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Electromagnetism. Zhu Jiongming Department of Physics Shanghai Teachers University. Electromagnetism. Chapter 1 Electric Field Chapter 2 Conductors Chapter 3 Dielectrics Chapter 4 Direct-Current Circuits Chapter 5 Magnetic Field Chapter 6 Electromagnetic Induction - PowerPoint PPT Presentation
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Electromagnetism
Zhu Jiongming
Department of Physics
Shanghai Teachers University
Electromagnetism
Chapter 1 Electric Field
Chapter 2 Conductors
Chapter 3 Dielectrics
Chapter 4 Direct-Current Circuits
Chapter 5 Magnetic Field
Chapter 6 Electromagnetic Induction
Chapter 7 Magnetic Materials
Chapter 8 Alternating Current
Chapter 9 Electromagnetic Waves
Chapter 5 Magnetic Field
§1. Introduction to Basic Magnetic Phenomena
§2. The Law of Biot and Savart
§3. Magnetic Flux
§4. Ampere’s Law
§5. Charged Particles Moving in a Magnetic Field
§6. Magnetic Force on a Current-Carrying Conductor
§7. Magnetic Field of a of a Current Loop
§1. Basic Magnetic Phenomena
Comparing with Electric Fields :E : charge electric field charge
( produce ) ( force )M :
Permanent Magnets Magnetic Effect of Electric Currents Molecular Current
Movingcharge
Movingcharge
magnetic field
Permanent Magnets
Two kinds of Magnets : natural 、 manmade Two Magnetic Poles : south S 、 north N Force on each other : repel ( N-N, S-S ) attract ( N-S ) Magnetic Monopole ?
Magnetic Effect of Electric Currents
Experiments Show Straight Line Current
I
S
N
I
N
S
Molecular Current—— Ampere’s Assumption
Two Parallel Lines Circular Current Solenoid and Magnetic Bar
Magnetic Field B
Experiment : Helmholts coils in a
hydrogen bulb , an electron gun
I I
M M’ Conclusion : moving charge
F = q v B ( Definition of B ) ( Electric Field : F = qE ) Unit : Tesla )Gauss10(
m/s1C
1NTesla 1 4
Magnetic Field Lines :( curve with a direction ) Tangent at any point on a line is in the direction of t
he magnetic field at that point
● Number of field lines through unit area perpendicular to B equals the magnitude of B
§2. The Law of Biot and Savart
1. The Law of Biot and Savart
2. Magnetic Field of a Long Straight Line Current
3. Magnetic Field of a Circular Current Loop
4. Magnetic Field on the Axis of a Solenoid
5. Examples
1. The Law of Biot and Savart
The field of a current element Idl
dB Idl , 1/r2 , sin r : Idl P : angle between Idl and r Proportionality constant : 0/4 = 10-7
20 sind
4d
r
lIB
20 ˆd
4d
r
I rlB
2
0 ˆd
4d
r
I rlBB
dB
Idl
r
P
rEE ˆd
4
1d
20
r
q
Direction : dBIdl , dB r
Integral :
Compare with :
2. Field of a Long Straight Line Current
current I , distance a
all dB in same direction
20 ˆd
4 r
I rlB
2
0 sind
4 r
lIB
2
1
dsin1
40
a
I
)cos(cos4 21
0
a
I
r
2
1
a PO
I
dllsin = a/r
ctg = - l/a
r = a/sin l = - a ctg
dl= ad/sin2Infinite long : 1= 0 , 2= ,
a
IB
2
0 Direction : right hand rule
3. Magnetic Field of a Circular Current
current I , radius R ,P on axis , distance a
20 ˆd
4d
r
I rlB
zoR
r
a
dB
P
dl
I
cos
sind
4 20
r
lIB
= 90o
cos = R/r
r2 = R2 + a2
lr
RId
4 30
2/322
20
)(2 aR
IR
Rl 2d
R
IBa
20,Oat)1( 0
:3
20
2,far)2(
a
RIBRa
:
component dB||= dBcossymmetry , dB cancel , B = 0
4. Field on the Axis of a Solenoid
current I, radius R, Length L,
n turns per unit length
dB at P on axis caused by nIdl
( as circular current )
I
PR l
dl
L
2/322
20
)(
d
2d
lR
lnIRB
d)sin(
20 nI
1
2
d)sin(20
nIB
)cos(cos2 210
nI
ctg = l/R
l = R ctg
dl= - Rd /sin2R2+ l2 = R2/sin2
Field on the Axis of a Solenoid
Direction :right hand rule
)cos(cos2 210
nI
B
PR
L
2
1
B
I
B
O L
(1) center ( or R << L ) 1= 0 , 2= , B = 0nI
(2) ends ( Ex. : left ) 1= 0 , 2= /2 , B = 0nI /2
(3) outside, cos1 、 cos2 same sign, minus, B small
inside, opposite sign, plus , B large
Example ( p.345/5 - 3 -11)Uniform ring with current , find B at the center.Sol. :
I
I
O
B
C
12
I1
I2
20 ˆd
4d
r
I rlB
0ˆd rlI
R
IB
20
2
2
210
1
R
IB
22
202 R
IB B1= B2
opposite direction
B = 0
2
2
1
R
R
21 )2( II
Straight lines : ( circular current : )
arc 1 :
arc 2 :
parallel : I1R1 = I2R2
Exercises
p.212 / 5-2- 3, 8, 12, 13, 16
§3. Magnetic Flux
1. Magnetic Flux
2. Magnetic Flux on Closed Surface
3. Magnetic Flux through Closed Path
Flux on area element dS
dB = B · dS = B dS cos Flux on surface S ( integral ) if B and dS in same direction ( = 0 ), write dS
= Magnitude of B
Unit : 1 Web = 1 T · m2
define number of B lines through dS = B · dS = dB
then line density =
1. Magnetic Flux
dS
B
SB B
d
dB : Flux per unit area perpendicular to B
BS
B
d
d
Show : (1) dB of current element Idl
B lines are concentric circles
these circles and the surface S either not intercross ( no contribution to flux ) or intercross 2 times ( in/out , flux +/- )
2. Magnetic Flux on Closed Surface
)surfaceclosedany(0d SS
SB
dB
11111 dddddin SBSB:
22222 dddddout SBSB:21 dd BB
21 dd SS
21 dd 0dd 21 0d
S
Idl
Magnetic Flux on Closed Surface
Show : (2) magnetic field of any currents
superposition : B = B1 + B2 + …
0dddd 21 SSSSSB
B lines are continual , closed , or
—— called The field without sources
Compare with : E lines from +q or , into -q or
—— called The field with sources
Turn the normal vector of S1
opposite, same as that of S2
then
3. Magnetic Flux through Closed Path
Any surfaces bounded by the closed path L have the same fluxShow :
L
S1 S2
n
n
0ddd21
SSSSBSBSB
21
ddSS
SBSB
21
ddSS
SBSB
—— called Magnetic Flux through Closed Path L
Exercises
p.214 / 5-3- 1, 3
§4. Ampere’s Law
1. Ampere’s Law
2. Magnetic Field of a Uniform Long Cylinder
3. Magnetic Field of a Long Solenoid
4. Magnetic Field of a Toroidal Solenoid
1. Ampere’s Law
Ampere’s Law : L : any closed loop I : net current enclosed by L
Three steps to show the law : L encloses a Long Straight Current I L encloses no Currents L encloses Several Currents
IL 0d lB
I
L
L Encloses a Long Straight Current I
Field of a long line current I : I
La
IB
2
0
sBlB dcosdd lB
d
20 aa
I
d2
0I
II
LL 00 d
2d
lBI
ds dld
LB
( direction: tangent )
L Encloses no Currents
Current I is outside L
21
dddLLL
lBlBlBI L2L1
)dd(2 21
0 LL
I
0)(2
0
I
L Encloses Several Currents
L encloses several currents
Principle of superposition : B = B1 + B2 + …
LL
lBBlB d)(d 21
I is algebraic sum of the currents enclosed by L direction of Ii with direction of L ( integral ):
right hand rule , take positive sign
)( 210 II I0
I0
2. Field of a Uniform Long Cylinder
radius R , current I ( outgoing ),find B at P a distance r from the axis
concentric circle L with radius r ,symmetry : same magnitude of B on L ,
direction: tangent
P
L
rBL
2d lB
)(2
0 Rrr
IB
rBL
2d lB
)(2 2
0 RrR
IrB
0 r
B
R
outside :
inside : 2
2
0 R
rI
radius R , current I ( outgoing ),field B at P a distance r from the axis
symmetry : B in direction of tangent
Direction is along the Tangent
P
B
3. Magnetic Field of a Long Solenoid
Field inside is along axis
Show : turn 180 o round zz’ : B B’
I opposite : B’ B’’
B’’ should coincide with B
a
d
d
c
c
b
b
aLlBlBlBlBlB ddddd
nIllBlB cdab 000 nIBab 0
0 cdB
nIllBlBab 0outin 00axison not if :nIB 0in
B’B
B’’
z’
z
ab
dc
direction :right hand rule
4. Field of a Toroidal Solenoid
Symmetry : B on the circle L
magnitude : same
direction : tangent
( L >> r , N turns )in :
out :
NILBL 0ind lB
nIL
NIB 0
0in
0d out LBL
lB
0out B
direction : right hand rule
if L , becomes a long solenoid
Surface current ( width l , thickness d )
5. Field of a Uniform Large Plane
dB
l
Jdl
Jld
l
I
llBlB zzL012d lB z
20
12
zz BB
012 2
nn EE比较电场:
Direction : parallel opposite on two sides
( right hand rule )
Exercises
p.215 / 5-4- 2, 3, 4, 5
§5. Charged Particles Moving in B
1. Motion of Charged Particles in a Magnetic Field
2. Magnetic Converging
3. Cyclotrons
4. Thomson’s e/m Experiment ( skip )5. The Hall Effect
1. Motion of Charged ParticlesLorents Force : F = q ( E + v B )if E = 0 , F = q v B
if v B , q moves in a circle
with constant speed
Centripetal force :qvB
R
mvF
2
C
OR
v
F
m, q=- e
Radius : R = mv/qB Period : T = 2R/v = 2 m/qB Frequency : f = 1/ T = qB/ 2 m Ratio of charge to mass : q/ m= v/BR = /B
2. Magnetic Converging
v making an angle with B : v || = v cos
v = v sin
Helical pathradius : sin
qB
mv
qB
mvR
cos
2|| qB
mvTvh
)( small ~sin vv
)small (~cos vv
R
h
P P’
pitch :
Magnetic Converging : different R , same h from P to P’ distance h
Take period of emf same as that of qaccelerated 2 times per revolution
v r ( ), T not changed
3. Cyclotrons
Principle : uniform field , outward
2 Dees , alternating emf
q accelerated as crossing the gap
qB
mT
2 ( not depend on v, r )
qB
mvr
Application : accelerating proton 、 etc. to slam into a solid target to learn it’s structure
Ex. : deuteron q/ m ~ 10 7 , B ~ 2 , R ~ 0.5
need U ~ 10 7 ( volts ) frequency of emf f = qB/ 2m ~ B magnetic field relativity : v m f varying frequency —— Synchrotrons
Cyclotrons Compare with straight line accelerator
Str. :Cyc. :
qUmv 2
2
1
m
RBq
m
qBRmmv
2)(
2
1
2
1 22222
m
RqBU
2
22
22
0
/1 cv
mm
To gain the same v , need
Exp. carrier q , force fL = q v B
q > 0 , v - positive x , fL - positive z
q < 0 , v - opposite x , fL - positive z direction
A’
5. The Hall Effect A conducting strip of width l, thickness d x - current , y - magnetic field z - voltage UAA’
x
yz
I
BA
l
d
fL
fe
for q > 0 , positive charges pile up on side A , negative on A’ produce an electric field Et
fe = qEt opposite to fL slow down qEt = qvB
stop piling q moves along x ( as without B ) the Hall potential difference : UAA’ = Et l = vBl
The Hall Constant
I = q n ( vld )
v = I/qnld
UAA’ = IB/qnd
write : UAA’ = K IB/d
proportional to IB/d ( macroscopic )Hall constant : K = 1/qn ( microscopic )
determined by q 、 n q > 0 , K > 0 UAA’ > 0
q < 0 , K < 0 UAA’ < 0
( A - negative charges , A’ - positive )
Exercises
p.216 / 5-5- 1, 3, 4, 5, 6
§6. Magnetic Force on a Conductor
1. Ampere Force
2. Rectangular Current Loop in a Uniform
Magnetic Field
3. The Principle of a Galvanometer
1. Ampere Force
current carriers magnetic force on conductor
electron : f = - ev B
current : j = - env
force on current element Idl : dF = N (- ev B )
= n dS dl (- ev B )
= dS dl ( j B )
= Idl B
Ampere force :
L
I0
d BlF
I
B
dldS
dl and j in same direction
j and dS in same direction
I = j dS = j dS
2. Rectangular Loop in Magnetic Field
Normal vector n and current I
------ right-hand ruleu① :
d③ :l ② :r ④ :
II
B
n
①
②③
④
l2
l1
)90sin(d o
01
1 l
lIBF
cos1IBl ( up )cos13 IBlF ( down )
2
02 dl
lIBF 2IBl ( ⊙ )
24 IBlF ( )F1 , F3 cancel out
B
n
l1
F2
F4
F2 , F4 produce a net torque : T = F2l1sin = IBl2l1sin = ISBsin
The Magnetic Dipole Moment
Torque on a current carrying rectangular loop :T = ISBsin ( direction : n B )
Definition :Magnetic Dipole Moment of a
current carrying rectangular loop
pm = IS n
then the torque
T = pm B
B
pm
I
T
( Comparison : in an electric field
p = ql , T = p E )
Magnetic Moment of Any Loop
Divided into many small rectangular loops
outline ~ the loop , inner lines cancel out
dT = dpm B = IdS n B
all dT in the same direction
T = dT = IdSnB = InBdS
= IS n B = pm B
Definition : Magnetic Dipole Moment of Any Loop pm = IS n
no matter what shape
( same form as that of a rectangular loop )
n
BI
S
Magnetic Dipole Moment of Any Loop
pm making an angle with B
maximum T for = /2 T = 0 for = 0
equilibrium, stable
lowest energy T = 0 for =
equilibrium, unstable
highest energy
n
BI
3. The Principle of a Galvanometer
n turns : T = nISB
countertorque by springs
T’ = kwhen in balance
= nISB/ k I
( = 0 for I = 0 )
NS
Exercises
p.217 / 5-6- 1, 5, 8
§7. Field of a Current Loop
Circular loop of radius R , current I , on axis
o
R
a PI2/322
20
)(2 aR
IRB
3
20
2for
a
RIBRa
:
ISpRS m2
3m0
2 a
pB
)2
1 withcompare(
30 a
pE
:
pm = IS n is important
• torque exerted by magnetic field• produce magnetic field
B
Exercises
p.219 / 5-6- 11