There are several questions asking by the meaning of Time-Energy uncertainly relation and also by its derivation.
My problem is about the second. In all documents I have seen, the same is supposed alwas: Let $A$ an observable which does not depend explictly on $t$. (from John Baez's web page to Griffiths (p.113) and also in the original paper, formula 4). Then
$$\Delta T_A \Delta H \geq \frac{\hbar}{2} . $$
My question is: What happens if we allow $\langle \partial A/ \partial t \rangle \neq 0$?.
EDIT.
@ZoltanZimboras demands me to write the definition of $\Delta T_A$. The truth is I'm not sure how to answer him. Usually, $\Delta T_A$ is defined as
$$ \Delta T_A = \frac{\langle A \rangle}{\frac{d\langle A\rangle}{dt}}. $$
If we set the same definition, then the Heisenberg's inequality comes
$$\Delta T_A \Delta H \geq \frac{\hbar}{2}\left| 1-\frac{\langle\partial A/\partial t\rangle}{d\langle A\rangle /dt } \right|. $$
The advantage of this definition is physics understand very well the meaning of the quantity $\Delta T_A$, but then the above equation comes more difficult. On the other hand, if we set
$$\Delta T_A = \frac{\langle A \rangle}{\frac{d\langle A\rangle}{dt}-\left\langle \frac{\partial A}{\partial t}\right\rangle}, $$
Then the Heisenberg's principle takes its usual form, but we have to reinterpret the quantity $\Delta T_A$.