As far as i understand it, total differentials are linear maps that map vectors to numbers. In thermodynamics we encounter statements that a we have reached equilibrium when a total differential of a certain function is zero. For example equilibrium is reached when the Helmholtz free energy function differential at constant temperature is zero, $$ \mathrm{d}A = 0. $$
But that seems strange to me. $A$ map=the total differential=$\mathrm{d}A$ is a different "object" than the value of a map evaluated at a certain point. So what exactly does a statement like $\mathrm{d}A=0$ mean? I guess what is meant is the value of the total differential evaluated at some point with some vector?
So what is the vector and the point that we are feeding in?
EDIT:
Perhaps i should not have used the case $\mathrm{d}A=0$ since that seems to be unambiguous. But what is meant when we say for example the total differential is positive ? I've also read that in textbooks. A statement like that doesn't make sense unless i refer to an assumption/convention about the input vector, or does it ? I mean the value "positive" does vary in general with the input vector unless i have exactly the zero map. Please include a discussion about that also in an answer.
Optionally, I would also like a better understanding what the actual vectors are in the context of thermodynamics.