thermal stability of superconducting magnet system in a tokamak

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Thermal stability of superconducting magnet system in a tokamak Dr hab. inż. Leszek Malinowski, prof. PS Dr inż. Monika Lewandowska

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Thermal stability of superconducting magnet system in a tokamak. Dr hab. inż. Leszek Malinowski, prof. PS Dr inż. Monika Lewandowska. Elevation of the ITER magnet system. TF coil conductor design. PF coil conductor design. CS coil conductor. Conductor quantities for ITER magnets. - PowerPoint PPT Presentation

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Page 1: Thermal stability of superconducting magnet system in a tokamak

Thermal stability of superconducting magnet

system in a tokamak

Dr hab. inż. Leszek Malinowski, prof. PS

Dr inż. Monika Lewandowska

Page 2: Thermal stability of superconducting magnet system in a tokamak

Elevation of the ITER magnet system

Page 3: Thermal stability of superconducting magnet system in a tokamak

TF coil conductor design

PF coil conductor design

Page 4: Thermal stability of superconducting magnet system in a tokamak

CS coil conductor

Page 5: Thermal stability of superconducting magnet system in a tokamak

Conductor quantities for ITER magnets

Page 6: Thermal stability of superconducting magnet system in a tokamak

Heat loads

Page 7: Thermal stability of superconducting magnet system in a tokamak

• Conductors made of pure superconducting material are thermally unstable

• Cables constituted of the superconducting material embeded in the normal metal can operate stable.

Thermal stability

Page 8: Thermal stability of superconducting magnet system in a tokamak

Full stabilizationq > Q

1max

cI

I where oc

c

TThPRI

2

Imax - maximum stable operating current, R - normal state resistance, h - heat transfer

coefficient, P - cooled perimeter, Tc - critical temperature, To - coolant temperature.

Page 9: Thermal stability of superconducting magnet system in a tokamak

Main disadvantage of fully stable wires is large amount of stabilizer. This implies:

• low overall current density of the conductor• large size and big cost of a superconducting device

Modern superconducting wires are partly stable.

It implies limited amount of energy which can be dissipated in a cable without disturbing its safe operation.

Page 10: Thermal stability of superconducting magnet system in a tokamak

Critical energy

crEE

E - energy of dissipationEcr - critical energy of the conductor.

Critical energy - the minimum energy of the thermal disturbance destroying the superconductivity

Page 11: Thermal stability of superconducting magnet system in a tokamak

Mathematical model of normal zone

quu

gu

au

m

sxxxt

e

h

h

h

n

I

T

p

V

T

u

Tn - temperature of the n thermal component

Vh - volumetric flow in the h cooling channel

ph - pressure in the h cooling channel

Th - temperature in the h cooling channel

Ie - current in the e conducting component

Page 12: Thermal stability of superconducting magnet system in a tokamak

Main goals of studies and anticipated results

• Identification and quantification of energy disturbances and heat sources in superconducting magnet system in a fusion reactor.

• Analysis and modelling of heat transfer phenomena in cable-in-conduit-conductors (CICC) used in fusion reactor magnets.

• Development of an analytical model of a normal zone in CICC.

• Formulation of stability criteria for CICC.• Performance of sample calculations and validation

of the results by comparison with experimental results.