Vector calculus formulas, Study notes of Accelerator Physics

Vector Formulas used for electromagnetics and other Vector related fields

Typology: Study notes

2015/2016

Uploaded on 07/19/2016

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COORDINATE CONVERSION FORMULAS
Rectangular to Cylindrical, P(x, y, z)P(ρ,φ, z )
ρ=!x2+y2,
φ="tan1#y
x$,if x>0
tan1#y
x$+ 180o,if x<0
Cylindrical to Rectangular, P(ρ,φ, z)P(x, y, z )
x=ρcos φ,
y=ρsin φ
Rectangular to Spherical, P(x, y, z)P(r, θ,φ)
r=!x2+y2+z2
θ= cos1z
!x2+y2+z2
φ="tan1#y
x$,if x>0
tan1#y
x$+ 180o,if x<0
Spherical to Rectangular, P(r, θ,φ)P(x, y, z)
x=rsin θcos φ
y=rsin θsin φ
z=rcos θ
Cylindrical to Spherical, P(ρ,φ, z)P(r, θ,φ)
r=!ρ2+z2
θ= cos1z
!ρ2+z2
Spherical to Cylindrical, P(r, θ,φ)P(ρ,φ, z)
ρ=rsin θ
z=rcos θ
VECTOR CONVERSION FORMULAS
Rectangular to Cylindrical, $
Arec(x, y , z)$
Acyl(ρ,φ, z )
$
Acyl =$
Treccyl $
Arec
%
&
Aρ
Aφ
Az'
(=%
&
cos φsin φ0
sin φcos φ0
0 0 1 '
(%
&
Ax
Ay
Az'
(
Cylindrical to Rectangular, $
Acyl(ρ,φ, z )$
Arec(x, y , z)
$
Arec =$
Tcylrec $
Acyl
%
&
Ax
Ay
Az'
(=%
&
cos φsin φ0
sin φcos φ0
0 0 1 '
(%
&
Aρ
Aφ
Az'
(
Rectangular to Spherical, $
Arec(x, y , z)$
Asph(r, θ,φ)
$
Asph =$
Trecsph $
Arec
%
&
Ar
Aθ
Aφ'
(=%
&
sin θcos φsin θsin φcos θ
cos θcos φcos θsin φsin θ
sin φcos φ0'
(%
&
Ax
Ay
Az'
(
Spherical to Rectangular, $
Asph(r, θ,φ)$
Arec(x, y , z)
$
Arec =$
Tsphrec $
Asph
%
&
Ax
Ay
Az'
(=%
&
sin θcos φcos θcos φsin φ
sin θsin φcos θsin φcos φ
cos θsin θ0'
(%
&
Ar
Aθ
Aφ'
(
Cylindrical to Spherical, $
Acyl(ρ,φ, z )$
Asph(r, θ,φ)
$
Asph =$
Tcylsph $
Acyl
%
&
Ar
Aθ
Aφ'
(=%
&
sin θ0 cos θ
cos θ0sin θ
0 1 0 '
(%
&
Aρ
Aφ
Az'
(
Spherical to Cylindrical, $
Asph(r, θ,φ)$
Acyl(ρ,φ, z )
$
Acyl =$
Tsphcyl $
Asph
%
&
Aρ
Aφ
Az'
(=%
&
sin θcos θ0
0 0 1
cos θsin θ0'
(%
&
Ar
Aθ
Aφ'
(
1
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COORDINATE CONVERSION FORMULAS

Rectangular to Cylindrical, P (x, y, z) → P (ρ, φ, z)

ρ =

x

2

  • y

2 ,

φ =

tan

− 1

y

x

, if x > 0

tan

− 1

y

x

o , if x < 0

Cylindrical to Rectangular, P (ρ, φ, z) → P (x, y, z)

x = ρ cos φ,

y = ρ sin φ

Rectangular to Spherical, P (x, y, z) → P (r, θ, φ)

r =

x

2

  • y

2

  • z

2

θ = cos

− 1

z

!

x

2

  • y

2

  • z

2

φ =

tan

− 1

y

x

, if x > 0

tan

− 1

y

x

o , if x < 0

Spherical to Rectangular, P (r, θ, φ) → P (x, y, z)

x = r sin θ cos φ

y = r sin θ sin φ

z = r cos θ

Cylindrical to Spherical, P (ρ, φ, z) → P (r, θ, φ)

r =

ρ

2

  • z

2

θ = cos

− 1

z

!

ρ

2

  • z

2

Spherical to Cylindrical, P (r, θ, φ) → P (ρ, φ, z)

ρ = r sin θ

z = r cos θ

VECTOR CONVERSION FORMULAS

Rectangular to Cylindrical,

Arec (x, y, z) →

Acyl (ρ, φ, z)

A

cyl

T

rec→cyl

A

rec

%

A

ρ

A

φ

A

z

cos φ sin φ 0

− sin φ cos φ 0

A

x

A

y

A

z

Cylindrical to Rectangular,

A

cyl

(ρ, φ, z) →

A

rec

(x, y, z)

A (^) rec =

Tcyl→rec

Acyl

Ax

Ay

Az

cos φ − sin φ 0

sin φ cos φ 0

Az

Rectangular to Spherical,

A

rec

(x, y, z) →

A

sph

(r, θ, φ)

Asph =

Trec→sph

Arec

Ar

sin θ cos φ sin θ sin φ cos θ

cos θ cos φ cos θ sin φ − sin θ

− sin φ cos φ 0

Ax

Ay

Az

Spherical to Rectangular,

A

sph

(r, θ, φ) →

A

rec

(x, y, z)

Arec =

Tsph→rec

Asph

Ax

Ay

Az

sin θ cos φ cos θ cos φ − sin φ

sin θ sin φ cos θ sin φ cos φ

cos θ − sin θ 0

Ar

Cylindrical to Spherical,

A

cyl

(ρ, φ, z) →

A

sph

(r, θ, φ)

Asph =

Tcyl→sph

Acyl

Ar

sin θ 0 cos θ

cos θ 0 − sin θ

Az

Spherical to Cylindrical,

A

sph

(r, θ, φ) →

A

cyl

(ρ, φ, z)

Acyl =

Tsph→cyl

Asph

Az

sin θ cos θ 0

cos θ − sin θ 0

Ar

GRADIENT OF A SCALAR FIELD

Rectangular Coordinate System (x, y, z)

∇V =

∂V

∂x

ax +

∂V

∂y

ay +

∂V

∂z

az

Cylindrical Coordinate System (ρ, φ, z)

∇V =

∂V

∂ρ

a ρ

ρ

∂V

∂φ

a φ

∂V

∂z

a z

Spherical Coordinate System (r, θ, φ)

∇V =

∂V

∂r

a r

r

∂V

∂θ

a θ

r sin θ

∂V

∂φ

a φ

DIVERGENCE OF A VECTOR FIELD

Rectangular Coordinate System (x, y, z)

F =

∂Fx

∂x

∂Fy

∂y

∂Fz

∂z

Cylindrical Coordinate System (ρ, φ, z)

F =

ρ

∂(ρFρ )

∂ρ

ρ

∂Fφ

∂φ

∂Fz

∂z

Spherical Coordinate System (r, θ, φ)

F =

r

2

∂(r

2 F r

∂r

r sin θ

∂(sin θF θ

∂θ

r sin θ

∂F

φ

∂φ

CURL OF A VECTOR FIELD

Rectangular Coordinate System (x, y, z)

∇ ×

F =

ax ay az

∂x

∂y

∂z

Fx Fy Fz

Cylindrical Coordinate System (ρ, φ, z)

∇ ×

F =

ρ

aρ ρaφ az

∂ρ

∂φ

∂z

Fρ ρF (^) φ Fz

Spherical Coordinate System (r, θ, φ)

∇ ×

F =

r

2 sin θ

ar raθ (r sin θ)aφ

∂r

∂θ

∂φ

F

r

rF θ

(r sin θ)F φ

LAPLACIAN OF A SCALAR FIELD

Rectangular Coordinate System (x, y, z)

2 V =

2 V

∂x

2

∂V

2

∂y

2

∂V

2

∂z

2

Cylindrical Coordinate System (ρ, φ, z)

2 V =

ρ

∂ρ

ρ

∂V

∂ρ

ρ

2

2 V

∂φ

2

2 V

∂z

2

Spherical Coordinate System (r, θ, φ)

2

V =

r

2

∂r

r

2

∂V

∂r

r

2 sin θ

∂θ

sin θ

∂V

∂θ

r

2 sin

2 θ

2 V

∂φ

2

DIVERGENCE THEOREM

S

F · d

S =

v

F

dv

STOKES’S THEOREM

C

F · d

L =

S

∇ ×

F

· d

S

MAXWELL’S EQUATIONS

Differential Form

E =

ρv

0

∇ ×

E = −

B

∂t

H = 0

∇ ×

H =

J +

D

∂t

Integral Form

S

E · d

S =

v

ρv

0

dv

C

E · d

L = −

∂t

S

B · d

S

S

H · d

S = 0

C

H · d

L =

S

J +

D

∂t

· d

S

TEX Typeset:jmmartinezjr