• Tidak ada hasil yang ditemukan

gdhszmuia-ciifcaptfdv.mu?vIscap

N/A
N/A
Protected

Academic year: 2024

Membagikan "gdhszmuia-ciifcaptfdv.mu?vIscap"

Copied!
11
0
0

Teks penuh

(1)

4/12/2021

, current

/

charge

(

drift

Fent

n - E

)

-- so

s -7

mandate

: en

LE 't iixis 's

- v. p + R,

+5

, - moi's.

dqfzpj-5zpio.ie

) e i. E'i'+

E' jar

.-ii.

pies

. -ii.

5. etgmuso

* Two - fluids relations s = (x.

p

)

Cl) momentum conservation

Ei fodvamiincap III

I

,

=

I' apt EI

. =

fair maiiacapempvpcpa

-- o

L2)

energy

conservation

Rs

Jd 've fmri cap

=

gdhszmuia-ciifcaptfdv.mu?vIscap

I

Qapt Fap

E.

Rs --

Qapto-patu%FFptiej.FI 's

so

e3 ) current &

Resistivity

- f-rook collision

approximation

IIe

-- -

msnarapcui

-

rip

)

I c.elision

frequency

(2)

- fur electron d-- e ,

DIT

ions

p

-- T

Fei

- - mene

Vertue

-

city

- momentum conservation

EI

, +

I'

ie -- o menever -- minivie

if

near Vei Vie

-

-

proportional

to currents

j

's -

enlai

-

iii

)

Feit me I

'

parallel

momentum EG .

for

electron

medc=

renee. + is It

Fei

. "

tf

small inertia p - homogeneous

F- 9

' Ea =

etaeEei.ci

' a

'

.

" " "

yay

- E ( Oke~

.io#..m 159

Dm

I

' .

I

'

÷ :)

n... -

worm

6,2261 i.e Me, I 2ha

' In

general

,

I

' can't be determined

p

alone

by

I

need

E'

p
(3)

147 Ohmic

heating

energy

conservation

Rei e are = -

ii. Fei

. -

iii. Iie

= -

Eirene

- i'is

= -

meveeij

' .

ten )

--

nj

e5) charge

density

Typically

. we don't use E. E- E

'

= ecni -ne )

to determine E' = - of .

Rather ,

parallel

momentum balance

gives a useful

info

for

ol steady

state . cnet.it Vape = o

const.

Te

. ene Jud = J. . Pe = Tea, ne

ne a

etpleolte

?

at a ete

le

) en Ene

?

Very

good approximation .
(4)

167 Draft of fluid

In

steady

state , w/o source

(

exchange

B'

+ ( en

tenures

-

Ep

3=0

iii.

r. +

5'Ii

'

vi. evi

. is

t

-099 for

E-+ B'' drift diamagnetic £ 9

d.rife Up

Q ) where are B , curvature drifts ?

consistent with particle motion ?

vigor

.

VI.

t + Kuru

* As sump

g Itis

' ro emagneticlow -p assumptionfield

by

externalcoils) Maxwellion

EA) charge accumulation

A

simplified

example .

^

if

, per) I

°

- Z consider Ton drifts

<##

- particle picture

F

¥# E

Igor

,

25253×-813=21

"

measure q

Yaffa

t

BT

e.

Brit

charge

q t

accumulation

Nq opto f F

dfs.ge

Tee

--

envgc

f-

-

we:*, =

:L

. - I

Tp soonstrfo robo

like

pedestal

(5)

- flood picture v

;

=

B→xo

en Bt

Ep

=

jpr

=

envpr

" = en BE x e-

HpbE

*

=

-4¥

:

= - r kept a

- r

to Bo

dear

. -

I

'

reader :# )

--

2÷÷

''

-

-

fee :÷

=

-- do

:#

A bit more

generally

,

- wi

's

=

E. vj ?

e.

try

it

for

+

E'

so

)

CB

) drift

( or current

) itself

?

B Goldston 's book .

,

chapter 7.4.

cancelled since Us

remains same

(

Laboratory

frame

) lmoviny frame

)

A bit more

generally

,

ji

.

I'

got +

It

.

Ei

= -

547=-573

en

E.ie?..I.vgo

wi --

via

Exit

en

Ext

. . - E'+

(

E'

:3

.

)

=

Baton

-

2Pi5×E!3

iii.

=

then :tE#

+

ten .it:7

-

seeing

(6)

4/14/21

Single fluid

Magnetohydrodynamics

CMH b)

Ton & electron

. plasma

density

n = he = hi

- Mass

density

pm =

Is

msns = Mini

- charge

density

6 =

jeans

= o

- Mass

velocity

is

g msn.is/pm=U7tme-m..iie

- current

density j

' =

Is

esnsie

's

=

eneui

-iie 7

§

wire at

mermaid

{ Eerie

-

Een

- y.ee pressure tensor

95

=

Is

Msn, Liv's-E'vis- it's>

- Total heat flat

af

,

ggtzmsns (

(Js-

Tiflis

-ie

)

( Ignore source terms )

Cl )

continuity

Is

Ms +

( continuity

for each 7

'

feet E

'.

cpmii

) - o

Es

es x (

continuity

for each

)

agree

E'-

j

' so

123

Equation of

motion

Is

l momentum conservation

for

each

)

pond :{

= 6

E'

+

j 't E

' -

E. Y

'

TERI

(7)

e.37 Equation

of energy

Is

e energy conservation

for

each

)

Feel 'zp

) +

5zpc-E.ci

)

EET

:

use of

'

=

ej

- hi' ) - CE'eEtB' ? t

-3k€

147

Generalized

Ohm's law

Is Engine

momentum conservation

for

each

)

or electron equation

of

motion l two species)

mee=

- ene

E

' - eneTs

B

-

E. ietenenj

'

electron inertia if - I

ene

E' tu 'xB→=nj

' ,

I

ene Hall term

t Matuell

equations

E'

ni

--

Mj 't I. IIe

+

E

' = - 25'

to :* . :÷ :

(8)

Approximation

for 4¥

low

frequency : :c .is?::...y

phenomena

a : scale

of interest

6 -

EoE/a

w .-

Ier Vania

,

ii

-

E' YI

,

-

E

. .

-

j

-

II

, - e

;ua

CA) small gyro radius

1a

KI

EB) high collisional

icy ÷

, n

tha

k /

cc) low

resistivity

?

Goldston

Friedberg

lo) Maxwell

Y÷¥÷

-

EEE

-

uve÷ ⇐

, a

""

E' xei-rojtt.IE/

Ll)

continuity

n

:÷÷¥ne¥e÷÷

Veni .

*

eyed

. -

term

-

II al

¥e I

so

many

insta. eieies

* .

w→=o

Incompressible

.

( defence

. so

Effect

-

Pacino

(9)

EZ) momentum

:÷÷÷:w÷n÷i÷ ⇐⇒

. .

Pm ai

'

be

-z→

n

pmuvth.la

~ a-

Pm Ven? la Vthi

Pm ii. E' E

TE ~Yn÷z { cgchzj

Ol') MHDdrift-

ordering

-MHD

ordering

"

Hazeltine

u :÷n←÷ii÷x¥÷

p a "

pen

momentum ~

plz

,,

viscosity

pm

DII

= +

Exit

-

Ep

-

E3)

Energy

Millen

?

" ÷w"n#¥÷

Puth-. la

/ ⇐ It÷÷t

.

kn -

Plmevei

,

Ki -

( Iie )£k

,

fake )tIapcE

.

tEEtE

=

of

-

E' taxis )

=

ng

2
(10)

( 47 Ohm 's law

u¥ .sn

.

:::÷÷ii÷i7 ⇒ ¥÷It

since

jxis

' -

E'

per

E'

p,

:¥;÷

-

minister

( OCI )

MHD -

ordering

OCD

drift MHD

un O

( Ia )

- Ken,-

E' tuxes -mjeIxEe

resistive MH17

for

parallel

motion .

J

, ~Mod

Be

n-

u¥e

-

Foa

-

Tn

Magnetic Reynolds

( Lnundqaist )

number

I

' + it

B'

to ideal MH17
(11)

* MHD

equations

E'

+

E' =µj

by eliminating

E' -

j

'

E'

c-

E'

= -a'

I

see dem

Fet

pm CE

'

-i' 7=0

defeat pm

-

E)

" O de

PmdII=jx5

'-

Ep

Eet Esp

'i' 7=0

dIetEp Ezo

"

diet 4tB%

.> sis.

Bye

.

E'

+ E'

xpgen.jo III

- E'

utBCE.u7-z.IE

( 4 equations 8 equations

for ( E'. -

E.

ii.

j.pm.PT

for c. ii.

5.

pm . P)

simple

geometry (

ie -

15×-547%5

Bt

B=bz5t5xEy

l 4. &.bz , -47 Pa , P

four field equations.

Referensi

Dokumen terkait