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3.2.2.
Magnetic
Field Sources <CJ chap 21.7-21.10 >
3.2.2.1.
Discussion
3.2.2.1.1.
The
Right Hand Rule (RHR): determines the x product, and the direction of B around
currents
3.2.2.1.2.
Magnetism
in matter arises from the currents in matter and magnetic moments of particles
3.2.2.1.2.1.
The magnetic moment of a loop of
current is the ‘fundamental magnet’
3.2.2.1.2.2.
Use the RHR to get the N and S poles
for such a loop.
3.2.2.1.3.
3.2.2.2.
Mathematical
3.2.2.2.1.
Biot-Savart
law: Magnetic fields arise from the motion of electric charge, i.e. electric
currents
3.2.2.2.1.1.
DB = (mo/4p) I Ds x runit / r2 where I = current, Ds = length of wire, DB = mag. Field
3.2.2.2.1.2.
(mo/4p) = km = 1E-7 exactly thus defining the value of mo, the permeability of free space
3.2.2.2.1.3.
The unit vector runit points from the
current segment Ds to the point r where B is to be found
3.2.2.2.2.
B = mo I /(2pa) gives the
magnetic field a distance ‘a’ from an infinite straight wire
3.2.2.2.3.
B = mo I R2 /(2 x2 + R2)3/2 = B field on the axis a distance x
from a circular loop of current I, Radius R,
3.2.2.2.4.
F/s = mo I1 I2 /(2pa) =
force between two long parallel wires a distance ‘a’ apart with currents I1 and I2
3.2.2.2.4.1.
Defines the Ampere if the force per
m = 2E-7 results from equal currents I1 and I2 of both 1 Amp
3.2.2.2.5.
Ampere’s
law: B x distance around a closed
loop = moI
3.2.2.2.6.
B = mo n I = B field in a solenoid with n = N / l (# of turns per length)
3.2.2.3.
Advanced
3.2.2.3.1.
Biot-Savart
law: dB = (mo/4p)
I ds x runit / r2 where I = current, ds = length of wire, DB = mag. Field
3.2.2.3.2.
Gauss
Law for Magnetism
B
ds = 0 = the magnetic flux through any closed
surface
3.2.2.3.3.
Ampere’s
law:
B
ds = mo I
3.2.2.3.4.
Ampere’s
law modified by Maxwell displacement current
B
ds = mo I + mo eo d(
B
ds)/dt
3.2.2.3.4.1.
Using a cylindrical surface around a
wire ending in a capacitor then EA = Q/eo
3.2.2.3.4.2.
thus eo dF/dt = dQ/dt = IMaxwell & using this IMaxwell in addition to the I in
Amperes law gives result
3.2.2.3.5.
The
Magnetization vector, M, = magnetic moment per unit volume and
3.2.2.3.5.1.
Thus B = B0 + Bm = B0 + moM = mo (H + M)
3.2.2.3.5.2.
For paramagnetic and diamagnetic
substances, M = c H where c = the magnetic susceptibility
3.2.2.3.5.2.1.
with mm = mo (1 + c) substances are classified as
3.2.2.3.5.2.2. paramagnetic mm > m0 , diamagnetic mm < m0 , and ferromagnetic mm >> m0