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Test Program and Results
Guram Chlachidze for
FNAL-CERN CollaborationSeptember 26-27, 2012
Outline• Test program• Quench Performance• Quench Protection• Magnetic Measurements• Summary
MBHSP01 Test at VMTF
• MBHSP01 - the first 11T demonstrator dipole magnet was tested at Fermilab’s Vertical Magnet Test Facility (VMTF) in June-July 2012
• VMTF was designed for testing magnets up to 4-m length and 0.6-m diameter at temperatures between 1.8 K and 4.6 K
– 30 kA power system– 30 kA/1 kV DC rated dump resistor (15 mΩ – 120 mΩ)– Two 15 kA/1 kV DC rated solid-state dump switches
• 60-mΩ dump resistor was used for the stored energy extraction
Guram Chlachidze, FNAL-CERN Collaboration 2
MBHSP01 instrumentation
• Voltage tap system covers the inner and outer coil layers, pole turn, multi-turn and splice sections. There are 10 voltage taps on the inner layer and 9 voltage taps on the outer layer
Guram Chlachidze, FNAL-CERN Collaboration 3
Magnet instrumentation (cont’d)
• Each coil was equipped 2 pairs of protection heaters. Each pair covers 28% of the total coil surface
• 1-layer or 2-layer 5-mil (125 µm) Kapton insulation was placed between the heaters and the outer-layer coil block
Guram Chlachidze, FNAL-CERN Collaboration 4
PH-1L (1 layer)
PH-2L (2 layers)
PH-1L (1 layer)
PH-2L (2 layers)
Magnet instrumentation (cont’d)
• 64 strain gauges (SG) were installed on shell, coils and bullets for monitoring mechanical strain and coil stresses during the magnet construction and testing
• 4 resistive temperature sensors (RTD) were mounted at top, middle and bottom of the magnet outer skin
• No quench antenna was available for this 60-mm aperture magnet
Guram Chlachidze, FNAL-CERN Collaboration 5
MBHSP01 Test at VMTF
• Cold test program included quench training, ramp rate dependence study, protection heater study and field quality measurements both at 4.5 K and 1.9 K
• Temperature dependence study, RRR and splice resistance measurements also are part of our standard test program. AC loss measurement was not included in the test program
• The original test program was modified due to limited magnet performance– Quench training at various ramp rates– Additional tests to investigate magnet stability– Field quality measurements at a maximum current of 6500 A– Heater study at a maximum of ~ 65% of SSL
• Long test with several interruptions
Guram Chlachidze, FNAL-CERN Collaboration 6
Quench Performance
Guram Chlachidze, FNAL-CERN Collaboration 7
1.9 K4.5 K
TC-1
4.5 K 1.9 K
TC-2
2.6-4.5 K
Unscheduled thermal cycle at the very end of the test
SG data: cool-down
Guram Chlachidze, FNAL-CERN Collaboration 8
Pole gauges in coils 2 (top) & 3 (bottom)
SG data: cool-down
Guram Chlachidze, FNAL-CERN Collaboration 9
LE Bullets RE Bullets
LE and RE Skin
Strain gauges on shell (skin)and bullets
Ramp rate dependence
Guram Chlachidze, FNAL-CERN Collaboration 10
SSL:4.6 K 13 kA1.9 K 15 kA
Possible conductor damage in the mid-plane blockmay be reason for a limited magnet performance
10.4 T or 78% of SSL
No quench when ramping down from 8 kA at a ramp rate of 120 A/s
Quench locations
Guram Chlachidze, FNAL-CERN Collaboration 11
2b2_b1 splice segment picks up asignal from the quenching 2b3_b2 Segment (mid-plane block)- checked for a PH induced quench
Upper limit of b2_b1 splice resistance estimated as <2 nΩ
Heater induced quench
2b2_b1 x 10
2b2_b1 x 10
Quench Locations
Guram Chlachidze, FNAL-CERN Collaboration 12
Coil-2/3 IL/OL MP: A2-A3, B2-B3
Coil-2/3 IL: A4-A5, A5-A6Coil-2/3 OL: B3-B4, B5-B6
• Only few training quenches in pole turns
Holding quenches
Ramp to a pre-set current at 20 A/s and hold this current until quenchAll holding quenches initiated in the mid-plane block of coil 2 OL (B2-B3)
– Zero holding time is a regular quench at 4.5 K or 1.9
Reproducibility test, tests at different ramp rates were not done
Guram Chlachidze, FNAL-CERN Collaboration 13
Guram Chlachidze, FNAL-CERN Collaboration
Test with DC powered heaters
• Instability test - reducing Jc in the mid-plane area• Small DC current through the protection heaters
– PH cover also multi-turn pole block
• No improvement in quench performance when DC current in PH is ON
Name 14
Temperature Dependence
50 A/s ramp rate in most quenches. All quenches at intermediate temperatures were initiated in the mid-plane block of coil 2 OL (B2-B3)
Magnet showed temperature dependence of quench current, but exhibited degradation and instability
Guram Chlachidze, FNAL-CERN Collaboration 15
SSL
RRR measurement
Guram Chlachidze, FNAL-CERN Collaboration 16
Average RRR ~ 100 (lowest 80, highest 118)
Same segments in different coils have similar RRR
Coils with RRP 108/127 strandTQ coil 34: 185HQ coil 14: 80LQ coil 14 (RRP 114/127): 180
More tests: voltage spikes, quench propagation speed
Guram Chlachidze, FNAL-CERN Collaboration 17
Quench propagation speed was estimatedin ramp # 5 (Iq 9.4 kA) : ~27 m/s
Voltage Spike Detection System captures half-coil signals at a sampling rate of 100 kHz
Guram Chlachidze, FNAL-CERN Collaboration
Summary on Quench Performance
• Magnet showed limited quench performance and reached only 10.4 T or 78% of SSL at 1.9 K. Magnet did not reach quench plateau
• Most quenches at low ramp rates, as well as holding quenches and quenches at intermediate temperatures were initiated in the mid-plane block of the outer-layer coil
• Only few training quenches occurred in the high field area at the very beginning of test at 4.5 K and 1.9 K
• Plan to have a quench antenna for a better quench localization
• Quench location, ramp rate and temperature dependences and additional tests indicate magnet degradation and related instability. Possible conductor damage in the mid-plane area (presentation by F. Nobrega) could be a reason for this degradation
Name 18
Protection Heater Study• Heat transfer from the heater to the outer coil layer and then from the
outer-layer to the inner-layer coil helps to spread and absorb the magnet stored energy
• Temperature profile in the magnet after 48 ms (left) and 96 ms (right) from the PH induced quench at a nominal current of 11.8 kA
Guram Chlachidze, FNAL-CERN Collaboration 19
Experimentally verified for aPH induced quench at 8 kA with dump delayed for 120 msAfter 65 ms quench starts in the outer coil layer and after 150 ms - in the inner coil layer - More tests expected with next 11T prototypes
Protection Heater Study (cont’d)
• PH-1L and PH-2L are heaters with one and two layer Kapton insulation respectively
• PH peak power 25 W/cm2, HFU voltage decay time 25 ms• PH-2L delay is large at low currents
Guram Chlachidze, FNAL-CERN Collaboration 20
PH-1L
PH-1L
PH-2L
PH-2L
Protection Heater Study (cont’d)
Guram Chlachidze, FNAL-CERN Collaboration 21
Peak power in heaters only 25 W/cm2
Compare to 50 W/cm2 in LQ magnets
Summary on PH study
Guram Chlachidze, FNAL-CERN Collaboration 22
• Heat transfer from the PH to the outer layer coil and then to the inner layer coil was experimentally observed. This effect helps to spread and absorb magnet stored energy
• More tests will be done with next 11T prototypes
• Protection heaters with different insulation were tested both at 4.5 K and 1.9 K
• Protection heater with 2 layers of 5-mil (125 µm) Kapton insulation found less efficient than PH with 1 layer of Kapton insulation
• Heaters with 1 layer of Kapton insulation will be used in next magnet for protection and heater study
Magnetic measurements
• Warm and cold magnetic measurements were performed at VMTF with the magnet in a vertical position
• Fast rotating coil magnetic measurement system based on a digital signal processor (DSP) was used for the measurements
• 250 mm long and 25 mm diameter tangential probe, as well as printed-circuit board (PCB) based 26 mm long and 130-mm long probes were used for measurements
– 25-cm tangential probe was used only at room temperature and for few “cold” measurements at 4.5 K . This probe was rejected after signals were found noisy
Guram Chlachidze, FNAL-CERN Collaboration 23
Magnetic measurements (cont’d)
• All harmonics are presented at a reference radius of 17 mm• Data measured with the tangential probe and 130-mm PCB probe are
consistent• Sign inconsistency was found for a2 and other even-ordered harmonics
– 180 degree phase shift between the probes– Absolute values are consistent – Currently under investigation
Guram Chlachidze, FNAL-CERN Collaboration 24
sign mismatch corrected
Impact of ramp rate
Guram Chlachidze, FNAL-CERN Collaboration 25
Impact of temperature
Guram Chlachidze, FNAL-CERN Collaboration 26
• Only tangential probe data available for comparison• We see about 3% decrease in strand magnetization at 1.9 K
- 7% increase expected from the simulation (see next presentation by Mikko Karppinen)
• Need to verify with PCB probes during the next test
Impact of reset current
Guram Chlachidze, FNAL-CERN Collaboration 27
20 A/s loops
Accelerator cycle measurements
• Only tangential probe data available• Maximum current of cycle 6500 A• Reset current 100 A, ramp rate 10 A/s• Injection plateau at 760 A, dwell time 900 s• No snap-back or decay was observed• Injection plateau close to the b3 minimum
Guram Chlachidze, FNAL-CERN Collaboration 28
Stair-step measurements
• 130-mm long PCB probe data• Stair steps up and down from 1000 A to 6500 A• Dwell time at flattop 120 s
Guram Chlachidze, FNAL-CERN Collaboration 29
Summary
• The first 11T demonstrator magnet was assembled and tested at Fermilab
• Magnet showed limited quench performance and reached only 10.4 T or 78 % of SSL at 1.9 K
• Most quenches at low ramp rates, all holding quenches and quenches at intermediate temperatures initiated in the mid-plane block of the outer coil layer
• Quench location, ramp rate and temperature dependence studies indicate magnet degradation and related instability. Possible conductor damage in the mid-plane area during fabrication could cause the observed degradation
• Protection heaters (PH) with different insulation thickness were tested
Guram Chlachidze, FNAL-CERN Collaboration 30
Summary (cont’d)
• PH with 2 layers of 5-mil (125 µm) Kapton insulation found not efficient, therefore PH with 1 layer of Kapton insulation will be used in next magnet for protection and heater study
• Heat transfer from the PH to the outer layer coil and then to the inner layer coil was experimentally observed. This effect helps to spread and absorb magnet stored energy– More tests to be done
• Magnetic measurements were performed with tangential probe and PCB based probes– Need to investigate source of noise in signals from the tangential probe– Need to understand source of 180 degree phase shift in data from the tangential and
PCB probes
• Measurements at two different facilities (FNAL and CERN) would be very useful
• First demonstrator test experience will be used in test preparation and test of next 11T magnets
Guram Chlachidze, FNAL-CERN Collaboration 31
Guram Chlachidze, FNAL-CERN Collaboration
Backup Slides
Name 32
SG data: cool-down in coil 2
Guram Chlachidze, FNAL-CERN Collaboration 33
Coil 2
SG data: cool-down in coil 3
Guram Chlachidze, FNAL-CERN Collaboration 34
Coil 3
Excitation SG data: Pole gauges
Guram Chlachidze, FNAL-CERN Collaboration 35
Excitation SG data: Coil gauges
Guram Chlachidze, FNAL-CERN Collaboration 36
Excitation SG data: Bullets
Guram Chlachidze, FNAL-CERN Collaboration 37