Jeremy McCreary
Well-Known Member
- Region
- USA
- City
- Carlsbad, CA
My mind wonders when I ride. And when I'm really feeling the total resistance (TR), it sometimes wonders which part I'm fighting most at that moment — air resistance (AR), slope resistance (SR), or rolling resistance (RR)?
Since the question's not entirely academic, decided to find out with a little help from Google Sheets and my bike engineering bible, Bicycling Science (Wilson and Schmidt, 2020, 4th ed). Started close to home with an upright 200 lb rider in street clothing on a 65 lb commuterish ebike on smooth pavement at ground speeds up to 12.5 m/s (28 mph).
Below are some of the resulting plots. These let me find the "crossover" ground speed (Vc) at which AR becomes 50% of TR for the bike and rider above. As ground speed (Vg) leaves Vc behind, AR's piece of the TR pie can only grow, and quickly. Having some feel for which side of Vc you're on could come in handy when you need to conserve battery or legs.
Looked at 4 common cases:
A. No wind, no grade
B. No wind, 5% grade
C. Moderate (4.5 m/s, 10 mph) headwind, no grade
D. 4.5 m/s headwind, 5% grade
Each plot splits out the relative contributions that AR, SR, and RR make to TR. They show power loss rather than resistance, but the relationships are exactly the same through either lens. Note that these plots say nothing about TR itself. I try to give some idea of how TR varies from case to case in the text. Look for Vc in each case.
Case A: No wind, no grade, Vc ≈ 4.1 m/s (9 mph). Compared to the other cases, TR is at a minimum at all speeds, and below this rather slow Vc, RR dominates.
Case B: No wind, 5% grade, Vc ≈ 12.5 m/s (28 mph). TR is significantly greater than in Case A at all ground speeds, and below Vc, SR dominates.
Case C: Moderate (4.5 m/s, 10 mph) headwind, no grade, Vc ≈ 0 m/s (0 mph). TR is less than in Case B at all ground speeds, and AR dominates throughout.
Case D: 4.5 m/s headwind, 5% grade, Vc ≈ 8.0 m/s (18 mph). Compared to the other cases, TR is maximal at all ground speeds — even below Vc, where SR dominates.
Things to note
AR and RR are always present, and AR always dominates TR sooner or later — until even a moderate hill intervenes. At that point, you may get nowhere close to Vc. Not much point in tucking then.
AR grows with the square of airspeed — which of course exceeds Vg in a headwind — but is unaffected by total (bike+rider) weight. Conversely, SR and RR grow linearly with total weight but don't change with speed. RR dominates TR only at very low Vg on the flat with no wind.
A closer look at the plots
Case A vs. B: With no wind and no grade (A), Vc ≈ 4.1 m/s but jumps to 12.5 m/s when a 5% grade comes along (B). Since the latter Vc is generally out of reach on a 5% uphill, SR dominates TR at all feasible speeds in Case B.
Case C vs. D: In a 4.5 m/s headwind, Vc drops to zero on the flat (C) but jumps to 8.0 m/s on adding a 5% grade (D). Since AR will be your main nemesis at all speeds in Case C, makes sense to reduce it on long, flattish rides into a headwind at low or no assist. Your battery and legs will thank you.
Case B vs. D: On a 5% grade, Vc ≈ 12.5 m/s in still air (B) but drops to 8.0 m/s when the headwind comes up (D). Since you're unlikely to reach Vc in either case at low or no assist, small AR countermeasures make little sense.
As you can guess from these trends, reducing AR by getting the rider to streamline by wearing lycra and tucking will raise all Vc values and reduce all TRs. When your goal is to ride far and fast with little or no assist, this can be a signicant effect. The roadies know what they're doing in this regard.
Explanation of symbols in tables accompanying plots (all in SI units)
o Vw = wind speed component in direction of travel relative to ground, headwind-positive
o CdA = drag area
o Da = air density at sea level
o M = mass of bike+rider system
o g = standard acceleration of gravity
o S = road gradient
o Rs = slope resistance
o Cr = coefficient of rolling resistance
o Rr = rolling resistance
Source
The necessary bike and rider parameters CdA and Cr came from Table 5.1, p. 230, Wilson and Schmidt, 2020, Bicycling Science, 4th ed. All resistance and power loss formulas came from elsewhere in the same book, as did determinations of the losses safely ignorable here.
Since the question's not entirely academic, decided to find out with a little help from Google Sheets and my bike engineering bible, Bicycling Science (Wilson and Schmidt, 2020, 4th ed). Started close to home with an upright 200 lb rider in street clothing on a 65 lb commuterish ebike on smooth pavement at ground speeds up to 12.5 m/s (28 mph).
Below are some of the resulting plots. These let me find the "crossover" ground speed (Vc) at which AR becomes 50% of TR for the bike and rider above. As ground speed (Vg) leaves Vc behind, AR's piece of the TR pie can only grow, and quickly. Having some feel for which side of Vc you're on could come in handy when you need to conserve battery or legs.
Looked at 4 common cases:
A. No wind, no grade
B. No wind, 5% grade
C. Moderate (4.5 m/s, 10 mph) headwind, no grade
D. 4.5 m/s headwind, 5% grade
Each plot splits out the relative contributions that AR, SR, and RR make to TR. They show power loss rather than resistance, but the relationships are exactly the same through either lens. Note that these plots say nothing about TR itself. I try to give some idea of how TR varies from case to case in the text. Look for Vc in each case.
Case A: No wind, no grade, Vc ≈ 4.1 m/s (9 mph). Compared to the other cases, TR is at a minimum at all speeds, and below this rather slow Vc, RR dominates.
Case B: No wind, 5% grade, Vc ≈ 12.5 m/s (28 mph). TR is significantly greater than in Case A at all ground speeds, and below Vc, SR dominates.
Case C: Moderate (4.5 m/s, 10 mph) headwind, no grade, Vc ≈ 0 m/s (0 mph). TR is less than in Case B at all ground speeds, and AR dominates throughout.
Case D: 4.5 m/s headwind, 5% grade, Vc ≈ 8.0 m/s (18 mph). Compared to the other cases, TR is maximal at all ground speeds — even below Vc, where SR dominates.
Things to note
AR and RR are always present, and AR always dominates TR sooner or later — until even a moderate hill intervenes. At that point, you may get nowhere close to Vc. Not much point in tucking then.
AR grows with the square of airspeed — which of course exceeds Vg in a headwind — but is unaffected by total (bike+rider) weight. Conversely, SR and RR grow linearly with total weight but don't change with speed. RR dominates TR only at very low Vg on the flat with no wind.
A closer look at the plots
Case A vs. B: With no wind and no grade (A), Vc ≈ 4.1 m/s but jumps to 12.5 m/s when a 5% grade comes along (B). Since the latter Vc is generally out of reach on a 5% uphill, SR dominates TR at all feasible speeds in Case B.
Case C vs. D: In a 4.5 m/s headwind, Vc drops to zero on the flat (C) but jumps to 8.0 m/s on adding a 5% grade (D). Since AR will be your main nemesis at all speeds in Case C, makes sense to reduce it on long, flattish rides into a headwind at low or no assist. Your battery and legs will thank you.
Case B vs. D: On a 5% grade, Vc ≈ 12.5 m/s in still air (B) but drops to 8.0 m/s when the headwind comes up (D). Since you're unlikely to reach Vc in either case at low or no assist, small AR countermeasures make little sense.
As you can guess from these trends, reducing AR by getting the rider to streamline by wearing lycra and tucking will raise all Vc values and reduce all TRs. When your goal is to ride far and fast with little or no assist, this can be a signicant effect. The roadies know what they're doing in this regard.
Explanation of symbols in tables accompanying plots (all in SI units)
o Vw = wind speed component in direction of travel relative to ground, headwind-positive
o CdA = drag area
o Da = air density at sea level
o M = mass of bike+rider system
o g = standard acceleration of gravity
o S = road gradient
o Rs = slope resistance
o Cr = coefficient of rolling resistance
o Rr = rolling resistance
Source
The necessary bike and rider parameters CdA and Cr came from Table 5.1, p. 230, Wilson and Schmidt, 2020, Bicycling Science, 4th ed. All resistance and power loss formulas came from elsewhere in the same book, as did determinations of the losses safely ignorable here.
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