So . . .
I promise, last post of polar charts. I need to show one more thing, but in the process, I noticed something . . .
Pulling up the polar charts of each airfoil over several Re, something popped out:
If you look, the tan line is for 50k Re, which equates to roughly 10mph for this wing . . . notice on several of the charts it separates from the others -- it's particularly obvious on the Cl v. Alpha. What's going on? This airfoil can't maintain laminar flow over that low of an Re -- it's going to work very poorly at low speeds, which is decidedly not-friendly in a landing.
So GOE 611, it was an interesting run, but you're out!
. . . and then there was one . . .
So the last thing I wanted to show with the charts was how to set the AoA on the airframe. We'll assume everything else is streamlined to the fuselage in cruise. Two of the Alpha charts become handy for setting the angle -- Cl/Cd v. Alpha, and Cd v. Alpha -- depending on what we want from the plane:
So if we wanted to go for an efficient flight -- glider or cargo planes -- we look at the Cl/Cd v Alpha. Find the peak and we have roughly the most efficient AoA for that airspeed (Re). The wing will be generating the most lift there for the same drag cost, and the peak doesn't shift much with airspeed. For a glider this means it can create the most lift per unit drag at that AoA, so in strong lift, this is an ideal angle to take in lift (for streamline out of lift we'll pick a different AoA on the airframe, but in flight it will set this my pitching up). For a cargo plane, it sets this angle in cruise and can adjust it's airspeed to balance the lift with it's weight. For this airfoil, it happens just over 6 degrees . . .
. . . and is totally wrong for a racer.
A racer is about speed at all costs. Efficiency isn't the mountain to climb, instead drag is the enemy to conquer. For that, we look at the Cd v. Alpha. Find the bottom of the trough, and there we are. Pulled up the numbers and Cd hit's bottom about 0.5 degrees. At other Re, it varied between 0.5 and 0.75 degrees . . . so 1/2 a degree it is!
Not a huge surprise, but if you look at the foil, the centerline has an upward tilt to it already, pushing the nose down . . . anyone want to guess by how much?
So we import the foil, rotate it up 0.5 degrees (BTW, the bottom is now flat and level), draw a line off the cockpit to the top of the wing, nudge the airfiol a bit to line up . . .
and the wing has a cross section
'bout time
Now we're ready to trace some points, and flatten a few of the primary structures . . .
I promise, last post of polar charts. I need to show one more thing, but in the process, I noticed something . . .
Pulling up the polar charts of each airfoil over several Re, something popped out:
If you look, the tan line is for 50k Re, which equates to roughly 10mph for this wing . . . notice on several of the charts it separates from the others -- it's particularly obvious on the Cl v. Alpha. What's going on? This airfoil can't maintain laminar flow over that low of an Re -- it's going to work very poorly at low speeds, which is decidedly not-friendly in a landing.
So GOE 611, it was an interesting run, but you're out!
. . . and then there was one . . .
So the last thing I wanted to show with the charts was how to set the AoA on the airframe. We'll assume everything else is streamlined to the fuselage in cruise. Two of the Alpha charts become handy for setting the angle -- Cl/Cd v. Alpha, and Cd v. Alpha -- depending on what we want from the plane:
So if we wanted to go for an efficient flight -- glider or cargo planes -- we look at the Cl/Cd v Alpha. Find the peak and we have roughly the most efficient AoA for that airspeed (Re). The wing will be generating the most lift there for the same drag cost, and the peak doesn't shift much with airspeed. For a glider this means it can create the most lift per unit drag at that AoA, so in strong lift, this is an ideal angle to take in lift (for streamline out of lift we'll pick a different AoA on the airframe, but in flight it will set this my pitching up). For a cargo plane, it sets this angle in cruise and can adjust it's airspeed to balance the lift with it's weight. For this airfoil, it happens just over 6 degrees . . .
. . . and is totally wrong for a racer.
A racer is about speed at all costs. Efficiency isn't the mountain to climb, instead drag is the enemy to conquer. For that, we look at the Cd v. Alpha. Find the bottom of the trough, and there we are. Pulled up the numbers and Cd hit's bottom about 0.5 degrees. At other Re, it varied between 0.5 and 0.75 degrees . . . so 1/2 a degree it is!
Not a huge surprise, but if you look at the foil, the centerline has an upward tilt to it already, pushing the nose down . . . anyone want to guess by how much?
So we import the foil, rotate it up 0.5 degrees (BTW, the bottom is now flat and level), draw a line off the cockpit to the top of the wing, nudge the airfiol a bit to line up . . .
and the wing has a cross section
'bout time
Now we're ready to trace some points, and flatten a few of the primary structures . . .