It's a common misconception that entropy is disorder in the usual sense: a gas of molecules in a box cannot be said to be any more ordered than a gas of molecules in a box twice the original box's size, yet the latter will have twice the entropy of the first.
Entropy can be defined in two ways:
(a) The statistical mechanics way: it's proportional to the logarithm of the number of available microstates that lead to the same macrostate.
(b) The sum of infinitesimal heat supplied to the system divided by the temperature at which it is supplied, during a reversible process which starts and ends at macrostates A and B is the
change in entropy of the system as it moves from macrostates A to B (NB. this definition does not tell us what zero entropy is; for that we must rely on definition A).
As for the first definition, microstate means the exact specification of the position and momentum of every molecule and macrostate means the specification of thermodynamic variables such as volume, pressure, temperature, etc.
The second definition is motivated by Clausius' theorem, and I could provide more information if anyone wants.
It's easy to see how the first definition can be confused with disorder, and often saying that a system can access more microstates while being in the same macrostate is confused to the system possessing more disorder, but that is, in many opinions, quite misleading.