Racecar Engineering – September 2019

(Joyce) #1
76 http://www.racecar-engineering.com SEPTEMBER 2019

TECHNOLOGY – LSR AERO STABILITY


In a perfect world the wheel downloads
would remain constant throughout the speed
range, but in reality this is not possible. Instead,
the wheel loads need to remain positive (to
avoid leaving the ground) and bounded (to
avoid structural overload of the chassis or
indeed the surface). The generic target we
identified for Bloodhound was to bound the
wheel loads to between 50 per cent and 150
per cent of the load due to gravity (from which
the above 10kN minimum is derived). This target
is simple to express but extraordinarily difficult
to achieve across a speed range from zero to
Mach 1.4 (1000+ mph). Nonetheless, it provided
the essential objective that drove the five years
and more of aerodynamic research that went
into establishing Bloodhound’s basic shape.
An alternative approach to bounding
wheel loads is to trim the vehicle using active

aerodynamic surfaces (such as winglets) to
adjust the vertical loads during the run. But
having assessed the complexity of a suitable
system to achieve this, and the huge negative
implications for safety if it malfunctioned in
any way at high speeds, we decided to take
the longer route for Bloodhound, and to find a
shape that would stay on the ground by itself
without active aero trimming.

Static stability
Now we will consider static stability in pitch.
Static stability is the tendency to return to the
neutral position when the vehicle is displaced.
Put simply, if a displacement caused the vehicle
to diverge, it is statically unstable, while if it
returns to the neutral position, it is said to be
statically stable. In theory, a vehicle will remain
on the ground if the total vertical down-load

(the sum of gravity, aerodynamic forces, pitch
due to thrust, pitch due to drag, etc.) acts
anywhere within the trapezium shape defined
by the wheel/ground contact points. In practice
more stringent criteria apply, and the centre of
download should act somewhere near the mid-
point of the wheelbase or problems of stability
and control are likely to result.
It is sometimes stated, erroneously, that it
is the aerodynamic centre that controls pitch
stability. The aerodynamic centre does indeed
have significance, but in connection with
dynamic stability (of which more later).
But it’s with stability in yaw where the
differences between automobile stability
theory and aircraft stability theory really
become apparent. An automobile is said to be
stable if the centre of download is behind the
centre of gravity as in Figure 1 (here the rear
axle is experiencing more download than the
front axle, generating more lateral grip and
ensuring the car has understeer).
An aircraft is considered stable if the yaw
centre of pressure is behind the centre of gravity
(like an arrow), as in Figure 2.
For a high-speed record car both are
significant, as automobile stability dominates
atlowvelocities(sincetheaerodynamicforces
willbesmall)butaircraftstabilityis massively
dominantathighvelocities.Andtherewillalso
beintermediatevelocities,likelytobeinthe
regionof200mphto400mph,wheretheywill
eachmakea significantcontribution.
However,therecouldbea problemwith
theautomobilecomponentofstabilityofjet

In a perfect world the wheel downloads would remain constant


throughout the speed range, but in reality this is not possible


Thrust Programme Ltd
Thrust SSC broke the Land Speed Record with 763mph in 1997, making it the first supersonic land vehicle


While Dieselmax was not jet-propelled it was
technically transonic – in that localised parts of it
experienced both supersonic and subsonic flows
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