Entropy is - to me still - a strange concept. There are two ways to look at it.
The first is from an intuitive point of view. We (at least I, hopefully you too) know that the infinitesimal change in energy of a system is
dE = T dS - p dV + [itex]\mu[/itex] dN
with E energy, T temperature, S entropy, p pressure, V volume, [itex]\mu[/itex] chemical potential and N number of particles.
If you bring two systems into contact, they will flow until the temperature, pressure and chemical potential are equal. To get the pressure equal, they will exchange volume (when allowed; for example, if you have a box with a movable wall, the wall will go to that position where the pressure in both parts is equal). To get the chemical potential equal, they will exchange particles (when allowed; for example through a permeable membrane). To get the temperature equal, heat flows from one system into another, you could consider entropy the quantity (whatever it is) that is exchanged to reach equilibrium.
Yet another way to introduce entropy is by the microcanonical ensemble. What you actually do is, given the energy of a system, count the number of microstates g it can be in. As these numbers often get very large, we can introduce entropy as the logarithm of this number, so that numbers in the order of [itex]10^{23}[/itex] get order 23, which is more managable.
By the way, a book I can recommend to you is "Thermal Physics" by Charles Kittel / Herbert Kroemer. It's a very gentle and intuitive introduction to thermal physics.