I'm looking for a parameterization $(x\_1(u,v),x\_2(u,v),x\_3(u,v),x\_4(u,v))$ of a knotted sphere in $\mathbb R^4$. How might one go about finding such a parameterization?



Parameterization of a knotted surface?
If you know how to parameterize a nontrivial knot in $R^3$ (say, the [trefoil](https://mathoverflow.net/questions/91444/what-is-parameterization-of-the-trefoil-knot-surface-in-r%C2%B3?rq=1) knot), you can use Artin's "spinning" construction to parameterize a nontrivial knot in $R^4$ via map $S^2\to R^4$ written in spherical coordinates on $S^2$. Take, say, the trefoil $T$ in $R^3$ parameterized by some smooth periodic function $f(\theta), 0\le \theta\le a$ where $a$ is the period. Let $L$ denote the straight line in $R^3$ through the points $f(0), f(c)$, $c=a- \epsilon$ where $\epsilon>0$ is sufficiently small (if you want to know how small is small, ask me and I can explain). I will choose the coordinates $x\_1, x\_2, x\_3$ so that $L$ is the $x\_3$-axis. Let $R\_\phi$ denote the rotation by the angle $\phi$ in $R^4$ around the plane $x\_1=x\_2=0$ (thus, fixing $L$). Now, consider the map 
$F: [0, c]\times [0, 2\pi]\to R^4$, given by 
$$F(\theta, \phi) = R\_\phi\circ f(\theta)$$ 
Its image is a knotted 2-sphere $\Sigma$ in $R^4$. It is smooth away from the points $f(0), f(c)$. If this bothers you, it can be fixed (explicitly). Now, rescale the interval $[0, c]$ to $[0, \pi]$ via the map $s: t\mapsto \frac{\pi}{c}t$. Then the map $$G= F\circ (s^{-1} \times Id): [0,\pi]\times [0,2\pi]\to R^4$$ parameterizes the same surface $\Sigma$ as before. Lastly, use the spherical coordinates on $S^2$ to convert the map $G$ to a homeomorphism $S^2\to \Sigma$. 


This, I think, is as an explicit construction as it can be (provided you are not bothered by smallness issue for $\epsilon$). 


Edit: Upon your request, smallness of $\epsilon$ is defined as follows: There exists a round ball $B$ (or a half-space) in $R^3$ with points $p=f(a-\epsilon), q=f(a)$ on its boundary such that the arc $\alpha=f([a-\epsilon, a])$ is contained in $B$ and is unknotted in $B$, i.e., is isotopic to the line segment $pq$ in $B$ via an isotopy fixing the boundary sphere of $B$. (In practical terms, you can think of the unknottedness property of $\alpha$ as assuming that $\alpha$ is a graph of a function on the segment $pq$, with values in the plane orthogonal to $pq$.) 


See for instance [here](http://faculty.tcu.edu/gfriedman/papers/spinHKT.pdf) for details. 


