Assume $$u_k\rightharpoonup u,\quad v_k\rightharpoonup v\quad\text{in}\quad L^1(0,T;Y)\tag{1}$$ and $$\int_0^T u_k(t)\varphi'(t)\ dt=-\int_0^T v_k(t)\varphi(t)\ dt\tag{2}$$ for some $\varphi\in C_0^\infty(0,T)$. "Passing to the limit" we get $$\int_0^T u(t)\varphi'(t)\ dt=-\int_0^T v(t)\varphi(t)\ dt.\tag{3}$$
My question is: How to justify this passage to the limit?
Remark: this passage to the limit is a step of the proof that "generalized derivatives are compatible with weak limits" in the following sense: $$u_k\rightharpoonup u\text{ in }L^p(0,T;Y)\quad \text{and}\quad u_k'\rightharpoonup v\text{ in }L^q(0,T;Y)\qquad \Rightarrow \qquad u_t=v,$$ where $1\leq p,q<\infty$ (page 419 of Zeidler's book). Writing $u_k'=v_k$, $(2)$ is obtained from the definition of generalized derivative. And $(1)$ is obtained from the continuous embedding $$L^s(0,T;Y)\subseteq L^r(0,T;Y),\quad 1\leq r\leq s\leq\infty.$$ The author says that $(3)$ follows from the proposition below, but I didn't understand it. So, I'd like an explanation.
Thanks.
