That's ok. I think I will do your approach it's an approximation I know. Also I will be taking structural for the pm so hopefully nothing this complicated will show up in the am.
I think that's a bad idea, both here and in general... while you can often take a shortcut by neglecting small factors, it's a bad habit if you don't understand each and every one made, and the impact to process.
What's tripping you up here? There are only two preliminary steps to this problem: 1) Drawing a free body diagram and 2) F=ma.
For the free body diagram, the forces that retard the thrust of the car are gravity (what's been called grade resistance) and friction (rolling resistance). In the real-world, you'd need to add drag (air resistance) to the friction, but as you're not given the fluid density, cross-sectional area, and drag coefficient, you cannot reasonably add here. Drag would also complicate the solution as it's proportional to the square of the velocity (so acceleration wouldn't be constant) and you'd have to integrate. In any case, sum up the forces parallel to the direction of travel and you're done.
Anyway, back to the problem: once you get the net thrust (F), you can use it to calculate the constant acceleration (a). Again, you are forced to assume constant acceleration because you don't have enough to factor in air resistance. Then it's a simple application of the constant acceleration formulas (v=u+at and s=ut+0.5at^2) to get you to the answer.
Make sense?