+ All Categories
Home > Documents > Challenges on demountable / segmented coil concept for ... · High-Temperature Superconductor (HTS)...

Challenges on demountable / segmented coil concept for ... · High-Temperature Superconductor (HTS)...

Date post: 22-Jul-2020
Category:
Upload: others
View: 1 times
Download: 0 times
Share this document with a friend
29
1/27 Challenges on demountable / segmented coil concept for high-temperature superconducting magnet N. Yanagi 1 , S. Ito 2 , H. Hashizume 2 , A. Sagara 1 1 National Institute for Fusion Science 2 Tohoku University 1/27 Fifth IAEA DEMO Programme Workshop (DPW-5) May 7-10, 2018, Daejeon, Republic of Korea. In collaboration with Z. Hartwig MIT, Plasma Science and Fusion Center
Transcript
Page 1: Challenges on demountable / segmented coil concept for ... · High-Temperature Superconductor (HTS) (1) High critical current to high field (2) High cryogenic stability (3) Low cryogenic

1/27

Challenges on demountable / segmented coil

concept for high-temperature

superconducting magnetN. Yanagi1, S. Ito2, H. Hashizume2, A. Sagara1

1National Institute for Fusion Science2Tohoku University

1/27

Fifth IAEA DEMO Programme Workshop (DPW-5)

May 7-10, 2018, Daejeon, Republic of Korea.

In collaboration with

Z. HartwigMIT, Plasma Science and Fusion Center

Page 2: Challenges on demountable / segmented coil concept for ... · High-Temperature Superconductor (HTS) (1) High critical current to high field (2) High cryogenic stability (3) Low cryogenic

2/27

Contents

Quick overview of the fusion reactor design employing HTS

Quick overview of the HTS conductor development for fusion magnets

Demountable / segmented (joint-winding) coil concept using HTS conductors

Joint-winding concept for the helical fusion reactor FFHR

Demountable coil concept for the compact tokamak reactor ARC

“Pros and Cons” for the demountable / segmented (joint-winding) coil concept

Page 3: Challenges on demountable / segmented coil concept for ... · High-Temperature Superconductor (HTS) (1) High critical current to high field (2) High cryogenic stability (3) Low cryogenic

3/27

High-Temperature Superconductor (HTS)

(1) High critical current to high field

(2) High cryogenic stability

(3) Low cryogenic power

(4) High mechanical rigidity

(5) Industrial production of tapes

(6) Saving helium resources

Rare-Earth Barium

Copper Oxide

(REBCO)

Hastelloy

Copper

REBCO

pQ C T

Stability Margin

Higher than CIC conductor

Low quench risk!

5 32 10 (J/m K) 10 (K)

2 (J/cc)

pC T

N. Yanagi, S. Ito, et al.,

Plasma and Fusion Research

9 (2014) 1405013

High field

High temp.

High heat

Page 4: Challenges on demountable / segmented coil concept for ... · High-Temperature Superconductor (HTS) (1) High critical current to high field (2) High cryogenic stability (3) Low cryogenic

4/27

Pioneering Work of

applying HTS to tokamak reactor designs

copper

YBCO

Hastelloy Substrate

VECTOR (JAEA)

T. Ando, S. Nishio, H. Yoshimura

(2004)

YBCO

Bi-2212

ARIES-AT (USA)

YBCO

Bi-2212 CIC conductor

10 kA@20 K, 12 T

T. Isono et al.

(2003)

F. Dahlgren et al.

(2006)

Page 5: Challenges on demountable / segmented coil concept for ... · High-Temperature Superconductor (HTS) (1) High critical current to high field (2) High cryogenic stability (3) Low cryogenic

5/27

Sagara 12

Another approach using Another approach using HTcSC HTcSC for magnet coilsfor magnet coils

Even the shielding efficiency is poor,

● temperature margin is wide,

● controllability becomes high

at high T operation,

(because specific heat ~ T3)

T.Horiuchi et al., Fusion Technol. 8 (1985) 1654.

Conventional SC joint design

Re-mountable coils

using HTcS.C. joints

H.Hashizume et al.,

J.Plasma Fusion Res.

SERIES 5 (2001) 532.

● SC joint is promising

and innovative.

  (Ohmic heat on cryo.

< a few % of Pf)

Pioneering Work of

applying HTS to helical reactor designs

H. Hashizume, S. Kitajima, S. Ito, K. Yagi, Y. Usui, Y. Hida, A. Sagara

“Advanced Fusion Reactor Design using Remountable HTc SC Magnet”

J. Plasma Fusion Res. SERIES 5 (2002) 532.

FFHR-2

(1) Construction cost reduction of magnet

(2) Repair of magnet module if damaged

(3) Maintenance of blanket modules

LHDcontinuous helical winding

(1995-1996)

×3~4

Page 6: Challenges on demountable / segmented coil concept for ... · High-Temperature Superconductor (HTS) (1) High critical current to high field (2) High cryogenic stability (3) Low cryogenic

6/27

ARC (MIT, US)

Tokamak Energy (UK)

CFETR-Phase II

(ASIPP, China)

HTS Magnet Concepts for Fusion in the World (2018)

FNSF-ST (PPPL, US)

EU DEMO HTS option (EUROfusion)

FFHR-d1 (NIFS, Japan)

Page 7: Challenges on demountable / segmented coil concept for ... · High-Temperature Superconductor (HTS) (1) High critical current to high field (2) High cryogenic stability (3) Low cryogenic

7/27

Large-Current HTS Conductors

Twisted and Transposed REBCO Conductors

Simply-Stacked REBCO Conductors

Roebel (KIT)

CORC (ACT)

TSTC (MIT)CroCo (KIT)

RSCCCT (SPC)

Slotted Core (ENEA)Roebel (CERN)

STARS (NIFS)

Bi-2212 CIC Conductors

Bi-2212 (ASIPP)

QI (NCEPU)

CSRC (ASIPP)

Page 8: Challenges on demountable / segmented coil concept for ... · High-Temperature Superconductor (HTS) (1) High critical current to high field (2) High cryogenic stability (3) Low cryogenic

8/27

Large-Current HTS Conductors

Achievement by Prototype Conductor Samples

SPC RSCCCT conductor

60 kA @5 K, 12 T

CERN CORC conductor

80 kA @4 K, 12 T

NIFS-Tohoku STARS conductor

100 kA @20 K, 5.3 T

120 kA @4 K, 0.45 T

Page 9: Challenges on demountable / segmented coil concept for ... · High-Temperature Superconductor (HTS) (1) High critical current to high field (2) High cryogenic stability (3) Low cryogenic

9/27

100 kA-class HTS Conductor for FFHR-d1

”STARS” (Stacked Tapes Assembled in Rigid Structure)

Operation current 94 kA @12 T

Operation temperature 20 K

Conductor size 62 mm ×62 mm

Current density 24.5 A/mm2

Number of tapes 40

Cabling method Simple Stacking

Stabilizer OFC

Outer jacket Stainless Steel

Electrical insulation Organic or Inorganic

Cooling method GHe or LNe

Superconductor REBCO

Critical current >900 A/cm @77 K, s.f.

Type-2

not rotatable

Type-1

rotatable

Simply-stacked HTS conductor for DC helical coils

Non-uniform current distribution may be allowed

High mechanical strength (no void & no local deformation)

Low cost and low resistance joint

Page 10: Challenges on demountable / segmented coil concept for ... · High-Temperature Superconductor (HTS) (1) High critical current to high field (2) High cryogenic stability (3) Low cryogenic

10/27

H. Hashizume (2000)

Demountable TF and helical coils with HTS

Concept of Demountable / Segmented Fabrication

of Helical Coils

N. YanagiOnce-through joint of HTS coils (2006)

“Joint-winding” of HTS conductors (2010)

K. Uo (1985)

Demountable helical coils with LTS

A. Sagara (2001.6)

Excavation of the idea for FFHR design

H. Hashizume, S. Ito“Remountable” (demountable) HTS coils

for advanced option of helical coils

for advanced TF coils

H. Hashizume, A. Sagara (2001.12)

Demountable helical coils with HTS

Page 11: Challenges on demountable / segmented coil concept for ... · High-Temperature Superconductor (HTS) (1) High critical current to high field (2) High cryogenic stability (3) Low cryogenic

11/27

“Joint-Winding” of Helical Coils

390 turns×5 segments×2 coils

3,900 joints

Helical Coils

if 1 day / joint

and 4 parallel works (2 helical coils, 2 directions)

3,900 / 4 = 2.7 years

if 0.5 day / joint

and 4 parallel works (2 helical coils, 2 directions)

3,900 / 2 / 4 = 1.3 years

Lift up by 0.5-1 m

Welding of neighboring windings

No VPI

Helium gas cooling

Simple cooling system

Page 12: Challenges on demountable / segmented coil concept for ... · High-Temperature Superconductor (HTS) (1) High critical current to high field (2) High cryogenic stability (3) Low cryogenic

12/27

Applying contact pressure to each layer

Checking overlapping, contact pressure distribution, joint quality After joining all layers

Placing copper jacket

Fabrication of Prototype Conductor Joint

Arranging GdBCO tapes (3 rows, 14 layers) in a stair-case structure

Polishing joint surface (#400), Cleaning joint surface (Ethanol), Inserting indium foils

S. Ito (Tohoku Univ.)

Placing stainless steel jacket and applying contact pressure again

Page 13: Challenges on demountable / segmented coil concept for ... · High-Temperature Superconductor (HTS) (1) High critical current to high field (2) High cryogenic stability (3) Low cryogenic

13/27

Joint resistance : ~2 nW Joint resistivity : ~10 pWm2

Evaluation of Joint Resistance

Required electrical power of the cryoplant at R.T. < 5 MW (for 3,900 joints)

Bridge-type mechanical lap joint

“Invisible joint” S. Ito (Tohoku Univ.)

Page 14: Challenges on demountable / segmented coil concept for ... · High-Temperature Superconductor (HTS) (1) High critical current to high field (2) High cryogenic stability (3) Low cryogenic

14/27

Joint resistance versus heating temp.

(1-layer, indium inserted mechanical lap joint)

Joint resistivity was reduced by 60%

Before heating

60%

Variation of resistance was reduced

Contact pressure:

100 MPa

Applying large-scale conductor

3-row 1-layer, bridge-type lap joint

before heating:25 pWm2

after heating(90C, 30 min):8 pWm2 !

Not needing oxygen annealing

→ Application to other HTS devices,

e.g., HTS power cables

Reduction of Joint Resistance by Low-Temp. Heat Treatment

T. Nishio, S. Ito (Tohoku Univ.)

Page 15: Challenges on demountable / segmented coil concept for ... · High-Temperature Superconductor (HTS) (1) High critical current to high field (2) High cryogenic stability (3) Low cryogenic

15/27

Tensile and shear strength

test for single-tape joint

Maximum shear strength

obtained by 3D-FEM analysis

50 MPa

Normal strain distribution along the

winding direction of the helical coil

Distributions of in-plane shear strain in the helical

coil and its xy component in the HTS tape region

H. Tamura

EM Stress Analysis of the Helical Coil and

Tensile Test on a Single HTS Tape Joint

S. Ito (Tohoku Univ.)

Page 16: Challenges on demountable / segmented coil concept for ... · High-Temperature Superconductor (HTS) (1) High critical current to high field (2) High cryogenic stability (3) Low cryogenic

16/27

We successfully achieved…- 1.8 nW (~10 pWm2) at 100 kA using prototype STARS conductor joint.- Sufficient strength at 77 K using mechanical lap joint of REBCO tapes.

Can we achieve sufficient strength for STARS conductor joint at lower temperature?

Measurement at KIT- Critical current and joint resistance at 4.2 K

and different fields

- Joint resistance at 4.2 K and 12 T for

various sample elongationsFBI test facility at KIT

Courtesy of C. Barth, Ph.D. Thesis 2013

(http://digbib.ubka.uni-karlsruhe.de/volltexte/1000035747)

100

kN

12 T10 kA

Sample preparation and pre-measurement at Tohoku Univ.- Design and fabricate a 10 kA class STARS conductor joint- Measure critical current and joint resistance at 77 K

- Apply a tensile force of 10 kN at room temperature

Measure critical current and joint resistance at 77 K again

Current achievements

Future tasks

Mechanical Test of HTS STARS Joint

Page 17: Challenges on demountable / segmented coil concept for ... · High-Temperature Superconductor (HTS) (1) High critical current to high field (2) High cryogenic stability (3) Low cryogenic

17/27

ARCR = 3.3 m, Bt ~ 9 T, Bmax ~ 23 T

Pf ~ 500 MW

ARC & SPARC @MIT

SPARCR = 1.65 m, Bt ~ 12 T

Pf ~ 50-100 MW

Page 18: Challenges on demountable / segmented coil concept for ... · High-Temperature Superconductor (HTS) (1) High critical current to high field (2) High cryogenic stability (3) Low cryogenic

18/27

Page 19: Challenges on demountable / segmented coil concept for ... · High-Temperature Superconductor (HTS) (1) High critical current to high field (2) High cryogenic stability (3) Low cryogenic

19/27

F. J. Mangiarotti, Ph.D. Thesis, MIT, 2016

https://dspace.mit.edu/handle/1721.1/103659

Page 20: Challenges on demountable / segmented coil concept for ... · High-Temperature Superconductor (HTS) (1) High critical current to high field (2) High cryogenic stability (3) Low cryogenic

20/27

F. J. Mangiarotti, Ph.D. Thesis, MIT, 2016

https://dspace.mit.edu/handle/1721.1/103659

Page 21: Challenges on demountable / segmented coil concept for ... · High-Temperature Superconductor (HTS) (1) High critical current to high field (2) High cryogenic stability (3) Low cryogenic

21/27

F. J. Mangiarotti, Ph.D. Thesis, MIT, 2016

https://dspace.mit.edu/handle/1721.1/103659

Page 22: Challenges on demountable / segmented coil concept for ... · High-Temperature Superconductor (HTS) (1) High critical current to high field (2) High cryogenic stability (3) Low cryogenic

22/27

F. J. Mangiarotti, Ph.D. Thesis, MIT, 2016

https://dspace.mit.edu/handle/1721.1/103659

Page 23: Challenges on demountable / segmented coil concept for ... · High-Temperature Superconductor (HTS) (1) High critical current to high field (2) High cryogenic stability (3) Low cryogenic

23/27

“Pros and Cons” on Demountable Coil Concept

Pros Cons

General remarks Fabrication of large and complex

magnet becomes easy and shorter

in time

Too many joints and high risk

(failure of SC coils happens

often from joints, e.g., LHC)

Conductor Short-length high-performance

tapes can be used and simple-

stacking can be assured with joints

Repair of coil module Damaged coil segments are

individually repairable

Repairing radio-activated coil

with remote handling is difficult

Joint resistance Can be sufficiently low for HTS Difficult to ensure low resistance

for all the joints simultaneously

Electrical insulation Can be made with the present

structure,

Non-insulation can be an option

Difficult to ensure perfect

insulation for all the turns

simultaneously

Mechanical strength Can be assured with a slight

reinforcement at the joint section

Additional support structure

may be needed

Maintenance of in-

vessel components

Accessing in-vessel components

becomes easy, w/o. remote handling

Applicable only to small-sized

tokamaks (VV + BB altogether)

in comparison to the conventional winding method

debating…

Page 24: Challenges on demountable / segmented coil concept for ... · High-Temperature Superconductor (HTS) (1) High critical current to high field (2) High cryogenic stability (3) Low cryogenic

24/27

“Pros and Cons” on Joint-Winding Concept

Pros Cons

General remarks Fabrication of large and complex

magnet becomes easy and shorter in

time

Too many joints and high risk

(failure of SC coils happens often

from joints, e.g., LHC)

Conductor Short-length high-performance tapes

can be used and simple-stacking can

be assured with joints

Fabrication Easy by using an industrial robot

(with inspection also)

Difficult to make joints and also

prefabricated segments with high

accuracy

Joint resistance Can be sufficiently low for HTS Difficult to ensure low resistance

for all the joints

Electrical

insulation

Can be made using an industrial

robot,

Non-insulation can be an option

Difficult to ensure perfect

insulation for all the joints

debating…

in comparison to the conventional winding method

Page 25: Challenges on demountable / segmented coil concept for ... · High-Temperature Superconductor (HTS) (1) High critical current to high field (2) High cryogenic stability (3) Low cryogenic

25/27

Inductance of one double-pancake of the

helical coil of FFHR-d1: ~0.5 H

Resistance by “partial insulation” between

terminals : ~ 5.6×10-8 W

Charging time : ~ 100 days…

Might be much shorter for ARC?

Electrical insulation

HTS tapes

Copper stabilizer

Stainless steel jacket

w./ electrical insulation w/o. electrical insulation

Non-insulation coil option ? Trend for small DC HTS coils

S. Hahn, IEEE TAS 21 (2011) 1592

Page 26: Challenges on demountable / segmented coil concept for ... · High-Temperature Superconductor (HTS) (1) High critical current to high field (2) High cryogenic stability (3) Low cryogenic

26/27

13 T, f700 mm

SC Magnet

Experimental Plans at 13-T, f700-mm Magnet Facility

NIFS

STARS

Conductor

M. Takayasu (MIT)

TSTC

Conductors

First Sample

Second Sample

Z. Hartwig, B. Sorbom, R. Vieira

(MIT)

Page 27: Challenges on demountable / segmented coil concept for ... · High-Temperature Superconductor (HTS) (1) High critical current to high field (2) High cryogenic stability (3) Low cryogenic

27/27

Summary

HTS option is being employed in some fusion reactor designs

Demountable / segmented coil fabrication concept is supposed to be a revolutionary idea to facilitate the construction and maintenance

For the LHD-type helical fusion reactor FFHR-d1, “joint-winding” option is being explored

For the compact tokamak reactor ARC, demountable TF coils concept supports a dramatic facilitation of the maintenance work

Pros and cons for demountable / segmented coil fabrication are summarized

Future Work Prototype conductor sample tests at NIFS (13 T, f700 mm)

Mechanical test of a STARS conductor joint at KIT

Large-scale R&D coil tests employing demountable coil concept and/or joint-winding

Development of industrial robot for joint-winding

Page 28: Challenges on demountable / segmented coil concept for ... · High-Temperature Superconductor (HTS) (1) High critical current to high field (2) High cryogenic stability (3) Low cryogenic

28/27

Extra Slides

Page 29: Challenges on demountable / segmented coil concept for ... · High-Temperature Superconductor (HTS) (1) High critical current to high field (2) High cryogenic stability (3) Low cryogenic

29/27

F. J. Mangiarotti, Ph.D. Thesis, MIT, 2016

https://dspace.mit.edu/handle/1721.1/103659


Recommended