I’m trying to get a better grasp on cosmological horizons and have a question regarding recessional velocity. In particular:
What is the average recessional velocity of a cosmological object (irrespective of distance) an observer would expect to observe if measured at some time in the future?
Here is my attempt:
If the current cosmic event horizon $D_{eh}$ is the maximum proper distance from which light emitted now can ever reach the observer in the future, then to calculate the average recessional velocity $\bar v_{rec}$ of an observable that could potentially be detected by the observer at some time between now $t_0$ and $t=\infty$, one can calculate the recessional velocity of the current event horizon $v_{eh}$ and divide by two—i.e., as recessional speed is proportional to distance, this is the average between $v_{eh}$ and the observer’s recessional velocity, $v_{ob}=0$. Therefore, \begin{align} \bar v_{rec} = \frac{1}{2}v_{eh}(t_0) = \frac{1}{2}H_0 D_{eh}. \end{align} If the Hubble constant $H_0$ is about $70$ km/s/Mpc, and assuming a standard $\Lambda$CDM-model, $D_{eh}$ is about 5 Gpc, then \begin{align} \bar v_{rec} \approx 0.58c. \end{align}
Does this reasoning make sense? Thanks for your help.