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C4CM
Section Five


Singularities
___

23. Poincare Sections
24. Linear Algebra
25. Optimal Controls
26. Potential Theory
27. Envelope Curve
28. Vibrations
29. Time
30. Uncertainty
31. Quantum
Chemistry
32. Fractal Theory
TAB 24
Linear Algebra Rules Logo
LINEAR ALGEBRA

The equations of motion for the Two Body Problem can be represented as the modal matrix

then

in two dimensions. Since is a conservative field, then

which actually does not work because is conservative only in the plane of the orbit. To see this create a hodograph with two separate circles for the bi-elliptic Earth to Mars trajectory. If were a conservative force then the intersection of the two circles would coincide, but it does not. To see why, consider the Cayley Hamilton theory, which says that a matrix satisfies its own characteristic equation. There is a contradiction that the f and g equations solve the Two Body Problem, but not the f and g matrix. That is, the fact that a matrix satisfies it's own differential equation (the C H Theory) means the matrix is an envelope curve.

Note that the transformation to the symmetric plane is linear. This implies other systems can be approximated by a matrix (e.g. in orbital estimation theory) which is of a linear operation of independent vectors ~ that being the case, this system can be studied using linear programming techniques.


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© 2004 WH Clark