Let's do this in spherical coordinates. For spherical coordinates, I'll use triples $(r,\theta,\phi)$ where $r$is length, $\theta$ is the angle a vector's projection to the $xy$-plane makes with the $x$-axis, and $\phi$ is a vector's angle from the $z$-axis.
Now, I don't like balls that aren't centered at $(0,0,0)$, so let's translate the ball so it's centered at the origin. The trick here is completing the square:
$$ x^2 - x + y^2 + z^2 = 0 $$
$$ x^2 - x + \frac{1}{4} + y^2 + z^2 = \frac{1}{4} $$
$$ \bigg(x - \frac{1}{2}\bigg)^2 + y^2 + z^2 = \frac{1}{4} $$
so the ball has radius $\frac{1}{2}$ and is centered at $(\frac{1}{2}, 0, 0)$.
Translation doesn't change volume, so the volume is the same as the volume of a ball of radius $\frac{1}{2}$ centered at $(0,0,0)$.
Now, to sweep out a whole sphere of fixed radius $r$ exactly once, we'll have $\theta$ ranging from $0$ to $2\pi$, $\phi$ ranging from $0$ to $\pi$; we'll integrate these spheres from $0$ to $\frac{1}{2}$:
$$ \int_0^\frac{1}{2} \int_0^{2\pi} \int_0^\pi r^2\sin\phi\ d\phi d\theta dr $$
Bonus:
$$ \cdots = \int_0^\frac{1}{2} r^2\ dr \int_0^{2\pi}\ d\theta \int_0^\pi \sin\phi\ d\phi $$