Edited by Valentin Fadeev, Sunday, 18 Sept 2011, 23:24
The first (unguided) steps in dynamical systems. The task is to prove that the phase paths of the following system:
are isochronous spirals, that is, every circuit of every path around the origin takes the same time. It looks a bit scary, because it involves not one but two "bad" functions. Thle easiest way to deal with these is to break the picture in quadrants and examine each part separately.
First quadrant: ,
Second quadrant: ,
Third quadrant: , , the same solution as for the first quadrant.
Fourth quadrant: , , the same solution as for the second quadrant.
Introduce polar coordinates.
I,III:
II,IV:
Let be a closed circuit enclosing the origin. The elapsed time is given by the following formula:
As the functions are periodic, it is sufficient to give proof for one loop. Due to the axial symmetry of the trajectory we can calculate transit time only in the first and the second quadrants and then double the result. If we integrate counter-clockwise, then we would follow the trajectory in a reversed direction. Therefore, we need to put the negative signe before the integrals.(oh, how long it took me to realize this..) In polar coordinates this expression has the following form:
Differentiating the expression for by we obtain:
A-ha, that's where we get the independence of the final result on the path choice: the arbitrary constant gets cancelled out.
Let , then ,
I made some false starts on getting a negative answer which is impossible for a strictly positive integrand. Still not quite sure where I went wrong. Normally these things happen when a singularity sneaks in inside the domain of integration after variable change. Anyway, I decided to cheat and shift the scale.
Descending to chaos
The first (unguided) steps in dynamical systems. The task is to prove that the phase paths of the following system:
are isochronous spirals, that is, every circuit of every path around the origin takes the same time. It looks a bit scary, because it involves not one but two "bad" functions. Thle easiest way to deal with these is to break the picture in quadrants and examine each part separately.
First quadrant: ,
Second quadrant: ,
Third quadrant: , , the same solution as for the
first quadrant.
Fourth quadrant: , , the same solution as for the
second quadrant.
Introduce polar coordinates.
I,III:
II,IV:
Let be a closed circuit enclosing the origin. The elapsed time
is given by the following formula:
As the functions are periodic, it is sufficient to give proof for one loop. Due to the axial symmetry of the trajectory we can calculate transit time only in the first and the second quadrants and then double the result. If we integrate counter-clockwise, then we would follow the trajectory in a reversed direction. Therefore, we need to put the negative signe before the integrals.(oh, how long it took me to realize this..) In polar coordinates this expression has the following form:
Differentiating the expression for by we obtain:
A-ha, that's where we get the independence of the final result on the path choice: the arbitrary constant gets cancelled out.
Let , then ,
I made some false starts on getting a negative answer which is impossible for a strictly positive integrand. Still not quite sure where I went wrong. Normally these things happen when a singularity sneaks in inside the domain of integration after variable change. Anyway, I decided to cheat and shift the scale.
Hence the total transit time equals: