cire792 said:
and O_O about all that gravity force~
Well, gravity is a force, nothing to wonder about. What I wrote is just basics and also proof that g is independent of the object's mass that is falling towards the other object. Of course we can turn it the other way round and say that Earth is falling towards a, say, feather. However, now the Earth's mass cancels out of the equation and we get an acceleration in reference to the feather to be Tiny, with capital T because it is very small.
About your original question, here's my approach (quite similar to yours but I'll write it using LaTex):
S - displacement
[itex]v_{0}[/itex] - initial velocity
a - acceleration
t - time
The equation to solve your problem is as you've mentioned:
[tex]
S = v_{0}t + \frac{at^2}{2}[/tex]
We have to solve it in terms of a, so we rearrange it:
[tex]2S = 2v_{0}t + at^2[/tex]
[tex]2S - 2v_{0}t = at^2[/tex]
[tex]a = \frac{2S - 2v_{0}t}{t^2}[/tex]
Because [itex]v_{0}[/itex] = 0 we get
[tex]a = \frac{2S}{t^2}[/tex]
Now input the numbers given:
[tex]a= \frac{2 * (-2.36)}{0.86^2} \approx -6.38[/tex]
So the object is falling with an acceleration of 6.38 [itex]\frac{m}{s^2}[/itex] which isn't much of a problem. The object needn't have an acceleration of 9.81 [itex]\frac{m}{s^2}[/itex] because of the reasons I've explained in this thread, unless it is explicitly stated that the experiment takes place close enough to the Earth's surface.
I hope that helps.