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Research Needs for Magnetic Fusion Energy Sciences - US Burning ...

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gROuP 1a<br />

MEaSuREMEntS FOR MaCHinE<br />

PROtECtiOn anD baSiC COntROL<br />

Plasma shape and position, separatrix-wall<br />

gaps, gap between separatrices<br />

Plasma current, q(a), q(95%)<br />

loop voltage<br />

<strong>Fusion</strong> power<br />

b n = b tor (ab/i)<br />

line-averaged electron density*<br />

impurity and d, t influx (divertor*, & main<br />

plasma)<br />

surface temperature (divertor & upper plates)*<br />

surface temperature (first wall)<br />

Runaway electrons<br />

halo currents<br />

Radiated power (main plasma, X-pt & divertor)<br />

divertor detachment indicator<br />

(J sat , n e , t e at divertor plate)<br />

disruption precursors (locked modes, m=2)<br />

h/l mode indicator*<br />

z eff (line-averaged)<br />

n t /n d in plasma core<br />

elms<br />

Gas pressure (divertor & duct)<br />

Gas composition (divertor & duct)*<br />

dust<br />

gROuP 1b<br />

MEaSuREMEntS FOR<br />

aDVanCED COntROL<br />

neutron and a-source profile<br />

helium density profile (core)<br />

Plasma rotation (toroidal and<br />

poloidal)*<br />

current density profile (q-profile)*<br />

electron temperature profile (core)*<br />

electron density profile (core and<br />

edge)*<br />

ion temperature profile (core)*<br />

Radiation power profile (core,<br />

X-point & divertor)<br />

z eff profile<br />

helium density (divertor)*<br />

heat deposition profile (divertor)*<br />

ionization front position in<br />

divertor<br />

impurity density profiles*<br />

neutral density between plasma<br />

and first wall<br />

n e of divertor plasma*<br />

t e of divertor plasma<br />

a-particle loss<br />

low m/n mhd activity<br />

sawteeth<br />

net erosion (divertor plate)<br />

neutron fluence<br />

237<br />

gROuP 2<br />

PERFORManCE<br />

EVaLuatiOn anD PHySiCS<br />

confined a-particles<br />

tae modes, fishbones*<br />

t e profile (edge)<br />

n e , t e profiles (X-point)<br />

t i in divertor<br />

Plasma flow (divertor)<br />

n t /n d /n h (edge)<br />

n t /n d /n h (divertor)<br />

t e fluctuations<br />

n e fluctuations*<br />

Radial electric field and field<br />

fluctuations<br />

edge turbulence<br />

mhd activity in plasma core<br />

Color coding: Expect per<strong>for</strong>mance to meet measurement requirements; maybe/maybe not; expect not to meet requirements.<br />

Indicates at least one primary technique at risk due to mirror degradation.<br />

* Indicates measurement <strong>for</strong> which <strong>US</strong> ITER Project has responsibility to provide a primary diagnostic.<br />

Table 1. ITER measurements categorized by role, per<strong>for</strong>mance expectation, mirror risk, and <strong>US</strong> ITER Project<br />

involvement.<br />

Why a new burning Plasma Measurement Program?<br />

The understanding and control of fusion plasma behavior relies on a comprehensive set of measurements.<br />

table 1 shows the diagnostic set currently planned <strong>for</strong> iteR. a broad variety of issues<br />

challenge designers in providing these needed measurements:<br />

1) There are “acknowledged gaps,” i.e., cases where it is recognized that no compatible<br />

techniques exist to measure a needed plasma parameter. an example is the lack of a qualified<br />

technique <strong>for</strong> the measurement of lost alpha particles.<br />

2) some presently planned iteR diagnostics are vulnerable due to potential failure of nearplasma<br />

components. an example is degradation of plasma facing diagnostic mirrors due<br />

to plasma-induced deposition or erosion. Failure of such “at-risk” systems could effectively<br />

create more “gaps” in the measurement capability, leading ultimately to reduced effectiveness<br />

of the research program. iteR measurements, indicated by brown shading in table 1, carry<br />

this risk. it would be prudent to develop robust methods to supplement or replace “at-risk”<br />

diagnostics.

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