I'd appreciate your help with the following: I am looking for formulas $\phi$ and $\psi$ (in any suitable language $\mathcal{L}$) such that in the following exactly one condition is fulfilled, the other not:
a) For all $\mathcal{L}$-structures $\mathcal{M}$: if $\mathcal{M} \vDash \phi$, then $\mathcal{M} \vDash \psi\\$.
b) For all $\mathcal{L}$-structures $\mathcal{M}$: $\mathcal{M} \vDash \phi \rightarrow \psi \\ \\$
($\mathcal{M} \vDash \phi$ means that the formula $\phi$ is valid in $\mathcal{M}$)
I am looking forward to your replies!
Using the same convention that Mauro does:
a first-order example that actually works is:
It is clear that (a) holds: For every $\mathcal M$ such that $\mathcal M\vDash(\forall x)(\forall y)\,x<y$ we also have $\mathcal M\vDash(\forall x)(\forall y)\,y<x$.
But (b) does not hold: There is an $\mathcal M$ such that $\mathcal M \not\vDash (\forall x)(\forall y)(x<y \to y<x)$. Namely, $\mathcal M$ can be taken to be any set with a non-symmetric binary relation.