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Lecture 9
Vector Magnetic Potential
Biot Savart Law
Prof. Viviana Vladutescu
Figure 1: The magnetic (H-field) streamlines inside and outside a
single thick wire.
Figure 2: The H-field magnitude inside and outside the thick wire
with uniform current density
Figure 3: The H-field magnitude inside and outside the thick
conductors of a coaxial line.
0
0
A
B)( TAB
A - vector magnetic potential (Wb/m)
Vector Magnetic Potential
Figure 1: The vector potential in the cross-section of a wire with
uniform current distribution.
Figure 2: Comparison between the magnetic vector potential component of a wire with uniformly distributed current and the
electric potential V of the equivalent cylinder with uniformly
distributed charge.
JAA
AAAAA
JA
02
2
0
)(
)()()(
JAA 020
Vector Poisson’s equation
Laplacian Operator (Divergence of a gradient)
Poisson’s Equation
In electrostatics
ED
VE
E
D
0
V
EE
V2 Poisson’s Equationin electrostatics
4
4
1
00
2
00
2
dvR
JAJA
dvR
VV
v
v
Magnetic Flux
(Wb) )(
cs
s
ldAdsA
dsB
The line integral of the vector magnetic potential A around any closed path equals the total magnetic flux passing through area enclosed by the path
Biot Savart Law and Applications
The Biot-Savart Law relates magnetic fields to the currents which are their sources. In a similar manner, Coulomb’s Law relates electric fields to the point charges which are their sources. Finding the magnetic field resulting from a current distribution involves the vector product, and is inherently a calculus problem when the distance from the current to the field point is continuously changing.
)( TAB
4
0 c R
ldIA
4
0
c R
ldIB
GfGfGf
11
40
c
ldR
ldR
IB
2
11
Ra
R R
By using
(T) 4 2
0
c
R
R
aldIB
(see eq 6.31)
Biot-Savart Law
20
4
R
aldIBd
BdB
R
c
In two steps
Illustration of the law of Biot–Savart showing magnetic field arising from a differential segment of current.
212
12112
4 R
aLdIHd
rzR arazaR
Example1Component values for the equation to find the magnetic field intensity resulting from an infinite length line of current on the z-axis. (ex 6-4)
r
aIH
rzr
zaIr
rz
dzaIr
rz
arazaIdzH rzz
24
)(4)(4
)(
222
23222
322
Example 2We want to find H at height h above a ring of current centered in the x – y plane.
The component values shown for use in the Biot–Savart equation.
2
0 2322 )(4
)(
ah
aaahaIadH rz
The radial components of H cancel by symmetry.
23
22
2
2
023
22
2
2
4
ah
aIaH
dah
aIaH
z
z
Solenoid
Many turns of insulated wire coiled in the shape of a cylinder.
For a set N number of loops around a ferrite core, the flux generated is the same even when the loops are bunched together.
Example : A simple toroid wrapped with N turns modeled by a magnetic circuit. Determine B inside the closely wound toroidal coil.
b
a
)()(,2
2
0
0
abrabr
NIaaBB
NIrBldB
Ampere’s Law
a) An iron bar attached to an electromagnet.b) The bar displaced by a differential length d.
Electromagnets
Levitated trains: Maglev prototype
Electromagnet supporting a bar of mass m.
Applications
Wilhelm Weber (1804-1891). Electromagnetism.