Why is the orbit of an alpha particle in the Rutherford gold foil scattering experiment a hyperbola?
The equation of orbit of a two-body system under the influence of gravity ($F_g = -\gamma/r^2$) is given by
$$r(\phi) = \frac{c}{1+\epsilon \cos\phi} $$
where
$$c = \frac{\ell ^2}{\gamma\mu}$$ with $\ell$ the angular momentum and $\mu$ the reduced mass of the system. $\epsilon$ turns out to be the eccentricity of the orbit
For a hyperbolic orbit, $\epsilon > 1$ or $E > 0$ where the energy $E$ is
$$E = \frac{\gamma ^2 \mu}{2\ell ^2}(\epsilon ^2 -1)$$
All these equations were derived given that the force of interaction is $-\gamma/r^2$. In Rutherford's case, the force of interaction is electrostatic between the positive nucleus and positive alpha, so $F = +\gamma/r^2$.
From this alone can we use the above equations to see that the orbit of the alpha particle is a hyperbola? If you sketch the alpha particle and the nucleus, it certainly looks like the orbit is hyperbolic, but how do we know it's not parabolic ($\epsilon = 1$ for parabola). How do we know $\epsilon > 1$?