Displacement after Time T in a Velocity Field

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In a static velocity field, the displacement of a particle after T seconds can be determined using the equation dx/dt = v(x), which leads to a separable differential equation. The integral ∫(dx/v(x)) = ∫dt provides a solution for the final time T in terms of the initial position x_0 and the final position x_f. To find the ending position for a given total time, the inverse function x_f = f^{-1}(T) must be utilized, where T is derived from the integral. However, obtaining a closed form solution requires specifying the velocity field, and a general expression is not feasible for arbitrary velocity functions. For two-dimensional cases, this process must be applied to each component of the position vector.
Teg Veece
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I have a velocity field that is static in time. At every location, x, there is a corresponding velocity vector.

I'm trying to work out the displacement of a particle after T seconds if I drop it into the velocity field at time t=0 and at location x_0.

I was thinking something along the lines of ∫v(x_0)dt between the limits of t=0 and t=T but it doesn't seem right because the integrand doesn't seem to depend on t at all (in fact v(x_0) is a constant so it can't be right). Maybe there's a double integral involved...

Anyone know what a suitable form for this equation would be?
 
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For simplicity, you could consider a one dimensional case:

\frac{dx}{dt}=v(x)

This is a separable differential equation, so:

\int_{x_0}^{x_f}\frac{dx}{v(x)}=\int_0^T dt

But it gets you a solution for the final time, T.

T = \int_{x_0}^{x_f}\frac{dx}{v(x)}

If for a fixed x0, you can suppose that the total time is a function of the ending position.

T = f(x_f), where this function is given by the right hand side of the equation above.

So, to get the ending position for a given total time, you would need to take the inverse of that function

x_f = f^{-1}(T)

In order to get a closed form for this, you need to plug in the velocity field. I don't think there's a way to get a general expression for an arbitrary velocity function.

Now, for a two dimensional problem you need to do this for each component of the position vector.
 
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