student34 said:
I thought that if time has more than one direction, then it should have more than one dimension.
You thought wrong. In fact you aren't even thinking clearly about what a "dimension" is--despite repeated attempts to get you to do so. Some of the things you say appear to be groping in the right direction, but very slowly. For example:
student34 said:
I am trying to say that space is different than time. I don't believe that is a controversial statement.
A better way of stating this would be that
spacelike vectors and curves are fundamentally different from
timelike vectors and curves. And there is a third category in spacetime,
null (or lightlike) vectors and curves, which are fundamentally different from both.
student34 said:
It makes a difference because now we csn have a space of time instead of just a line of time.
This is where you are sort of groping in the right direction; but you sidetrack yourself by not thinking clearly about what "time" is, what a "dimension" is, and what the different directions in spacetime of the worldlines of different observers in relative motion actually mean.
What you should do is step back from all that and, first of all, ask this question:
(Q1) How many distinct parameters does it take to describe all of the possible directions in spacetime that a timelike worldline (i.e., the worldline of an inertial observer) can have at a particular point?
The answer, of course, is "more than one". (I won't give the exact number right now because I want you to think about the question in those terms.) But
why is it more than one?
Consider: suppose spacetime were 2-dimensional. That would mean the spacetime diagrams we draw on 2-dimensional sheets of paper (or the electronic equivalent) would be diagrams of actual spacetime, not just a 2-dimensional "slice" of 4-dimensional spacetime. And in a 2-dimensional spacetime, the answer to question Q1 above
would be one. The "directions in spacetime" that a timelike worldline could have could be described by
one parameter, which we could think of as the ordinary speed in the x-direction of that worldline in some fixed inertial frame. (Or, if we wanted our parameter to have the range ##- \infty < p < \infty## instead of ##-1 < p < 1##, we could use the gamma factor or the rapidity.)
From the above, you should already be able to figure out the answer to question Q1 above for our actual 4-dimensional spacetime.
But now, take another step back, and ask a different question:
(Q2) How many timelike eigenvalues does the metric of spacetime have?
By "timelike eigenvalue" I just mean an eigenvalue of whichever sign we are using for timelike squared intervals in the metric. For example, if we write the metric as ##d\tau^2 = dt^2 - dx^2 - dy^2 - dz^2##, timelike squared intervals are positive, so that is the timelike sign. (This "timelike convention" is more common in introductory books on SR and in particle physics. The opposite "spacelike convention" is more common in GR and more advanced relativity literature.)
The answer to Q2 above is
one. That is, one always. It doesn't matter what frame you choose. It doesn't matter if spacetime is curved. It doesn't matter if you adopt some weird coordinate chart, even one in which you don't have one timelike and three spacelike coordinates as you do in a standard inertial frame. The metric always has precisely
one timelike eigenvalue. And it always has precisely
three spacelike eigenvalues.
What do the metric eigenvalues mean? They tell you
what kinds of dimensions the space, or spacetime has. And
that is why we say that spacetime has one timelike dimension and three spacelike dimensions, for four dimensions total: because of the eigenvalues of the metric. (Similarly, ordinary Euclidean 3-space has a metric with three spacelike eigenvalues--here we always adopt the spacelike convention so the metric is positive definite--and so we say it is a 3-dimensional space.) And note that, since the answers to Q1 and Q2 are different, the question of what kinds of dimensions the space or spacetime has is a
different question from the question of how many different directions a particular kind of vector can point. Both are properties of the spacetime and its geometry; but they're
different properties.