This sections details the high current magnets and power supplies in the Hall B experimental area. Figure 1 shows a schematic of the large magnets and their supplies, power supply specifications are given in Table 1, and magnet specifications are given in Table 2. Several supplies serve dual uses depending on whether the experiment is performing electron scattering or real photon experiments. There are many safety issues for magnets and their power supplies that are addressed in the following sections. The main safety issue is personnel safety, the magnets, supplies and bus lines must be safe enough so that workers can work in the vicinity of the magnets and supplies without any risk of electrical exposure. Equipment protection is also a concern since the magnets and power supply represent a substantial tax payer investment. The equipment is actively protected by hardware interlocks that prevent the power supplies from damaging themselves or the magnets they supply.
Figure 1. Schematic of the large magnets and their power supplies in Hall B. The order shown is the order in which the magnets reside on the beamline, with the beam running left to right. The solid lines between magnets and power supplies represent 535 high current cable, dashed lines represent water cooled bus lines either thick-walled copper or thick walled aluminum pipe.
magnet | power supply | ||
---|---|---|---|
The magnets in the experimental hall are typically energized by remote control to simplify operation when there is beam in the hall. During major down times the magnets are powered down for personal safety reasons as well as to reduce electrical power con sumption. During short interruptions of beam delivery, with hall personnel entering the hall in the controlled access mode, the magnets are typically left energized. The main reason is that the time constants of large size magnets are long (of the order o f hours), and frequent ramping or cycling will lead to inefficient operation. Also, every ramp of a large superconducting magnet involves some risk of permanent damage to the magnet coil.
Personnel working in the proximity of energized magnets are exposed to the following hazards:
Two different modes of operation need to be distinguished: (1) routine operation involving work in the vicinity of the magnets, but not in close proximity to the electrical connections, and not involving any work that could result in purposely getting in to contact with the coils or the leads, and (2) non-routine operation involving work on or near the exposed current conductors or connections (typically requiring removal of the shield) or any work that could result in contact, intentional or otherwise, w ith the coils or the leads.
DANGER
THIS GUARD MAY ONLY
BE REMOVED BY
AUTHORIZED PERSONNEL
UTILIZING JLAB
LOCKOUT - TAGOUT
PROCEDURES
DANGER SAFETY HAZARDS MAY EXIST FROM THE MECHANICAL FORCES EXERTED BY THE MAGNETIC FIELDS UPON MEDICAL IMPLANTS NO PACEMAKERS
The following measures shall be taken during non-routine operation to mitigate the hazards described in Section 3.2.1 :
The two blue dipoles downstream of the tagger magnet are used during real photon experiments. These magnets remove secondary charged particles originating at the collimator from the photon beam. Magnetic field stability is not an issue with these magnets. Each dipole achieves maximum field at ~950A with a resulting voltage drop of 38V.
The sweep magnets are powered by an old accelerator arc power supply. The supply is manufactured by Dynafysik and is located on the ground floor of the hall. The supply is light blue in color and is between the tagger supply and the Dyna-A (mini-torus/pai r-spectrometer supply) supply. The two sweep dipoles are connected in series to the power supply. The power supply when connected to the sweep magnets is current limited at 220Amps and this is the operation point.
At present the supply does not have remote control or monitoring, and is run in local mode. The supply should be set to 100% full current from the front panel and current and voltage are read on the front panel.
Møller Quadrupole magnets are an integral part of the Møller polarimeter. Their function is to transport the two electrons to the detectors downstream of the magnets. Since the polarized electron beam can be of different energies the magnets are to be operated at different currents. In fact the first quadrupole must have its polarity changed depending on the beam energy. For this reason the first quadrupole is connected to the Dyna-B supply and Dyna-switch. In order for these supplies to ene rgize the quadrupoles the individual pole coils were reconfigured to be parallel instead of in series. Each pole is still in series with the other poles, thereby each pole still has the same current flowing through it. The bus lines from the power supply or switch are water cooled aluminum bus.
Møller Quadrupole operation checklist
The following checklist must be completed before energizing the Møller Quadrupole magnets to protect personnel and the equipment.
The Mini-Toroid magnet consists of six resistive water cooled coils. The magnetic field produced by the Mini-Toroid protects the drift chamber from low energy Møller electrons originating from the target. The magnet was designed for a maximum curre nt slightly more then 8000 Amps, however, the Dyna-A power supply becomes voltage limited at about 7900 Amps. The Mini-Torus is used during electron scattering experiments, and is removed for real photon and polarized target experiments.
The following items must be performed during installation and operation of the Mini-Torus.
The pair spectrometer magnet is located in the downstream tunnel behind the first shield wall. This magnet is only used during real photon experiments and is powered by the Dyna-A power supply. When operating this supply the following items need to be ver ified first:
The tagger magnet is a large C magnet which is installed in the upstream alcove in Hall B. Its purpose is to deflect the full-energy electron beam through an angle of 30 degrees into the tagger beam dump, while deflecting lower-energy electrons into the d etectors of the tagging system. The magnet is suspended from a steel support structure called the gantry.
The tagger power supply is located on the floor in Hall B, next to the wall on the north side of the alcove. Power is supplied to the magnet by eight 535 mcm insulated copper cables, four supply and four return. The power cables run in grounded cable tray s along the wall of the hall. The magnet is grounded by a bare 500 mcm copper cable which runs in the same cable trays. The ground cable is connected to the grounding plate in the hall floor, adjacent to the power supply. Additionally, the gantry steel is grounded directly to the magnet steel; ground does not rely on the support connections between the magnet and the gantry. Strain relief is provided for all cables.
The power supply delivers up to 2400 Amps DC, at approximately 70 Volts. At full 2400 Amp excitation, the magnet can deflect a 6.1 GeV electron beam into the tagger beam dump.
The power supply doors are interlocked. Additional interlocks are from a flow meter on the cooling water return for the magnet (not currently connected), and on a series of `Klixon' temperature gauges in contact with the magnet coils. The LCW system is u sed to cool both the power supply and the magnet. The power supply has an internal flow meter for its cooling water that is interlocked as well.
Access to the high-field region is very restricted by the stainless steel vacuum extension to the magnet gap. Furthermore, the field is less than 100 gauss at distances greater than 1 foot from the magnet, and less than 5 gauss at distances greater than 1 0 feet from the magnet.
The power supply can be run locally using front-panel controls, or remotely under EPICS control. During run conditions, the magnet is controlled via EPICS from MCC.
DANGER
Strong Magnetic Fields - No Pacemakers
No Access Except Authorized Personnel
will be posted at all access points, including the entrance to the alcove from the tunnel.
The EPICS control program shall ensure that, whenever beam is present in the Hall B channel, the current in the power supply is within 5 percent of the nominal calculated value. The nominal value is calculated from the beam energy by the EPICS program. Fo r reference, some of the nominal values are listed in Table 3.
The magnet will be used for its designed purpose during all photon beam runs in Hall B, and may also be used for beam steering and tuneup during electron beam runs. During all beam runs, the power supply is controlled exclusively from MCC via EPICS.
During short controlled accesses to the hall the power supply may remain energized. During longer controlled accesses (longer than 4 hours) or when the Hall is in a state of restricted access, the power supply shall be turned off, or the current set to ze ro, unless an authorized person is present in the magnet area.
The power supply may be run under local control by authorized personnel for the purpose of making magnetic field measurements, testing the interlock systems, or degaussing the magnet, under local control. The power supply shall be energized only while aut horized personnel are present in the magnet area.
This document will give the operator a basic description of the KNUTH computer, and the Oxford Annunciator located in the Hall B Counting House. It will also provide operating and troubleshooting procedures that the operator will need to bring the magnet up to a desired field (current setting). Details of operation can be found in Appendix A.
The operator will use the KNUTH computer and the Oxford Annunciator to interface with the magnet from the Hall B Counting House.
The KNUTH computer has two monitors for operator interface. The top monitor is configured with the Magnet Power Supply screen and the bottom monitor with the Service Module Mimic screen. The Magnet Power Supply screen is used to adjust magnet current and observe key error indicators. The Service Module Mimic screen shows the status of the cryogen systems valves, pressures and levels.
The Oxford Annunciator provides a means of alerting the operator to problems that he might not have observed from KNUTH due to operating restraints. The panel will give a audible alarm and display a red light for the following conditions: generator engine fault, pneumatic fault, watchdog timer fault, and power supply setpoint fault (MAG PWR). A yellow light (emergency power) without any audible alarm is given when the generator is providing power. The alarm given when the magnet is not at setpoint is the best indication that a fault has occurred because any fault on the magnet will cause the current to ramp down.
To ramp the current up or down the operator performs the following steps on the Magnet Power Supply screen:
If the screens on either monitor lock-up, perform the following steps:
All personnel must do a walk through of this procedure with a fully trained person before using it. This procedure is meant for reference only. It is assumed that all individuals using this procedure fully understand electrical safety, lock & tag out procedures, and a fundamental knowledge of magnet operations.
To reverse the polarity of the Oxford Magnet Power Supply perform the following steps:
The CLAS uses several low voltage, high current power supplies, specified by VME, VXI, FASTBUS standards and CEBAF-designed ADB crates. The operation of all these is in accordance with the new "High Current Power Supply Systems" Section of the EH&S Manual 6240. Special precautions are taken to protect exposed leads from accidental contact. The crates protects from over-current condition by means such as a fuse or circuit breaker. Each type of powered crate in CLAS has been specified to include overtemperature protection circuits which will remove crate power in the case of an overtemperature condition.