The wind vector thing and how it affects the wheel aerodynamics still bugs me.
If the wind is coming from straight ahead of you, it’s obviously a headwind. Let’s call straight ahead “Zero Degrees”. Directly behind you is 180 degrees. Zero degree apparent wind only happens in three instances when riding a bike: 1) when there is no wind. 2) when there is a headwind directly in front of you. 3) when there is a tailwind directly behind you…but, you are going faster than the tailwind. Of course, the only time there is no apparent wind is when you have a wind from 180 degrees and you are matching that wind speed exactly.
As the wind comes from somewhere within 90 degrees from Zero, it’s direction originates from a point that allows us to refer to it as a headwind, but with an apparent direction (or vector) skewed somewhat towards Zero depending upon your forward speed and the speed of the wind. When the wind originates from Greater than 90 degrees in front of you, it is often referred to as a tailwind, but, the resultant vector (or apparent direction) of the wind is STILL somewhere in front of you, i.e., you still have wind on your nose, as long as you are going faster than the tailwind.
On a relatively calm day, the wind vector is mostly going to stay fairly close to Zero…if you have sufficient speed…say 20 mph. At 20 mph, it takes a 10 mph 90 degree side wind to give you an apparent wind vector of 22.5 degrees. According to the charts, it isn’t until you get to at least 15 degree yaw angles that the tri-spoked wheels finally have less drag than the deep dished wheel. And according to The Committee, I believe it was, the wind speed at the ground is often significantly less than the windspeed at the height of the bicyclist. So, AT THE WHEEL, the wind vector in the above example might be only 15 degrees…something less than 22.5 anyway. Again, the charts tell me the deep dish wheels have less drag than the trispoke until you reach 15 degree yaw conditions.
Summarizing, it seems to me that the greatest apparent wind vector in our example would be something less than 22.5 degrees (assuming riding 20 mph, with the ground wind speed less than the 10 mph wind speed up on the bicyclist’s nose). Just barely enough apparent wind to produce a yaw angle where the trispoke begins to outperform the deep dish wheel. Hold that thought.
Here’s where it seems to get tricky: as long as your bike speed is at least as fast as the wind speed (in our rider going 20 mph, lets increase the wind speed to 20 mph 90 degree side wind) the greatest apparent wind vector is 45 degrees (remember it would probably be less at the ground level of the wheel). Because as we turn away from the wind, it becomes a rear-quartering wind, i.e., the wind is now coming at 95 degrees, then 110, then 135, etc., BUT the vector moves incrementally back away from 45 degrees toward Zero. IOW, when wind speed equals rider speed, the apparent wind direction doesn’t keep increasing past 45 degrees as the wind becomes rear-quartering.
At 180 degrees, the wind vector in the first example is now 10 mph at Zero degrees (20 mph rider speed minus 10mph tailwind speed). In the second example, there is no apparent wind, because tailwind speed matches the rider’s speed. What is enlightening to me is how the vector changes from Zero when going directly into the wind, to 22.5 degrees as we turn and the wind is coming directly from the side, then incrementally back towards Zero degrees as we continue turning away from the wind until we’ve turned enough to have a 180 degree tail wind, where the vector again reaches Zero.
All this makes me think tri-spokes aren’t nearly as aero as many deep dish wheels in relatively calm conditions under a fast rider, because the tri-spoke advantage doesn’t really show up until you get somewhere over 15 degrees apparent wind vector at the wheel.
It just makes me think the higher wind conditions are where the trispoke design shines, and USUALLY, at least around where I live, we don’t often have strong enough winds to get a 15+ degree apparent wind vector if I’m traveling at 25+mph. That would take at least a 12.5 mph wind from 90 degrees to get the apparent wind vector at the wheel up to the mid-high teens (although the apparent wind vector is at 22.5 at the level of the rider’s nose.)
Furthermore, as the wind leaves the front 90 degree quadrant, your speed should increase due to less wind resistance, which tends to move the apparent wind vector closer to Zero at a given wind speed. That means, on a circular course, with a 12.5 mph wind, and a rider averaging 25 mph, maybe the entire course is ridden with an effective yaw angle at the wheel that favors a deep dish wheel over a trispoke.
I know that side force means a lot regarding handling problems with any wheel, and maybe the deep dish wheels experience a higher side force…but, the part of the deep dish right against the ground may be experiencing much less side force than the part of the wheel at the top…and since you are removing the middle of the trispoke area, maybe the resultant side forces aren’t really all that bad on a deep dish wheel, as long as it isn’t too deep, but, that’s another question.
Any enlightening someone could shine on this model? Something I’m missing or mis-interpreting?