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Prepared By: Shankar Gangaju
Divergence
z
D
y
D
x
D
D:Cartesian zyx










z
DD1)D(1
D:lCylindrica z

























D
sinr
1)sinD(
sinr
1
r
)Dr(
r
1
D:Sphecrical r
2
2

Gradient
zyx aˆ
z
V
aˆ
y
V
aˆ
x
V
V:Cartesian









zaˆ
z
V
aˆ
V1
aˆ
V
V:lCylindrica









 










 aˆ
V
sinr
1
aˆ
V
r
1
aˆ
r
V
V:Spherical r
Curl
z
xy
y
zx
x
yz
aˆ
y
H
x
H
aˆ
x
H
z
H
aˆ
z
H
y
H
H:Cartesian 






































z
zz
aˆ
HH(1
aˆ
H
z
H
aˆ
z
HH1
H:lCylindrica 
















































































 aˆ
H
r
rH(
r
1
aˆ
r
)rH(H
sinr
1
r
1
aˆ
H)sinH(
sinr
1
H:Spherical rr
r

Laplacian:
Cartesian:
Cylindrical: ( )
Spherical: ( ) ( )
Electromagnetic formula

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Electromagnetic formula

  • 1. Prepared By: Shankar Gangaju Divergence z D y D x D D:Cartesian zyx           z DD1)D(1 D:lCylindrica z                          D sinr 1)sinD( sinr 1 r )Dr( r 1 D:Sphecrical r 2 2  Gradient zyx aˆ z V aˆ y V aˆ x V V:Cartesian          zaˆ z V aˆ V1 aˆ V V:lCylindrica                       aˆ V sinr 1 aˆ V r 1 aˆ r V V:Spherical r Curl z xy y zx x yz aˆ y H x H aˆ x H z H aˆ z H y H H:Cartesian                                        z zz aˆ HH(1 aˆ H z H aˆ z HH1 H:lCylindrica                                                                                   aˆ H r rH( r 1 aˆ r )rH(H sinr 1 r 1 aˆ H)sinH( sinr 1 H:Spherical rr r  Laplacian: Cartesian: Cylindrical: ( ) Spherical: ( ) ( )