X 0 1 2 3 4 5 6 7 8 |
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 ALGEBRAThe equations of motion for the Two Body Problem can be represented as the modal matrix
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then
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in two dimensions. Since
is a conservative field, then
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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.