fyzika tokamaků1: Úvod, opakování1 tokamak physics jan mlynář 6. transport: theory and...
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Fyzika tokamaků 1: Úvod, opakování 1
Tokamak PhysicsJan Mlynář
6. Transport: Theory and experiments
Bootstrap current, revision of transport, dimensional analysis, Buckingham theorem, dimensionless quantities, scale invariance of equations, Bohm and Gyro-Bohm scaling,identity and similarity experiments, etc.
Tokamak Physics 2
Bootstrap current
7: Transport: Theory and experiment
Tokamak Physics 3
Bootstrap current
7: Transport: Theory and experiment
Tokamak Physics 4
Bootstrap current
7: Transport: Theory and experiment
Tokamak Physics 5
Bootstrap current
"I was still a couple of miles above the clouds when it broke, and with such violence I fell to the ground that I found myself stunned, and in a hole nine fathoms under the grass, when I recovered, hardly knowing how to get out again. Looking down, I observed that I had on a pair of boots with exceptionally sturdy straps. Grasping them firmly, I pulled with all my might. Soon I had hoist myself to the top and stepped out on terra firma without further ado." Campaigns and Adventures of Baron Munchausen (Baron Prášil in Czech), 1786.
7: Transport: Theory and experiment
Tokamak Physics 6
Revision of transport
7: Transport: Theory and experiment
What can be done if “first principles” (models based on plasma theory)
won’t fit the data?
- dimensional analysis
- scale invariance
-33 1 3 [ Wm ]
2 2e e
e e he ei e e e
T ndn T P R P r D T
dt r r r r
-33 1 3 [ Wm ]
2 2i i
i i hi cx ei i i i
T ndn T P L P r D T
dt r r r r
radiation conductive loss convective loss
charge exchange
electrons:
ions:
Neoclassical transport
However, in experiments:
3/2 2. . ( . .) 2
( )P S G S L ei
nD q r
B T
2p
E
B
nT
Tokamak Physics 7
Dimensional analysis
7: Transport: Theory and experiment
Courtesy of C C Petty fromthe General Atomics, USA
Buckingham - theorem
Tokamak Physics 8
Buckingham theorem
7: Transport: Theory and experiment
Boris Kadomtsev 1928-1998
Kadomtsev applied the theorem on tokamaks
in 1975. Published in a brief and simple article.
Choice of dimensional quantities defining state of the system:
BT, Bp, T, n, mi , R, a
+ „fundamental“: me , e, m0 (c)
Tokamak Physics 9
Dimensional analysis
7: Transport: Theory and experiment
But there are only 7 quatnitites + 3 ratios:
eT
p i
mBaq
R B m
4 independent quantities BT, T, n, a
4 dimensionless independent parameters required
to describe the tokamak plasma
Typical choice:
02
3/2
* normalised Larmor radius
2 beta
* normalised collisionalityv
* normalised Debye length
Li
T b
D
r
anT
B
Rq
a
Tokamak Physics 10
Dimensional analysis
Physical limitations: Does
the set Q1, ... Qn describe
the system completely?
7: Transport: Theory and experiment
1 2
1 2 1 2
( , , ) 0
( , , , , , ) 0n
p p p n
F Q Q Q
F r r r
e.g. following the Buckingham recipe:
independentdimensionless
ratios
1 2 3 4 *
1where 1 0 1
2
a b c d
a b c d
Tokamak Physics 11
Scale invariance
7: Transport: Theory and experiment
Complementary to dimensional analyses• take equations that describe the system• find transformations for which the equations are invariant
e.g. the Vlasov (collisionless) equation + quasineutrality:
3
( ) 0
0
j jj
j
j jj
f ef f
t m
e f d
vv E v B
v
3 invariant transformations:
1 2
1 1
(1)
(2) v v t
(3)
j jf f
t E E B B
t t x x E E B B
Tokamak Physics 12
Scale invariance
7: Transport: Theory and experiment
From Kadomtsev, we expect: p q r sE n B T a
3 2 31v
3n fd nT m fd v v
substituting to
2 2
(1) 01
(2) 2 1
(3) 0
r
E
pT
r qB a B
s q
Physical limitations:does the system of equations describe the system correctly ?
Collisional high-beta equation is more realistic than Vlasov equation
results in 54
1( )E F Ba
B
For constant n, T that is, constant
i.e. “identity experiments” 5 54 4const. (only)EBa a
*, *,
Tokamak Physics 13
Combining scale invariance and dimensional analysis
7: Transport: Theory and experiment
4 dimensional independent parameters
n, B, T, a 4 dimensionless independent parameters
e.g. **, *, ,D
(notice: all doubts concerning completeness of this choice remain valid)
* * *r s q pE n B T a
It can be speculated that * has no influence on transport, i.e. = 0
a constraint on r, s, q, p known as the “Kadomtsev condition”:
1( *, , *)E F
Tokamak Physics 14
Identity and similarity experiments
7: Transport: Theory and experiment
Identical & “ratios” (see below) * *, ,
“Identity experiments” are based on the same idea as
the “wind-tunnel” experiments (remember the exercise
with the Reynolds number, from Feynman part II)
Two fixed parameters, and one changing (usually the *)
Identity experiments:
Similarity experiments:
However, some authors tend to use “identity” for equal dimensional values.
Notice that the ratios must be fixed as well!
, , , , , ,eeff
i s
vTq a Z M
T c
M …. Mach number… this can cause difficulties due to different plasma rotation in different facilities !
Tokamak Physics 15
Identity and similarity experiments
7: Transport: Theory and experiment
Tokamak Physics 16
Bohm and Gyro-Bohm scaling
7: Transport: Theory and experiment
? Scaling with * ?
1. Bohm scaling
also known as “Bohm-like diffusion”
i.e. independent of *
fluctuations are driven by gradient lengths
2
( , *)
where 16
E B
Be
F
eBa
T
2. Gyro-Bohm scaling( , *)
*B
E F
2
3
* Bohm scaling
* gyro-Bohm scaling
E
E
B
B
Experiment decides!
Notice: „Global scaling“ need not be realistic.
Tokamak Physics 17
Bohm and Gyro-Bohm scaling
7: Transport: Theory and experiment
Tokamak Physics 18
Pedestal profiles – no atomic physics
7: Transport: Theory and experiment
Tokamak Physics 19
Hidden physics
7: Transport: Theory and experiment
Tokamak Physics 20
Regression analysis
7: Transport: Theory and experiment
can help to distinguish the transport processes, e.g.
breaks the zonal flows
But stabilises TEM (~ bananas)
Important : driven by electrostatic or magnetic turbulences?
It is significant, as the former option may mean
higher than predicted Q in ITER.
Tokamak Physics 21
Role of scale experiments
7: Transport: Theory and experiment
( *)E ii
( )E( )E
( )E
ei
Tokamak Physics 22
Promise for ITER ?
7: Transport: Theory and experiment
Extrapolation of scale invariance has large error ITER has to be built
Tokamak Physics 23
Conclusions
7: Transport: Theory and experiment
To remember
Experiments can clarify whether certain processes are
important for plasma dynamics, via their scaling
properties (e.g. atomic physics proved irrelevant for the
edge dynamics)
On the other hand, sometimes the experiments do not
scale as expected
this means there is some hidden physics
(e.g. influence of ripple)
Multiparameter regression analysis is not consistent
with separated scaling experiments
extrapolations have large error and
tend to be conservative (crossfingers !!)
1)
2)
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