This is a road I know very well.Hello,
First of all, I would like to apologize for the delay in my new post. Before Christmas, there was a lot of work to be done in the office/job and I deliberately wanted to switch off and spend the Christmas holidays with my family in peace. But now it's starting again.
Finding a good sparring partner for the outer airfoil has proven to be very difficult. It should be a well-known airfoil with comparable thickness and camber and designed for a similar purpose. In the end, I ended up with the good old MH30 from Martin Hepperle. This airfoil is very suitable for small and fast slope gliders up to about 2.0m wingspan. In the mid/late 90s, a large number of F5b class models were profiled with the MH30 because it was simply a force in high-speed flight. It is slightly thinner than my THOR.2 design; the camber is almost identical... About 10 years ago, Philip Kolb published a profile strake for medium-sized slope and aerobatic models based on the MH30. Due to his fame, the similar “hard facts” and the public availability, it seems to me to be a good choice for a airfoil comparison.
The following picture shows the MH30 and the Thor.2 outer profile in comparison. The equivalent Vrace profile is also included again. In the area of the main wing with a class-typical chord length, we are in the range of Re100k – Re400k, depending on the flight speed. Whereby Re400k is already very fast...
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A similar design philosophy can certainly be seen here. The THOR.2 has a clear advantage here, although its lead decreases as the Re numbers increase.
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Like the base, the THOR.2 outer profile is at its strongest in EM-style turns. The MH30 is on a comparable level. However, Martin Hepperle's design is clearly at a disadvantage in tight turns. At this point, even the Vrace has a strong opponent in the THOR.2.
Finally, here too is the glide polar (type 2 – constant lift). Here, the MH30 is slightly ahead at the maximum rate of climb. When gliding in the slope flight typical range, the THOR.2 is again ahead.
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There is another Re-number-adapted profile at the very outer wing. Basically, it is “only” the profile presented here, slightly thinned out and with a stronger thickness overlay. Finally you can see the entire profile strake of the THOR.2 wing.
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FLZ-Vortex
I use a small program called FLZ-Vortex to simulate the wing. This tool is very good at simulating the stall behavior in a surprisingly realistic way. In the following picture, you can see how the stall announces itself on the THOR.2 wing.
The green dashed line represents the lift that the profile can provide. The solid green line shows the actual lift coefficient. If this is now above what the profile can deliver, the flow breaks away (stall). Shown here as a red area. In this simulation, the very outside wing tip should be treated with caution. At such small Re numbers/wing depths, these simulations fail. The middle area of the wing is more exciting:
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Here you can clearly see that the stall begins in the middle of the entire wing and expands outwards with increasing lift. This causes the aircraft to feel rather spongy or soft at first, or ideally it simply sags. This is exactly what we want to achieve for a gentle stall behavior.
If the stall were to occur first on the outer wing, the model would most likely tip over to one side...
As mentioned at the beginning, I didn't want to design an ultra-thin wing with the THOR.2. Thin profiles may feel light and agile and, in the Re number range relevant to this model, they also have good drag coefficients, but in my experience they also need more attention in flight and certainly during construction. When it comes to getting torsion under control in the wing, it takes either height or (high-quality) material. The latter costs more to buy and ultimately drives up the model price. I would like to mitigate this by using height/thickness. 8.14-8.00-7.54% are not exactly thick profiles either, but I think they are a good compromise.
So, that was the layout of the wing roughly explained.
Next up is the tail unit (only very briefly) and the fuselage design. Jerry and his team have also been very busy. Shortly before Christmas, I received a photo of the first finished model. I can't wait to finally hold the first two models in my hands!
Kind regards,
Mario
Planform is the secret.Yes, Wayne, correct! There is no twist in the wings. It‘s just taking an eye on the airfoil and planform… I do not like twist on speedwings.
At the moment I‘m working on a Pilatus B4 wing… maybe this will be the first time I need a twist![]()
That depends entirely on why the designer would even consider adding a twist to the wing in the first place. No designer ever does something unless there is a requirement or a perceived advantage - at least, I don't.Personally, I wouldn't want to install a twist on a speed or all-round model. I see absolutely no need for it. But on a highly specialized thermal model, e.g. F3j or F5j, you can think about it. When circling tightly in the beard, perhaps only just above the ground, foolproof stall behavior is important. A moderate twist (see Prestige2 PK model) can certainly help here.
Well, designing a Horten-Wing cleanly is actually something else... The missing vertical tail must be compensated for by appropriate adjustments to the wing. Birds have a similar “problem”... But they also have fly-by-wire integrated as standard.
Fast birds are not necessarily fast in pure gliding flight. They are very fast in a nosedive (peregrine falcon, golden eagle), but here they have their wings largely laid out. The overall shape of the body is important here. Birds can also become fast in flapping flight. In this case, their wings not only fulfill the purpose of generating lift, but also propulsion. In pure gliding flight, a bird must fly mainly energy-efficiently. There is very interesting research into bird flight and we can still learn a great deal from nature...
There are applications for twisting, but I don't see them on speed or allround-oriented models with tail units.
Hi Andrew.I saw a link to this thread in an email from Aloft and thought I'd pop in and take a look.
The reference to wing twist was what caught my eye. From other reading, I remember that the NASA Prandtl-D flying project from a few years back claimed a significant reduction in induced drag, more than 10%, I believe.
One proposed real world application was for improved fuel economy in commercial aviation. I don't know if the concept has been acted on, but certainly wingtip devices are in widespread usage for the same reason -- and they could be considered a variant of the Prandtl approach. I suppose it would be better to say that the Prandtl bell-shaped span loading could be considered a more extensive implementation of the same principles. At least, these are the thoughts of some much more experienced aerodynacists than yours truly.
Ever since coming across the Prandtl project, I've wondered if there might benefits for a model glider model with a conventional tail. If someone's tried it, I haven't found any info on their results. The challenge of building a wing with a non-linear twist is definitely a bit off-putting. That said, there are a number of documented Prandtl-type models in existence, including a least one offered as a kit. I have one in progress at the moment.
I'll add a few links that I've enjoyed:
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US9382000B1 - Aircraft design - Google Patents
The present invention is an aircraft wing design that creates a bell shaped span load, which results in a negative induced drag (induced thrust) on the outer portion of the wing; such a design obviates the need for rudder control of an aircraft.patents.google.com
There is a trick to reducing the interference and induced drag.I'm amazed that fuselage drag adds up to that much especially since he broke out induced drag into its own section.
I'm curious if you have seen a study or have studied a low mounted wing on the same fuselage section compared to a top mount?
Yes, I was surprised by that too. The graphic shown with Martin Hepperle (MH-Airfoils) is already a few years old. The late Max Steidle, designer of many really excellent models (e.g. Shino F3f/b, Sensor F5J), did wind tunnel tests with the Shinto some time ago and was able to confirm MH's statements about the fuselage resistance, among other things. I don't know the exact results, but it led to Max also slimming down his fuselage designs for fast models.I'm amazed that fuselage drag adds up to that much especially since he broke out induced drag into its own section.
I'm curious if you have seen a study or have studied a low mounted wing on the same fuselage section compared to a top mount?