00:01
All right, so the given matrix represents a rotation by 90 degrees.
00:05
This is going to be a rotation by 90 degrees, counterclockwise.
00:14
And then the direction, field, and trajectories, we can let x vector be the vector, x, y.
00:21
And then we have d, d, dt of x, y, is going to be equal to the matrix, negative 1, 1 ,0 times the vector xy, which is going to be equal to negative y, x.
00:44
So this means the velocity vector at point x, comma, y, is going to be perpendicular to the position vector x, y, rotating it 90 degrees, and it's going to be counterclockwise.
00:58
So the trajectories are going to be circles, and they're centered at the o 'clock.
01:04
Origin...