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ADVICE
Wing
selection
We then recommend the configuration best suited to your application. Fine tuning in testing and events will, however, be necessary to get a good balance. Further frequently asked questions are dealt with below under FAQs Whole car advice A comprehensive whole car advisory service is also available to non-wing purchasers through SM AeRo Techniques. GET
A BETTER GRIP WITH Our wings have been proven in the wind tunnel, in CFD studies and on-track to give high levels of downforce with relatively low drag, giving customers good confidence in cornering with good straight line speed. We can also provide CFD evaluations of your wing profiles, either in isolation in 'freestream air' or on a simplified competition car model. We currently have reduced detail models of a GT car and a single seater that can be used for more realistic wing evaluations and comparisons.
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Q. Wings add drag, so won’t I go slower? Q. How wide should my wing be? Q. How high up and how far back should my rear wing be? Q. Is a wing with spanwise ‘twist’ better than a plain, straight wing? Q. How can I tell what the maximum angle of my wing should be?
This answer takes on a more serious technical tone though when discussing applications on closed saloons/sedans and GT cars especially, although this also applies to any type of car really including sports racing and single seater racing cars. Essentially the airflow to the centre section of any wing is the part most adversely affected by the car ahead of it, and the outer sections generally see the ‘cleanest’, most energetic air. Even with a relatively ‘sleek’ GT car the air that encounters the centre part of the wing loses energy during its passage over the car. So it is often the outer sections of a wing that generate the most downforce, and generally speaking because of this a wider wing just adds efficient benefit.
In the case of closed saloons/sedans and GT cars that apply maximum height and maximum rearward positions (often related to maximum roof height and the rearmost extent of the vehicle), generally speaking put the wing as high and as far back as you can. This will enable it to work as well as it can by putting it in the ‘cleanest’ air available. With sports racing and single seater racing categories, usually wing position is defined in technical regulations too, and as high and far back as allowed often works best, and it certainly works well. However, there are instances where a lower and possibly more forward position can interact with a rear diffuser exit and help to generate more efficient downforce from the underbody even though wing downforce might decrease in such a modified location. This is something that can only really be quantified with some form of instrumented testing on track or in a wind tunnel, although a good test driver can help determine the best solution here too. Some single seaters (and some sports racers) run a lower wing tier and an upper wing tier to gain benefit all round in this regard, though this configuration is generally for more potent racecars that are less sensitive to the additional drag that inevitably accrues. Where there are no positional limits, it should be borne in mind that any wing that is behind the rear axle (and the reverse applies to front wings ahead of the front axle) exerts leverage and as such adds more force to the rear wheel contact patches than the wing itself generates. It also exerts leverage that reduces the forces felt at the front wheel contact patches too, and the greater the wing overhang the greater these effects will be. The car’s aerodynamic balance will also be more sensitive to wing angle changes too, since these will have greater effect with greater ‘mechanical overhangs’. A helpful rule of thumb to begin with though is to aim for similar overhangs front and rear, measured to the lowest point on the wing (or front splitter’s) underside, which is roughly where the respective centres of pressure are. At least if the mechanical effects start off similar, it’ll be easier to find an aerodynamic balance. And fine-tuning on track to achieve a balance will always be required once you’ve fitted your wings. With closed saloons/sedans and GT cars with no limit to the rearward location of the wing, it can be of benefit to mount the wing further rearwards so that it’s leading edge is between just overlapping the rearmost part of the car’s boot/trunk by a few centimetres to about roughly in line with it. Two benefits can accrue here; first, the low pressure region that develops below the wing is moved behind the rear ‘deck’ area, which means it all goes towards sucking the wing downwards instead of also sucking the rear deck upwards; and second, that same low pressure region may interact with any rear diffuser that may exist now or in a future development. In terms of how high to put a wing where there is no limit, keep in mind here that the higher a wing is, although it may be in cleaner air and thus perform more as if it was in ‘freestream’ air, the greater will be the leverage from the drag component too, which will also tend to take more weight off the front tyre contact patches as speed builds. The more ‘powerful’ the wing is, the greater this effect will be. But there isn’t really any need to go much over the maximum height of any vehicle to get a wing to work well. The image below shows ‘total pressure’, which is a measure of the total energy of the airstream, along the centreline of a single seater model tested in CFD, and you can see where energy losses occurred compared to the full energy (red) regions. The rear wing seemed to be getting almost a full energy feed at its regulation height (900mm here), and it wouldn’t appear to need raising very much to get it into full energy air, if that were permitted. And as mentioned above, with any vehicle there might even be a lower height at which a stronger interaction with the underbody occurred that could yield a net gain in downforce.
First, there are many forms that spanwise twist can take, but the common form that will be discussed here has the centre section of the wing at reduced angle, relative to the horizontal, compared to the outer sections (see below). The width and angular difference of the ‘raised’ centre section can be more or less than shown in this generic CAD drawing.
But what does this particular spanwise twist do? It’s a shape that is often seen on the back of saloons/sedans and GT cars and simply put, by reducing the angle of the centre section it aims to align the wing profile with the angle of the airflow actually approaching it across the span. The airflow coming down a rear screen is not at the same angle as the airflow that encounters the outer sections of the wing, which if the wing is as wide as the car, is virtually horizontal. If you like, it attempts to achieve the same effective angle of attack relative to the airflow across the whole wingspan. Without this particular twist, a plain wing that is set at a moderate angle relative to the horizontal will effectively be at a steeper angle in the centre, and as the wing’s angle is increased above a moderate angle the flow under the wing may actually start to separate and ultimately stall in the centre as the effective angle becomes too steep. The twist form we see here was one of the earliest methods devised of enabling a single element wing to be pushed to steeper angles on GT cars without causing flow separation or stall in the centre section. However, what this also does is to reduce the wing’s downforce potential at more moderate angles. How so? Well, the centre section of the wing on a closed car already generates less downforce than the outer sections because the air that encounters the centre part of the wing has had to do some ‘work’ in passing over the car’s upper surface, and it loses energy during this passage. The wing cannot therefore develop the same magnitude of low pressure on its central underside, or indeed magnitude of raised pressure on its central upper surface, as the relatively undisturbed air that encounters the wing’s outer sections. See the figure below, which shows the lower surface of a half wing with no twist tested in CFD in freestream (top) and on a GT car (bottom), where the wing end plate is on the right in both cases.
Notice that the region of lowest pressure (blue) in freestream (that is, not on a car but in isolation) is in the centre of the wing, whereas when the wing is on the car the central low-pressure region is much reduced in magnitude (less blue in the centre). This is essentially why wings generate less downforce on a car than they do in isolation, and the extent to which the wing’s performance is affected depends on the extent to which the car affects the airflow that reaches the wing. But even a sleek GT shape will create this effect – a GT car was used in the above trial . So if you then reduce the effective angle of attack of the wing’s centre section by incorporating the type of twist we are discussing here, you further reduce its ability to generate downforce by ‘weakening’ the wing in the region where its downforce potential has already been weakened by the car ahead of it. As was stated above though, a wing incorporating this twist can be set at steeper angles before it starts to stall anywhere across its span, and this is certainly why this form was originally developed, But it is also true that if you need to run a single element wing at or near its peak angle then you might be wise to consider running a dual element wing at a low to medium angle instead, which will allow you to develop greater downforce than a single element’s peak downforce level for less drag, or significantly less drag at the single element wing’s peak downforce level. You will also be able to generate much greater peak downforce should it be required. The twisted wing form here was most likely first developed on GT cars where the regulations did not permit dual element wings, and so it was necessary to maximise the downforce potential of the single element wings that were permitted. However, it is interesting to note that other very different forms of twist were later adopted as more and more efficient plan forms and profile forms were developed for particular applications. Meanwhile, our advice is first and foremost to check that the wing you are thinking of buying has a profile developed specifically for motorsport, as ours have. And to keep things simple, go for a straight untwisted wing that you can optimise the location and angle of on your particular car through testing and evaluation using ‘flow visualisation fluid’ (see below).
However, once you have your wing installed, the question still remains, but there are ways in which you can determine how steep you can set your wing. This is something touched on in the response to the question above, and is probably more applicable to closed saloons/sedans and GT cars where the flow down the rear screen can change the angle of the airflow that encounters the centre section of the wing, depending on the car’s shape and the wing’s position above the car. Ignoring for a moment that you may not want or need to run your wing as steep as possible, here is a method of determining for yourself what the maximum angle of your wing should be. Start this experiment with the wing set to the steepest angle available. Now mix up a small volume of paraffin or diesel fuel (say 25ml) with a few spots of copper grease (to colour the oil). Prepare to run the car, and just before setting off, apply drops of this liquid across the wing along the leading edge. Then accelerate the car quickly up to an appropriate test speed and hold it for 10 to 15 seconds to allow the fluid to streak out along the wing’s underside. Stop, examine and photograph the patterns on the underside. Ideally you will see streak marks all the way back to the trailing edge. But you may not, because parts of the wing may be showing ‘flow separation’. This will be visible where the streak marks stop trailing backwards and instead go sideways. The amount of wing thus affected will hopefully be quite small, but if a significant area is showing flow separation, clean the wing, reduce its angle by one increment and re-run the test. Repeat until at least 90% of the wing is showing good flow attachment, that is, streak marks reach the trailing edge over most of the wing. This can now be taken as the effective maximum angle at which to run your wing. You can also re-run this test at lower speeds to determine the slowest speed at which you see adequately attached flow, which if you like is the speed at which the wing starts to ‘work’. In the case of closed cars with low mounted wings, because the centre section of the wing may be prone to flow separation before the outer sections, it will be tempting to reduce the wing’s angle until the centre section shows full flow attachment, as described above. But in reality, because the outer sections of a full width wing on a closed car generate most of the downforce, aiming for full attachment across the whole span would miss out on a lot of available downforce. In such a case the wing can be run steep enough that the centre section may show significant flow separation, but as long as the outer sections show no signs of flow separation, additional downforce may still accrue. Unfortunately the only way to be sure of the maximum wing angle in such a case is to carry out some form of instrumented testing on track or in a wind tunnel to measure downforce and drag over the range of available wing angles. But it is possible to make an educated guess for wings mounted within the region bounded by the maximum roof height and the rear of the car (as they often are because of technical regulations). Let’s look at an example. The graphic below from a CFD simulation shows a close up of the rear end of a GT car with a rear spoiler and a rear wing sitting above the spoiler. Velocity vectors are plotted on the centreline here.
The wing is set at +8 degrees here, but it can be seen that the flow vectors are approaching the wing at a downward angle along this centreline slice of roughly 8 degrees with the wing in the location shown. Thus the wing’s effective angle in the centre is more like 16 degrees. And although it can barely be seen in this view, the wing is actually just beginning to show signs of flow separation along its rearmost third at this point across its span. So in all likelihood, if the wing is only just beginning to ‘give up’ in the centre, it would be possible to run it somewhat steeper still, perhaps by another 2 to 4 degrees or so, before downforce gains tailed off and drag started to climb further. So in this instance the maximum angle might be estimated to be in the 10 to 14 degree range. Interestingly, the CFD did show the downforce gains tailing off above 12 degrees, and drag began to climb more steeply. But it’s easy to see that a lot depends on the car’s shape and the exact wing location.
(Divide Newtons by 9.81 to get kg, and multiply kg by 2.2 to get pounds). So looking at the 'alpha' (angle of attack) versus downforce plot, we can see that the dual element wing generated slightly more downforce than the single element wing with similar chord dimension at each of the angles tested. Furthermore, the single element wing’s performance had started to decline at the upper end of the angle range, suggesting the wing was nearing its peak angle, whereas the dual element wing’s plot line was still fairly linear, suggesting its peak was at a higher angle yet, which could yield potentially greater peak downforce when required.
In terms of efficiency, which is to say, downforce versus drag (in BHP absorbed here), there was very little to choose between the wings across much of the range tested. The fact that the curves are virtually coincident tells us that they generated very similar levels of drag at the same level of downforce. At the lowest angle tested the hypothetical single element wing only absorbed 0.63bhp less at 100mph than the dual element wing. In the middle of the range the two curves were essentially coincident, so drag was the same at these downforce levels. And then the hypothetical 400mm single element wing started to generate slightly more drag as it neared the steepest angle tested here, so the dual element wing was more efficient at higher angles and downforce levels. So if you need a 400mm chord wing and your technical regulations allow you to use more than one element, look no further than the high efficiency SM183 dual element wing that can be run across a wide range of angles to match a wide range of applications and downforce requirements. If even higher downforce is required, then the high camber SM203 dual element wing could suit your application. Multi-element configurations are also available. Please enquire for further details. |
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