Back to Magnetic Modelling

Model Details

November 2013

November 2013 notes.

Model 133 - 25/11/2013
Solve Time = 50 hours. (hep 21)
Model Element Type = Quadratic.
Surface Element Type = Quadratic.
Model Configuration: Step IV
Magnet Configuration: Solenoid (centralised)
Momentum: 240 MeV/c
PRY: Yes

As Model 132 but with the steel floor-plates on the SSW set to Air. This is run as a full model including the SSB.

Model 132 - 23/11/2013
Solve Time = 41 hours. (hep 21)
Model Element Type = Quadratic.
Surface Element Type = Quadratic.
Model Configuration: Step IV
Magnet Configuration: Solenoid (centralised)
Momentum: 240 MeV/c
PRY: Yes

As model 131 but this also uses the recent changes to the magnet files. (Less steel mass in the core of the quads.) The exact mass of the quads in the model has not been calculated but this change should give closer agreement between the amount of steel mass in the quads and in the model.

PRY Model 116 - 22/11/2013
Solve Time = ~xx. (hep 39)
Model Element Type = Quadratic.
Surface Element Type = Quadratic.
Model Configuration: Step IV
Magnet Configuration: Solenoid (centralised)
Momentum: 240 MeV/c
PRY: Yes
Symmetry: Quarter Model
This model has used 100 mm thick Virostek Plates and 100 mm thick End Plates. BH curve reduced by 20%

PRY Model 115 - 21/11/2013
Solve Time = ~8 hours (hep 39)
Model Element Type = Quadratic.
Surface Element Type = Quadratic.
Model Configuration: Step IV
Magnet Configuration: Solenoid (centralised)
Momentum: 240 MeV/c
PRY: Yes
Symmetry: Quarter Model
This model has used 100 mm thick Virostek Plates and 100 mm thick End Plates. BH curve reduced by 10%

PRY Model 124 - 25/11/2013
Solve Time = ~8 hours. (hep 39)
Model Element Type = Quadratic.
Surface Element Type = Quadratic.
Model Configuration: Step IV
Magnet Configuration: Solenoid (centralised)
Momentum: 240 MeV/c
PRY: Yes
Symmetry: Quarter Model
This model has used 90mm thick Virostek Plates and 90mm thick End Plates. Virostek Plates run as Air.

PRY Model 123 - 25/11/2013
Solve Time = ~8 hours. (hep 39)
Model Element Type = Quadratic.
Surface Element Type = Quadratic.
Model Configuration: Step IV
Magnet Configuration: Solenoid (centralised)
Momentum: 240 MeV/c
PRY: Yes
Symmetry: Quarter Model
This model has used 90mm thick Virostek Plates and 90mm thick End Plates. BH curve reduced by 20%

PRY Model 122 - 21/11/2013
Solve Time = ~8 hours. (hep 39)
Model Element Type = Quadratic.
Surface Element Type = Quadratic.
Model Configuration: Step IV
Magnet Configuration: Solenoid (centralised)
Momentum: 240 MeV/c
PRY: Yes
Symmetry: Quarter Model
This model has used 90mm thick Virostek Plates and 90mm thick End Plates. BH curve reduced by 10%

Model 131 - 19/11/2013
Solve Time = 40 hours. (hep 21)
Model Element Type = Quadratic.
Surface Element Type = Quadratic.
Model Configuration: Step IV
Magnet Configuration: Solenoid (centralised)
Momentum: 240 MeV/c
PRY: Yes

Full Hall Model with the NEW PRY geometry for comparison with the older models. This model reverts to the old meshing resolution that was used before I started the PRY investigation. The meshing will be similar to what was used for the 90 series results.

PRY Model 120 - 13/11/2013
Solve Time = ~5 hours. (hep 39)
Model Element Type = Quadratic.
Surface Element Type = Quadratic.
Model Configuration: Step IV
Magnet Configuration: Solenoid (centralised)
Momentum: 240 MeV/c
PRY: Yes
Symmetry: Quarter Model
This model has used 90mm thick Virostek Plates and 90mm thick End Plates

PRY Model 121 - 13/11/2013
Solve Time = ~5 hours. (hep 39)
Model Element Type = Quadratic.
Surface Element Type = Quadratic.
Model Configuration: Step IV
Magnet Configuration: Flip (centralised)
Momentum: 240 MeV/c
PRY: Yes
Symmetry: Quarter Model
This model has used 90mm thick Virostek Plates and 90mm thick End Plates

Model 130 - 14/11/2013
Solve Time = 100 hours. (hep 21)
Model Element Type = Quadratic.
Surface Element Type = Quadratic.
Model Configuration: Step IV
Magnet Configuration: Solenoid (centralised)
Momentum: 240 MeV/c
PRY: Yes

Full Hall Model with the NEW PRY geometry for comparison with the older models.



Back to Magnetic Modelling