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Physicsissuef
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Why a magnetic flux in closed surface area is always 0?
dst said:Apply Lenz' law to a spherical hollow surface, all the charges move to oppose the magnetic field and each other and it all cancels out.
Compare with gravity...
This is one of Maxwell's equations. It essentially says that there are no magnetic monopoles (only dipoles, which give no net flux through any surface surrounding them). See: http://hyperphysics.phy-astr.gsu.edu/hbase/electric/maxeq2.html#c2"Physicsissuef said:Why a magnetic flux in closed surface area is always 0?
I saw that law, but still can't understand what is happening inside the closed surface.Doc Al said:This is one of Maxwell's equations. It essentially says that there are no magnetic monopoles (only dipoles, which give no net flux through any surface surrounding them). See: http://hyperphysics.phy-astr.gsu.edu/hbase/electric/maxeq2.html#c2"
Contrast this with Gauss's law for electric fields. No problem getting a non-zero electric flux through a closed surface--just have it enclose a net charge.
Yep. Maxwell's equations still hold.jdg812 said:In the case of STATIONARY fields, the magnetic flux through a closed surface is definitely zero.
And what about non-stationary fields? Is it still zeroing?
Does it help to think about the fact that lines of magnetic flux are always closed loops (since there are no monopoles for them to begin or end on)? You can't draw a closed loop that intersects a closed surface at only one point; it goes in at one point and out at another - i.e. number of "innies" = number of "outies", hence zero net flux.Physicsissuef said:Why a magnetic flux in closed surface area is always 0?
belliott4488 said:Does it help to think about the fact that lines of magnetic flux are always closed loops (since there are no monopoles for them to begin or end on)? You can't draw a closed loop that intersects a closed surface at only one point; it goes in at one point and out at another - i.e. number of "innies" = number of "outies", hence zero net flux.
Not really - as stated in a previous post, the lines of electric flux do not have to total zero through a closed surface. The Faraday cage has more to do with charges in the cage realigning themselves to cancel the contained field. It works only with an electrically conductive closed surface; it's not true for just any mathematical closed surface, as it is for the case of the magnetic flux through a closed surface.Physicsissuef said:Does it have something with the Faraday's cage?
But isn't the magnetic flux, a magnetic field perpendicular to some area? How is possible that the magnetic field is 0, when still it exists?belliott4488 said:Not really - as stated in a previous post, the lines of electric flux do not have to total zero through a closed surface. The Faraday cage has more to do with charges in the cage realigning themselves to cancel the contained field. It works only with an electrically conductive closed surface; it's not true for just any mathematical closed surface, as it is for the case of the magnetic flux through a closed surface.
You can define a surface perpendicular to the lines of the magnetic field if you want to, but that's not necessary for the statement in question - it's true for any closed surface, no matter how it is oriented.Physicsissuef said:But isn't the magnetic flux, a magnetic field perpendicular to some area? How is possible that the magnetic field is 0, when still it exists?
Ok, I understand now. And what happens in the Faraday's cage? Are just the sum of all the flux lines zero?belliott4488 said:You can define a surface perpendicular to the lines of the magnetic field if you want to, but that's not necessary for the statement in question - it's true for any closed surface, no matter how it is oriented.
And no - the magnetic field is not zero, nor is the flux (this was stated in an earlier post - please read them all). It's the net flux, i.e. the sum of all the flux lines across the surface, that is zero. It just means that there is much field "flowing" out of the surface as there is field "flowing" into the surface. Again, it has to do with the closed loops: every one that exits must also reenter.
Well, that's kind of a funny question, since a Faraday cage relies on the presence of electric charges on the surface, so there will be flux line originating on the surface itself. I guess the correct thing to say, since there are no flux lines in the space inside the surface, is that the flux lines from any external field are exactly canceled by the flux lines from the rearranged charges on the cage, so you could conclude that the flux is zero everywhere on the surface, not just summed up.Physicsissuef said:Ok, I understand now. And what happens in the Faraday's cage? Are just the sum of all the flux lines zero?
And can I ask you another question? How is possible that the field of the permanent magnet is changed (delta B)? Here is the http://hyperphysics.phy-astr.gsu.edu/hbase/electric/farlaw.html#c2"belliott4488 said:Well, that's kind of a funny question, since a Faraday cage relies on the presence of electric charges on the surface, so there will be flux line originating on the surface itself. I guess the correct thing to say, since there are no flux lines in the space inside the surface, is that the flux lines from any external field are exactly canceled by the flux lines from the rearranged charges on the cage, so you could conclude that the flux is zero everywhere on the surface, not just summed up.
That's my immediate response, anyway. Maybe someone else will disagree ...
The field of the permanent magnet is not being changed. The field (and thus flux) within the conducting loop changes as the magnet is moved.Physicsissuef said:How is possible that the field of the permanent magnet is changed (delta B)?
But I think, if I get close permanent magnet (depends on the material), the magnetic domains inside the loop will align, so it will become also permanent magnet. So when I'll return the magnet back, the domains will not align like on the start, right?Doc Al said:The field of the permanent magnet is not being changed. The field (and thus flux) within the conducting loop changes as the magnet is moved.
No. Treat the conducting loop as being made from a non-magnetic material, such as copper wire.Physicsissuef said:But I think, if I get close permanent magnet (depends on the material), the magnetic domains inside the loop will align, so it will become also permanent magnet. So when I'll return the magnet back, the domains will not align like on the start, right?
Doc Al said:No. Treat the conducting loop as being made from a non-magnetic material, such as copper wire.
The only magnetic field contribution from the conducting loop is due to the current flowing through it.Physicsissuef said:So, when I put back the magnet, the magnetic field of the conducting loop will realign, right?
Yes, but there are 3 kinds of fields, in this case. B induced, the magnetic field induced due to flowing current, B, the field of the permanent magnet, and delta B, which is actually I think the field inside the coil, but from the spin and orbital momentum of the electrons. So, I think that when I approach permanent magnet, so it will align the domains (temporary), because there is non-magnetic material. But when I get back the permanent magnet, the domains will realign in their first condition. What do you think?Doc Al said:The only magnetic field contribution from the conducting loop is due to the current flowing through it.
I think you're confusing issues when you speak of domains realigning in this case. The induced electric current is what creates a B field to compensate for the changing flux. There's no need to speak of domains, nor of additional fields - not explicitly, at least. You can just use Faraday's Law to calculate the induced current, and you don't have to think about the induced B field at all.Physicsissuef said:Yes, but there are 3 kinds of fields, in this case. B induced, the magnetic field induced due to flowing current, B, the field of the permanent magnet, and delta B, which is actually I think the field inside the coil, but from the spin and orbital momentum of the electrons. So, I think that when I approach permanent magnet, so it will align the domains (temporary), because there is non-magnetic material. But when I get back the permanent magnet, the domains will realign in their first condition. What do you think?
I think, I am right in this case. How does the delta B field changes than, by your opinion?belliott4488 said:I think you're confusing issues when you speak of domains realigning in this case. The induced electric current is what creates a B field to compensate for the changing flux. There's no need to speak of domains, nor of additional fields - not explicitly, at least. You can just use Faraday's Law to calculate the induced current, and you don't have to think about the induced B field at all.
No, there are only two sources of magnetic field in this situation. The field from the magnet and the induced field from the current. "Delta B" is an attempt to describe how the magnetic field is changing due to the movement of the magnet. For example: When you move the north pole towards the coil, delta B points towards the coil (since the field in the coil is increasing).Physicsissuef said:Yes, but there are 3 kinds of fields, in this case. B induced, the magnetic field induced due to flowing current, B, the field of the permanent magnet, and delta B, which is actually I think the field inside the coil, but from the spin and orbital momentum of the electrons.
I think you're mistaken.So, I think that when I approach permanent magnet, so it will align the domains (temporary), because there is non-magnetic material. But when I get back the permanent magnet, the domains will realign in their first condition. What do you think?
Doc Al said:No, there are only two sources of magnetic field in this situation. The field from the magnet and the induced field from the current. "Delta B" is an attempt to describe how the magnetic field is changing due to the movement of the magnet. For example: When you move the north pole towards the coil, delta B points towards the coil (since the field in the coil is increasing).
I think you're mistaken.
Yes, B is the external magnetic field. That page doesn't talk about delta B, since the field isn't changing. The loop moves in this case, so the flux through the loop changes. But it's the same idea as in all the other pages on this site: What matters is how the flux changes due to the external field. That determines the induced EMF and current in the loop.Physicsissuef said:Btw- Here says that B is external magnetic field, thus delta B is change of the external magnetic field. What is http://hyperphysics.phy-astr.gsu.edu/hbase/electric/imgele/fday.gif"
"Delta" just means change. It's just a way of describing how the field in the loop is changing. It's not a separate field.Physicsissuef said:So delta B in practical way, doesn't exists, right?
Doc Al said:"Delta" just means change. It's just a way of describing how the field in the loop is changing. It's not a separate field.
There's no delta B mentioned on this link. In http://hyperphysics.phy-astr.gsu.edu/HBASE/electric/farlaw.html" there appears delta (B*A), which is the change in magnetic flux. In your link, only A changes so the change in flux = delta (B*A) = B*delta(A).Physicsissuef said:And in the http://hyperphysics.phy-astr.gsu.edu/hbase/electric/imgele/fday.gif" , there is delta B * delta A. In this case, delta B is the change of the field of the loop?
And can I ask you why on the 1-st example there is so much bigger voltage (-16 volts), and in the example below (-0,004 volts)? What is the difference? In the first example there are two coils (it is actually transformator).Doc Al said:There's no delta B mentioned on this link. In http://hyperphysics.phy-astr.gsu.edu/HBASE/electric/farlaw.html" there appears delta (B*A), which is the change in magnetic flux. In your link, only A changes so the change in flux = delta (B*A) = B*delta(A).