Monday, September 30, 2013

Rush and the 1976 Austrian Grand Prix

Rush is currently No. 1 at the UK box-office, and Ron Howard's populist mix of stereotypical rivalry, heroism, sex and danger, is sure to attract a new generation of fans to the fight between 3-stop strategies and pace-managed 2-stoppers.

For those seeking the real thing from 1976, this was the video of the entire Austrian Grand Prix at the Osterreichring. It has now been stripped from Youtube by the guardians of copyright, who don't appear to be protecting any commercial interest given that there is no alternative outlet in which the entire race can be viewed. 

Which is a pity, because the original Osterreichring was a majestic, Styrian theatre of motorsport. The 1976 race started with localised showers of rain, until, as Pete Lyons reported, "The Sun now broke out on the highest slopes above, kindling the tents there into incandescent yellows and reds. Within minutes the entire landscape was brilliant, rain-washed green." 

Proper drivers, proper cars, and a proper circuit.


Wednesday, September 25, 2013

Chapman, side-thrust, and the America's Cup

In the summer of 1975, Colin Chapman composed a list of requirements for a Future F1 Car.  Reproduced in Karl Ludvigsen's excellent engineering biography (Colin Chapman - Inside the Innovator), many of the points continue to be relevant today. In particular, the list includes the following laudable objectives:

5...We must get maximum cornering force from the tyres. This is maximised by:
(i) The largest possible contact patches.
(ii) With the softest compound.
(iii) Kept in contact with the ground as long as possible.
(iv) With highest possible download.
(v) Spread as evenly as possible over the contact patch.
(vi) And spread as evenly over the four contact patches in proportion to the sideloads they have to carry.

In a more quirky vein, Chapman includes the following speculative thought:

9. Total cornering force can also be increased aerodynamically
Should we try to use vertical lifting surfaces to provide additional side load derived from the speed and yaw angle of the car whilst cornering?

Which is interesting, because apart from the use of fins atop the engine cover, there appears to have been little effort in Formula 1 to generate a direct aerodynamic side-thrust. In contrast, it seems to be an extremely important part of racing yacht design, of which The America's Cup might be held as the foremost example.

If a yacht is your chosen mode of travel, and the wind rather inconveniently happens to be blowing from a direction close to the direction in which you wish to travel, you can still generate a thrust in that direction by means of some aerodynamic and hydrodynamic magic.

Firstly, you use your sail as an aerofoil, and generate low pressure on one side of it, so that an aerodynamic force is produced at right angles to the effective direction in which the wind is travelling. This alone wouldn't get you to where you want to go, but here you can use the fact that there are actually two fluids in play: air and water. Whilst your sail can generate a force from the airflow, the hull of your yacht can also generate a force from the flow of water. With a yaw angle between your direction of travel and the effective wind direction, the water will accelerate around one side of the hull, creating a hydrodynamic side-force which can be used to cancel out the sideways component of the force generated by the sail. What remains of the aerodynamic force is a component pointing in the direction you wish to travel!











As Alfio Quarteroni explains (Mathematical Models in Science and Engineering, from which the diagram above is taken), the presence of two fluids with different densities and viscosities, separated by a free surface endowed with surface tension and variable curvature, adds many interesting dimensions to the fluid mechanical problem. Moreover, the sail itself needs to be treated as an aero-elastic medium, deforming in response to the pressure field upon it, and thereby changing the airflow, in a coupled manner. Seen in this light, it's no surprise that The America's Cup once exerted such a pull over the imagination of Chapman's modern counterpart, Adrian Newey.

Friday, August 16, 2013

What is a quantum field?

Philosopher of Physics Meinard Kuhlmann has a brilliant article, What is real?, in the August 2013 edition of Scientific American.

Kuhlmann provides a clear account of why the particle and field ontologies provide equally inadequte interpretations of quantum field theory. Whilst most physicists tend to resort to the lazy claim that the particle and field concepts are somehow 'complementary', Kuhlmann points out that this doesn't help "because neither of these conceptions works even in those cases where we are supposed to see one or the other aspect in purity."

Kuhlmann's account of how a quantum field is mathematically defined is particularly striking: "A classical field is like a weather map that shows the temperature in various cities. The quantum version is like a weather map that does not show you '40 degrees', but '√'.

The article concludes with a nice explanation of two alternative ontologies: structural realism, and the bundle theory of properties.

If you want an insight into the philosophical problems of modern physics, this is an excellent introduction.

Sunday, July 28, 2013

Front-wing vortex breakdown

With the assistance of Mercedes GP, Jacques Heyder-Bruckner completed a PhD thesis in 2011 which analysed the front wing-wheel interaction on a racing car. Of particular interest in this work is the fact that Detached Eddy Simulation (DES) was used to represent the phenomenon of vortex breakdown, which occurs when the front-wing approaches low ride-heights under conditions of roll and pitch.

Whilst Reynolds Averaged Navier-Stokes (RANS) simulations are the CFD workhorse of modern motorsport, RANS is known to be inadequate for representing separated flows, and in particular for representing large-scale vortical phenomena, such as vortex evolution and breakdown. In contrast, Detached Eddy Simulations use RANS to represent the attached flow, but directly solve the Navier-Stokes equations in the regions of separated flow.



















Q-criterion isosurfaces of the vortex breakdown phenomenon, taken from the instantaneous DES flowfield, are depicted here. Bruckner points out that “the vortex breakdown moves forward as the wing is moved closer to the ground…The large vortex expansion…is composed of a recirculation region enclosed by the spiralling tail shed from the vortex breakdown.This causes high pressure fluctuations on the endplate and flap, resulting in a more unstable wing with variations in downforce and drag three times larger than at higher ride-heights.” (p116).

 

Saturday, June 15, 2013

The Lynx effect


Hidden within the dark torrent of subliminal messages communicated by commercial advertising and branding, it seems that aerodynamic information from contemporary Formula One is being transmitted on the side of Lynx anti-perspirant cans.

In the case shown here, one can see the vortices on a transverse plane just in front of the floor. The large structure on the right is clearly the Y250 vortex, created by the transition between the front-wing camber and the mandatory neutral central section astride the nose pylons. To the left, one can see two smaller vortices, probably shed by a guide vane hanging down from the underside of the nose.

Doubtless, the transient effect that such products have on axillary diaphoresis is matched only by the transient instability of these vortices.

Thursday, May 02, 2013

Tyre feathering

"If a new tyre is punished too heavily, too quickly, its critical tread compound temperature may be exceeded and blisters will appear and burst...Heavy cars, unsympathetically-driven cars and badly set-up cars may burn-out their tyres (particularly at the front) in a less abrupt manner. This phenomenon, known as 'graining' or 'feathering', rolls little pieces of rubber off the tread - diminishing its grip. A watchful driver will recognise the condition as one edge of his front tyres - or of the rears seen in his mirrors - will blacken. The car's cornering power will be limited and if he presses on the condition will worsen. A sensitive driver will ease off, roll-away the loose granulation, and after a few laps will see his tyres regain their normal appearance and will find much of their adhesion restored."

(Doug Nye, Motor Racing in Colour, Blandford Press, 1978, p44).

Saturday, February 23, 2013

BBC Sport and Potential Flow theory

It is a fact, sadly unacknowledged, that BBC Sport's default background animation represents a doublet from Potential Flow theory.

Potential Flow theory is a branch of aerodynamics in which flows are idealised as being inviscid and irrotational. This means, respectively, that there is no friction resistance to shear between adjacent layers of fluid, and there is no vorticity. Hence, Potential Flow theory does not recognise the existence of boundary layers adjacent to solid objects.

Now, there is, within aerodynamics, a distinction between circulation and rotation, which has the potential (if you'll excuse the term) to confuse. In a flow with circulation, you can integrate the velocity vector around a closed loop and obtain a non-zero value. In a rotational flow, the vorticity field is non-zero.

In a Potential Flow (guaranteed, by definition, to be irrotational), if the region of space occupied by the fluid is simply connected topologically-speaking, (entailing that any loop can be smoothly deformed to a point) then the flow will have zero circulation. However, if the region is not simply connected, then the irrotational flow can possess circulation. The presence of solid objects in a fluid prohibits the region of space occupied by the fluid from being simply connected, (in 2-dimensional terms, at least), hence Potential Flows around solid objects can possess circulation.

This loophole (if you'll excuse the term) within Potential Flow theory enables one to represent the circulatory flow around wing sections. Because the equations of Potential Flow theory are linear, one can superpose several solutions of the theory to obtain other solutions. To represent the flow around a cylinder, for example, one superposes a uniform flow with a so-called doublet. The latter provides the stagnation points to the flow at the leading and trailing points of the cylinder.

To represent the circulatory flow around a wing section one basically just adds a free vortex to the superposition.

Hence, despite the BBC's apparent aversion to covering all the Grands Prix in a Formula One season, aerodynamics is clearly a subject close to their heart.

Sunday, February 10, 2013

Descent to bathos

Whilst the odiferous obligations of life suggest a strictly utilitarian approach to bathroom use amongst much of the population, there are those of us who continue to resist the anxious, volatile, blinding spray of the shower-head, and stubbornly insist on prolonged semi-submergence in a liquid heat source as an opportunity for rest, relaxation, and consumption of excellent prose.

This sub-class of the population, however, has to endure a flagrant design flaw which besets many a bathroom, yet receives scant public attention. This, namely, is the tendency of negligent bathwrights to erroneously align the tap-end of the tub towards the centre of the bath-space. This places the reclined reader's head at the opposite end of the bath-axis, where illumination from the central, ceiling-located light source is typically inadequate.

Until bathwrights can be prevailed upon to mend their ways, there is, fortunately, an interim measure which can be undertaken: remove a large mirror from the hallway, and balance it on the junction between the bath and the ceramically tessellated wall; obtain a lofty chair, a long electrical extension cable, and place an anglepoise lamp on the chair, facing the mirror. This cunning configuration will provide the recumbent, heat-absorbent reader with an adequate level of reflected light, from which the world of the imagination can once more be accessed, and the stresses of the modern world temporarily dissolved. There is nothing which could possibly go wrong.

Thursday, December 20, 2012

City-Link's delivery standards

Autocourse 2012-13 arrived today. Courtesy of City-Link, it was left unprotected, outside the house, on one of the wettest days of the year. The book is ruined.

I presume the package was left in such a manner by an individual who faces a daily struggle to successfully wield a knife and fork.

I'm certainly looking forward to asking the Managing Director of City-Link, Mr David Smith, how employing such individuals contributes to the company's business plan.

Saturday, October 13, 2012

Red Bull's double-DRS



Is there a connection between Red Bull's new double-DRS system, and their unique 'underpass' duct?

To recall, the underpass is a means of separating the 'coke-bottle' flow along the flank of the sidepod, from the exhaust-flow, sweeping down from the top of the sidepod. The coke-bottle flow feeds the starter-motor slot and the top surface of the diffuser's trailing edge, while the exhaust jet partially seals the side of the diffuser and increases the flow over the rear brake-duct assembly.

The underpass is fed by the flow along the flanks of the sidepods, which in turn is fed by the front-wing wake. By connecting the flow along the flanks of the sidepods to the low pressure area under the beam wing, the underpass not only assists with rear downforce, but also pulls the air faster over the front-wing.

Red Bull's double-DRS system purportedly stalls the central section of the beam wing, (although Craig Scarborough suggests that it is the tips of the beam-wing which are being stalled, in order to reduce the wing-tip vortex drag). 

The central part of the beam wing is the section which is pulling the air out of the underpass. Thus, if the beam wing stalls, then the underpass stalls, the flow along the flanks of the sidepods weakens, and front-wing downforce and drag are reduced.

The image above here illustrates how the front-wing streamlines on a generic open-wheeled race-car are the same streamlines which pass along the flanks of the sidepods, and thence between the rear wheels, (although there is no sidepod undercut or beam wing in this illustrative case, courtesy of the 2012 University of Southampton Racecar Aerodynamics MSc Group Design Project).

Red Bull introduced a smaller underpass inlet for the Korean Grand Prix, and if the double-DRS really does stall the centre of the beam wing, it would certainly make sense to change the underpass as well. Autosport's Mark Hughes comments in his Korean Grand Prix report that the changes to the sidepod area gave "more downforce and more diffuser stall." 

One can speculate then, that Red Bull's double-DRS is a system which reduces front-wing drag as well as helping to stall the beam wing and diffuser.

Tuesday, October 09, 2012

Lasers, plasmas and diffusers


The first laser, invented in 1960 by Theodore Maiman, an engineer-turned-physicist, was a product of the aerospace industry. Maiman was working for Hughes Research Laboratories, and was given nine months and $50,000 to make a laser work by Mr Hughes, (And then there was light, Pauline Rigby, Physics World, May 2010).

Perhaps it's time, then, for the introduction of the laser into Formula One, not merely as a ride-height sensor, but as a flow control device.

Racing cars have, traditionally, used the short-range repulsive forces of solid surfaces to control the flow of air. This, however, is merely one particular, very convenient solution to the engineering problem. Lasers can also control the flow of air, either by directly delivering radiation pressure to a specific region of the airflow, or by creating a plasma whose pressure can instead be used to the same effect.

The question here is merely one of practicality. Do modern lasers combine sufficient power in a lightweight, compact package? Well, probably not quite yet, but there are already some tantalising glimpses of the possibilities.

The Curiosity Rover currently exploring Mars is equipped with a Laser-Induced Breakdown Spectroscopy (LIBS) system. The laser vaporises rocks some distance away, and a separate camera system analyses the light to make inferences about the chemical composition of the rock. Most intriguingly, the weight of this powerful laser system was reduced to 500g.

A LIBS system focuses a laser on an object and ablates the surface layer of the object to create a plasma plume. This high-temperature plume has a momentum flux, and it has long been suggested that this could be used to propel lightweight objects.

In terms of an immediate Formula One application, however, one might install a laser unit low down in the aft region of the sidepods, and train the laser light upon an aluminium foil surface attached to the floor in the region where one currently finds vortex generators, just inside the rear wheel. The resulting plasma plume could be used as a surrogate exhaust jet to seal the diffuser, with perhaps the odd magnet to focus the plasma. Depending upon how the regulations evolve, KERS energy could be used to power the laser.

There are some potential hazards, such as the possibility of vaporising the rear end of the car if the laser is incorrectly focused, but these are small matters in comparison to the potential advantages of a laser-sealed diffuser system.