erobz said:
I think I've over complicated my first approach.
The input power ##P_{in}## should simply be given by:
$$ P_{in} = \frac{1}{\eta_o} \left( F_s + \beta v_o^2\right) v_o $$
Still too complicated in my opinion.
If we are being asked for a percentage improvement in gas mileage then ##v_o## is irrelevant, ##\beta## is irrelevant and ##{v_o}^2## is irrelevant.
All that matters for the mileage ratio is the power ratio.
If we are holding velocity fixed, all that matters for the power ratio is the force ratio.
Per the model you have chosen, we are reducing the "drag" portion of the total force by a fraction of 4/7 and leaving the static ("s") portion unchanged.
So the mileage would improve by a ratio of: ##\frac{F_s + F_\text{drag}}{F_s + \frac{4}{7}F_\text{drag}}##
We could express the same formula a bit differently if instead of knowing both retarding forces we knew only their ratio. Call it ##S## for how "streamlined" the car is (at the selected cruising speed) with ##S = \frac{F_s}{F_\text{drag}}##.
Then the mileage improvement ratio would be ##\frac{S + 1}{S + \frac{4}{7}}##
In the limit of high ##S## (very stylish car with all the brakes locked hard on), air resistance is not even a factor and mileage improves negligibly when you reduce air resistance by a factor of 4/7.
In the limit of low ##S## (a huge sail on a cart with high pressure tires and teflon-coated ball bearings), air resistance is everything and you get a 7/4 improvement in mileage.
If ##S## = 1 then you get 27% improvement in fuel economy.