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Slide through the integral! j(r’) r’ ur’ - r + B(r) r

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Page 1: Slide through the integral! j(r’) r’ ur’ - r + B(r) r
Page 2: Slide through the integral! j(r’) r’ ur’ - r + B(r) r

B r A r

''

4 '

j rB r

r rO dv

''

4 '

j rB r

r rO dv

Slide through the integral!

Page 3: Slide through the integral! j(r’) r’ ur’ - r + B(r) r

j(r’)

r’

ur’ - r

'2' '

4 'r ru

B r j rr r

O dv

+ B(r)

r

Page 4: Slide through the integral! j(r’) r’ ur’ - r + B(r) r

3/ 22 2

''

4 '

u uu z rOz

z rI dz

z r

2 22uOI L

r L r

R

z’

r

dz’2 L

I

B

z

'2' '

4 'r ru

B r j rr r

O dv

Page 5: Slide through the integral! j(r’) r’ ur’ - r + B(r) r

2 22

B r uOI L

r L r

lim

2B r uoI

L r

R

z’

r

dz’2 L

I

B

z

Page 6: Slide through the integral! j(r’) r’ ur’ - r + B(r) r

3/ 22 2

'4

u uu r zO

a zI ad

a z

2

3/ 22 22O

z

I aB

a z

'2' '

4 'r ru

B r j rr r

O dv

Page 7: Slide through the integral! j(r’) r’ ur’ - r + B(r) r

summary

js

Three techniques to find B

1] Ampere’s circuital law - lots of symmetry

2] find vector potential A, then B = x A

3] Biot - Savart law

B

A

BB

Page 8: Slide through the integral! j(r’) r’ ur’ - r + B(r) r
Page 9: Slide through the integral! j(r’) r’ ur’ - r + B(r) r

magnetic forces

BvF Q

x

yz

BV

F+

F-Lorentz force

BvEF Q

Page 10: Slide through the integral! j(r’) r’ ur’ - r + B(r) r

jjaMF

vBQF j

j

2

jj r

vMvBQ

j

jj BQ

vMr

B

v

Ma

Mb

j

2

j r

vM

Page 11: Slide through the integral! j(r’) r’ ur’ - r + B(r) r
Page 12: Slide through the integral! j(r’) r’ ur’ - r + B(r) r
Page 13: Slide through the integral! j(r’) r’ ur’ - r + B(r) r

Please Note: Rocket Sets contain rocket motors that are classified as hazardous materials for shipping purposes. Given this, we must ship Rocket Sets via surface mail through the USPS.

Page 14: Slide through the integral! j(r’) r’ ur’ - r + B(r) r

MHD plasma drift F = Q (E + v x B) = 0 0 = E x + v B x V v B x

C 60

+ -B

B

Page 15: Slide through the integral! j(r’) r’ ur’ - r + B(r) r

BvEF Q

LBvLEV

hours2

miles25000v

Tesla105B 5

miles12L volts5000V

electric power in space!

12 miles

Page 16: Slide through the integral! j(r’) r’ ur’ - r + B(r) r
Page 17: Slide through the integral! j(r’) r’ ur’ - r + B(r) r

plasma physics

N

S

N

S

Page 18: Slide through the integral! j(r’) r’ ur’ - r + B(r) r

N

S

plasma physics

Page 19: Slide through the integral! j(r’) r’ ur’ - r + B(r) r

plasma physics

magnetic field

particle loss

Page 20: Slide through the integral! j(r’) r’ ur’ - r + B(r) r

Example: Charged Particle Orbits

in a Tokamak

finite element method

FEMLAB using MATLAB

Page 21: Slide through the integral! j(r’) r’ ur’ - r + B(r) r

poloidal coils

transformer core

BIp

Icoil

primary winding

Tokamak principleTokamak – Problem Definition

Page 22: Slide through the integral! j(r’) r’ ur’ - r + B(r) r

Introduction A tokamak is a “magnetic bottle” for the

confinement of high energy plasmas in Controlled Nuclear Fusion.

The ions and electrons in the plasma travel far between collisions.• collisionless model• particle motion is governed by the EM field• losses are mainly due to collisions with the

walls

Tokamak

Page 23: Slide through the integral! j(r’) r’ ur’ - r + B(r) r

Modeling approach

Coils and plasma current are modeled in FEMLAB and the magnetic field is computed.

• plasma current = 2.2 MA• peak toroidal magnetic field = 2 T

Particle orbits are computed using an ODE solver.

Tokamak

Page 24: Slide through the integral! j(r’) r’ ur’ - r + B(r) r

Results – particle simulation

Proton orbit - Results

banana orbits

Page 25: Slide through the integral! j(r’) r’ ur’ - r + B(r) r

work

b

aW dlF

xxQW uBv

xyx xBvQ uuu 0

x

yz

BV

F

x

Page 26: Slide through the integral! j(r’) r’ ur’ - r + B(r) r
Page 27: Slide through the integral! j(r’) r’ ur’ - r + B(r) r
Page 28: Slide through the integral! j(r’) r’ ur’ - r + B(r) r

VIS Dr. Lou Frank & Dr. John Sigwarth

Page 29: Slide through the integral! j(r’) r’ ur’ - r + B(r) r
Page 30: Slide through the integral! j(r’) r’ ur’ - r + B(r) r

1

I1 dl1

B2

I2 dl2

B1

BvdF dQ

dvv BvdF dsdlBjdF

BIdldF

Page 31: Slide through the integral! j(r’) r’ ur’ - r + B(r) r
Page 32: Slide through the integral! j(r’) r’ ur’ - r + B(r) r

lightning arrestor or STAR WARS

Page 33: Slide through the integral! j(r’) r’ ur’ - r + B(r) r

Magnetic resonance imaging?

Page 34: Slide through the integral! j(r’) r’ ur’ - r + B(r) r

electric machines

rotate about an axis

no translation

torque

Page 35: Slide through the integral! j(r’) r’ ur’ - r + B(r) r

(forces)

z

x

yI

y B

x

BIdldF zoB uB

looponforces

zox BxI uu zoy ByI uu zoy ByI uu zox BxI uu

Page 36: Slide through the integral! j(r’) r’ ur’ - r + B(r) r

Torque

cos 2

yFcos

2

yFT

zx uuF Bx I

+

y

zB

y

x

Page 37: Slide through the integral! j(r’) r’ ur’ - r + B(r) r

Never Use Detergent Again! What would you say if I told you that one of the great inventions of the modern age has no moving parts, doesn't have anything to do with the Internet, doesn't even use Microsoft software? What is this wondrous invention... the Euro-Wash Laundry Ball... a collection of rubber and magnets that cleans clothes, even in the hardest of waters without soaps or detergents.

Euro-Wash Laundry Ball

Page 38: Slide through the integral! j(r’) r’ ur’ - r + B(r) r

MagneForce The first shoe with its own power supply. Comfortable, quality footwear constructedwith a lightweight, flexible magnetic insole to generate a deep penetrating magnetic field which increases circulation; reduces foot, leg, and back fatigue; provides natural pain relief and improved energy level. The James Randi Educational Foundation offers $1 million to Florsheim if it can demonstrate its claims for MagneForce Footwear in a formal double-blind scientific test.

Page 39: Slide through the integral! j(r’) r’ ur’ - r + B(r) r
Page 40: Slide through the integral! j(r’) r’ ur’ - r + B(r) r

Variable Specific Impulse Magnetoplasma Rocket

The VASMIR engine has three magnetic cells.

1) Hydrogen is ionized.

2) Microwaves heat the plasma.

3) Magnetic nozzle converts energy into a directed flow.

Mars, here we come!

cnn 6/2000

Page 41: Slide through the integral! j(r’) r’ ur’ - r + B(r) r

1) Hydrogen is ionized.

2) Microwaves heat the plasma.

3) Magnetic nozzle converts energy into a directed flow.

Page 42: Slide through the integral! j(r’) r’ ur’ - r + B(r) r

1) Hydrogen is ionized.

2) Microwaves heat the plasma.

3) Magnetic nozzle converts energy into a directed flow.

Page 43: Slide through the integral! j(r’) r’ ur’ - r + B(r) r

1) Hydrogen is ionized.

2) Microwaves heat the plasma.

3) Magnetic nozzle converts energy into a directed flow.