I Determine P(t)=(Px(t),Py(t)) given (x0,y0) and v(x,y,t).

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The discussion centers on solving a 2D particle motion problem given a velocity field v(x,y,t). The approach involves using first-order ordinary differential equations (ODEs) to determine the particle's position over time, starting from an initial position at time t0. The equations dpx/dt = vx(px, py, t) and dpy/dt = vy(px, py, t) are set up to describe the motion of the particle. The solution involves integrating these equations, which can be complex due to their time dependence. Ultimately, this method effectively transforms Eulerian coordinates to Lagrangian coordinates, providing a clear framework for understanding particle trajectories in a fluid flow.
Wiccan
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Dear all,

I'm a bit confused about a 2D problem which I thought had a simple solution...
I don't know if I'm correct, so:

I have a 2D space, and time. I know the velocity field v(x,y,t). I would like to know where the particle which start at the position x0,y0 at an istant t0 is at a certain istant t>t0.My idea is:
p(t)=<px(t),py(t)>

dp/dt=v(p,t)=<vx(px,py,t),vy(px,py,t)>
%%%
dpx/dt=vx(px,py,t)
dpy/dt=vy(px,py,t)
%%%

Then I would solve it by part...even if the solution can be not easy due to dependence on time,
Ex:
vx=px*t, vy=px*py
%%% % %%
dpx/px=t dt %px=c1*exp(0.5*t^2)
dpy/py=px dt %dpy/py=c1*exp(0.5*t^2)dt etc...
%%% %%%

Is this answer formally correct?
 
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These are the path lines of particles. They are given via the velocity field by solving the 1st-order set of ODE's
$$\frac{\mathrm{d} \vec{x}(t)}{\mathrm{d} t}=\vec{v}(t,\vec{x}(t))$$
with the initial condition
$$\vec{x}(0)=\vec{x}_0.$$
The solution of the ODE's describes the motion of a fluid element that was located at ##\vec{x}_0## at time ##t=0##. In other words it gives you the transformation from Euler to Lagrange coordinates.
 
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