next up previous
Next: References Up: Review of the astrophysical Previous: Basic N-body Equations

Jacobian of an N-M fixed-particle system

Let the function computing the derivative of tex2html_wrap_inline4367 be tex2html_wrap_inline4369 . f has no dependence on time. The Jacobian of f, tex2html_wrap_inline4375 is

displaymath4377

where tex2html_wrap_inline4379 is the 3N-square zero matrix, and I is the 3N identity matrix. If all particles move, then the entire Jacobian is 6N square. If only M particles move, then there is no meaning to the entries in the Jacobian owned by particles that do not move, and so the Jacobian is only 6M square. The only difficult part of this Jacobian is tex2html_wrap_inline4393 , which is a 3N-square matrix, and tex2html_wrap_inline4397 where tex2html_wrap_inline4399 is the acceleration of particle i, given by equation A.1, and tex2html_wrap_inline4403 is its position in 3-space. Thus,

displaymath4405

Finally, if we let tex2html_wrap_inline4407 represent one of tex2html_wrap_inline4409 , it can be shown that

displaymath4411

where, for example, tex2html_wrap_inline4413 is the tex2html_wrap_inline3367 component of tex2html_wrap_inline4317 . If softening is employed, substitute tex2html_wrap_inline4419 for tex2html_wrap_inline4421 and tex2html_wrap_inline4423 for tex2html_wrap_inline4425 .


next up previous
Next: References Up: Review of the astrophysical Previous: Basic N-body Equations

Wayne Hayes
Sun Dec 29 23:43:59 EST 1996

Access count (updated once a day) since 1 Jan 1997: 10133