SLYU067 December 2023 DRV5011 , DRV5012 , DRV5013 , DRV5013-Q1 , DRV5015 , DRV5015-Q1 , DRV5021 , DRV5021-Q1 , DRV5023 , DRV5023-Q1 , DRV5032 , DRV5033 , DRV5033-Q1 , DRV5053 , DRV5053-Q1 , DRV5055 , DRV5055-Q1 , DRV5056 , DRV5056-Q1 , DRV5057 , DRV5057-Q1 , TMAG3001 , TMAG5110 , TMAG5110-Q1 , TMAG5111 , TMAG5111-Q1 , TMAG5115 , TMAG5123 , TMAG5123-Q1 , TMAG5124 , TMAG5124-Q1 , TMAG5131-Q1 , TMAG5170 , TMAG5170-Q1 , TMAG5170D-Q1 , TMAG5173-Q1 , TMAG5231 , TMAG5253 , TMAG5273 , TMAG6180-Q1 , TMAG6181-Q1 , TMCS1107 , TMCS1108
The last requirement is to define the magnet travel. All motion types begin by defining the starting location of the magnet. Coordinates (X,Y,Z) of the magnet are defined at the center of the magnet. Re-orienting the magnet by performing rotations in XYZ order are possible at the start position. This orientation allows for any possible start orientation. The rotation steps are applied around the magnet center and not the origin.
The various fields for each type of motion are shown in subsections Section 4.1.4 through Section 4.1.7.