MQXFSM1 results Guram Chlachidze Stoyan Stoynev 10 June 2015LARP meeting.

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Presentation transcript:

MQXFSM1 results Guram Chlachidze Stoyan Stoynev 10 June 2015LARP meeting

Status The magnet was cooled down on May 3 RRR measurements and warm up completed on June 1 st Number of testing days: 15 Highlights – 30+ training quenches at 1.9 K, maximum current A (91.3% of SSL at 1.9 K) – Reached 82% of SSL in 5 quenches but hit a limit (~90% of SSL) after 18 quenches 2 May 3

Quench detection instrumentation 3 Voltage taps and quench antennas positions IL OL QA:

Quench location 4 Few days difference All the a3_a4 and a4_a5 (after hitting the plateau) points are very similar with hard to distinguish time difference between a3_a4 and a4_a5 (that is – it is likely a single location quenching all the time); quench antennas support this as well – always LE ones active retraining (ramp rate studies; quench protection studies) Quench antennas: 1 (LE) to 5 (RE)

Training in terms of SSL fraction 5 In addition to the quenches shown there were also quenches related to other studies (like ramp rate dependence) and also few re-training ones. No improvement was observed. HQM04 is another magnet we can tentatively compare to (it is a quadrupole mirror)

Temperature dependence 6 In terms of SSL fraction of the quench current there are no large variation with temperature for MQXFSM1.

Ramp rate dependence 7 The magnet did not quench at ramping down (from 18 kA) at 300 A/s Quench current

RRR 8 RRR values of 150 are typically obtained, no outliers. ILOL

Holding current time 9 The magnet was at 16.5 kA flat top for two hours at 4.5 K The magnet was at 17.8 kA flat top for two hours at 1.9 K However at 1.9 K it quenched during ramp down at 20 A/s (I q = 17.6 A)

Inductance measurement 10 The measured inductance at 300 K and 20 Hz is 5.2 mH 4.5 K 200 A/s 1.9 K Measurements at 200 vs 300 A/s (4.5 K) are consistent (despite some technical issues)

11 Splice resistance IL (A) OL (B)

12 Spike analysis Spikes depend on the length and quality of cable, there is typically a peak (magnitude, frequency of occurrence) at relatively low current (long mirror) (quadrupole)

Quench protection studies 13

14 Two inner layer PH strips, as well as 2 pole and 2 mid-plane outer layer strips were connected in series internally, during the magnet assembly. The 2 OL heaters are connected in parallel or tested/fired individually IL OL IL – copper cladded SS OL (LQ style)

15 Minimum power density PH power density: IL (OL) Minimum heater power density inducing a quench Time const  ≈ 40 ms

16 Heater delay vs current Reproducibility test – there are three repeated measurements (points) here Reproducibility test – there are three repeated measurements (points) here These are the time differences between heater firing and the start of quench development For OL pole and middle plane tests  ≈ 94 ms, for IL -  ≈ 40 ms

17 Heater delay vs peak power density For OL pole and middle plane tests  ≈ 94 ms, for IL -  ≈ 40 ms

18 Heater delay vs decay time constant The time constant was changed by changing the HFUs capacitance – 19.2/14.4/9.6 mF The power density was ~ W/cm 2 (same for a given set)

19 Quench propagation schematics t HFU1 t’ q t 0 (≡0) t’’ q t dump time ILOL Magnet current Quench development (for a given segment) t HFU1 : heater fired t q : start quench development t 0 (≡0) : quench detected t dump : dump resistors engaged t ata : layer-to-layer propagation time FOR ILLUSTRATIVE PURPOSES Example configuration: - IL heater to unit HFU1 - OL heater off-line - Dump delay of 1000 ms t ata

20 Quench propagation Quench propagation time between layers { t=0 < t q (layer1; heater induced) < t q (layer2; propagated) } Dump delay is large (1000 ms).

21 Quench integral t = 0 ms here refers to the manual trip initiation time t q is the start of (heater induced) quench development

Summary 22 Quench training of MQXFSM1 reached 90 % of SSL Behavior remains similar at higher temperature Very good performance vs ramp rate (eddy current losses well controlled by SS cored cable) Holding current tests – stable performance Good RRR and splice resistances Consistent inductance measurements Rich quench protection related data (reproducibility checked)