Such a system is used for chambers constructed from wires and planes unless one of the following conditions is met:
Polar coordinates are internally dealt with by the conformal mapping:
(x,y) = exp(\ρ,\φ) z = \ζthanks to which the potential functions and drift-line integration procedures for Cartesian coordinates can be used. Most of the commands accept polar coordinates for input and translate the the output to polar coordinates. Procedures as a rule don't do this. A set of procedures is therefore provided for these transformations: CARTESIAN_TO_POLAR, CARTESIAN_TO_INTERNAL, INTERNAL_TO_CARTESIAN, INTERNAL_TO_POLAR, POLAR_TO_CARTESIAN and POLAR_TO_INTERNAL.
The tube coordinates are special in the sense that the wire locations are listed in Cartesian coordinates, while the tube is an object with a polar shape.
Garfield internally uses Cartesian coordinates for cells of this type. Potentials in round tubes are computed using the conformal mapping:
z - z0 z = ----------- 1 - z0bar zwhich maps z0 to 0 and which maps the unit circle onto itself.
Potentials in polygonal tubes are computed by mapping the centre of the tube to a round tube, while the edges are mapped with a local Schwarz-Christoffel expansion.
Formatted on 21/01/18 at 16:55.