Rolling Resistance & Grade

The two road-load terms that don't need a wind tunnel: the tyre's rolling drag and the weight you lift up a hill.

Automotive EngineeringLongitudinal DynamicsFree preview
⏱️ About 14 min
Rolling Resistance & Grade — illustration
Decorative illustration.

Underinflate your tyres by a third and your fuel economy quietly drops several percent. That invisible loss is rolling resistance — and it is one of the easiest road-load terms to quantify.

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The big idea: Rolling resistance is approximately a constant fraction of the vehicle's weight (F = Cr·mg); grade resistance is the component of weight acting down a slope (F = mg·sin θ) — together they form the speed-independent part of road load.
🎯 By the end, you'll be able to
  • Compute rolling resistance from a rolling-resistance coefficient
  • Compute grade resistance from road slope
  • Explain the physical origin of rolling resistance (tyre hysteresis)
  • Combine rolling and grade into the low-speed road load
📎 Helpful to know first

Where rolling resistance comes from

A rolling tyre looks round, but under load it flattens into a contact patch and the carcass deforms continuously as it rolls. The rubber and casing are not perfectly elastic — energy goes into deforming the tread as it enters the patch and is not fully recovered as it leaves. That hysteresis loss shows up as a small but persistent retarding force: rolling resistance. Remarkably, over normal driving speeds it is nearly proportional to the vertical load, so engineers lump it into a dimensionless rolling-resistance coefficient Cr and write the force as Frolling = Cr·mg. Passenger-car radials have Cr around 0.008–0.015; low-rolling-resistance 'eco' tyres push toward the bottom of that range; soft off-road tyres are higher.

On a slope, a second, larger effect appears. Gravity pulls the car straight down, and on an incline a component of the weight acts down the slope, resisting forward motion uphill (or aiding it downhill). This grade resistance is mg·sin θ for a road at angle θ to the horizontal. Road signs express slope as a percentage rise (a 10% grade rises 10 m per 100 m horizontal); for modest grades, sin θ ≈ tan θ ≈ grade fraction, so a 10% grade gives roughly mg × 0.10 of resistance — far larger than rolling resistance.

\[ F_{\text{rolling}}=C_r\,mg,\qquad F_{\text{grade}}=mg\sin\theta\approx mg\cdot(\text{grade fraction}) \]
Rolling resistance is a fixed fraction of weight; grade resistance is the downslope weight component (≈ mg × grade for modest slopes).
Rolling resistanceF_roll = Cr·mg (hysteresis)energy lost deforming the patchGrade resistanceslope thetamg (weight)mg·sinθ down slope
Rolling resistance arises from tyre hysteresis in the contact patch (energy lost deforming the carcass). Grade resistance is the downslope weight component mg·sin theta.
🔑 Grade dwarfs rolling resistance

Compare the two at the same weight. Rolling resistance at Cr = 0.012 is about 1.2% of the car's weight. A 12% mountain grade is ten times larger — 12% of the weight pulling the car downhill. This is why a car that cruises effortlessly on the flat labours up a steep hill: the grade term, not rolling resistance or drag, suddenly dominates the road load. It is also why heavy vehicles need such low crawl gears on grades.

📝 Worked example: A 1500 kg car on radial tyres (Cr = 0.012) climbs a 8% grade at low speed. Find the rolling resistance and the grade resistance, and their sum (use g = 9.81 m/s², and approximate sin θ ≈ 0.08).
  1. Rolling resistance = Cr·mg = 0.012 × 1500 × 9.81 = 176.6 N
  2. Grade resistance = mg·sin θ = 1500 × 9.81 × 0.08 = 1177.2 N
  3. Combined low-speed road load = 176.6 + 1177.2 = 1353.8 N
✓ F_roll ≈ 177 N, F_grade ≈ 1177 N, total ≈ 1354 N
✏️ Practice: A 1200 kg car on tyres with Cr = 0.010 rolls on the flat (no grade). What is its rolling resistance? (g = 9.81)
N
Solution
  1. F_roll = Cr·mg = 0.010 × 1200 × 9.81 = 117.7 N

Check your understanding

1. Rolling resistance is best modelled as approximately:
Tyre hysteresis loss scales with the vertical load, so rolling resistance is a roughly constant fraction C_r of weight over normal speeds.
2. Compared to rolling resistance on a steep (12%) grade, the grade resistance is:
A 12% grade resists with ~12% of the vehicle weight, versus ~1.2% for rolling resistance — about ten times larger, which is why hills dominate road load.
✅ Key takeaways
  • Rolling resistance ≈ Cr·mg, a fixed fraction of weight (passenger radials Cr ≈ 0.008–0.015) from tyre hysteresis
  • Grade resistance = mg·sin θ ≈ mg × grade fraction for modest slopes
  • On a steep grade, grade resistance dominates total road load (a 12% grade ≈ 10× a typical rolling term)
  • These two form the speed-independent part of road load; aerodynamic drag is quantified in Module 11
➡️ With rolling and grade quantified, the leftover tractive effort becomes acceleration — which the next lesson integrates over speed to predict the 0–100 km/h time.