With those skinny cables, I can’t believe that they really are that much of a factor aerodynamically, either, but I could be wrong.
Chet Kyle gives the drag of cable housing as 18 g/in (yes, he used those mixed units).
Cable housing has an OD of less than 0.200". Assuming a Cd of ~1 for a cylinder perpendicular to airflow with Reynolds number of 3000, a 1-inch long cylinder has a CdA of 0.000130 M^2. Using your ROT, this should be worth only 130mg of drag, not 18g. Is that Kyle figure off by a factor of 10?
CdA = (1.0 ) * ( 0.005m x 0.0254m ) = 1.27e-04 m^2 (check)
F = CdA * 1/2 * rho * v^2
= ( 1.27e-04 m^2) * ( 0.5 * 1.2 kg/m^3 * 12 m/s * 12 m/s ) @ 12 m/s
= 0.0109 N
We have to remember that the grams reported are at a tunnel speed of 30 mph (i.e. 13.4 m/s). Also, I get an Re of ~7000 and assume a cylinder Cd of ~1.2, meaning a CdA of .00016 m^2…
In that case (and using the same rho) I get a drag force (@30 mph) of .017 N, or .017 kg-m/s^2.
Not sure why one would want to translate this to grams…
Yeah…that’s one of those “tradition” things…anyway, to check on the original question we divide the force value in Newtons by g, or 9.81 m/s^2
.017 N / 9.81 m/s^2 = .0018 kg = 1.8 g
Looks like AC was off by a factor of 10 when quoting Mr. Kyle, not 100.
… but multiplying by velocity will give the power lost:
P = 0.0109 N * 12 m/s
= 0.132 W
The ROT says at race speeds the 1.8g per inch would be worth ~ 0.2W per inch of exposed housing.
Double checking with the CdA calculated above:
Power = 1/2 * (1.2 kg-m/s^2) * (.0016 m^2) * (12 m/s)^3 = 0.17W per inch of exposed housing.
This leads into a related question regarding housing-less center-pull brakes. Does eliminating, say, 4 inches of housing in a brake setup (a la Hooker) have a measurable CdA reduction? (Using the .000130 M^2/in number, the CdA reduction is only .0005 M^2 – worth maybe 0.5W
For 4 inches of exposed cable, it looks more like closer to 1W…but, 4 inches seems a bit short for most folks’ setups…
Of course, none of this takes into account (for a front brake) the reductions in drag gained by eliminating the large brake arms hanging out in the breeze and the smaller overall frontal area and “smoothness” of something like a Hooker brake.