A Study Of Aerodynamic Drag On Faired HPV's
by John Lafford

I was inspired to run some comparison calculations following the publication of the data from Sam Whittingham in BHPC issue 66, particularly after his predictions proved to be quite accurate.  The equations for the calculations are taken from my note in 'So You Want to Build an HPV' entitled "Drag Coefficients for All' on page 40, and inserted into an Excel spreadsheet.

The calculations have been grouped into sets to give interesting information in a number of areas and allow comparisons to be made between different venues (altitude) and slopes. Also information about several famous machines is included. The info about US machines is gathered from IHPVA magazines and the Bean data is from wind tunnel tests conducted at MIRA in 1992, courtesy of John Kingsbury, plus results from the successful hour record run.

All the machines are compared at sea level on level ground at 50 mph to show how the power requirements differ between them. Then all the machines make an attempt on the hour record using a known standard 1 hour power input , PKH, (Pat Kinch for 1 hour). This shows the Yellow Bean at 47 miles (as set) rising to 51.5 miles for the Varna Diablo.  Finally, a selection is made of the best features from all the contenders, plus very good available tyres to show what could be achieved.  This shows that there is still plenty of scope for designers and riders to make new records.


Set 1

Diablo as used to set the record at 4500 ft altitude with 0.006 slope and tyres with Crr = 0.006. The drag coefficient is selected as 0.11 to fit the information supplied by Sam Whittingham.

Machine Weight
kg
Rolling
Resistance
Coefficient
Crr
Drag
Coefficient
Cd
Area
sq.m
Cd.A
sq.m
Air
density
factor
Slope Speed
mph
Speed
km/h
Power
Watts
Conditions
(altitude / slope)
Diablo 100 0.0060 0.110 0.1830 0.0201 0.816 -0.006 20 32.2 7 At 4500 ft. altitude and 0.006 slope
30 48.3 24
40 64.4 58
50 80.5 112
60 96.5 194
70 112.6 309
80 128.7 461
82.2 132.3 500



Set 1a

This shows that the slope was worth 216 Watts of extra effective power.

Machine Weight
kg
Rolling
Resistance
Coefficient
Crr
Drag
Coefficient
Cd
Area
sq.m
Cd.A
sq.m
Air
density
factor
Slope Speed
mph
Speed
km/h
Power
Watts
Conditions
(altitude / slope)
Diablo 100 0.0060 0.110 0.1830 0.0201 0.816 0 82.2 132.3 716 Level ground



Set 2

As Set 1 but using better (available) tyres, showing that the record could go up to 88mph at the 500 W input power.

Machine Weight
kg
Rolling
Resistance
Coefficient
Crr
Drag
Coefficient
Cd
Area
sq.m
Cd.A
sq.m
Air
density
factor
Slope Speed
mph
Speed
km/h
Power
Watts
Conditions
(altitude / slope)
Diablo 100 0.0030 0.110 0.1830 0.0201 0.816 -0.006 20 32.2 -19 At 4500 ft. altitude and 0.006 slope; better tyres
30 48.3 -15
40 64.4 5
50 80.5 47
60 96.5 116
70 112.6 217
80 128.7 356
88.1 141.8 500



Set 3

As set 1 but coming down to sea level, which would make a record at 77mph.

Machine Weight
kg
Rolling
Resistance
Coefficient
Crr
Drag
Coefficient
Cd
Area
sq.m
Cd.A
sq.m
Air
density
factor
Slope Speed
mph
Speed
km/h
Power
Watts
Conditions
(altitude / slope)
Diablo 100 0.0060 0.110 0.1830 0.0201 1 -0.006 20 32.2 9 At sea level, 0.006 slope
30 48.3 30
40 64.4 71
50 80.5 138
60 96.5 238
70 112.6 378
76.9 123.7 501



Set 4

As Set 3 but on level ground giving a 'true' record of 66.6mph.

Machine Weight
kg
Rolling
Resistance
Coefficient
Crr
Drag
Coefficient
Cd
Area
sq.m
Cd.A
sq.m
Air
density
factor
Slope Speed
mph
Speed
km/h
Power
Watts
Conditions
(altitude / slope)
Diablo 100 0.0060 0.110 0.1830 0.0201 1 0 20 32.2 61 At sea level, level ground
30 48.3 109
40 64.4 176
50 80.5 269
60 96.5 396
66.6 107.2 501



Set 5

As Set 4 but using better tyres takes the record to 71.6mph.

Machine Weight
kg
Rolling
Resistance
Coefficient
Crr
Drag
Coefficient
Cd
Area
sq.m
Cd.A
sq.m
Air
density
factor
Slope Speed
mph
Speed
km/h
Power
Watts
Conditions
(altitude / slope)
Diablo 100 0.0030 0.110 0.1830 0.0201 1 0 20 32.2 35 At sea level, level ground; better tyres
30 48.3 69
40 64.4 123
50 80.5 203
60 96.5 317
70 112.6 470
71.6 115.2 499



Set 6

As Set 3 at sea level and level ground, but using better tyres, showing the best legal record possible with the Diablo at sea level of 82.0mph. But compare with Set 1 at 50mph where it required 112 W, but in Set 6 only required 72 Watts.

Machine Weight
kg
Rolling
Resistance
Coefficient
Crr
Drag
Coefficient
Cd
Area
sq.m
Cd.A
sq.m
Air
density
factor
Slope Speed
mph
Speed
km/h
Power
Watts
Conditions
(altitude / slope)
Diablo 100 0.0030 0.110 0.1830 0.0201 1 -0.006 20 32.2 -17 At sea level, 0.006 slope; better tyres
30 48.3 -10
40 64.4 18
50 80.5 72
60 96.5 159
70 112.6 286
80 128.7 459< /td>
82 131.9 500



Set 7

Yellow Bean using data from MIRA tests, 1 hour world record set at 47mph and tyre test data from the actual tyres tested by me [I think the tyres were Moulton slicks.  This was the machine in which Pat Kinch set the Hour record of 46.96 miles / 75.6 km - DL].

Machine Weight
kg
Rolling
Resistance
Coefficient
Crr
Drag
Coefficient
Cd
Area
sq.m
Cd.A
sq.m
Air
density
factor
Slope Speed
mph
Speed
km/h
Power
Watts
Conditions
(altitude / slope)
Yellow Bean 98 0.0054 0.075 0.4153 0.0311 1 0 20 32.2 60 At sea level, level ground
30 48.3 115
40 64.4 202
50 80.5 329
60 96.5 507
70 112.6 747



Set 8

Bean II with data from MIRA, and using the same tyres as the Yellow Bean. This shows about 6% improvement over the Yellow Bean [The brown one - slightly improved shape and full monocoque construction.  Set assorted sprint records at RAF Fairford in 1992 - DL].

Machine Weight
kg
Rolling
Resistance
Coefficient
Crr
Drag
Coefficient
Cd
Area
sq.m
Cd.A
sq.m
Air
density
factor
Slope Speed
mph
Speed
km/h
Power
Watts
Conditions
(altitude / slope)
Bean II 98 0.0054 0.065 0.4450 0.0289 1 0 20 32.2 59 At sea level, level ground
30 48.3 112
40 64.4 194
50 80.5 313
60 96.5 481
70 112.6 705



Set 9

This shows what the Bean II could have achieved in the sprint event at Battle Mountain where it could have given Diablo [and Kyle Edge - DL] a good challenge at 77mph.

Machine Weight
kg
Rolling
Resistance
Coefficient
Crr
Drag
Coefficient
Cd
Area
sq.m
Cd.A
sq.m
Air
density
factor
Slope Speed
mph
Speed
km/h
Power
Watts
Conditions
(altitude / slope)
Bean II 98 0.0030 0.065 0.4450 0.0289 0.816 -0.006 20 32.2 -15 At 4500 ft. altitude and 0.006 slope; better tyres
30 48.3 -4
40 64.4 31
50 80.5 97
60 96.5 202
70 112.6 354
77.4 124.5 500



Set 10

Data for Cheetah at the 8000 ft altitude used to record 68mph. No slope is allowed for, though there probably was one.

Machine Weight
kg
Rolling
Resistance
Coefficient
Crr
Drag
Coefficient
Cd
Area
sq.m
Cd.A
sq.m
Air
density
factor
Slope Speed
mph
Speed
km/h
Power
Watts
Conditions
(altitude / slope)
Cheetah 93 0.0060 0.055 0.5063 0.0278 0.75 0 20 32.2 58 At 8000 ft. altitude, level ground
30 48.3 104
40 64.4 171
50 80.5 265
60 96.5 394
68 109.4 526



Set 11

Data for Gold Rush at 8000 ft and 0.004 slope as used in winning the Du Pont prize at 65.45mph in 1986. It shows that a whopping 672 Watts was required from Fred Markham to achieve this.

Machine Weight
kg
Rolling
Resistance
Coefficient
Crr
Drag
Coefficient
Cd
Area
sq.m
Cd.A
sq.m
Air
density
factor
Slope Speed
mph
Speed
km/h
Power
Watts
Conditions
(altitude / slope)
Gold Rush 80 0.0100 0.100 0.4645 0.0465 0.75 -0.004 20 32.2 57 At 8000 ft. altitude, 0.004 slope
30 48.3 115
40 64.4 206
50 80.5 344
60 96.5 538
65.45 105.3 672



Set 12

Data for Cutting Edge as quoted by Matt Weaver.

Machine Weight
kg
Rolling
Resistance
Coefficient
Crr
Drag
Coefficient
Cd
Area
sq.m
Cd.A
sq.m
Air
density
factor
Slope Speed
mph
Speed
km/h
Power
Watts
Conditions
(altitude / slope)
Cutting Edge 96 0.0060 0.110 0.2601 0.0286 1 0 20 32.2 63 At sea level, level ground
30 48.3 118
40 64.4 201
50 80.5 322
60 96.5 490
57.6 92.7 445



Set 13

Comparison of all the vehicles at 50mph, which approximates to the present world hour record, where the slope is zero, and at sea level. The machines are listed in descending order of power required showing Gold Rush to be least efficient and Diablo the most efficient with the other machines quite similar.

Machine Weight
kg
Rolling
Resistance
Coefficient
Crr
Drag
Coefficient
Cd
Area
sq.m
Cd.A
sq.m
Air
density
factor
Slope Speed
mph
Speed
km/h
Power
Watts
Conditions
(altitude / slope)
Gold Rush 80 0.0100 0.1000 0.4645 0.0465 1 0 50 80.5 493 At sea level, level ground
Yellow Bean 98 0.0054 0.0750 0.4153 0.0311 50 80.5 329
Cutting Edge 96 0.0060 0.1100 0.2601 0.0286 50 80.5 322
Bean II 98 0.0054 0.0650 0.4450 0.0289 50 80.5 313
Cheetah 93 0.0060 0.0550 0.5063 0.0278 50 80.5 313
Diablo 100 0.0060 0.1100 0.1830 0.0201 50 80.5 269



Set 14

All the machines make an attempt on the hour record using a known standard 1 hour power input , the PKH, (Pat Kinch for 1 hour). This shows the Yellow Bean at 47 miles (as set) rising to 51.5 miles for the Varna Diablo.

Machine Weight
kg
Rolling
Resistance
Coefficient
Crr
Drag
Coefficient
Cd
Area
sq.m
Cd.A
sq.m
Air
density
factor
Slope Speed
mph
Speed
km/h
Power
Watts
Conditions
(altitude / slope)
Gold Rush 80 0.0100 0.100 0.4645 0.0465 1 0 38.9 62.6 286 At sea level, level ground
Yellow Bean 98 0.0054 0.075 0.4153 0.0311 47.0 75.6 286
Cutting Edge 96 0.0060 0.110 0.2601 0.0286 47.4 76.3 286
Bean II 98 0.0054 0.065 0.4450 0.0289 48.0 77.2 286
Cheetah 93 0.0060 0.055 0.5063 0.0278 48.0 77.2 286
Diablo 100 0.0060 0.110 0.1830 0.0201 51.5 82.9 286



Set 15

A selection is made of the best features from all the contenders, plus very good available tyres to show what could be achieved.  This shows that the hour record could be raised to 72.5 miles with existing technology, showing that there is still plenty of scope for designers and riders to set new records.

Machine Weight
kg
Rolling
Resistance
Coefficient
Crr
Drag
Coefficient
Cd
Area
sq.m
Cd.A
sq.m
Air
density
factor
Slope Speed
mph
Speed
km/h
Power
Watts
Conditions
(altitude / slope)
Choice 80 0.0030 0.055 0.1830 0.0101 1 0 72.5 116.7 286 At sea level, level ground



Comment

If we take the parameters of the Choice Machine and run it at Battle Mountain with 500 Watts power input, the speed possible is a staggering 111mph. It is of course not quite valid to do that, as it would take a longer distance to get up to speed, which may not be available, and the rider would not have so much power left at the end of the acceleration phase. However, it would still be frighteningly quick. The results call into question the validity of allowing a small slope to be used on the course as it has such an enormous effect on the results. It is clear that location, location, location is all-important. Ideally we would use courses that are dead flat. In the real world this is unlikely, but I venture to suggest consideration that start and end points of courses should have the same altitude which might make the results more credible.

© John Lafford, January 2002


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