You have asked more than one question. In your last paragraph, I believe your main question is this:
... if we reverse the roles of time and space here, and instead give information about a single point of space for all of time, it seems we cannot predict spatially. Are there equations in physics that can be considered to predict across space (for a given time)
No.
A space-like slice (subspace) of spacetime stores information, whereas a time-like slice (a worldline) does not. More to the point, the very way a "particle" is defined is an attempt to trim away as much variable information as possible, so that the continuity of conserved quantities such as mass, charge, and spin is emphasized.
In classical physics this focus on reductionism across the time axis leaves you with not much more than the history of how the particle was "bumped," billiard-ball style, as it moves across its path across time. Those deflections provide a small amount of information about the universe as a whole, but the total information encoded is quite trivial compared to that contained in any space-like slice, and is certainly never enough to reconstruct the universe as a whole. The amount of information contained in a single particle path is also highly variable. It approaches zero in the case of a particle that simply sits in a very dark corner of intergalactic space and never interacts with much of anything, so in that case you are left in the dark pretty much about everything else going on in space.
Incidentally, you may wonder why in defining time slices I have focused on the worldlines of individual particles, instead say of a single fixed point in space from the start to the end of the universe. You could use the latter approach, and it gives the same result, since for example a single dark spot in deep intergalactic space has even less information about the rest of the universe than a very bored particle sitting there. However, I don't use that definition because "where" that specific point in space really is quickly becomes entangled with the question of "where it it relative to some set of particle worldlines." Since that is the only way to make such an assertion meaningful, it's easier and more honest simply starting with the particle worldlines.
You also noted in your second paragraph:
... Dimensionality (the fact that there are three spatial dimensions but only one temporal) surely cannot be sufficient ...
Yes. In fact, if you look at what I just wrote, it applies just as well to a 1-to-1 ratio of space axes to time axes as it does to a 3-to-1 ratio. Time is simply the axis of quantity (e.g. mass) conservation, while space is the axis on which the relationships (information) that capture the variable relative configurations of those conserved quantities is expressed.
So what does any of this have to do with my earlier answer about time operating first as cyclic rather than length-like? Quite a bit, actually. The cycles are just repeating patterns of relationships between the conserved, particle-like conserved quantities. So, the conserved-over-time mass of a planet orbits the similarly conserved mass of the sun, and from that detectably similar pattern we define as the year.
It's not that you cannot have change without cycles. It's just that without the concept of some patterns "repeating," you cannot create a truly metric concept of time that like space includes definite lengths and distances. That makes the time version of "distance" rather odd, and a lot more complicated than the space-like version.