MBSMH101 11T practise coil Collaboration meeting Gerard Willering TE-MSC-TF 21-07-2014 on behalf of the test team: Jerome Feuvrier, Vincent Desbiolles with thanks for support during test to Susana Izquierdo, Juho Rysti and Philippe Grosclaude with thanks to everyone involved in the design and preparation of the coil that deserve the credits
MBSMH101 11T practise coil Collaboration meeting. Gerard Willering TE-MSC-TF 21-07-2014 on behalf of the test team: Jerome Feuvrier, Vincent Desbiolles with thanks for support during test to Susana Izquierdo, Juho Rysti and Philippe Grosclaude - PowerPoint PPT Presentation
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MBSMH10111T practise coil
Collaboration meeting
Gerard WilleringTE-MSC-TF 21-07-2014
on behalf of the test team: Jerome Feuvrier, Vincent Desbiolleswith thanks for support during test to Susana Izquierdo, Juho Rysti and Philippe Grosclaude
with thanks to everyone involved in the design and preparation of the coil that deserve the creditsnanos gigantum humeris insidentes
Similar cable as for SMC_11T coil #1 that had magneto-thermal instabilities
SMC_11T #1 MBSMH10148 hrs 210 °C 48 hrs 210 °C48 hrs 400 °C 48 hrs 400 °C50 hrs 650 °C 50 hrs 640 °C
KeystoneLower T should increase RRR and lower Ic
Measured RRR of full coil 77
Rectangular
Short sample and load line
Reference: Internal note to be published, B. Bordini, A. Ballarino, A. Bonasia, L. Oberli, «Cable H15OC0127A for Coil 105 (11 T Magnet Project)»Loadlines calculated by S. Izquierdo using Roxy.
0 2 4 6 8 10 12 14 160
10
20
30
40
50
60
VAMAS 1 - XS, 1.9 KVAMAS 2 - XS, 1.9 KParam. XS, 1.9 KVAMAS 1 - XS, 4.3 KParam. XS, 4.3 KVAMAS 2 - XS, 4.3 KLoadline Roxie 2D w SFLoadline Roxie 2D wo SFLoadline Roxie 3D w SFLoadline Roxie 3D wo SF
Magnetic field [T]
Cab
le c
urre
nt [k
A]
2 sets of Vamas witness samples measured.
Load lines calculated
Resulting short sample current limits:4.3 K: 15.15 kA ± 1 %1.9 K: 16.69 kA ± 1 %
Variation inbetween 2 samples about 300 A.
Uncertainties on loadline Field modulus is usedTheoretical position of the coil is used3D loadline will be re-evaluated
Cooldown
0
50
100
150
200
250
300
0 10 20 30 40 50
Tem
pera
ture
(K)
Time (hours)
Temperature first cooldownT_bottom
T_top
Inner coil
Outer coil
Rather fast cooldown in 45 hours with a ΔT between top and bottom of the yoke of 100 K.Temperature in the coil (calculated from ρ) follows closely the top temperature.
Short circuit in the coil? First ramp of the magnet led to trip at 2.5 kA. Suspicion of a short circuit in the coil
Jumps in total voltage and inner layer voltage during discharge after the quench
2.52.62.72.82.9
33.13.23.33.43.5
0 1 2 3 4 5
Indu
ctan
ce (m
H)
Current (kA)
Ramp up
Ramp down
Only 3.3 mH instead of 3.8 as was calculated!Strong jumps in voltage from 1 to 3 kA
Only normal behavior: Time constant and inductance during energy extraction: coil inductance around 3.8 mH.
2.2
2.25
2.3
2.35
2.4
2.45
2.5
2300
2305
2310
2315
2320
2325
2330
2335
2340
12.22 12.24 12.26 12.28
Volta
ge (V
)
Curr
ent (
A)Time (s)
I_MEAS
V_MEAS
Changes in load on Power ConverterConclusion: No short between turns, but shorts through instrumentation.Post mortem investigation started last Friday.
Inductive voltage on coil not equal to resistive voltage in the dump (6 kA, no quench)
Instrumentation – outer layer
12 outer layer voltage taps2 outer layer heaters
Instrumentation – Inner layer
15 inner layer voltage tapsMany signals for investigation of events !!
Training Quench performanceTraining at 4.3 K up to 14.3 kA
First quench at 9 kA
After 5 quenches at “nominal” 11.8 kA
After 16 quenches 11 T in the coil ends
Most training quenches seem to initiate in the coil ends, but in both inner and outer layer.
I_QH = 150 A, T = 1.9 KQuench heater response time within calculated range, except at 14 kA
Calculations by S. Izquierdo
Resistance growth comparison between model and measurements is progressing
0
20
40
60
80
100
120
5 7 9 11 13 15
Que
nch
dela
y (m
s)
Current (kA)
150 A - 1.9 K
100 A - 1.9 K
80 A - 1.9 K
150 A - 4.3 K
Quench Heater studies
QH delay at 4.3 K is very consistent up to 14 kA.
QH delay at 1.9 K is very fast at 13 and 14 kA, faster than at 4.3 K.
Confirmed for multiple cases
Cannot be explained with “normal” heat transfer from heater to coil.
In addition the quench starts in interlayer jump, far from Quench heaters
Small benefit in resistance growth, but not an effect to count on for protection.
Quench Heater studies
Resistive voltage in the coil at 1.9 K following QH discharge
Large set of data acquired for model validation and futher QH efficiency studies
Resistive voltage different coil blocks at 12 kA at 1.9 K
Example 1 Example 2
Preliminary conclusions
- Good training performance up to 16 kA, 13 T- Very good memory after thermal cycle- No “Holding quenches”- No degradation during testing- Quench heater delays as expected- QH efficiency studies is work in progress, in the right direction