Entropy is this awesome concept with many faces.
For a classical mechanics point of view, it would represent all the possible properties of a physical system, which is supposed to be unknown.
For a quantum mechanics point of view, it would represent all the possible microstates of a system.
To my knowledge, I assume that the first is a more simple approach of the second, and the second apporach contains the first in it.
So, there would be one basic definition of entropy for both together:
Entropy: The amount of possible microstates a system can have
This is pretty understandable, also I can see that if it is a made-up concept, it can be as abstract as we want, because yeah, words may go beyond reality as much as we want them to.
But, doubts come into the game when we start measuring entropy.
In thermodynamics, we will say that this measure equals the sum of all the infinitely-small-quotients of transferred heat by the temperature of the system, in a reversible process.
$$ \Delta S_{12}=\int_1^2 (\frac{\delta Q}{T})_{rev} $$
But how does that relate with the word definition of entropy? How is that quotient of heat divided by temperature related to the microstates?
And, if we cannot speak about stuff having heat, but only about energy flowing in form of heat, and being entropy a heat-related concept, why do we speak about stuff having entropy?