highlight that magnetostatics involves steady currents, which may lead to non-zero curl of H, indicating a potential misunderstanding of the definitions involved. The discussion reveals uncertainties regarding the relationship between current, magnetic fields, and the conditions for magnetostatics.

pivoxa15
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In my textbooks it shows curl of H = 0 is a situtaion of magnetostatics but in here http://en.wikipedia.org/wiki/Magnetostatics it shows otherwise assuming J can be anything. Which is correct?

Magnetostatics is defined to be when the magnetic field is constant so H should be a vector field with scalar components suggesting that curl of H=0.
 
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curl of H will be 0 outside regions with currents.
 
I also should have mentioned that magnetic fields can only arise when a current is present. So a constant current must be present. But it means H will be a non constant field so can't be magnetostatics?

Outside regions with current, magnetic fields don't even exist - which can't be magnetostatics can it? i.e. no charges is not electrostatics.

We seem to have a problem either way. What am I missing?
 
pivoxa15 said:
I also should have mentioned that magnetic fields can only arise when a current is present. So a constant current must be present. But it means H will be a non constant field so can't be magnetostatics?

I wonder how you make that conclusion. It is readily seen from say Biot savard law, or Ampere law over a circle centered on the axis of a wire in which a steady current flows that the megnetic field is constant in time.

pivoxa15 said:
Outside regions with current, magnetic fields don't even exist

wahoo! Then how can a magnet work?! No, a steady current creates a steady magnetic field in all space.
 
The relation between the magnetic field and its div and curl is the following:

https://www.physicsforums.com/showthread.php?t=127264&highlight=helmholtz

Open the doc file called "Question.doc" and replace F by H in that equation. The integrals are over the whole universe. The first integral is always 0 because the divergence of H is always 0. But you see that as soon as there is a current somewhere in space, the the integral is non- vanishing.

The main lesson here is that [itex]\nabla\cdot \vec{H}=0[/itex] and [itex]\nabla\times \vec{H}=0[/itex] at some points [itex]\vec{r}[/itex] does not imply [itex]\vec{H}(\vec{r})=0[/itex]. The value of H at some point depends on the value of J everywhere in space.
 
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quasar987 said:
I wonder how you make that conclusion. It is readily seen from say Biot savard law, or Ampere law over a circle centered on the axis of a wire in which a steady current flows that the megnetic field is constant in time.

I am thinking about the curl of H = 0 => constant vector field H => magnetostatics.

But on the website curl of H = nonzero constant current density => H is a nonconstant vector field => B is non constant vector field hence not megnetostatics.

The problem is the current density should not be 0 for anything to do with magnetics but that leads to nonconstant B field so no magnetostatics.
quasar987 said:
wahoo! Then how can a magnet work?! No, a steady current creates a steady magnetic field in all space.

In classical physics, we are taught to think about magnets as having mini current loops inside hence with many magnetic dipoles meaning magnetised material.
 
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I think I've hit it now:

The curl operator has nothing to do with how B behaves in time! It says something about how H changes in space. Magnetostatic is by definition a case where B is constant in time, not where the magnitude of B is the same at all points in space.
pivoxa15 said:
In classical physics, we are taught to think about magnets as having mini current loops inside hence with many magnetic dipoles meaning magnetised material.
Well exactly. A magnet's magnetic field is cause by its surface current. But the point is that it is a current that causes the field, but there is a non zero B field all around the magnet, not only where the current itself it.
 
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quasar987 said:
I think I've hit it now:

The curl operator has nothing to do with how B behaves in time! It says something about how H changes in space. Magnetostatic is by definition a case where B is constant in time, not where the magnitude of B is the same at all points in space.

Okay that makes more sense now. But there is still the question why my textbook shows magnetostatics only when curl of H = 0. The book later addressed with the fact that there are no free current in magnetostatics, which means the B fields in magnetostatics are never generated by electrical coils but rather by the magnets themselves (bound currents). But you could set up a constant B field with electrical coils without a magnet in sight couldn't you?
 
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pivoxa15 said:
Magnetostatics is defined to be when the magnetic field is constant so H should be a vector field with scalar components suggesting that curl of H=0.
Your problem is that this statement is wrong.
Magnetostatics means that all partial time derivatives are zero, so steady currents are allowed. The key equations are Curl H=4 pi j/c and
div j=0.
 
  • #10
pivoxa15 said:
Okay that makes more sense now. But there is still the question why my textbook shows magnetostatics only when curl of H = 0. The book later addressed with the fact that there are no free current in magnetostatics, which means the B fields in magnetostatics are never generated by electrical coils but rather by the magnets themselves (bound currents). But you could set up a constant B field with electrical coils without a magnet in sight couldn't you?

Certainly. Talk to your instructor about it.
 

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