Suppose we model component lifetimes with a two-parameter Weibull distribution. With $\alpha$ as the scale parameter and $\beta$ as the shape parameter, the component's mean survival time is known to be: $$E(t) = \int^{\infty}_{0}S(t)dt = \int^{\infty}_{0}e^{-(\frac{t}{\alpha})^\beta}dt = \alpha \Gamma(\frac{1}{\beta}+1)$$ where $\Gamma$ is the Gamma function and the remaining useful life $m$ of a component aged $t_0$ is: $$m(t_0)=\frac{\int^{\infty}_{t_0}S(t)dt}{S(t_0)}=\frac{E(t) - \int^{t_0}_{0}S(t)dt}{S(t_0)}$$
My question is: why is the remaining useful time not simply $m(t_0)=E(t)-t_0$?