Bài giảng Electromagnetic Fields – Prob - Chapter 1 - Trần Quang Việt
Electromagnetic Fields – Prob – ch_1
D1.2. Give three vectors:
A = 3a1 + 2a2 + a3;B = a1 + a2 − a3
ꢀꢁ ꢁ
C = a1 + 2a2 + 3a3
ꢁ
ꢁ
ꢀꢁ ꢀꢁ ꢀꢁ
( a ) A + B − 4C
Find the following:
(b) Unit vector along :
A + 2B − C
( c ) A.C;( d ) B×C; ( e )A.( B×C )
Ans: (a) 13; (b)( 2a1 + a2 − 2a3 )/ 3; (c ) 10;( d ) 5a1 − 4a2 + a3
(e) 8
Trần Quang Việt – BMCS – Khoa Điện – ĐHBK Tp.HCM
Electromagnetic Fields – Prob – ch_1
D1.3.
Three vectors A, B and C given by:
ꢀꢁ ꢁ ꢁ ꢀꢁ ꢁ ꢀꢁ ꢁ
A = a1 + 2a2 + 2a3;B = 2a1 + a2 − 2a3;C = a1 − a2 + a3
ꢁ
ꢁ
ꢁ
ꢁ
ꢁ
Find the following: ( a) A×( B×C ); (b) B×(C × A) and
( c) C×( A× B )
ans : (a) 2a1 + a2 − 2a3;(b ) a1 + 2a2 + 2a3;
ꢁ
( c ) -3a1 − 3a2
ꢁ
Trần Quang Việt – BMCS – Khoa Điện – ĐHBK Tp.HCM
1
Electromagnetic Fields – Prob – ch_1
D1.4. Three points P1, P2 and P3 are given by (1, -2,2), (3,1,0), and
(5,2,-2) respectively. Obtain the following: (a) the vector
drawn from P1 to P2; (b) the straight-line distance from P2 to
P3; and (c) the unit vector along the line from P1 to P3
ans : (a) 2ax + 3ay − 2az ;(b ) 3;(c) (ax + ay − az )/ 3
Convert into cyclindrical coordinates the following points
D1.8.
specified in cartesian coordinates : (a) (-2,0,1);
(b ) (1,- 3,-1); and (c) (- 2,- 2,3)
ans :( a ) ( 2,π ,1); (b ) ( 2,5π / 3,−1); (c ) ( 2,5π / 4,3)
Trần Quang Việt – BMCS – Khoa Điện – ĐHBK Tp.HCM
Electromagnetic Fields – Prob – ch_1
Convert into spherical specified in cartesian coordinates :
D1.9.
(a) (0,-2,0);
(b ) (-3, 3,2); and (c) (- 2,0,- 2)
ans :( a ) ( 2,π / 2,3π / 2 );
(b ) ( 4,π / 3,5π / 6); ( c ) ( 2,3π / 4,π )
Three unit vectors are given in cyclindrical coordinates as
follows:
P1.17.
A = ar at ( 2,π / 6,0 ),B = aφ at (1,π / 3,2 )
and C = aφ at (3,5π / 6,1). Find: (a) A.B,(b) B.C
and (c) B×C
Trần Quang Việt – BMCS – Khoa Điện – ĐHBK Tp.HCM
2
Electromagnetic Fields – Prob – ch_1
Three unit vectors are given in spherical coordinates as
follows:
P1.17.
A = ar at ( 2,π / 6,π / 2 ),B = aθ at (1,π / 3,0 )
and C = aφ at (3,π / 4,3π / 2 ). Find: (a) A.B,(b) B.C
(c) A.C, and (d) A× B.C
Find the outward pointing unit vectors normal to the closed
surface 2x2+2y2+z2=8 at the following points:
D5.1.
( a ) ( 2, 2,0); (b) (1,1,2); and (c) (1, 2, 2)
ans : (a) (ax + ay )/ 2, (b) (ax + ay + az )/ 3
ꢁ
ꢁ
ꢁ
(c) ( 2ax + ay + az )/ 7
Trần Quang Việt – BMCS – Khoa Điện – ĐHBK Tp.HCM
Electromagnetic Fields – Prob – ch_1
D5.2. Two scalar functions are given by:
Φ1( x,y,z ) = x2 + y2 + z2
Φ2( x,y,z ) = x + 2y + 2z
Find the following at the point (3,4,12) : (a) the maximum rate of
increase of Φ1, (b) the maximum rate of increase of Φ2; and (c) the
maximum rate of increase of Φ1 along the direction of the
maximum rate of increase of Φ2
ans : (a) 26, (b) 3, (c) 2313
Trần Quang Việt – BMCS – Khoa Điện – ĐHBK Tp.HCM
3
Electromagnetic Fields – Prob – ch_1
P3.1. Find the curls of the following vectors fields:
( a ) zxax + xyay + yzaz
ꢁ
(b ) cos( y )ax − xsin( y )ay
ꢁ
ꢁ
2
( c ) e−r / r aφ in cyclindrical coordinates
(
( d ) 2r cosθ ar +raθ in spherical coordinates
)
ꢁ
ꢁ
Trần Quang Việt – BMCS – Khoa Điện – ĐHBK Tp.HCM
Electromagnetic Fields – Prob – ch_1
P3.8. Find the divergences of the following vectors fields:
( a ) zxax + xyay + yzaz
ꢁ
(b ) 3ax +( y −3)ay +( 2 + z )az
ꢁ
ꢁ
ꢁ
( c ) r sinφaφ in cyclindrical coordinates
ꢁ
( d ) rcosθ(cosθ ar - sinθaθ ) in spherical coordinates
ꢁ
Trần Quang Việt – BMCS – Khoa Điện – ĐHBK Tp.HCM
4
Electromagnetic Fields – Prob – ch_1
D1.16.
Infinite plane sheets of charge lie in the z=0, z=2, and z=4
planes with uniform surface charge densities ρs1, ρs2 and ρs3
respectively. Given that the resulting electric field intensities
at the points (3,5,1), (1,-2,3), and (3,4,5) are
0, 6az , and 6az
V/m respectively, find the following: (a) ρs1, (b) ρs2, (c) ρs3
E at (-2,1,-6)
and (d)
ans : (a) 4ε0 (C/m2 );(b ) 6ε0 (C/m2 );(c) -2ε0 (C/m2 );
ꢁ
(d) -4az (V / m )
Trần Quang Việt – BMCS – Khoa Điện – ĐHBK Tp.HCM
Electromagnetic Fields – Prob – ch_1
D1.20.
Infinite plane sheets of current lie in the x=0, y=0, and z=0
planes with uniform surface current densities :
Js0 az , 2Js0 ax , and -Js0 ax (A/m)
respectively. Find the
resulting magnetic flux densities at the following points :
(a) (1,2,2), (b) (2,-2,-1), and (c) (-2, 1,-2)
ans : (a) µ0Js0 (ay +az );(b ) -µ0Js0 az ;(c) µ0Js0 (-ay +az )
Trần Quang Việt – BMCS – Khoa Điện – ĐHBK Tp.HCM
5
Bạn đang xem tài liệu "Bài giảng Electromagnetic Fields – Prob - Chapter 1 - Trần Quang Việt", để tải tài liệu gốc về máy hãy click vào nút Download ở trên
File đính kèm:
bai_giang_electromagnetic_fields_prob_chapter_1_tran_quang_v.pdf

