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\[\frac{\text{d} \langle x \rangle}{\text{d} t}=\int x \frac{∂}{∂t}|\Psi|^2\text d x\] Why can't you do integration-by-parts of the expression on the right- pull the time derivative over onto x , note that ∂x/∂t =0 and conclude that \[\frac{\text{d} \langle x \rangle}{\text{d} t} =0\]?
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I think they should have put x(t).
Probably because Psi is a function of t, which makes x a function of t.
\[\Psi(x,t)\]
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