Just as an example, the so called stereographic projection could be generalized for the four dimensional case.
In three dimensions, the definition is as follows:
Let the Southern pole of the sphere of radius one above be tangent to the plane $z=0$. The coordinates of the North pole are then $(0,0,2)$. Say, we have a point $(a,b,c)$ on the sphere with an $\color{green}{R}$ on its surface. The vector pointing from $(a,b,c)$ to the North is $(a,b,c-2)$. So the equation of the straight line through the North pole and the point with the point $\color{green}{R}$ is
$$(x(t),y(t),z(t))=t(a,b,c-2)+(0,0,2).$$
This straight punches the plane $z=0$ at the $t$ for which $z(t)=t(c-2)+2=0$. So $t=\frac{2}{2-c}$ and the coordinates of the punching point are:
$$\left(\frac{2a}{2-c},\frac{2b}{2-c},0\right).$$
By definition the point above is the stereographic image of the green $\color{green}{R}$ on the horizontal plane.
It is easy generalize this projection if our sphere is four dimensional and its Southern pole touches the hyper plane $w=0$. (Let the coordinates of the North pole be $(0,0,0,2)$.) If we have a point $\color{red}{Q}$ on the surface of the four dimensional sphere at $(a,b,c,d)$ then the vector pointing from this point to the North pole is $(a,b,c,d-2)$, that is the equation of the straight through the North pole going through the point with the $\color{red}{Q}$ is
$$(x(t),y(t),z(t),w(t))=t(a,b,c,d-2)+(0,0,0,2).$$
We can repeat the last steps of the three dimensional case and we will find the location of the $\color{red}{Q}$ in the three dimensional space given by $w=0$.
I guess that any projection based on setting up equations of straights in the four dimensional space could be generalized for higher dimensions.