I was playing around with the equation in the title when I realized it isn't as simple as I thought. I basically changed the parameters in the derivation given in the book because I was wondering why $t=0$ in particular had to be the starting point. The result was the following, which I am unable to explain.
If we let the times be $t_1$ and $t_2$ instead of $0$ and $t$, then we get $\Delta x = v_{av} \Delta t=(\frac{v_a+v_b}{2})(t_2-t_1)$ where $a,b$ are arbitrary. This leads to the weird result $\Delta x = (\frac{v_0+at_a+v_0+at_b}{2})(t_2-t_1)=(v_0+\frac{1}{2}a(t_a+t_b))(t_2-t_1)=v_0\Delta t+\frac{1}{2} a(t_a+t_b)\Delta t$. *
My question is, is this a correct result? If so, how useful is it? If you replace $a,b$ by $1,2$ it becomes the general case of $\Delta x = v_0 t+\frac{1}{2} at^2$.
* $v_{av}$ means average velocity