Ok...my physics book doesn't really have much along the lines of explanations for these things...so I have a few questions I'd like to clear up:
Diamagnetism is a direct result of Lenz's Law, right? Like, in the presence of a magnetic field, the electrons in the (otherwise neutral) diamagnetic material will begin to spin in the opposite direction to resist the incoming field, which results in an induced, anti-parallel B-field. Is that correct?
Now, if that's the case...if I place a diamagnetic material in a constant B-field, after some amount of time, the 'net change' effect would settle down and eventually stop...wouldn't it? And then in that case, wouldn't the induced dipoles under go a torqe-ing force in the same way that paramagnetic materials do? Or does this not happen b/c diamagnetic materials have induced dipoles? In that case, would it work more like...once the 'change' stops, if the induced-dipoles move back to their normal, non-magnetic state, lenz's law will cause them to return to their previous state (antiparallel to the comparatively strong magnet)? Sorry...I'm confused, lol
As for ferrogmagnets & paramagnets...why is it that ferromagnets are so much stronger than paramagnets? I read on google about the whole 'domain' theory and this "long range order" of electrons that creates domains, but I don't follow why that makes ferromagnets so much stronger. I mean, in a weak B-field, I can see why the already strong domains would experience significantly more torque than the individual dipoles of a paramagnet, which would result in a larger total # of dipoles reinforcing the external B-field...right?
However, if we have an extremely strong external magnet acting on both materials, wouldn't the net B-fields of both systems be about equal? I mean, in an extremely strong (infinitely strong?) magnetic field, one might expect all of the dipoles of both to allign in the same direction. In that case, would the ferromagnet and paramagnet still behave differently? I mean, if all the domains are pointing in the same direction (ferro), wouldn't that mean all the individual dipoles are pointing in the same direction...just like what would be happening in the paramagnet...??
I hope I'm not missing something incredibly obvious here...lol
TIA,
-Eric
Edit: ferro/paramagnets both experience the diamagnetic effects right? Is it just that the net-field generated by the parallel-aligned dipoles dominates the diamagnetic effect?
Edit2: Does the strength of ferromagnets have something to do with the fact that they don't lose strength under high temperature (well, until the Curie temp)? B/c I take it that paramagnets will grow weaker as the temperature rises, due to higher random movement of the atoms...
Diamagnetism is a direct result of Lenz's Law, right? Like, in the presence of a magnetic field, the electrons in the (otherwise neutral) diamagnetic material will begin to spin in the opposite direction to resist the incoming field, which results in an induced, anti-parallel B-field. Is that correct?
Now, if that's the case...if I place a diamagnetic material in a constant B-field, after some amount of time, the 'net change' effect would settle down and eventually stop...wouldn't it? And then in that case, wouldn't the induced dipoles under go a torqe-ing force in the same way that paramagnetic materials do? Or does this not happen b/c diamagnetic materials have induced dipoles? In that case, would it work more like...once the 'change' stops, if the induced-dipoles move back to their normal, non-magnetic state, lenz's law will cause them to return to their previous state (antiparallel to the comparatively strong magnet)? Sorry...I'm confused, lol
As for ferrogmagnets & paramagnets...why is it that ferromagnets are so much stronger than paramagnets? I read on google about the whole 'domain' theory and this "long range order" of electrons that creates domains, but I don't follow why that makes ferromagnets so much stronger. I mean, in a weak B-field, I can see why the already strong domains would experience significantly more torque than the individual dipoles of a paramagnet, which would result in a larger total # of dipoles reinforcing the external B-field...right?
However, if we have an extremely strong external magnet acting on both materials, wouldn't the net B-fields of both systems be about equal? I mean, in an extremely strong (infinitely strong?) magnetic field, one might expect all of the dipoles of both to allign in the same direction. In that case, would the ferromagnet and paramagnet still behave differently? I mean, if all the domains are pointing in the same direction (ferro), wouldn't that mean all the individual dipoles are pointing in the same direction...just like what would be happening in the paramagnet...??
I hope I'm not missing something incredibly obvious here...lol
TIA,
-Eric
Edit: ferro/paramagnets both experience the diamagnetic effects right? Is it just that the net-field generated by the parallel-aligned dipoles dominates the diamagnetic effect?
Edit2: Does the strength of ferromagnets have something to do with the fact that they don't lose strength under high temperature (well, until the Curie temp)? B/c I take it that paramagnets will grow weaker as the temperature rises, due to higher random movement of the atoms...