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Just a couple more comments on the E&M topics we covered in this thread:
Back in post 111 , the magnetomotive force (mmf) was discussed, and IMO it makes for much better physics if the mmf (## NI ## ) is taught as ## \oint H \cdot dl=NI ##. [Edit: It should be mentioned that instead of going along the path of the wire of the coil, as the integral of ## E ## that we computed to calculate the voltage, this integral goes around/through the core of the transformer, and the current is found from the amount of current that goes through a cross-section. The closed loop line integral comes from Stokes' theorem, with the area that has the loop as its perimeter defines the cross-section for the current].
Perhaps one item that arises in this case though is that the ## H ## needs some clarification on exactly what it is. I tried to present ## H ## with some detail starting in post 130. Without the extra detail, I think much of the magnetism subject with the ## B ##, ## H ##, and ##M ## can be a real puzzle.
On another item, the formula ## B=H+4 \pi M ##(cgs) and ## B=\mu_o H+M ## (mks) holds in all cases, even when currents in conductors are present. This necessarily results because ## H ## is defined to include currents in conductors as sources, as was mentioned in post 146 above. If we can write ## M=M(B) ##, then we can also write ## M=M(H) ##, but we find in many cases that ## M=M(B) ## isn't exactly the case either, largely because of the exchange interaction. With this interaction, the ## M ## at nearby locations, (i.e. neighboring atoms), has an effect on the ## M ## at a given location, and thereby the magnetic field ## B ## is not the only factor in determining what the magnetization ## M ## is at a given location.
The mathematical relationship between ## M ## and ## H ## remains a peculiar one at times in any case. In the case of linear ferromagnetic materials we have ## M=\mu_o \chi_m H ## where ## \chi_m ## can be 500 or more. Then we have cases such as the permanent magnet, where ## H ## points opposite the ## M ## in a permanent magnet. For a spherical shaped permanent magnet, ## H=-M/(3 \mu_o) ##, so we can draw the line ## M=-3 \mu_o H ## on our hysteresis curve of ## M ## vs. ## H ## to find the value that ## M ## will have for a permanent magnet with a spherical shape for that material. Why some materials make good permanent magnets while other materials (e.g. the linear ferromagnetic materials) have their ## M ## return to zero when the ## H ## that is applied from currents in conductors returns to zero could be worth further discussion, but I have yet to figure that part out yet. I think it is related to the way the domains are formed, but it seems to be somewhat complicated and there probably isn't a real simple answer.
In any case, I did want to present the ## H ## in as much detail as possible, because it sees some very widespread use. Hopefully we did a better job of presenting it above than some textbooks do, where they might define ## H ## as ## \mu_o H=B-M ##, and leave the reader guessing what it represents. And hopefully at least a couple readers found some of the details to be good reading. I welcome any feedback.
Back in post 111 , the magnetomotive force (mmf) was discussed, and IMO it makes for much better physics if the mmf (## NI ## ) is taught as ## \oint H \cdot dl=NI ##. [Edit: It should be mentioned that instead of going along the path of the wire of the coil, as the integral of ## E ## that we computed to calculate the voltage, this integral goes around/through the core of the transformer, and the current is found from the amount of current that goes through a cross-section. The closed loop line integral comes from Stokes' theorem, with the area that has the loop as its perimeter defines the cross-section for the current].
Perhaps one item that arises in this case though is that the ## H ## needs some clarification on exactly what it is. I tried to present ## H ## with some detail starting in post 130. Without the extra detail, I think much of the magnetism subject with the ## B ##, ## H ##, and ##M ## can be a real puzzle.
On another item, the formula ## B=H+4 \pi M ##(cgs) and ## B=\mu_o H+M ## (mks) holds in all cases, even when currents in conductors are present. This necessarily results because ## H ## is defined to include currents in conductors as sources, as was mentioned in post 146 above. If we can write ## M=M(B) ##, then we can also write ## M=M(H) ##, but we find in many cases that ## M=M(B) ## isn't exactly the case either, largely because of the exchange interaction. With this interaction, the ## M ## at nearby locations, (i.e. neighboring atoms), has an effect on the ## M ## at a given location, and thereby the magnetic field ## B ## is not the only factor in determining what the magnetization ## M ## is at a given location.
The mathematical relationship between ## M ## and ## H ## remains a peculiar one at times in any case. In the case of linear ferromagnetic materials we have ## M=\mu_o \chi_m H ## where ## \chi_m ## can be 500 or more. Then we have cases such as the permanent magnet, where ## H ## points opposite the ## M ## in a permanent magnet. For a spherical shaped permanent magnet, ## H=-M/(3 \mu_o) ##, so we can draw the line ## M=-3 \mu_o H ## on our hysteresis curve of ## M ## vs. ## H ## to find the value that ## M ## will have for a permanent magnet with a spherical shape for that material. Why some materials make good permanent magnets while other materials (e.g. the linear ferromagnetic materials) have their ## M ## return to zero when the ## H ## that is applied from currents in conductors returns to zero could be worth further discussion, but I have yet to figure that part out yet. I think it is related to the way the domains are formed, but it seems to be somewhat complicated and there probably isn't a real simple answer.
In any case, I did want to present the ## H ## in as much detail as possible, because it sees some very widespread use. Hopefully we did a better job of presenting it above than some textbooks do, where they might define ## H ## as ## \mu_o H=B-M ##, and leave the reader guessing what it represents. And hopefully at least a couple readers found some of the details to be good reading. I welcome any feedback.
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