LBHB650 Magnets PIP2
Vikas Teotia, Elina Mishra, Sanjay Malhotra Bhabha Atomic Research Centre
LBHB650 Magnets PIP2 Vikas Teotia, Elina Mishra, Sanjay Malhotra - - PowerPoint PPT Presentation
LBHB650 Magnets PIP2 Vikas Teotia, Elina Mishra, Sanjay Malhotra Bhabha Atomic Research Centre Typical downstream Quadrupole Magnet View from high energy end View from low energy end Top View Side view Feedback from FNAL For the dipole
LBHB650 Magnets PIP2
Vikas Teotia, Elina Mishra, Sanjay Malhotra Bhabha Atomic Research Centre
Typical downstream Quadrupole Magnet
View from high energy end
View from low energy end
Side view Top View
Feedback from FNAL
The peak field in the flux return area is relatively large 1.5-1.59 T (See Fig. 20), which is less than the expected 2.1 T saturation of the material. The review panel suggests increasing the dimension of the yoke cross section (either width or height) to reduce the flux to a magnitude less than 1.3 T. This dimensional increase would offset any potential variability of the steel material. If increasing in the beamline direction, then dimensional extents of the yoke may approach outer coil dimension, but maintain the 60 mm dimension near the beam pipe. BARC will consider making these changes. 1.5 T should be Ok as maximum limit
The dipole has large harmonics (Fig. 19) which may be adjusted with pole profile tilt or pole end shims. The reviewers suggest incorporating this adjustment mechanism to minimize the harmonic effect with the quadrupole. The harmonics meet the TRS requirements.
The tolerances of the pole tip dimensions and curvature profile are not specified to corroborate field map
Only 33 windings of the conductor are shown in Fig. 5. Specify where the potential 34th winding would be placed if needed to achieve field magnitude. Along the same lines, 43 windings are shown for the individual quadrant in Fig. 40 suggesting ambiguity about the final conductor winding count. Ambiguity is removed
Similar saturation is occurring at the sharp corners of the pole (see Fig. 12). Including a radius to keep the maximum field below 1.3 T is necessary.
Feedback from FNAL contd …
unclear and require specification:
The positive/negative conductor spacing should have a minimum of 12.5 mm of separation in open air to prevent arc discharge. Ensured
Conductive routing jumpers shown in Fig 41 appear to be in free space and not adequately attached to the steel pole material. Implemented
Zinc plated steel bolts should be specified for good conductivity of copper- to-copper contacts. Implemented
The ground clearance of the negative conductor lead in Fig 41 should be increased to prevent damage when the assembled quadrupole is placed on a non-level work surface. Implemented
No terminal block for dipole electrical connection is shown in the models or 2D drawings. Implemented
Feedback from FNAL contd …
Conductor-to-LCW
conductor windings in parallel for uniform cooling. Interface features that should be specified prior to production:
should be avoided to prevent corrosion. There is no aluminum to copper connections.
is provided. Details of the electrically insulating connection to the manifold with individual in situ removal/replacement capability is needed. Included
flats will be available for LCW building connection (as indicated in text), the feature is not shown in the models provided. Implemented
Feedback from FNAL contd …
indicate that mechanisms will exist to meet the needs of handling and positioning. However, the following features require specific callout:
connections will be avoided to prevent galling/cold welding that will hinder disassembly Confirmed
horizontal or vertical direction) as well as separate top and bottom halves of the quadrupole
eye bolts for lifting. Drawings will include them in more details.
either bus bars or pin alignments are required. Implemented
that are non-ferromagnetic OK
provided as a reference. Needs discussion