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The Analysis
For an in-depth derivation of the power model
that I used for this analysis, check out
this article.
The crux of this analysis was in the
digitization of the racecourse. Using the
scanned drawings from the Redlands Race Bible as
shown below, I was able to numerically represent
the course heading and elevation at 304 discrete
points.

Below are 2-d and 3-d plots of the Mount
Rubidoux prologue TT course.


The next thing necessary to increase the
accuracy of the analysis was to incorporate the
ambient wind conditions. Having witnessed
the TT in person, I estimated the wind at about
2.5 m/s (5.6 mph) coming from the SW (315
degrees with North being 0 degrees). As a
backup, I looked up the average wind conditions
on the 10th of March from the Weather service in
Riverside (details are shown below). It
appears that my assumed wind speed was OK.

Armed with this information, it was simply a
matter of calculating the yaw angle (the angle
created by the rider velocity vector and the
ambient wind vector) at each of the 304 discrete
points along the course. This small detail
drastically increases the accuracy of the
analysis, since most objects that are
streamlined (wheels, aero tubed frames,
aerodynamically positioned cyclists) have drag
values that are dependent on the yaw angle.
As a rule of thumb, drag usually decreases as
yaw angle increases. Most back of the
envelope calculations neglect the yaw angle
dependence – I took the time to incorporate this
feature in my analysis. The following are
the instantaneous yaw angles that were
calculated for Chris Horner’s prologue (the
average yaw angle was 15 degrees):

The Assumptions
Like any theoretical analysis, assumptions
must be made. In this case, it is assumed
that the rider completes the course at a
constant velocity. This assumption is not
entirely realistic since it implies that brakes
are applied to reduce speed on the downhill
sections and that inhuman power output levels
are possible on some of the uphill sections.
This constant velocity assumption is acceptable
when doing a relative comparison of equipment
options. Reality lies somewhere between
the extremes of the constant velocity and
constant power assumptions. For our
purposes, the constant velocity assumption is
satisfactory. The following plot is what I
came up with for Chris Horner’s prologue effort
(note the negative power sections – this is
where it is assumed brakes are applied to reduce
speed).

The average power that Horner put out during
this effort was calculated to be 470 watts, or
6.7 watts/kg. This value is certainly
high, but seems to be reasonable for a
relatively short 9-minute effort. As a
point of reference, it has been rumored that
Lance Armstrong has maintained a 7+ watt/kg
output during the extend climbs during the Tour
de France.
The Results
With the baseline case of Chris Horner’s
prologue dialed in to produce believable results
(he used mid depth carbon wheels, a standard
road bike and mini aero-bar extensions), it was
time to start changing equipment and seeing how
it affected the final time.
Rear Disk: - 400 grams heavier:
Would have reduced the power requirement by 2.2
watts and saved 2.6 seconds.
Rear Disk and TT bike (10% lower drag
coefficient (Cd) of the frame and 2% lower Cd of
the rider):
6.1 watts less power and 7.0 seconds faster.
Lightweight box section,
conventional, wheels - 400 grams lighter:
Would have increased the power requirements by
9.2 watts and increased the overall time by 10.3
seconds.
No aero extensions: (10% greater Cd
of rider and 200 grams lighter):
Increases power requirements by 13.8 watts and
increases overall time by 15.4 seconds.
How much additional weight could have
Horner carried up the hill and still won?
3.4 kilos (7.5 lbs).
If the climb was twice as steep (~5%
grade) and Horner averaged 470 watts:
Time would increase by 146 seconds (average
speed of 28.4 kph/17.4 mph)
Using a rear disk would be .1 seconds slower
Using lightweight conventional wheels would be
4.7 seconds slower
If the climb was three times as steep
(~7% grade) and Horner averaged 470 watts:
Time would increase by 336 seconds (average
speed of 21.5 kph/13.3 mph)
Using a rear disk would be 2.7 seconds slower
Using lightweight conventional wheels would be
.3 seconds slower
These “steeper hill” results lead one to
believe that for Horner, the break even point
for a disk versus mid section carbon wheels is
17.4 mph or an ~5% grade. The break even
for lightweight conventional wheels versus mid
section carbon wheels is an average speed of
less than 13.3 mph or greater than a 7% average
grade.
It should be clear by now that even though
the Rubidoux TT is uphill, aerodynamics should
guide the equipment selection.
To go as fast as possible on this course,
the equipment used should be the same as for a
40k flat TT. Chris Horner
had a really great ride during the prologue and
completely demonstrated his intention to
dominate the stage race. However, I think
that he could have gone even faster if he had
used a TT bike with full aero bars and a rear
disk.
Team Saturn appears to have figured this
setup out – nearly all of their team (men’s and
women’s) rode full TT setups in 2001 and 2002.
They wound up taking 2 out of the top 5 spots in
the men’s race in 2001 and 3 out of the top 5
spots in the 2002 men’s race. Good form,
or good equipment choice? The truth
probably lies somewhere in between. More
importantly, though, Chris Horner proved that
the mind and the body are the most “significant”
variables when determining cycling performance.
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