Frontal area is but one variable that affects
the overall aerodynamics of a given object.
The equation minded folks out there might
recognize the following equation for aerodynamic
force:

Where: F= aerodynamic
force
= air density
u = air speed
Cd = non-dimensional force coefficient (function
of the shape of the object)
A = frontal area
In order to simplify things, it is often
convenient to rearrange the above equation such
that all the terms that don’t change during a
comparative analysis are on one side of the
equal sign and everything else is to the other.
In this case, the simplification looks something
like this:

You may have heard some of the geeky types
like myself refer to a thing known as “CdA” –
well, the above formula is what this term
references. It is simply a way of
describing the aerodynamics of an object.
The “A” is the projected frontal area; while the
Cd is the force coefficient and is a function of
the shape of the object (e.g. a flat plate has a
higher Cd than an equivalently sized sphere…)
Let’s take a look at an application of this
un-wieldy equation: a 0.5 meter tall by 0.5
meter wide piece of plywood presents a frontal
area of 0.25 m^2 (i.e., 0.5 x 0.5 =0.25) when it
is placed broadside to the wind. Cd for a
flat plate has been documented in the literature
as ~1.12 -> this Cd value has also been shown to
be independent of frontal area. The
resultant CdA for this particular piece of
plywood is therefore 0.28 (or just a shade worse
than Tyler Hamilton’s standard time trial
position - heh, does that mean that TH’s
position is not a whole lot better than a piece
of plywood???)
The logic of the argument presented then follows
that if Cd is constant and the frontal area is
subsequently decreased, the overall aerodynamics
of the smaller frontal area object will be
better (since the product of Cd and A will be
smaller). Looking at the plywood example
presented earlier, we can determine that a 0.4m
by 0.4m piece of plywood presents a frontal area
of 0.16 m^2 and therefore would have a CdA of
~0.18 – which means that the smaller piece of
plywood has a smaller CdA (due to its smaller
frontal area) and therefore, is more
aerodynamic. If these pieces of plywood
raced bikes, and produced the same amount of
power, the smaller CdA piece of wood would go
faster simply because it was more aerodynamic.
Pretty easy stuff, huh?
Well, the underlying assumption that this type
of analysis relies on is that the Cd of the
object (in this case, a cyclists’ hands) does
not change for small changes in orientation.
This assumption is more than likely a pretty
good one, and indeed there does exist some
tunnel data out there (based on cyclists, not
cyclist’s hands, however) that supports this
constant Cd assumption. Furthermore, from
my previous work in the wind tunnel where I
studied fork aerodynamics, projected area by
itself is an excellent proxy for evaluating
aerodynamics outside of a wind tunnel.
The Straight Aero Bar Extension Trend
Jan Ullrich, or was it Jens Voigt, has made the
straight aero bar extension the latest fad/trend
in the TT product world. The internet is
full of people describing just how they took a
hacksaw to their $400 one-piece bars (like the
Easton Attack, CSC Vision Tech, Profile Carbons,
etc...) so that they could adopt the Ullrich/Voigt
hand position. I mean heck, those guys are
winning with those style of bar extensions, so
it MUST be fast, right?
Applying the tenuous “constant Cd” assumption
discussed previously, I set out to see how these
straight aero bars, or more precisely, the
resultant hand position required to grab onto
that style of bar affected measured frontal
area. The reasoning goes that if the
frontal area was smaller with a particular hand
position, well, that would be the aero bar
extension that everyone’s just “gotta” have…
The experiment consisted of sitting myself in a
chair while wearing lots of black (so that my
hands would be easy to extract from the digital
picture) and rotating my hands downward in ~ 10
degree increments.