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HTS Roebel cables N.J. Long, Industrial Research Ltd and General Cable Superconductors Ltd HTS4Fusion Workshop, 26 May 2011
17

HTS Roebel cables N Long - KIT · HTS Roebel cables N.J. Long, Industrial Research Ltd and General Cable Superconductors Ltd HTS4Fusion Workshop, 26 May 2011. Contents • Cable dimensions

Apr 12, 2018

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Page 1: HTS Roebel cables N Long - KIT · HTS Roebel cables N.J. Long, Industrial Research Ltd and General Cable Superconductors Ltd HTS4Fusion Workshop, 26 May 2011. Contents • Cable dimensions

HTS Roebel cables

N.J. Long, Industrial Research Ltdand General Cable Superconductors Ltd

HTS4Fusion Workshop, 26 May 2011

Page 2: HTS Roebel cables N Long - KIT · HTS Roebel cables N.J. Long, Industrial Research Ltd and General Cable Superconductors Ltd HTS4Fusion Workshop, 26 May 2011. Contents • Cable dimensions

Contents

• Cable dimensions• Wire qualification• Manufacturing

– Punching– Retained Ic– Winding

• Performance– Current contacts– Cable Ic results– Potential performance– Ic-stress

• Coupling• Insulation options• Conclusions

Page 3: HTS Roebel cables N Long - KIT · HTS Roebel cables N.J. Long, Industrial Research Ltd and General Cable Superconductors Ltd HTS4Fusion Workshop, 26 May 2011. Contents • Cable dimensions

HTS Roebel Cable Dimensions

Cables are labelled with the convention# of strands / strand width

We are making two designs 15/5 and 10/2

More strands longer transposition length

Page 4: HTS Roebel cables N Long - KIT · HTS Roebel cables N.J. Long, Industrial Research Ltd and General Cable Superconductors Ltd HTS4Fusion Workshop, 26 May 2011. Contents • Cable dimensions

Wire qualification

0 10 20 30 40 500.90

0.92

0.94

0.96

0.98

1.00

Co

rre

latio

nPosition (m)

Wire 2

∑ ∑∑

−−

−−=

22 )()(

))((),(

yyxx

yyxxYXCorrel

For Roebel we require 2D uniformity

- Scan wire magnetically (penetrated or remnant field)

- Quantify uniformity using statistical correlation with an ideal magnetic profile

Correlation along a length of YBCO wire, a minimum Correlcan be specified for input wire

Where |Correl | ≤ 1 X is a dataset representing calculated field

Yy1…yj is magnetic data across tape

0.000 T

200mm

(a)(a)0.023 T

(b)

Use magnetic imaging to assess tape quality (a)

tape with a known defect, and (b) tape with only

small scale variability.

0 2 4 6 8 10 120.010

0.015

0.020

0.025

0.030

0.035

0.040 cor_0.99 cor_0.90 cor_0.75

Fie

ld (

T)

Position (mm)

Example Profiles

Some wire is extremely good !

Page 5: HTS Roebel cables N Long - KIT · HTS Roebel cables N.J. Long, Industrial Research Ltd and General Cable Superconductors Ltd HTS4Fusion Workshop, 26 May 2011. Contents • Cable dimensions

Automated punching

• Ltrans must have minimal error to enable long length winding

• Cutting tool is state-of-the-art

• Pattern is fixed by tooling

• Tool wear is negligible

Punch tool and

frame

Tape de-spool

Tape re-spool

Control

systems (a)

(b)

(c)

(d)

(a) 4 x 5 mm strands from 40 mm (b) 1 x 5 mm wide strand from 12 mm(c) 10 x 2 mm strands from 40 mm(d) 3 x 2 mm wide strands from 12 mm

10 strands cut from 40 mm AMSC strip

Wider feedstock less wastePunching patterns b) c) and d) have all been done

Page 6: HTS Roebel cables N Long - KIT · HTS Roebel cables N.J. Long, Industrial Research Ltd and General Cable Superconductors Ltd HTS4Fusion Workshop, 26 May 2011. Contents • Cable dimensions

Quality of punching

Electroplated copper/NiW

Electroplated copper/NiW

AMSC 4 ply Cu/2x NiW/Cu

AMSC 3 ply SS/NiW/SS

Page 7: HTS Roebel cables N Long - KIT · HTS Roebel cables N.J. Long, Industrial Research Ltd and General Cable Superconductors Ltd HTS4Fusion Workshop, 26 May 2011. Contents • Cable dimensions

Retained Ic

• Strands maintain the wire performance

– (Ic strand) / (Ic wire) ~ typically 90-95%, can be 110%

• High minimum value of Correl is necessary but not sufficient condition

∆Ic also needs to be considered

Length of defect important

Scaling to low T, defects look like a cross sectional loss of conductor

• Can we mitigate low Correl values?

– Strand reinforcement is OK for high I/Ic

Added section of wire (soldered)

defect

Page 8: HTS Roebel cables N Long - KIT · HTS Roebel cables N.J. Long, Industrial Research Ltd and General Cable Superconductors Ltd HTS4Fusion Workshop, 26 May 2011. Contents • Cable dimensions

Automated Cable Winding

• Planetary wind– Longitudinal phase

very important

– Set up is important

– Every wire guided carefully into place

• In principle can be fast ~ meters/min

• At present we go slow– We have $$$ at risk

Automated planetary wind system for 15/5 cable

Page 9: HTS Roebel cables N Long - KIT · HTS Roebel cables N.J. Long, Industrial Research Ltd and General Cable Superconductors Ltd HTS4Fusion Workshop, 26 May 2011. Contents • Cable dimensions

Current contacts

HTS Surface down-Direct contact with largest copper cross section

Apply solder with excess to fill interstrand gap

• Place cable in copper block• Apply solder to excess• Heat and apply pressure to flow solder• Cool down, then remove pressure

Page 10: HTS Roebel cables N Long - KIT · HTS Roebel cables N.J. Long, Industrial Research Ltd and General Cable Superconductors Ltd HTS4Fusion Workshop, 26 May 2011. Contents • Cable dimensions

Cable Ic test

Page 11: HTS Roebel cables N Long - KIT · HTS Roebel cables N.J. Long, Industrial Research Ltd and General Cable Superconductors Ltd HTS4Fusion Workshop, 26 May 2011. Contents • Cable dimensions

15/5 cable from SuperPower wire

Ic measurement of cables

•Measured Ic has been close to expected Ic

• For short length cables accurate Ic measurement is difficult

• At 77K there are strong self-field effects

• Calculation using method of K Thakur et al, Physica C 471, 42-47

13721410209315/5 SRC0027, d = 100 µm

11091010161615/5 SRC0024, d = 100 µm

10331100 145415/5, d = 160 µm

359.1341.94269/2, d = 350 µm

339.1318.84269/2, d = 136 µm

220.1 203 2525/2

ComputedMeasured Design Ic

Cable Ic(A)Cable details

Page 12: HTS Roebel cables N Long - KIT · HTS Roebel cables N.J. Long, Industrial Research Ltd and General Cable Superconductors Ltd HTS4Fusion Workshop, 26 May 2011. Contents • Cable dimensions

Expected Ic at high fields (15/5 cable)

The data is generated using the following

assumptions

• Self-field performance of wire is scaled to higher

fields using data from SuperPower

•We have assumed 280A/cm performance of wire

(most current wires from SP meet or exceed this

performance).

• Note the design current will be significantly

reduced by the cable self field at fields < 1T

• 15/5 = 15 strands of 5mm width

•We do not have parallel field data at this time,

parallel field Ic is generally much higher than

perpendicular field performance e.g. see

http://www.htspeerreview.com/2008/pdfs/presentat

ions/tuesday/joint/joint_2_scale_up_progress_supe

rpower.pdf

0 5 10 15100

1000

10000

I c (

A)

Perpendicular Field (T)

4.2K, 14K, 22K, 33K 45K, 50K, 65K

Page 13: HTS Roebel cables N Long - KIT · HTS Roebel cables N.J. Long, Industrial Research Ltd and General Cable Superconductors Ltd HTS4Fusion Workshop, 26 May 2011. Contents • Cable dimensions

Ic – longitudinal stress test

• 5/2 cable failed catastrophically at 453N (whilst still displaying 86% of maximum Ic)

• Roebel cable appears to exhibit identical ductile limit to Hastelloytape

– The Roebel strands lock together suppressing torque at the transpositions

• Increasing the tensile strain greatly improves current sharing between strands (data not shown).

Tensile ductile limit of Hastelloy276 ~ 700MPa @77K .From Clickner et al. Cryogenics 46 432-438 (2006)

Page 14: HTS Roebel cables N Long - KIT · HTS Roebel cables N.J. Long, Industrial Research Ltd and General Cable Superconductors Ltd HTS4Fusion Workshop, 26 May 2011. Contents • Cable dimensions

The magnetization loss with the applied field

Cable coupled by copper bridges R ~ 10 µΩµΩµΩµΩ

1 10 1001

2

3

4

5

6

7

Γ (

J m

-1 c

ycle

-1str

and

-1 T

-2)

B (mT)

30 Hz 59.5 Hz 120 Hz 175.5 Hz

0 50 100 150 2000

2

4

6

Γ (

J m

-1 c

ycle

-1 s

tra

nd

-1 T

-2)

Frequency (Hz)

5/2 coupled cableB = 2 mT

The magnetization loss v frequency

Loss increasing then decreasing with frequencyFit to Debye form

Strand coupling

Page 15: HTS Roebel cables N Long - KIT · HTS Roebel cables N.J. Long, Industrial Research Ltd and General Cable Superconductors Ltd HTS4Fusion Workshop, 26 May 2011. Contents • Cable dimensions

Strand insulation

Individual strands can be insulated with polymer coating to prevent current sharing

Roll coater to insulate strands

Page 16: HTS Roebel cables N Long - KIT · HTS Roebel cables N.J. Long, Industrial Research Ltd and General Cable Superconductors Ltd HTS4Fusion Workshop, 26 May 2011. Contents • Cable dimensions

Cable insulation

Extrusion coating: fluorinated polymer Wrapping: kapton, nomex paper

No in situ processing of wire flexible insulation options

Page 17: HTS Roebel cables N Long - KIT · HTS Roebel cables N.J. Long, Industrial Research Ltd and General Cable Superconductors Ltd HTS4Fusion Workshop, 26 May 2011. Contents • Cable dimensions

Conclusions

• We have established a pilot plant with automated production of 10/2 and 15/5 cable

• Demonstrated strand coupling and strand insulation

• Obtained first results on stress-Icproperties

• Magnetisation and transport AC loss results published

• Measurements on coil properties including AC loss in progress

• Likely route to low cost Roebelcable is through manufacture of wide REBCO strip Cable manufacture equipment at IRL site