minio said:
So "acceleration in universe expansion" simply means that Hubble constant is getting larger as time goes on? (from 70 to 80 and so on)
No, this is incorrect. The Hubble parameter is defined in terms of the scale factor, a(t), as
H = \frac{\dot{a}}{a}
(The Hubble constant is the Hubble parameter evaluated at the present time).
The scale factor simply governs the growth of measuring rods affixed to the expanding space (imagine a grid painted on a rubber sheet; as the sheet expands, the grid grows: a(t) determines this change in length scale). Now, by accelerated expansion what we mean is that the scale factor, a(t), has a positive second derivative: \ddot{a}>0.
Relating back to the Hubble parameter, by taking its derivative one finds
\dot{H} = \frac{\ddot{a}}{a} - H^2
so the answer to your question about how the Hubble parameter behaves during accelerated expansion is: it depends. For example, the simplest case of accelerated expansion is that due to a cosmological constant (a constant energy density.) In this case, a(t) \propto e^{Ht}: the scale factor grows exponentially in time (you can verify easily that this gives a positive \ddot{a}). Using the above equation for \dot{H}, one finds that \dot{H}=0 -- that the Hubble parameter in fact doesn't change at all!
EDIT: To make contact with George's post (that I just saw now), one finds that H indeed decreases for all other cases
except the one I just showed you (the case of a cosmological constant.)