- #1
da_willem
- 599
- 1
Suppose the magnetization of some substance depends on the field H and temperature, i.e. M(H,T) and we have the mathematical identity
[tex]\nabla \int _0 ^H M dH = M \nabla H + \int _0 ^H \nabla M dH[/tex]
then it is derived in Ferrohydrodynamics (fhd) by Rosensweig that
[tex]\nabla \int _0 ^H M dH = M \nabla H + \int _0 ^H \frac{\partial M}{\partial T} dH[/tex]
but what happened with the dependence of M on H?! Shouldn't the above include a term
[tex] \int _0 ^H \frac{\partial M}{\partial H} \nabla H dH[/tex]
or is there some reason this should vanish? Can someone help me out of my misery?
[tex]\nabla \int _0 ^H M dH = M \nabla H + \int _0 ^H \nabla M dH[/tex]
then it is derived in Ferrohydrodynamics (fhd) by Rosensweig that
[tex]\nabla \int _0 ^H M dH = M \nabla H + \int _0 ^H \frac{\partial M}{\partial T} dH[/tex]
but what happened with the dependence of M on H?! Shouldn't the above include a term
[tex] \int _0 ^H \frac{\partial M}{\partial H} \nabla H dH[/tex]
or is there some reason this should vanish? Can someone help me out of my misery?