I am considering the differential equation $$ x''(t) = a\frac{x'(t)}{x(t)} $$ where $a>0$ is an arbitrary constant. I cannot solve this equation directly, but I am wondering if there's still any way I could answer the following below.
Given an initial condition $x(0) = x_{0}$ and $x'(0) = -v_{0}$ where $x_{0}, v_{0}>0$, how can I determine the position $x(T)$ for which $x'(T) = 0$? I don't care what the time $T$ is, just what is $x(T)$? Maybe there is a clever method to figure out the answer.
If a simple formula can't be found, then I am wonder if there are any numerical technique, even approximate ones at that.
$\ddot x(t) = a\dfrac{\dot x(t)}{x(t)}; \; \; (1)$
$\ddot x(t) = a\dfrac{d}{dt}(\ln \; x(t)); \; \; (2)$
given that
$x(0) = x_0 > 0, \; \; (3)$
and
$\dot x(0) = -v_0 < 0, \; \; (4)$
(2) may be integrated with respect to $t$ 'twixt $0$ and $T$:
$\dot x(T) + v_0 = \dot x(T) - \dot x(0) = \displaystyle \int_0^T \ddot x(t) \; dt$ $= a \displaystyle \int_0^T \dfrac{d}{dt}(\ln \; x(t)) \; dt = a(\ln \; x(T) - \ln \; x(0))$ $ = a(\ln \; x(T) - \ln \; x_0) = a\ln \dfrac{x(T)}{x_0}. \; \; (5)$
Now if
$\dot x(T) = 0, \; \; (6)$
then (5) yields
$v_0 = a\ln \dfrac{x(T)}{x_0}, \; \; (7)$
whence
$x(T) = x_0 e^{v_0/a}, \; \; (8)$
a formula giving $x(T)$ in terms of $x_0$ and $v_0$.
One can also argue as follows:. from (2) we write
$\dfrac{d}{dt}(\dot x(t) - a\ln \; x(t)) = 0, \; \; (9)$
or
$\dot x(t) - a\ln \; x(t) = C, \; \text{a constant}; \; \; (10)$
thus,
$\dot x(T) - a\ln \; x(T) = \dot x(0) - a\ln \; x(0), \; \; (11)$
or
$\dot x(T) - \dot x(0) = a(\ln \; x(T) - \ln \; x(0)), \; \; (12)$
and in light of (3), (4) this becomes
$\dot x(T) + v_0 = a(\ln \; x(T) - \ln \; x_0) = a\ln \dfrac{x(T)}{x_0}; \; \; (13)$
applying (6) to this equation begets (7), and we may continue as before.