repeated vector operations curl (grad a) = 0 divcurl a = 0 div (grad a) = laplacian (a)

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Page 1: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)
Page 2: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)

repeated vector operations

curl (grad a) = 0

div•curl A = 0

div (grad a) = Laplacian (a)

Page 3: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)
Page 4: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)

a a aa

x y z

x y zu u u

ax y z

a a a

x y z

x y zu u uxux

Page 5: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)
Page 6: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)

y xz z

y x

A AA A

x y z y z x

A A

z x y

A

x y z

x y z

A A A

x y zu u u

A

Page 7: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)
Page 8: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)

a a aa

x y z

x y zu u u

aa ayx z

ax y z

x y z

x y zu u u

2 2 22

2 2 2

a a aa

x y z

Page 9: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)

Phasors v = V cos (t + ø) v = Re [V ejt] where V = V ejø

vjdt

dv

vj

1'vdt

Page 10: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)

LjRI

Vo

o

53j

120j

e10

e5

o120je5 V

o30t4sin5)t(v

oo 9030t4cos5

o173t4cos5.0)t(i

24j6

e5o120j

Page 11: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)
Page 12: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)

cb

ay

0.010.01

1 100

1

100

y

d

0.010.01

1 100

1

100

y

a0.01

0.011 100

1

100

y

b

0.010.01

1 100

1

100

y

c

Page 13: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)

Physics of Plasmas September, 2008

Page 14: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)

Electric charge force electric field

Page 15: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)
Page 16: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)
Page 17: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)

ruF2

o

21

r4

QQ

12o 10854.8

Coulombs10602.1Q 19

+Q +Q- Q+Q

meter

farads10

36

1 9

Page 18: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)

+Q - Q

Yes Senator, Electrical and Computer Engineers have particles that have

charges with different signs – positive and negative! This was not invented at

Microsoft in order to limit competition

Page 19: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)

10 to 20 Coulombs

Page 20: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)
Page 21: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)

ruF2

o

21

r4

QQ

2

2

o LF

Q 3

22

ML

TQ

22

2

LTL

M

Q

Page 22: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)

2o

21

r4

QQF

Charged dust grains

Coulombs10602.110Q 194

23

9

215

103610

4

10602.1

m10mm1r 3

Newtons10602.19 152

Page 23: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)

history 900 BC - Magnus, a Greek shepherd,

walks across a field of black stones which pull the iron nails out of his sandals and the iron tip from his shepherd's staff (authenticity not guaranteed). This region becomes known as Magnesia.

Page 24: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)

Thales of Miletus 624-547 BC amber rod picked up “fluff and stuff” “elektron” in Greek “elektrum” in Hebrew Ezekiel 1:27

history

Page 25: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)

history 1269 - Petrus Peregrinus of Picardy,

Italy, discovers that natural spherical magnets (lodestones) align needles with lines of longitude pointing between two pole positions on the stone.

Page 26: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)

x

y

3

3

00 6

6

Superposition of forces

vectors

Page 27: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)

5

43

54

QQ

5

43

54

QQ

yx

2o

gr

yx

2o

gr

uu

uuF

ruF2

o

21

r4

QQ

5

8

54

QQ y

2o

gr u

x

y

3

3

00 6

6

Page 28: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)

22

yx

2

o

gr

52

52

294

QQ

uuF

x

y

3

3

00 6

6

ruF2

o

21

r4

QQ

22

yx

2

o

gr

54

54

414

QQ

uu

Page 29: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)

21 Q

FE ru

2o

1

r4

Q

Coulomb

Newtons

Page 30: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)

21 Q

FE ru

2o

1

r4

Q

Coulomb

Newtons

Fundamental units

mass M, length L, time T, charge Q

QTL

M 2

2

2L

M1T

Q L

meter

CoulombJoules

Page 31: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)

Superposition of electric fields

x

y

3

3

00 6

6vectors

Page 32: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)

5

43

54

Q yx

2o

uuE

x

y

3

3

00 6

6ruE

2or4

Q

5

6

54

Q x2

o

u

5

43

54

Q yx

2o

uu

Page 33: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)

Distributed charge density

volume charge density

surface charge density

linear charge density

3v )meter/(Coulombs

2S )meter/(Coulombs

)meter/(CoulombsL

Page 34: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)

cosr4

dydE

2o

L

r

x

r4

dydE

2o

L

2o

L

r4

dydE

22 yxr

x

y

dyr

Page 35: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)

r

x

r4

dydE

2o

L

22 yxr x

y

dyr

a

a 22222

o

L

yx

x

yx4

dyE

22o

L

ax

a

x2

x2

Ea

lim

o

L

Page 36: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)

y

x

Z

dE

cosr2

dydE

o

s

22

o

s

yz2

zdyE

22o

s

yz

z

r2

dy

o

s

2

Page 37: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)

o

s

2E

r2E

o

L

2or4

QE

100

1

0.01

1 100 r

E

Page 38: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)

aa 2/3222

o

saa

zyx4

zdydxE

y

x

Z

-a-a

a

a

finite size square sheetuniform charge density

E

Page 39: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)
Page 40: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)

“Lately I've been wondering where the slide rules went. Back in the 1960’s, slide rules were a prime accessory for those with a quantitative bent. They were suspended from belts long before calculators. In fact, they were the personal calculation engine of choice for almost three centuries.”

Page 41: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)

The principle of the slide rule was first enumerated by E. Gunter in 1623, and in 1671, S. Partridge constructed an instrument similar to the modern slide rule. The slide rule was an indispensable tool for scientists and engineers through the 1960’s.

Page 42: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)

In 50 years, the computer you are using to view this will be landfill, but your slide rule will just be nicely broken in.

Page 43: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)

It happens elsewhere other than under the Iowa Avenue bridge

Page 44: repeated vector operations curl (grad a) = 0 divcurl A = 0 div (grad a) = Laplacian (a)