Geometrical interpretation of this property

brunob
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Hi there!

I have the following property:
If x(t) is a solution of \left\{ \begin{array}{l} \dot{x} = f(x) \\ x(t_0) = x_0 \end{array} \right. then the function y(t) = x(t+t_0) is a solution of the equation with initial data y(0) = x_0.

How could it be interpreted geometrically?
Thanks!
 
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Geometrically, think of f as a vector field. Imagine it as a collection of arrows describing the velocity of a fluid; that is, for each x, f(x) is the velocity of the fluid at the point x.

Now, imagine a small pebble moving in this fluid. At each point x, the trajectory of the pebble must be tangent to the vector f(x) (why?). Dropping a pebble into the fluid at a specific point x_0 represents an initial condition of your ODE. The answer to your question is the following: it doesn't matter what time you drop the pebble at x_0; the pebble's resulting trajectory will always be the same, because the fluid velocity field is unchanging with time.

The image of the solution of y is just a copy of the image of x, but shifted in time -- just like the pebble's motion when dropped at time t_0 is identical to its motion when dropped at 0, but shifted in time.
 
Nice example! So, if the velocity is constant it means that the position x(t) is linear and so y(t) is, and due the way the functions are linked I can say that their graphics are parallels.
Let me know if I'm wrong.

Thanks!
 
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