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Superconducting IR Magnets CHEN, Fusan May 11, 2007.

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Presentation on theme: "Superconducting IR Magnets CHEN, Fusan May 11, 2007."— Presentation transcript:

1 Superconducting IR Magnets CHEN, Fusan May 11, 2007

2 2/18 Outline Progress of the superconducting magnets and relevant systems. –Power supplies and QPS were testified to be workable. –Electronic test was done to the system. –The magnets were cooled down to superconducting temperature. –The whole system was assembled together. The first commissioning of the magnets. –All coils were powered to 10~20% operating current. –Quench protection system was proved to be reliable. –Many problems were revealed with the valve boxes. Schedule of the second commissioning and field measurement. –The valve boxes are rebuilt and the whole system is reassembled. –The second commissioning is in process. –Magnetic field measurement will be started after commissioning.

3 3/18 Progress of the PS and QPS Power supplies met the requirements. –After months of tuning work, all power supplies were workable. Power supply control system fulfilled the required functions. Quench protection assembly reacted fast and correctly. –Reaction of the system was tested with dummy load. Quench detection system was assembled. –Both hardware and software were ready.

4 4/18 Progress of the SC magnets Electronic test before cooling. –The environment was not ideal. Temperature: 25~28ºC Humidity: 95%~100% –Problems of the valve box. The insulator failed in the hipot test at ~220VDC when the humidity was higher than 95%. The temperature sensors were electrically connected to the current leads. The hipot performance was concerned with the vacuum of the valve box.

5 5/18 Progress of the SC magnets Monitoring the magnets during cooling. –To monitor the transformation from normal to superconducting of the coils, we powered the coils with low current (40mA) and monitored the voltage drops across the coils.

6 6/18 Progress of the SC magnets Electronic test after cool-down. –Measured the resistance of gas cooled leads. –Hipot tests were repeated with all coils. The grounding resistances of all coils were far less than requirement (20Mohm).

7 7/18 The first commissioning More study on the hipot problem with BNL experts, George Ganetis and Wing Louie. –The grounding resistance of coils ranges from 2 to 8000 ohms. The resistance decreases when the valve box gets cold. –The resistance is non-linear and does not start to have current flowing until the voltage is greater then 1 Volt. –In all circuits the short is at or near the gas cooled lead. But the exact location of the short can not be found. Possible causes of hipot failure. –All the electrical insulators used in the current leads have a creep path that is too small. –The G-10 insulators used on the top of the valve boxes can collect water.

8 8/18 Result of grounding resistance test Valve Box CircuitAC Ground Resistance DC Ground Resistance Shorts Locations Current Tested Comments SCQ- A AS50335 AS1-IN, AS2- 3 AS1-OUT 300Pre-cooled Leads, Bus Quench High Ground Current SCQ130363 SCQ-IN SCQ-OUT 250Pre-cooled Leads, Bus Quench SCB563633 SCB-IN SCB-OUT 10Low Current Shut-off SKQ301514 SKQ-OUT 6.6Low Current Shut-off VDC244490 VDC-IN VDC-OUT 5.1Low Current Shut-off SCQ- B AS126NA AS1-IN, AS1- 2 AS1-OUT 250SC bus went resistive SCQ18008000 SCQ-IN SCQ-OUT 150SC bus went resistive SCB533625SCB-IN40High Current Shut-off SKQ537NA 40High Current Shut-off VDC710NA 40High Current Shut-off * This table quotes from George’s report

9 9/18 The first commissioning New problems of valve boxes –The current leads could not be cooled down. The cold ends reached 20K with the flux controllers at max. Reached 6K with the bypass valves at max. AS, SCQ and SCB coils could not be powered more than 20% operating current, otherwise quenched. –The sensors could not indicate the temperature of the most critical points. –The inlet and outlet leads could not be cooled equally because they used common controller

10 10/18 The first commissioning Some typical data and the diagnosis The signals monitored during the commissioning

11 11/18 Data of SCQ Inlet Vt 146A 162A 58A Outlet Vt Inlet Vs Outlet Vs The SC bus quenches, but the normal region does not expand The SC bus cannot recover after opening the bypass valve The SC bus recoveres after decreasing the current with the bypass valve opened Keeping the bypass valve open, start the second ramping cycle The SC bus does not quench at 162A Vt almost equals to Vc and Vs equals to zero for both inlet and outlet With the flow controller max, start the first ramping cycle

12 12/18 Data of AS 297A 9A 49A 98A 148A 197A 245A Inlet Vt Outlet Vt Inlet Vs Outlet Vs The Vt difference between the inlet and outlet shows the imbalance of the helium flow The inlet SC bus quench causes the jump of voltage signals while current increases to ~260A The normal region does not expand at 297A It is important to analyze why the outlet does not quench even the Vt higher

13 13/18 146A 165A 175A 185A 195A 205A The normal regions do not expand under 200A The normal regions expand rapidly after 200A and the quench protection system is triggered. Inlet Vt Outlet Vt Learn more from SCQ

14 14/18 The second commissioning The valve boxes are rebuilt and installed. The quench detection circuit is set up and tested. The warm temperature electronic test is performed. –The insulation of some temperature sensors on the current leads is not satisfying. The power supplies are improved. The ps control system is updated. The interlock between systems is linked. The cryogenic pipes are connected.  Now, the temperature reaches 60K.

15 15/18 The second commissioning Next steps: (schedule is tight.) –Restore the quench protection software. (1 day) –Power the coils to 10~20% current. (5~6 days) Tuning the parameters of quench detection system. Check the ps and ps control system. Check the quench protection assembly. Configure the parameters of leads flux controller. –Power the coils to 50% current. (2 days) –Power the coils to 110% current. (2 days) Tuning the power supplies. Quench training if necessary. –The same powering procedure for the sync-rad mode. (4 days)

16 16/18 Schedule of field measurement Joint field measurement. (37 days) –Instruments alignment, assembly, de-assembly, replacement (5 days). –Longitudinal field measurement with salamander. Solenoid magnet off (1 day) & on (3 days). –Excitation curve measurement with stretch-line. Solenoid magnet off (7 days) & on (7 days). –Rotating coil measurement (long & short coil). Solenoid magnet off (4 days) & on (10 days).

17 17/18 Schedule of field measurement Individual field measurement. (33 days) –Instruments alignment, assembly, de-assembly, replacement (5 days). –Excitation curve measurement with stretch-line (8 days for one magnet, totally 16 days). –Rotating coil measurement (12 days). Long coil and short coil are used at the same time with different magnet. –Longitudinal field measurement with salamander (2 days).

18 18/18 Additional topic The force and torque of SC magnet coils. The special type magnets in IR work well. –Septum bending magnet: ISPB. –Dual aperture quadrupole: Q1a, Q1b. –Narrow quadrupole: Q2, Q3. Fx [kN]Fy [kN]Fz [kN] Mx [kN · m]My [kN · m] AS10.5 HDC (Iop=50A) ± 3.9 z=770mm z=1170mm 1.48 VDC (Iop=24A) ± 3.9 z=1020mm z=1400mm 1.49


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