Performance  
       
     
  Lateral Acceleration   Longitudinal Acceleration  
     
     
  Braking   Accelerating  
       
                                      
Power Limited   Traction Limited   Speed, Distance & Time   Hill Climbing   Axle Load Distribution

When a vehicle goes up a hill, the gravitational acceleration (g) stays vertical. Because it is a vector, this acceleration will be splitted into two smaller components: One that will push the vehicle down against the road (gcosθ) and another that will simulate an acceleration (gsinθ). We can find those components with trigonometry.

Note that we will also assume that the vehicle is at rest, trying to «hold on» with engine power, so we will neglect aerodynamic effects and rolling resistance.

hill climbing

The maximum slope that can climb a vehicle based on its maximum tractive capabilities is:

For an AWD: (more)
tanθ = μ (1)

*Since most vehicle have 4-wheel brake systems, this is also the maximum slope that your brake system will be able to support before the vehicle starts sliding down.
For a RWD: (more)
tanθ = μ
lf / L
1 − μ  h / L
(2)
For a FWD: (more)
tanθ = μ
lr / L
1 + μ  h / L
(3)
Flip over limit

Regardless of the automobile layout, there is a slope where the vehicle will flip over, i.e. the normal load on the front axle will be zero. The flip over limit is: (more)

tanθ =
lr / L
h / L
(4)

Where:

μ = tire-road friction coefficient
lr / L
= portion of the vehicle's weight on the front axle
lf / L
= portion of the vehicle's weight on the rear axle
h / L
= CG-height-to-wheelbase ratio