How to solve the Sepatrix Seperation in Mathematics?
Answers
Answer:
In mathematics, a separatrix is the boundary separating two modes of behaviour in a differential equation. Accounting for about six effects in differential equations can be tedious but needs to be done for interfaces and then you have a model for that part of the system model
Step-by-step explanation:
motion of a simple pendulum:
{\displaystyle {d^{2}\theta \over dt^{2}}+{g \over \ell }\sin \theta =0.}{\displaystyle {d^{2}\theta \over dt^{2}}+{g \over \ell }\sin \theta =0.}
where {\displaystyle \ell }\ell denotes the length of the pendulum, {\displaystyle g}g the gravitational acceleration and {\displaystyle \theta }\theta the angle between the pendulum and vertically downwards. In this system there is a conserved quantity H (the Hamiltonian), which is given by
{\displaystyle H={\frac {{\dot {\theta }}^{2}}{2}}-{\frac {g}{\ell }}\cos \theta .}{\displaystyle H={\frac {{\dot {\theta }}^{2}}{2}}-{\frac {g}{\ell }}\cos \theta .}
With this defined, one can plot a curve of constant H in the phase space of system. The phase space is a graph with {\displaystyle \theta }\theta along the horizontal axis and {\displaystyle {\dot {\theta }}}{\dot {\theta }} on the vertical axis – see the thumbnail to the right. The type of resulting curve depends upon the value of H.
The phase space for the simple pendulum
If {\displaystyle H<-{\frac {g}{\ell }}}{\displaystyle H<-{\frac {g}{\ell }}} then no curve exists (because {\displaystyle {\dot {\theta }}}{\dot {\theta }} must be imaginary).
If {\displaystyle -{\frac {g}{\ell }}<H<{\frac {g}{\ell }}}{\displaystyle -{\frac {g}{\ell }}<H<{\frac {g}{\ell }}} then the curve will be a simple closed curve which is nearly circular for small H and becomes "eye" shaped when H approaches the upper bound. These curves correspond to the pendulum swinging periodically from side to side.
If {\displaystyle {\frac {g}{\ell }}<H}{\displaystyle {\frac {g}{\ell }}<H} then the curve is open, and this corresponds to the pendulum forever swinging through complete circles.
In this system the separatrix is the curve that corresponds to {\displaystyle H={\frac {g}{\ell }}}{\displaystyle H={\frac {g}{\ell }}}. It separates — hence the name — the phase space into two distinct areas, each with a distinct type of motion. The region inside the separatrix has all those phase space curves which correspond to the pendulum oscillating back and forth, whereas the region outside the separatrix has all the phase space curves which correspond to the pendulum continuously turning through vertical planar circles.
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