kelmcguir said:
2) How does fuel consumption work with constant 1 g acceleration or acceleration in general? I read that "it doesn't take a constant amount of energy to maintain a constant acceleration...it takes twice as much energy to go from 1 to 2 m/s as it does to go from 0 to 1 m/s". Is this true and why?
You are missing the concept of power somewhere. Let's imagine you are driving a car with negligible resistance (aerodynamic drag & rolling resistance) and with negligible fuel mass with respect to the car mass ##m##. The car is going from point A to point B, separated by a distance ##x##, at a constant acceleration ##a## and the trip lasts 60 minutes in total.
How much energy is required for the trip? That would be based on the required work:
$$E = max$$
Time, thus speed, has no say in this. Twice the acceleration means twice the required energy. And twice the distance traveled means twice the energy needed too. So half-way on our trip we spent half of our energy (i.e. fuel):
$$E_{@x_{\frac{1}{2}}} = ma\frac{x}{2}$$
But how much time does it take to travel half-way? We know it takes 60 minutes for the total trip, so this holds up:
$$t = \sqrt{\frac{2x}{a}}$$
and half-way, it will be:
$$t_1 = \sqrt{\frac{2\frac{x}{2}}{a}} = \sqrt{\frac{x}{a}} = \frac{t}{\sqrt{2}}$$
If ##t## is 60 minutes, then it will take 42 minutes to travel the first half (##t_1##) and 17 minutes to travel the second half (##t - t_1##). This is true because during the second half we are driving a lot faster.
What is not constant throughout our trip is the power ##P## needed which, for a certain period of time, averages to:
$$P = \frac{E}{t}$$
For both halves of the trip, we have the same value for ##E##. But the time elapsed is different:
$$\frac{P_2}{P_1} = \frac{t_1}{t - t_1} = \frac{1}{\frac{t}{t_1} - 1} = \frac{1}{\sqrt{2} - 1} = 2.4$$
So, if you need, say, 100 hp on average during the first half of the trip, you will need an engine producing 240 hp on average during the second half of the trip. Of course, the actual power requirement is totally dependent on the speed of the car (##P = \frac{ma\Delta x}{\Delta t} = mav##).
In conclusion,
distance-wise, you will need as much fuel to travel the first meter of the trip as for traveling the last one. But
time-wise, you will need a lot more fuel to travel the last minute of the trip compared to what you will need for the first minute of your trip.