Here's a quick derivation for @Dave's answer.
Our goal is to optimize the output range of the voltage divider. This range is the difference between two voltage divider ratios.
$$ \frac{output\: swing}{V_{DDA}} = \frac{R_B}{R_B+R_{T,min}} - \frac{R_B}{R_B+R_{T,max}} $$
To optimize this, we can take the derivative with respect to \$R_B\$ and set it equal to 0. The math is simpler if \$R_B\$ and \$R_T\$ are flipped, you should get the same result either way.
$$ \frac{output\: swing}{V_{DDA}} = \frac{R_{T,max}}{R_{T,max}+R_B} - \frac{R_{T,min}}{R_{T,min}+R_B} $$
$$ \frac{d}{dR_B} \left[\frac{output\: swing}{V_{DDA}}\right] = \frac{R_{T,min}}{(R_{T,min}+R_B)^2} - \frac{R_{T,max}}{(R_{T,max}+R_B)^2}=0 $$
$$
\begin{align*}
\\
&R_{T,min}(R_{T,max}+R_B)^2-R_{T,max}(R_{T,min}+R_B)^2 = 0 \\
&(R_{T,min}-R_{T,max})R_B^2-(R_{T,max}R_{T,min}^2-R_{T,min}R_{T,max}^2) = 0 \\
&(R_{T,min}-R_{T,max})R_B^2-R_{T,min}R_{T,max}(R_{T,min}-R_{T,max}) = 0 \\
&R_B^2=R_{T,min}R_{T,max} \\ \\
&\boxed{R_B = \sqrt{R_{T,min}R_{T,max}}} \\
\end{align*}
$$
There's probably a deeper reason why it works out to be the geometric mean, but this is how I approached the problem. Hope this helps
Rb
should be very certain value. \$\endgroup\$Rb
, it's good idea to put preset resistor. \$\endgroup\$