electromagnetic fields and waves hw1 solution - iskander
TRANSCRIPT
t.2
CHAPTER 1. VECTOR ANALYSIS AND MAXWELL'S EQUATIONS IN INTEGRAL FORM
and OP.OQ = loPlloQlcos?
.'. cos9 = cosdcosc[, + cosBcospr + cosTcosTr
(a) B=QP
oP = QP+OQ
.'.8 = QP = OP-OQ| ^ ^ \ t^ \= [-/a] + za")-\zax +41, +Jaz/
= -2^,- 3a, -a.
(b) Assume the smaller angle between A and B is 9. The magnirude of projection of B on
is lBlcos0.
(c)
... A
'h, ^ A'B.'. |II|COSU = --:--- =
tAlt'^l
-5= -- =414
-1.336
B = lAllBlcoso
(a, +za. -:a.X-za, -:a" -a.)
-
.,!I'+2' -t(-3)rt.(-2) +2.(-3) + (-3)(-1)
-
114
-t.336
cosg=ry=
.'. 0 = 110.9"
"lt-zl' +(-3)'z+(-1)2
(d)
la- a.. a, I
| ' ' 'lAxB = lt 2 3llr
l-2 -3 -ll= (-2 -9)a,+(6+ 1)a, + (-3 + 4)a,
= -1la" +7ar+a,
lA x Bl = Jl l' +7\ l' = 13.017
.'. unit vector = ,A t B,
= -0.841a + 0.535a + 0.0765alAxBl r )
1.3 Atx= l,y=).,7={
.4.=a *4a +12ar_lz
unit vectorAIAIl^-l
=
a +4a +l2ar,yzr._.------i
"ll" +4'+12'0.0788a +03152a +0.9457arlz
L4 Atx=2,y=3A = 3a +2a +3aryz
B=4a +4a
(a)
(b)
A. B = (3x 4) + (2x 4)+ (3 x0) = 20
^ ABCOSU =:-:---: =
lAllBl= 0.7538
1.5
.'. I = 41.08"
(c) The projection of B along the direction of A is l8lcos0
lBlcosg = ^[4' + 4t .0.7538 = 4.264
If A, B, and C are perpendicular to each other, then
A.B=0 B.C=O A.C=0
CHAPTERI.vEcToRANALYSISANDMAXWELL'SEQUATIoNSININTEGRALFORM
1.6 (a)
A'C =
+
A'B =
B.C
BxC
(su, * za, + :a.)' (r a "
+ cra, + ^ ")
15+29+3 = 0
cr= -9
(sa,+zrr+:a.)'(4., * Zar+ B,a,)
58,+418,=O
(4u, * 2rr+ B,a,)'(r., - 9a, + a.)
34-18*8,=Q
+ B, = l4'5
B' = -25'5
lu' u' u'l
= l' r 'llo 2 6l
= (6 - 6)a, + (-12)a,
= -l2ar+ 4a,
+4a
t.'7
unit vector = ffi =-ffi = -g'95a'+ 0'3 16a'
(b) Area = lBx Cl = "J12' + 42 = 12'65
(a) If the two vectors are parallel, then A x B = 0'
CHAPTER 1. VECTOR ANALYSIS AND MAXWELL'S EQUATIONS IN INTEGRAL FORM
(b) If A and B are perpendicular to each other, then A 'B = 0.
A.B = t1 x (-1)l + (b x3)+ [c x (-8)] = Q
.'. 3b-8c=l or
l.l2 (a) A = x2 yN, + y2 za, + x2 znz
.'. A
:.A
, l+8cJ
x = pcosQ
y - psinf
.'. A, = p3 cos2 @sin p
A, = p2zsinz P
A, = p'zcos'q
Ao = A*cos@ + A sin@ - p'cos3 QsinQ + p2zsinj Q
AQ = -A,sin@ + A, cos@ - -p3 sint Qcos2 Q + pzzsinz QcosQ
A,- P2zcos'Q
Aour* Arar* A,a,
(p'"or'@sin@ + p2zsin3 O)"0+(o' sin'@cos2 Q + p2zsinz $cosQ)ao+ p'zcos' pa,
(b)x = rsin0cos@
y - rsin0sin@
z = rcosO
.'. A" = 13 sin3 g cos' P sin @
A, = 13 sin2 9cosOsin2 @
A, = 13 sin2 gcosgcos'@
A sinOcos@+ Arsin0sinP + A cos0
13 sin2 g(sin2 9cos3 Psinp + sinOcosgsin3 p + cos2 gcos'p)
1.13
1 1Al.l1
a0
ae
Oe
B=-a +3a^+2aru9
-ar
a^
a.I
=-& t2a^-32fvo
+5a^-a.rdA
AT= 0T-0A BT= 91-33
.'. AT=3a +5a +5a - bu *a )=3a +3a +4ar I z \ y zl r ) z
BT=3a +5a + Sa -(a +a )= 2a +4a +5ax y i \ r yl r t z
fl1
Oga0
= 13a
L = 2a', + a', -3a1,
a'^ =
A,, =
^;=.'. A - 2ar-a,-3a,
la. aa a"l
n*n=l-r ; -;l
['3zl
l0 CHAPTER 1. VECTOR ANALYSIS AND MAXWELL'S EQUATIONS IN INTEGRAL FORM
Unit vector:
AT 3a-+3a,.+4a-a - = :--- = --# = 0'5 l45a +'0.5 l45a -t- 0.686a-Ar lATl ^!3,
+32 +4, ' v z
BT 2a-+4a..+5a-A =----+=0.298a +0.596a +0.745a-Br lBTl ^12, + 42 + 5' x r z
abn, = T;; ry'ff'an_toooldLl ? t= ;T;rr-' *^'(o'st+su'
+0'5145a' +0'686a')
36tt= 0.409 x 10ea, + 0.409 x 10ea, + 0.545 x l0ea.
O,Eu" = T;;m'^,,= i
I : .(o.zesu,+0.596ar+0.745a,)
+tt;.-xl0-'x45= o.otl3!^10ea + o.rlgzxl0ea +0.149x10ea-
.'. E,o*t= En, * E"t = 0'4; x 10e a, + 0'52; 10ea, + o'ega * ton ^,
(t.o x to-'n)'=2.304x 10-8N1.15 lFl=
1.16
4o * -J-x lo-e x (t o-'o;'36n \
AP = 0P - 0A = (2.5 - l)a, * 2a, = 1.5a, + 2a,
BP = 0P - 0B = (2.5 - 4)a, + 2a, = -1.5a, + 2a,