lecture 5 - birminghamepweb2.ph.bham.ac.uk/user/lazzeroni/em2_2017/lecture5_em... · 2017. 1....
TRANSCRIPT
Maxwell’s equations for free space
They apply simultaneously at any given point in free space.How do they change in presence of material ?
Lecture 4:
Atomic/molecular dipoles
Macroscopic polarization P
Equivalent charge/current
Re-expression of M1 in dielectrics: electric displacement D
LIH:
Relative permittivity Electric susceptibility
Lecture 5: Magnetism (I)
Atomic / molecular magnetic dipoles Macroscopic magnetization MTypes of magnetism and their microscopic origin: diamagnetism paramagnetism ferromagnetism
Why useful ?
TransformersMotorsGenerators
Iron cores
Magnetic recording tapes
Computer disks
All depend directly on magnetic properties of materials
Magnetism
Magnetism is linked to the behaviour of electrons in materials:moving charges, orbital motion and intrinsic spin.
Net magnetic moment of atom is obtained by combining orbital and spin moments of all the electrons, taking into account their direction.
Why isn’t everything magnetic ?
In a sense, everything is magnetic !But material only exhibit “familiar” magnetic effects when: - atoms contain unpaired electrons and- large scale alignment of the dipole moments occur
Orbital motion
Spin :
Magnetic and electric dipoles :
Paramagnetism : Atoms of a paramagnetic material have permanent magneticdipoles. These dipoles are randomly oriented - magnetic fields averageto zero.
In external field B0, dipoles tends to align with B0.Result in an additional magnetic field Bm
N atoms, maximum dipole moment = µNThermal collisions randomize dipole orientation and reducetotal dipole moment.
Paramagnetism :
Relative permeability = ratio between field in material and applied field.If material doesn’t respond to B0, km =1
Magnetic moment per unit volume M (magnetization):
Magnetic susceptibility
Magnetic susceptibility: small, dimensionless number;value depends on temperature, pressure.
Paramagnetic: B > B0 , km > 1 , χB > 0Example: for Oxygen (atmospheric pressure, 20oC)
LIH material Linear : M is proportional to B Isotropic : M is in the same direction as B Homogeneous : same throughout the material
Paramagnetism : very temperature dependent
Glass km = 1 - 1.5 x10-5 Water χB / 10-6 = - 9.0
km<1
Superconductors are an exception χB = -1
Diamagnetism :
Ferromagnetism : Materials with atoms having unpaired electron spins.Electron spins become coupled to form a domain (~1010 atoms, scale of 10-7 m) Large electromagnetic moment
When domains are randomly arranged, material as a wholeis un-magnetised
Ferromagnetism :
km becomes very large: ~103 - 105
Domains which are magnetized in the direction of an appliedexternal field grow at the expenses of those which are not aligned to the magnetic field
Ferromagnetism :
Magnetization curve: M versus B0
Ferromagnetism : Hysteresis loop: BM versus B0
Ferromagnetism :
Ferromagnetism :
Magnetization is different when theexternal field is increasing fromwhen it is decreasing: hysteresis
Cause: reorientations of domaindirections are not totally reversible
Use: magnetic storage of information
Review : Materials can be grouped into para-, dia-, and ferro-magnetic
Diamagnetics: atoms don’t have intrinsic magnetic dipole moment. A dipole moment may be induced by an external field,its direction being opposite to that of the field (Lenz’s law).χB is negative and usually small.
Paramagnetics: atoms have a magnetic dipole moment due tounpaired electrons. Intrinsic magnetic dipole moments tend to line up with external magnetic field thus enhancing (slightly) the field. This tendency is interfered by thermal agitation whichrandomizes the alignment. χB is positive and small and very temperature dependent.
Review : Ferromagnetics: quantum interaction between neighbouringatoms locks atomic dipoles in rigid parallelism despite disordering tendency of thermal agitation (magnetic domains).Due to alignment of spin magnetic moments of electrons(quantum effect).M is no longer proportional to B.Hence χB not well defined, but generally positive and large.
Hysteresis: ferromagnetic magnetization curves do not retracethemselves. Some alignment of dipoles remain even whenthe external field if removed. Familiar “permanent” magnets.
Summary :
Effect χB km Origin
Recommended readings:Grant+Phillips: 4.3, 5.1, 5.2
Next Lecture: Magnetism (II)
Maxwell’s equations for magnetic materials