I am completely mystified about parameters in differential forms and wherever I looked it's just glossed over.
Take for example the $2-$form $\omega = dx\land dy$ in $\mathbb{R}^n$.
Usually it's just defined like that, but given two vectors $(x,v_1), (x,v_2)$ in the tangent space at $x$, it shold be that $dx \land dy = dy \land dx$, since $$(dx \land dy) (x)((x,v_1), (x,v_2)) = $$ $$- (dy \land dx)(x)((x,v_2)(x,v_1))=$$ $$ (dy \land dx)(x)((x,v_1)(x,v_2))=$$
According to my book, tough, $dx \land dy = - dy \land dx$. Where am i wrong?
First of all, you're writing incorrect equations. Once you evaluate individual terms, there are no more wedges. The correct equation, using your (cumbersome!) notation, is \begin{multline*} (dx\wedge dy)((x,v_1),(x,v_2)) = dx((x,v_1))dy((x,v_2)) - dx((x,v_2))dy((x,v_1)). \end{multline*} And of course from this you see that, in fact, $dx\wedge dy = -dy\wedge dx$.