If I have a 100 kg mass I can accelerate it with any force whatsoever. If I apply 1 Newton force I can accelerate it at 1/100 m/s^2. If I apply 10 N of force I can accelerate it at 1/10 m/s^2. If I shove it with 1,000,000 Newtons it will accelerate at 10,000 m/s^2. There is NO 'minimum force' required to accelerate any given mass, ignoring all other factors such as friction, rolling resistance etc.
Does anyone happen to know the coefficient of rolling friction for the LRV's tires? It would be good to know before we dismiss it as small compared to the inertial forces and gravity slope forces.
On earth, at least, rolling resistance can be characterized by a dimensionless coefficient that relates the tractive force required to overcome it to the vehicle weight. E.g., if the RR coefficient is 0.1, then a vehicle with a weight (gravitational force) of 100 N would require a horizontal tractive force of 10 N to keep it moving (at any speed above zero) on a level surface. This energy goes into flexing and heating the tires, crunching up a soft roadbed, etc. This is why it takes a minimum tractive force to budge a car, train or airplane even on a level surface.
Because the tractive force needed to overcome rolling resistance is proportional to weight, it is also proportional to the local gravity field. All other things equal, a rover that takes, say, 100 N of tractive force to budge on earth would take only 16.7 N of tractive force on the moon.
Because the rolling resistance is a fixed force, and energy is force times distance, the power needed to overcome it increases linearly with velocity. This sets a maximum velocity that a rover could achieve on a level surface with a given amount of motor power. Can we work out what that is for the LRV?