Electromagnetics in Arabic
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Transcript of Electromagnetics in Arabic
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8/2/2019 Electromagnetics in Arabic
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:- .
- .
-.
- .
. -.
-.
( ) . . . .
()
. ()
. ( ( .
1-1-: . ( ) .
1
-
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(). .
1-1-1-:
1.67 10-27 kg
(+) . 9.11 10-31 kg
C (-) 1.67 10-19 C.
) :- () (
( ( )) :-Point Charge -.C q
) :-Line Charge( - q C L
L / C/m.) :-Surface Charge( - q C
S .C/m2 / s
q C ) :-Volume Charge( - V v
.C/m3 / )1-1( .
( ) ( ).
2
z
y
x
L C/m
s
C/m2
v
C/m3
q1
C
q2
C
q3
CS
L
V
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) :-1-1( :- q1 Cq2Cq3 C L C/m s C/m2
v C/m2.:-2-1-1
)Coloumb Law( )Electric Force) F) (
q1 Cq2 C R12 )2-1(:-
NR4
qq12R2
12
2112 aF
= (1 - 1)
F12 q1 q2 F12 = -F21 121212R rrR == q1q2
12Ra 1r2r
) (m/F)36/(109
0 =
. )2-1(r1r2R12aR12 :-
z2,1y2,1x2,12,1r2,1z2,12,1r2,12,1zyxrzr aaaaaar ++==+=
z2,1y2,12,1x2,12,1zsinrcosr aaa ++=
z2,12,1y2,12,12,1x2,12,12,1cosrsinsinrcossinr aaa ++=
212
212
2121212 )zz()yy()xx(R ++== rr
12z12y12x1212RR/])zz()yy()xx[( aaaa ++=
3
q1
(x1y,
1z,
1)
(r1,
1,
1
) q 2(x
2y,
2z,
2)
(r2
,2
,2 )1r
12R
2r
12F
21F
z
y
x
) :-2-1(F
21 q
1
q2
R 21
.
(r2,
,2z
2)
(r1,
,1z
1)
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)1-1( .
q1 ( )
2212 mR4
q2.
E (Electric Field( E1 )x2, y2, z2(
q1 )x1, y1, z1(:-
m/VR4
q
q 12R12
1
2
121 a
FE
== (2 - 1)
N/CV/m. 'V V )3-1(
)x, y, z(:-
m/VR4
dV)r(R
'V
2
''V aE(r)
= (3 - 1)
'R r-r=RRa /R =.
4
'r
Rz
y
x
r
dV'
V
V'
)r(E
) :-3-1(
.
-
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))4-1 ) :-1-1(q1 = 1 nC )1,0,0(q2 = - 2 nC )0,0,0(q3
= 1 nC -)1,0,0(:-)i( ) )ii . ))iii .
P1 (x, y, z( P2 P3)0,0,1) (2,0,0.(
:-)i(
29x
99
121)36/10(4
)()102()101(
= aF nN18 xa=
29x
99
132)36/10(4
)()101()101(
=
aF nN25.2 xa=
)ii( :-
xx13123121 25.218 aaFFFFF +==+= nN75.15 xa=
)iii( P1
5
x
y
z
-)1,0,0(
)1,0,0(
P3
0 ,0 ,2))
P2
1 ,0 ,0))P1
)z ,y ,x)
q3
1 = nC
q2
2- = nCq1
1 = nC
) :-4-1( )1-1.(
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[ ]
++
++
=
2/3222
zyx9
9
zy)1x(
zy)1x(
)36/10(4
10)z,y,x(
aaaE
[ ] [ ]m/V
zy)1x(zy)1x(
zyx(zyx(2
2/3222)zyx
2/3222
)zyx
+++++++
++++ aaaaaa
P2:-
[ ]22/)(2)22(/)(9)1,0,0( zxzzx aaaaaE +++= m/V64.11 za=
P3:-
[ )11.05.0(9)0,0,2( xxx aaaE += m/V5.5 xa=
))5-1 ) :-2-1( LC/m z
.)P (0, y, 0
:-
Cdz 'dz 'L dE:-
6
x
y
z
(0,0, -z')
(0,0,z')
zd'
Ed
P(0,0 ,y)
) :-5-1(
z.
R
Ed
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m/VR4
dz)0,y,0(d R2
0
'L aE
=
2/12'2
)zy(R =+2/12'2
z'
yr )zy/()zy( += aaa.
:-
m/Vdz
)zy(
)zy(
4)0,y,0( '
2/32'2
z'
y
0
L
+
=
aaE
ay )E (
= Ey ay
2/32'2
'
0
Ly
)zy(
dz
4
y2)0,y,0(E
+
=
= tanyz '
= 2' cos/yddz=+ 232/32'2 cos/y)zy(
2
2/
0
2
02/32'2
'
y/1dcosy
1
)zy(
dz==
+
)0,y,0(:- m/V)y2/()0,y,0(E 0Ly =
ar:-
m/Vr2
)z,,r(E0
Lr
=
r .
:-3-1-1 V (Electric Potential(
7
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. +q ))6-1
P1(r1( )P2(r2 )P1(r1
. )(P )P1(r1 '2
'2 r
. -:
=2
1
12V dLE V (4 - 1)
E. ) (
EddL . dLzyx dzdydx aaadL =++
zr dzrddr aaadL ++= ++= aaadL dsinrrddr r.
) :-6-1( +q .
)6-1(dL = drar m/Vr4q
r20
aE
=
V12:-
8
+q)(P 22 r
)(P'
2'
2 r2r
1r
r
E
P1)r
1)
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Vr
1
r
1
4
qdr
r4
qV
120
2r
1r2
012
=
=
r2 = rr1 ) P r(
Vr4
q)r(V
0= (5 - 1)
r V)r4/(q 0
)7-1(
))5-1 .
'dV:-
R
dV
4
1)r(V
'v
'V0
= (6 - 1) R 'v dV
. ) )
.
9
qV
1 V2 V
3 V4
E
) :-7-1( E
.
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V12 ) )2-1:-)3-1(
r2 r2 r1 < r1. 2L z z = - Lz = L
.m/CL )0,y, 0(
:- )r2/(E 0Lr =
(r = r1 V12 (r = r2:-
++== )dzrddr(r2V zrr0L12 aaaadLE
Vr
rln
2r
dr
2 2
1
0
L2r
1r0
L
=
=
LzL
V )0,y, 0(:-
R
dz
4
1)0,y,0(V
'L
L
L0
=
2'2
'L
L0
L
zy
dz
4+
=
))tanyz ' =
= 2' cos/dydz
=+
cos
yzy
V 2'2
:-
+
=
=
1
1
0
L1
10
L
sin1
sin1ln
4cos
d
4)0,y,0(V
= y
Ltan 11
10
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VLyL
LyLln
4)0,y,0(V
22
22
0
L
+
++
=
)8-1(
V1V2 V1 - V2V2 - V1. .
EdL E dL dL
.E dL dL
.
) :-8-1(.
:-4-1-1 )Voltage Gradient(+ VV V L
E )9-1(
:-
=2
dLE
1
L12 LEVV
EL L
L/VEL (7 - 1)
11
E
V2
V1
V12
V21
V12
E
E
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. dL = dx axx
VEx
)x
VE(
xxxaaE
=
dL= dy ayy
VEy
dL = dz azz
VE z
dL = dx ax + dy ay + dz az
E :-
+
+
++= zyxzzyyxx zV
x
V
x
VEEE aaaaaaE
) :-9-1( VV + V L E.
0 dLL:-
+
+
= zyx zV
y
V
y
VaaaE
)z,y,x(Vzyx zyx ++=aaa (8a - 1)
V=E (8b - 1)
zyx zyxaaa
+
+
)gradient(
:- .
12
x
y
x)2y,
2(
L
Ld
E V
+V V
E
Ld
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:-
+
+
aaa
sinrrr r
,V(r ) :-4-1(:- , ) = 50 /r V (i(
. . V(x,y,z) = 5 x2 y V (ii)
:-
)i( )8a - 1( m/V
r
50V r2 aE ==
)ii( )8a - 1(
m/Vx5yx10V y2
x aaE ==
:-5-1-1 D
))3-1 :-
m/Vr4
q1r2
aE
=
. r
22 m/C)r4/q( )electric flux density) D displacement vector
2r2
m/Cr4
q aD
= (9a - 1)
ED = (9b - 1)
)9a-1( . D:- 'V v
13
zr zrraaa
+
+
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2
'V
r2
'v m/C
R4
dV
= aD (10 - 1)
q ))9a-1
D )10-1.( ( .( q q
:-
=
=0
2
0
r2
r2S
qddsinrr4
qaadSD
:- dVq v
VS
== dSD (11 - 1)
) q ) ))11-1
( ( S D . V . ( )
S(Closed )Gauss Law( )11-1(Surface( )Gauss Surface.(
D
.
14
Dq
V
S
) :-01-1( q S
.D
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))11-1 ) :-5-1(m/CL D E
.
:-
L )11-
1.( D ra z
2rr m/C)r(D aD =
) :-11-1( m/CL.
:-
( ) =
++=
L
L
3S2S1SS
dzdSDdSD
S3 S2 S1
:-
2LrLrL
2 L
0
r m/Cr2DLDLr2LdzrdD
===
=
m/V)r2/(/DE 0L0rr ==
15
x
y
z
r D
S
3
S 1
S 2
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2-1.
E D :-)6-1( 2s m/C
xyz = 0 )12-1.(
:- D x y
z zzD aD = L )12-1(
:-
=
++=
+++ S
s
6S5S4S3S2S1SS
dS)( dSDdSD
) :-12-1( 2
s m/C.
S3S4S5S6 :-
2sz
2s
2z
2z m/C2/DLLDLD ==+
m/V2/E sz =
16
z
y
x
L
D
D
S
1
S
2
m/C 2
s
,5S ,4S ,3S6S
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a ))13-1 ) :-7-1(3v m/C .
.
:- D
r 2rr m/C)r(D aD = D ar0
=
=
=
ddsinrD 22
0 0
r
1S
dSD
=2
0 0
r
0
'2'v dddrsinr
2vrv3
r2 m/C
3
rDr
3
4Dr4
=
=
m/V3
rE vr
=
r > a
=2
0 0
2r
2S
ddsinrDdSD =
ddsinr22
0 0
a
0
v
17
y
x
z
a
S1
S2
v
rr`
v
) :-31-1(
a .
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22v
3
rv3
r2 m/C
r3
aDa
3
4Dr4
=
=
)r > a(
m/Vr3aE 2v
3
r=
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zyx zyxaaa
+
+
)12-1(
D (Divergence ofD( . )6-III(D.
)) :-8-12
zyx m/Cnzyx aaaD ++=
2m.
:- )12-1(:-
zD
yD
xD zyx
v +
+
== D 2m/Cn3111 =++=
:-
nC24dzdydx3Q
2
o
2
o
2
o
== D) )7-1) :-9-1( > a < r .
:- )7-1( a < r< D:-
22v
3
r m/Cr3
aD
=
)6-III( D ) )D rr aD =:-
00)Dr(rr
1r
22v
++
== D 3m/C0=
>> ra.
:-7-1-1 )Poisson's & Laplace's equations( )(V r )(v r
)(rD)(V rv= D== /V DE
=
D)V(
19
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r)(r DD
=
1
=v2
)(V r (13 - 1)
22
2
2
2
22
zyx
+
+
)Laplacian( )6-III(. )13-1(
.:-
0V2 = (14 - 1)
.
)14-1( :-)10-1(a b
V0 0V
V (r, ,z(.
:-
. zV (r, ,z( z r
:-
00
r
V
r
1
r
V0)z,,r(V
2
22 ++
+
==
0rd
Vdr
rd
d
r
1
rd
Vd
r
1
rd
Vd2
2
=
=+
20
b
ra
br
a
0 V
0 V
0
V0
Vo
z
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:-)14-1( V0 V.
:- B)r(LnA)r(V +=
0V)a(V 0)b(V= =B)a(LnAV0 =+B)b(LnA0 +=
)a/b(Ln)b(LnVB 0= )a/b(Ln/VA 0=
V)a/b(Ln
)r/b(LnV)r(V 0=
:-8-1-1 )electric dipole(
. L
r r >> L )15-1( .
)r, , 0(:-
Vr
1
r
1
4
q
),r(V
= +
( ) ( ) ( )( ) 21
222 cosr/Lr2/L1rcosrL2/Lrr +=+= .
21
q
q
y
r
r+
r-
(r,,0)
x
z
L/2
L/2 ) :-51-1( +qq-
L.
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r >> L r )Taylor Series(:-
[ ] += cos)2/L(r...cos)r2/L(1rr
( )
222
cos2/Lr
cosL
4
q),r(V
Vcosr4
qL),r(V
2
= (15 - 1)
E V=E E:-
rr EE aaE += (16 - 1)
= cosr2
qLE 3r= sin
r4qLE 3.
+ qL az:-
CmqLq ze aLm == (17 - 1) )Electric Dipole Moment(
)15-1()16-1(:-
Vr4
),r(V 2re = am (18 a - 1)
( ) m/Vsincos2r4
r3e
+
= aam
E (18 b - 1)
)16-1( me.
22
q
q
V=0 Lm qe =
-
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:-)16-1( Cmqe Lm =.
))Dielectric Materials 9-1-1-: ( (
( ( . ) ( ) )
Cmqe Lm =L )
( .N 3mV :-
2e m/CV
NP
m
(19 - 1)
P )polarization vector( D
V )N(
)17-1(
VV0 d )vacuum( )17a - 1(
:-
23
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m/Vd
Vx
0 aE = (20 a - 1)
)fringing(
m/Vd
V 0x0
00 EaD == (20 b - 1)
)17b-1(.
)bounded charges( ) 1-1
. ) . ( )
. ( ) .
P PDD += 0
PED += 0 (21 a - 1)
d
V0== ED (21 b - 1)
:-
E
P
E
D+== 0 (22 - 1)
:-)17-1( V0 (a( )b(.
-: )22-1(
24
d
1 1
E
(a) (b)
V0
(V) V0 (V)
E 0
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+==
D
P100r (23 - 1)
r )1-1(r.
r):-)1-1
r 1
1.0006 ) )
2.1 3
4 6 81
P :-
DEEP )1()1()( r0r0 === (24 - 1) D P
) ( .
))Boundary Conditions 10-1-1-: )18-1(
E1D1 E2D2
: E1tE2tDt1 D2nD1nE2nE1n D2t .
-Dn:- ) (h 2,1S
)18-1( . :-
25
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dSDdSD
++=
3S2S1SS
dhdV vhS
v
V
==
dS (25 - 1)
h ( (3S
dhvh
2
svh
0hm/CdhLim
= -: )25-1( SDSDSD s22n11n
1S2S ) S ( :-
2s2n1n m/CDD = (26 a - 1)
Dn
2n1n DD = (26 b - 1)
26
L
h
1 h
11 D,E
11 ttD,E
11 nnD,E
2tE
1tE
2nD
1nD
na
ta
22 D,E E,D 22 nn
22tt D,E
S
S3
S1 S
2
2
1
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:-)18-1( ED 12.
:-
2s2n21n1 m/CEE = (27 a - 1)
2n21n1 EE = (27 b - 1)
.
- Et:- )18-1(
1-4-3-2-1 =1
2
2
1
dLEdLE
dLE
0
1
4
4
3
3
2
2
1
=
+++= dLEdLE
Et h
3
2
1
4
:-0LELE 1t2t
L :-
2t1t EE = (28 - 1)
) .(
:-
2
2t
1
1t DD
=
(29 - 1)
27
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Dn
En
0
D0E ==
s=1/ n C/m2
)27b - 1()28-1( 21 .
)26a - 1(s .
. sb :-
sb2n1n PPP = (30 a - 1)
1nP2nP ( )0P 2n =:-
sb1n PP = (30 b - 1)
m/F0))18-1 ) :-11-1(
2m/nC1
.
):-19-1(.
:-
0=D0=E )( . 1t2t E0E 1t2t== D0D ==
s2n1n DD = 0D 2n =
21n m/nC1
D
m/V36=D
E0
1n1n =
))19-1 .=
.
28
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10-1-1-:
)Capacitor( )
Stray Capacitors(.- +q
q V C :-
=dLE
V
v dV
V
qC (30 - 1)
F (Farad(
))parallel plate )20-1( ) :-12-1(0 d m A m2
VVV0 m/F0r . .
. . . ()
:- :-
m/Vd/VE 0z =
2
0r0z m/Cd/VD =
:-EP 0r )1( =
29
d
0V
V0
V))
y
z
E
m A 2
) :-02-1( P
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20rz m/Cd/V)1(P = :-
20r0s m/Cd/V =
2 0r0s m/Cd/V =
. :-2
00rsb m/Cd/V)1( =
2
00rsb m/Cd/V)1( =
. C :-
Fd
A
dV
AV
V
A
V
qC 0r
0
0r0
0
s
0
=
=
==
A d
.
)21-1( ) :-13-1(
a b
-
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aL)(Lr)DD( 2S1S2r1r +=+
2
2S1S2r1r m/C)(raDD +=+
1r11r ED =2r22r ED = )E(EE r2r1r ==) 120==
( :-
)(r
a)(E 2S1S21r +=+
)(
)(r
aE 2S1S
21
r +
+
=
) :-21-1( )a( )b( .
:-
)a/b(Ln)(
)(aV
21
2S1S
b
a
0 ++
== dLE
)(
)a/b(Ln)(
)(
)a/b(Ln)(aV
212L1L
212S1S0 +
+=+
+=
31
a
r
b
s2
s1
1
2
E2r
, D2r
E1r
, D1r
a
b 2
1
(a)(b)
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m/F)a/b(Ln
)(
V
)(C 21
0
2L1L +=+
=
m/F)a/b(Ln . 1
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r = b:-2
1S m/C55.0 =2
2S m/C11.0 =
m/pF8.51C =
-: - ) (
V . :-
Vqd
dWV e= (32 - 1)
edW dq
qd
Wd
C
qV e== qdq
C
1Wd e =
:-
JqV2
1CV
2
1
C2
qW 2
2
e === (33 a - 1)
JdV
2
1W
V
e DE = (33 b - 1) )33-1(
. m/F S
d 3mSdV = :-
32e
e m/JE21w
VW == (34 a - 1)
3e m/J2
1w DE = (34 b - 1)
a ))22-1 :-)14-1( q C:-)i(
33
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r0
:-2
2r2
r m/Cr4
qDqr4D
==
m/Vr4
qE
20
r
r < aDE=
.
)ii( :-
=r
V dLE
> ra :-
Vr4
qdr
r4
qV
0
r
'
2'0
=
=
> r0 :-
34
ar qC
Er
Dr
0
:-)22-1(
C q .
-
8/2/2019 Electromagnetics in Arabic
35/88
Va4
qV
0
r
a
a
=
+=
dLE
.
)iii( :-Fa4V/qC 0==
:-
Ja8
q
)a4(
qa4
2
1CV
2
1qV
2
1W
0
2
20
2
02
=
==
=
:-2-1
I)i(C/s A .
:-
Atd
qdi = (35 - 1)
. .
.
. .( )
.
) ) . .
.
35
-
8/2/2019 Electromagnetics in Arabic
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) ) .
.
.
.
.x1x2 x
) ( E x2 x1
t tx
(
. ( )Drift Velocity)
vd
Ev =d
(37 - 1)
)Mobility( )sV/m( 2 .
3v m/C s/mvd 2mA
Avi dv= (38 a - 1)
:-dv vA/iJ == (38 b - 1)
J)J( A vd )Ohm's Law( )V =
IR( V = ELI = JAR = L/( A( L ) (
36
-
8/2/2019 Electromagnetics in Arabic
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2m/AEJ = (39 - 1) )Conductivity(.
)1)m ))39-1
2m/AJ( ) E
) .(1)m ) )Resistivity(m1 = .
. ( )
. )2-1( . C20
)1)m ) :-2-1( .
1)m(
10-17
10-15
10-12 10-4 10-3 0.2
2 4
103
3 104
106 5 106
3.5 107 4.1 107 5.7 107
37
-
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G R (Conductance( :-
==L
)A(/dLdRR (39 a - 1)
==A
1)(L/dAdGG (39 b - 1)
)23-1( ) :-15-1(ba L
.
:--: dR
=ddrr
dzdR
122b
a
)(L
)ab(drr
L
2G
=
=
=)ab(
LR 22
) :-23-1( )a( )b( )c(.
-: dR
38
a
br
z
L I
V0
a
br
z
I
V0
a
br
z
I
V0
(c) (b) (a)
-
8/2/2019 Electromagnetics in Arabic
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=
=
= L2)a/b(Ln
Rr
rd
L2
1R
dzrd
drdR
b
a
-: dR
)a/b(Ln2
L
r
dr
2
LG
dzdr
drdR
b
a
=
=
=
=
)a/b(LnL
2R
)37-1()38b-1()39-1(
EvEJ === vdv1
v )m(= (40 a - 1)
sV/m/ 2v= (40 b -1)
.))40a-1 ))40b-1
)DC .
. . )
( .))38a - 1
S)0I( = :-
0S
S
=
dJ (41 a - 1)
0= J (41 b - 1)
3-1-:
.
39
-
8/2/2019 Electromagnetics in Arabic
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( )
.
1-3-1-:
( ) .
. .
:-
- )Line Current( :- .A I - )Line Current(:- I A
( )L .=Km/AL/IK
- )Surface Current(:- I A ) (S
2m/A)S/I(J =.
)24-1(.
) :-24-1( I AKA/m J A/m2.
40
L
x
z
y
I
I
I
S m2
J
K
-
8/2/2019 Electromagnetics in Arabic
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:-2-3-1 - 2' mS
2m/AJ
)25-1( -Biot-SavartLaw B Magnetic Flux density . 'dV 'dS'dL )z,y,x( )),,r''' '''
) P (x, y, z )),,r dB .
dBJ :-
22
R''
m/Wb
R4
dV)(
=
arJdB (42 - 1)
H/m|||| '
'
Rrr
rr
R
Ra
= R.
)42-1( dBJ .
J aR dB.-: P B
41
x
z (z,y,x)
(,r ,)P
r
R
'r
(z,'y,'x')
(,'r ,'')
J
S'
I
Vd'?B
y
I
) :-52-1( A IB
.P
-
8/2/2019 Electromagnetics in Arabic
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='V
'2
R'
dVR
)(
4
arJB(r) (43 - 1)
)26-1( ) :16-1(- z I A .B
))0,,r .
:- B z
)43-1( r
:-
='L
2R
R
I
4
adLB(r)
'
z'dz adL' z=
'z zr aaR =
2'2 zr +=|R|RR/a =R.
+
=+
=0
2/32'2
'
2/32'2
'
)zr(dz
2rI
)zr(dz
4rI)r(B
= tanrz '
=+
3
32/32'2
cos
r)zr(
=
2'
cos
drdz z = 00=
=z2
=
42
(,r0,)
R
r
x
y
z
zadL'' dz=(0,0,z')
za'z
I
) :-62-1( A I.
-
8/2/2019 Electromagnetics in Arabic
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22/
02
m/Wbr2
Idcos
r2
rI)r(B
=
=
I )27-1( ) :-17-1(A .a x y
.))0,0,z
:-
z )B )43-1( .(
:-
='L
2R
'
R
I
4)z,0,0(
adLB
'da = adLrz az aaR 22= az +=RRR/a =R.
) :-27-1( I A x y.
:-
43
z
R
'raa
x
y
''
da
'
= adL
(0,0,z)
zz a
I
a
`
'd
-
8/2/2019 Electromagnetics in Arabic
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=
+
+
=
+
=2
0
'2/322
zr2
0'2/322
rz''
d)az(
)az(
4
aI
)az(
)az(d
4
aI)z,0,0(
aaaaaB
Br) ar ' B ) Br
:-
22/322
2
z m/Wb)az(2
aI)z,0,0(B
+
=
B 2
z m/Wba2
I
)0,0,0(B
=
3-3-1-:
. ( )I1 A
) I2 A( dL
:-
NI 211 BdLFd = (44 - 1)
dL1 B2
. :-
=2L 1L
2R2121
R)(
4II adLdLF (45 - 1)
- B2 R dL1dL2.
)28-1(
44
-
8/2/2019 Electromagnetics in Arabic
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L2L1 L2L1 :-
2
R21
2L2L
21
R
)(
4
II adLdLF
= (46 - 1)
) :-28-1( I1 I2.
L1 ))29-1 ) :-18-1( L2 I A 2m/WbB .
:-)i( 2z1 m/WbB aB =.)ii( . xy
.
) :-29-1( L1 L2 I A .B
45
x
y
z
I
L1
ab
cd
L2
1B
2B
I2
I1
L1
L2
2B RLd
2
Ld1
-
8/2/2019 Electromagnetics in Arabic
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:-)i( z1B aB1 = :-
NBLI x12ab1 aF NBLI= y11bc1 aF =NBLI x12cd1 aF NBLI= y11da1 aF =
.
)ii( y2B aB = :-N0ab2 =FNBLI z21bc2 aF =N0cd2 =FNBLI z21da2 aF +=
bcda x
NmBLIL x221 aT zam = 21LIL=
NmBmT = .
3-4-1-: )42-1(
'dL :-
22
R m/WbR
I adLdB
' =
2
R
R
I adL'
)A / m( )Magnetic Field Intensity(
dH H B :-
HB = (47 a - 1)
H :-
='V
'2
R'
dVR
)(
4
1 arJH (47 b - 1)
,)r , 0( I A z :-)161(
r2
IH
=
46
-
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H= adL dr
Id
2
Idr
r2
I2
0L
=
=
=
=
dLH
:-
dSJdLH == SL
I (48 - 1)
)J(I )Amper's Law( H .
L.
))30-1 ) :-19-1( aIA z .H
> B r0.
:- H z
( ) a )48-1( ar0 i :-
m/Aa2
rIHr
a
Ir2H
2i2
i2i =
=
B :-
47
y
z
x
I
rir
0
) :-03-1(a
A I
.
-
8/2/2019 Electromagnetics in Arabic
48/88
22i m/Wb)a2/(rIB =
r0r > a :-
Ir2H 0 = m/A)r2/(IH 0= B :-
20 m/Wb)r2/(IB =
xy )31-1( )20-1(:- xy .
m/AKx0
aK= H .
)31-1(:- yx z=0 m/AK x0 aK=.
:- H x y
)31-1( yL m :-
LK0
1
4
4
3
3
2
2
1L
=
+++= dLHdLH
az |H1| = |H2|
48
x
y
z
K0 A/m
+
-
2 H
1 H
K0
L
-
8/2/2019 Electromagnetics in Arabic
49/88
LKdHdH 0
2/L
2/L
yyy2y
2/L
2/L
yyy1y =+
aaaa
m/A2/KHH 02y1y ==
202y1y m/Wb2/KBB ==
5-3-1:- )The Curl & Stocks Theory( JH )48-1(
L S L .LL S
))48-1 S
:-SJdLH
L
H
dLH
J
=
S
Lim L
0S0L
(49 - 1)
J ))49-1 . )32-1(
AI)m/A( 2J ))49-1
. .
49
S
L
LJ
J
L
) :-23-1(
J L
.
-
8/2/2019 Electromagnetics in Arabic
50/88
-: )49-1(
dSHdSJdLH ==
SSL (50 - 1) () H.
.
H B .
0mS
== dSB (51 a - 1)
0= B (51 b - 1)
m ) ( . .
.
:-6-3-1 )Magnetic Vector Potential(
- .
A
B :-
='V
'dVR4
)(rJ(r)A
'
(52 a - 1)
(r)A(r)B = (52 b - 1)
50
-
8/2/2019 Electromagnetics in Arabic
51/88
A J )52a - 1( )43-1(.
()52a - 1( ))43-1 ))52-152b - 1(
R
Vd
4V
=
)r(JB
r'r)xyz 'x'y'z(
=
'V
'dVR4
)(rJB
'
(53 - 1)
III)21h-III( )R/( )(rJ ' :-
( ) J)(rJ)(rJ ''
+=
R
1
R
1
R
( 0= )(rJ 'r r '( ) 2R R/R/1 a= )53-1( :-
=='V
'2
R dVR4
)(rJa
AB '
==
'V
'
2
R
dVR4
a)(rJ
AB
'
(54 - 1)
.))43-1
))33-1 ) :-21-1( L I A)
(
51
-
8/2/2019 Electromagnetics in Arabic
52/88
z .( )A),,r(P r>> L.
:-
A )52a-1( 'dV)(rJ 'z
'dzII adL' =
R
dz
4
IA
'2/L
2/L
z
=
+= cosrz2zrR '2'2 r >> L RR ~ r
Az
m/Wbr4
LIAz
=
= aaA sinAcosA zrz
)sincos(r4LI
r
= aaA
III )19c-III(AB =2
2m/Wbsin
r4
LIAr
r
1
=
= aaB
) ))34-1 :-)22-1(I A S m2)
xy .A
52
y
z
x
R
r
P ( r,,)
2/L
2/L
zaz
'
'dL
I
) :-33-1(
A I.
-
8/2/2019 Electromagnetics in Arabic
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B ),,r(P r >> D D .( )
:- A )52a - 1(
'dLJ IdV ' =
R
I
4 'L
'dLA
=
. III-: )22e-III(
=S
'n dSR
1
4
IaA
na)za(
z'y'x'' zyxaaa
=++)z,y,x( '''
2R
3'
RRR
1 aR==
. r >> DR ~ r
aR~ ar A :-
=
= aaaA sinr4
SI
r4
SI2rz2
53
y
z
x
R
r
P (r,,)
'dL
S m 2
D
I
) :-43-1(
yx I
) (.
-
8/2/2019 Electromagnetics in Arabic
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IS ) (2
m AmISm zm (= SI am A )=:-
rm2r4 amA
=
B AB =
= aaB )rA(rr
1)sinA(
sinr
1r
[ ] 2r3 m/Wbsincos2
r4
SI+
= aaB
N N .
JH HBA= == :-
H)BA) == ((
)
( JAA) += 2( (55 - 1)
A 0= J0= A JA =2 (56 - 1)
AJ.
)Magnetic Materials( 7-3-1-: () .
)Spinning( .
m2 S I A
2m AmI Sm =) ( .
54
-
8/2/2019 Electromagnetics in Arabic
55/88
.
)N( )S( -qmqm)
L Wb ) qmL .
)21-1( Im) ( L
ImL
LqLISI mm (56 -1)
)35-1( ) ( Im .
.
.
.
m/H104 70=
H B :-2
0 m/WbHB = (57 - 1)
V N
2e AmN m m/AV/N e m
H )MagnetizationVector(
)Magnetic Polarization) M
m/AV/N e = mM (58 - 1)
55
-
8/2/2019 Electromagnetics in Arabic
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m/AMH + B
:-
HMHB += )(0 (59 a - 1) :-
m/H)/1(00r HM+== (59 b - 1)
) :-35-1( )a( I A )b(
S (c( )d( )e(.
56
(b)(a)
=S
I
Im
(e)
B
1
2
-qm
+qm
(d)
B
N
S
(c)
B
B
-
8/2/2019 Electromagnetics in Arabic
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r
. )36-1(
( .(
.
) )
.( )
00
S
== dSBB (60 - 1)
)Ferromagnetic and Ferite( 1r >> 16
)m(10
16
)m(10
.
))boundary conditions 8-3-1-: )37-1(
H1B1
57
N S
N S
N S
N S
N S
N S
N S
N S
N S
N S
N S
N S
(a)
(b)
(c)
H
H
HH
HH
) :-63-1(
)a(
)b()c(.
-
8/2/2019 Electromagnetics in Arabic
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H2B2 .
. Bn1Bn2
0
S
=
dSB
Ht1Ht2 . )37-1(.
2,1S -: -Bn
h
( ) 0
3S2S1SS
=
++=
dSBdSB
0h0S3 0S 2,1
2n1n BB = (61 a - 1)
)28-1(
2n21n1 HH = (61 b - 1)
:-)37-1( HB 12.
- Ht:- 4-3-2-1 )37-1(
58
L
h
1 h
11 B,H
11 ttB,H
11 nnB,H
2tH
1tH
2nB
1nB
na
ta
22B,H
B,H22 nn
22tt B,H
S
S2
S3 S
1
2
1
2
-
8/2/2019 Electromagnetics in Arabic
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( ) ( ) =
+++=
S
1
4
4
3
3
2
2
1L
dSJdLHdLH
h
K )
-: ( LKLHLH 1t2t
L ( ) :-KHH 1t2t = (62 a - 1)
-: K/B/B 11t22t = (62 b - 1)
. K) (
-: )62a - 1( KHa =n (63 - 1)
.
9-3-1-: )Inductor(
m .)Inductance(L
:-
HI/L mL= (64 - 1) mL I.
)44-1(
:-BLIF =
JVHBBLHBLILF 32 ===
V .-: )33-1(
59
-
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==V
2m dV2
1IL
2
1W HB (65 a - 1)
-: Wm
JdV2IL2
1W
V
22m
== H (65 b - 1)
-: )65a - 1(
FdVI
1L
V2
HB = (66 - 1) V . )65-1(
32
m m/J|21
21w |HHB == (67 - 1)
)64-1()66-1( )38-1( B
I1 .B1B2 B4B3
. B1B2 L1
B3B4 L12 L21 .
:-)38-1( I1 I2B.
)39-1( ) :-23-1(am/H0 I b
m/H0 I- .
60
I2
I1
I2
B1
B2
B3
B4
-
8/2/2019 Electromagnetics in Arabic
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m/H0
.
:-)19-1( ab.
:- .
z
a
. ar0 :-
2
2
1
SL
1a
rIHr2 == dSJdLH
m/Aa2
rIH
21 =
22
01 m/Wb
a2
rIB
=
:-
dzdrdr2
1W
1
0
a
0
2
0
m =
HB
m/J16
I|
4
r
a4
Idzddr
a4
rI
2
20
a
0
4
4
20
42
321
0
a
0
2
0
0
=
=
=
61
b
a
ba
I
I
I
0
0
0
I
11 ,HB
22 H,BI
-
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m/H8
L16
IWIL
2
1 0i
20
m2
i
=
==
bra > a(.
:-m/AL/IN
m/AL/INK = .)17-1(
L/dzINKdz =
:-2
2/322
2
z m/Wb)az(L2
dzINadB
+
=
:-2/L
2/L222
22/L
2/L2/322
2
z |az
z
a
L
L2
INa
)az(L2
dzNIaB
+
=
+
=
62
-
8/2/2019 Electromagnetics in Arabic
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2
22z m/Wb
a4L
INB
+
=
) :-40-1()a( L a N
I (b( L/INK =.
L >> aLa4L 22 +
2
z m/WbL/INB =
:-
L
02222/322
z2L
0
z |az
z
a
L
L2
IN
)az(L2
dINaB
+
=+
= 2
22zm/Wb
L2
IN~
aL2
INB
+
=
)64-1(
2mL a)L/IN( = Wb
63
(a)
(b)
snrut - N
a
z
I I
(0,0,z)
B x
zd
L
y
L/IN=K
-
8/2/2019 Electromagnetics in Arabic
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N 22
mt a)L/IN( = Wb-:
Ha)L/N(I/L 22
mt==
N )Toroidal Coil())41-1 ) :-25-1( a r0
0r .
:-)41-1( N m/H0r .
:- )41
-1(0r2L = :-
Hr2
aNa
r2
Na
L
NL
0
222
0
22
2 =
=
=
B - H10-3-1-: B H
( ) HB = . BH 0= 0 .
BH .
L/INH 0r2L= .
64
a
B
r0
I
I
0 r
N
-
8/2/2019 Electromagnetics in Arabic
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)42-1( BH B .
. I = 0H =0 B
= 0 H H HB
HB .
H B H
. HHmax) H(maxBB =
maxHH > B 0) ( )43-1(B - H (B -H Curve( )Hysterics Loop(. H
Hmax BH 4-3-2-1 5-4 .H B
.)Br( )Br(Residual
H )Coersive)-Hc .H-HcB
. BH 7-6
.maxBB -HmaxH 5- = H-Hmax
BH 8-7 10-9-8 .10-9-8-7-6-5-4
. B - H
.))Hystresis Loss
65
r0
B
I
R
V0
IN
-
8/2/2019 Electromagnetics in Arabic
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) :-42-1( BH.
) :-43-1(B - H.
BrHc . Hc
.Br Hc
.
B-H .
66
Bmax
-Bxam
-Br
Br
H c
hr
-Hc
hr
-Hxam
hr
Hxam
hr
`
`
H
h
r
B
h
r
H-B
-
8/2/2019 Electromagnetics in Arabic
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. 0 B - H .85 96
+ 10-9- . B- H 8-7-6-5-4'44 '77 .-3-2-14 0
.
))Magnetic Circuits 11-3-1-: Vb)(
R1 R , R2 ,) ( )44a - 1( .)
... ( .
Vb R I .)44b - 1( N I
)WbBA(m = .N I )Reluctance(
m )44c - 1( -:.
VRIVb AR/VI= b=( )
==)A/(LI/VR
b
)44c - 1( :-AIN m = (67 a - 1)
Wb/INm = (67 b - 1)
( ) 1m H)A/(L)AH/(HL/IN=== (67 c - 1)
(I
m
bVIN
R ( .
.
67
N I
m
r0
B
I
N
A
R
I
Vb
(c) (b) (a)
-
8/2/2019 Electromagnetics in Arabic
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:-)44-1()a( )b( N)c( .
10cm ))54-1 ) :-26-1( 10cm2 2mm
m/H1000 0 100 10A
mB ) .( .
:- c g
)45b - 1(
1544
32
c H1098.410101041000 10210102AL
= ==
1547
3
g H1092.151010104
102
=
=
)2mm( 62.63mm . )( )
-: ).
mWb48.010100IN
cgm =+
=
=
gB2m
g m/Wb48.0AB =
=
68
-
8/2/2019 Electromagnetics in Arabic
69/88
) :-45-1()a( )b( .
)26-1() :-27-1( 2m/Wbm10
.
:-
c
g m Wb10101010 533m ==
A21.0N/I/NI mm ===
:-4-1
Eq-: q
Nq EF =
m 2s/ma
:-
2
2
td
dm
dtmmq
xdvaEF ==== (68 - 1)
69
10mc
B01A
001
01
mc 2
2mm
g
HM 95.1= 1-
0001nruT-A
-
m
c
HM 894.0= 1-
(b) (a)
-
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a m/s2 v m/s x x) (m.
)46-1( )68-1( .
)Oscilloscope( () )Cathode(
.))Anode )68-1( e
aE me =
x1x2 :-
12
2x
1x
x
2x
1x
VeedxmW === dxEaa
12x2x
1x
Vedxdt
dmW == av
dt
dxv 12=
21
22
2v
1v
Ve)vv(m2
1dm = vv
V0 :-
S/mV109.5m
Ve2v 0
50 ==
dL I ( ):-
BJBdLF == dVId
70
xFqm0
E
) :-64-1( qm E.
-
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:-vJ v=
:-BvdqBvF == dVd v
:-BvF = q (69 - 1)
)69-1( m kg :-
dt
dmq
vaBvF === (70 - 1)
a v )47-1( B.
x0V av =
t = 0 2z0 m/WbB aB = ( ))70-1
q Cm kg( . )70-1( :-
=
zzyy
xx
o
zyx
zyx
vv
v
dt
d
q
m
B00vvv
aa
aaaa
(71 - 1)
71
qx
z
y
R
F
) :-74-1(q m
0 = t.
-
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(m/)dtdv v z0B(B q aB =(
:-
dt
dv
q
mvB x
y0 = (72 a - 1)
dt
dv
q
mvB
yx0 = (72 b - 1)
dt
dv
q
m0 z= (72 c - 1)
-: )72c - 1( s/mvv z0z = (73 - 1)
z0v za za . )
72a - 1()72b - 1(vxvy
dt
dv
q
mv
m
qBB
dt
dvB xx
00
y0
=
0vdt
vd
x
2
2
x2
=+ (73 a - 1)
0vdt
vdy
22
y2
=+ (73 b - 1)
m
Bq 0m2Bq
f 0
= )
.(
x) y( :-tsinBtcosAvx += (74 a -1)
y )72a - 1(tcosBtsinAv y = (74 b - 1)
AB 0x vv 0v= y =
0VA = xy :-
72
-
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s/m)tsintcos(v yx0xy aav += (75 -1)
|| xyv 0v m)qB/(mv/vR 000 == .
vBqF =
Bvq)R/(vmF 2 )qB/(mvR == 00= . q Cm kg
z0B aB B = x0v av m)qB/(mvR = 00=
Hz)m2/(Bq/vf 00 == . s/mvv xz0x0 aav +=
)48-1(. .
.
) )
.
73
z
R
x
y
za0BB =
: R
xa0v (a)
R
x
yza0BB =
:
zxaa z00 vv +
z
(b)
-
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) :-48-1( 2
z0 m/WbB aB =)a( 2
x0 m/Wbv av =)b(zz0x0 vv aav +=.
5-1-: +q-q
2h )49-1(. z = 0
. )49-
0z)1 +q .
z =h )
74
z
h
h
y
q
q
xV=0
-V3
-V2
-V1
V3
V2
V1
V3
V . m/H0.
a 30-1-:x y xy
z )0,0,h( ba > bah >>.
:-31-1 )59-1( 100 2cm5m/H1000 0=
mm5.2 .I 2m/Wb5.0. .
) :-59-1( 100 .
85
I
2.5mm
51
mc
01mc 01mc
001
5mc 2
-
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s/m10 32-1-: x7
0 av = V100 )60-1(.
cm5cm5 cm1 z cm60x =.
) :-60-1( x0v a .
33-1-: 2y m/mWb1B = z cm60x = )61-1(.
) :-611( s/m10 x7
0 av =
2y m/Wbm1 aB =.
86
55mc5mc
z
x1
mc
z1
0V
001V
01 7s/m
0=x 5=xmc
mc 01=x
z
x1
mc
z1
01 7s/m
5mcy
mc 06=x
mc 0=x 2mWb/m1 yaB =
-
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h > a
q
a
x
y
:34-1- )62-1( 1 2)( 12 > VV0
EV )
.
) :-62-1( V0.VV0
m/CL 35-1-: h EV
.
:-36-1 )63-1( +q E
x y.
87
2
1 V
0V
0V
-
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) :-62-1( q.