After reading the post on How is the acting of $H^{-1}$ on $H^1_0$ defined?, I have the following question.
For each $v \in H^1_0$, then I can associate the functional $\phi_v:=f \to (v,f)_{L^2}$ for $f \in H^1_0$, as is done in the linked answer above. But, it seems to me that I can define $\chi_v = f \to (v,f)_{H^1}$.
But then, if I use the mapping $\chi$, I wouldn't get the following result
- If $v,u\in H^1_0$, $$(u,v)_{L^2} = \langle u,v\rangle$$ where the latter should denote again the dual pairing of $H^1_0$ and $H^{-1}$.
because it would mean that $(u,v)_{L^2} = (u,v)_{H^1}$
What is wrong with using functional $\chi_v$?