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VECHILE AERODYNMICS
PRESENTED BY
PRADEEP KUMAR S L
Characteristics of flow past vehicle bodies
Complex 3D turbulent flow in
relative co-ordinate system.
Classification of flow field:
Flow past
• front,
• side walls and roof,
• in underbody gap,
• behind the rear wall (wake).
• Front: stagnation point, overpressure, accelerating flow
• Side walls, roof: boundary layer separation depending
on the rounding up of leading edges around the front.
• Rear wall: in separation bubble nearly constant pressure
below the ambient, strong turbulent mixing
• Underbody gap: surrounded by „rough” and moving
surfaces, decreasing velocities downstream, sideward
outflow
Relation between curvature of
streamlines and pressure distribution
p
 
v2
n R
where
n co-ordinate normal to streamline
R radius of streamline curvature
If the streamlines are curved pressure increases
perpendicular to them, outwards from the centre of curvature
Aerodynamic forces and viscosity
In case of inviscid flow =0 (no shear
stresses exist) and   p dA 0 the resultant
of pressure forces is 0
A
. (In case of cylinder
symmetrical flow field.)
So Faer = 0
In case of viscous flow   0 (shear
stresses exist) and (the
resultant of pressure fA
orcesis different
from 0). In case of cylinder non-
symmetrical flow field.
So Faer  0
p dA  0
Cause of drag forces at streamlined
and bluff bodies
Streamlined bodies are
characterized by attached flow.
The share of pressure forces in
drag force (component of
aerodynamic force parallel to
undisturbed flow) is small. Drag is
caused mainly by shear stresses.
Since shear forces are small cD is
relatively small.
Bluff bodies are characterized by
boundary layer separation and
separation bubbles. Drag is caused
mainly by pressure forces, since
p-p0  cD is relatively big.
Boundary layer (BL) separation
On solid surface BL
develops
Adverse pressure gradient
causes BL separation
Adverse pressure
gradient over the plate
BL at accelerating and
decelerating flow
Separation bubble is
confined by shear layer
BL separation causes
asymmetry in flow field
Where to expect BL separation
Between points
a) 7-16 behind the leading edge,
b) over the bonnet, in front of the
windscreen
c) 21-25 after the upper horizontal
leading edge over the windscreen
d) 1-35 behind the upper horizontal
trailing edge, over the rear window
Ad a)
Ad b), d)
Components of the drag of a brick
shaped bluff body and their reduction
Drag
type
% of
cD
Caused by Way of reduction and measures
Forebody
drag
65% Overpressure
on the
front face
Reduction of overpressure by
accelerating the flow: rounding up of
upper horizontal and vertical leading
edges, slanting the front face
Base
drag
34.9% Depression on
the rear end
Increase of pressure: boat-tailing,
tapering the rear part of the body,
rounding up of trailing edges
Side wall,
roof and
under-
body drag
0.1% Shear stresses
over the walls,
roof and
underbody
Decrease of shear stresses: reduction of
roughness, decrease of the velocity in the
underbody gap
Reduction of forebody drag (decrease
of overpressure on the front) 1
Boundary layer separation is
a good indicator of high drag
Rounding up of upper
horizontal leading edge
Rounding up of vertical
leading edges
Reduction of side wall, roof and underbody
drag (decrease of shear stresses)
Conclusions
a)Roof and side wall drag can be reduced by reduction
of roughness of the wall (no protruding parts, frames)
b)Underbody drag can be reduced by reducing the
roughness (covering) and reducing the velocity in
underbody gap (tight underbody gap, front spoiler )
Example: wind tunnel investigations aiming
at reduction of aerodynamic drag of buses
Wind tunnel: recirculating, 2.6 m x 5 m open test section,
vmax= 50 m/s wind velocity, 6 component overhead
balance, when necessary, ground simulation with moving
belt, flow visualisation with oil smoke.
Bus model: 1:5 scale bus models with rotating wheels,
detailed underbody and interchangeable parts.
Increase of driving stability 1
reducing aerodynamic lift
Effect of the gap size
on the lift
Airfoils, side box provided with wing increase
the negative lift: acp= v2/R = 2-3
Experimental investigations of mud
deposition on bus body
Reduction of mud deposition an side walls and rear wall by using wind
tunnel experiments
• simulation of moving ground with moving belt
• rotating wheels, detailed underbody
• Measurement of mud deposition
- with water of increased conductivity, introduced over the
moving belt: measurement of conductivity
- measurement of concentration of tracer gas
- flow visualisation using oil smoke
Conclusions
Small changes in rear wall
geometry reduces mud deposition
on rear wall by 73%.
The area of side walls covered by
mud can be reduced considerably
by reducing the deceleration of
underbody flow.
Numerical simulation of mud deposition
on rear wall of buses
Unfavourable flow conditions
 extensive mud deposition
on rear wall
Conclusion
Optimisation of vehicle bodies results in
• considerable reduction of fuel consumption
• improvement of comfort characteristics and
• more favourable driving characteristics of
ground vehicles.
In optimisation besides wind tunnel
investigations numerical simulation of flow
field has become more and more important.
THANK YOU ALL

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Vechile aerodynamics

  • 2. Characteristics of flow past vehicle bodies Complex 3D turbulent flow in relative co-ordinate system. Classification of flow field: Flow past • front, • side walls and roof, • in underbody gap, • behind the rear wall (wake). • Front: stagnation point, overpressure, accelerating flow • Side walls, roof: boundary layer separation depending on the rounding up of leading edges around the front. • Rear wall: in separation bubble nearly constant pressure below the ambient, strong turbulent mixing • Underbody gap: surrounded by „rough” and moving surfaces, decreasing velocities downstream, sideward outflow
  • 3. Relation between curvature of streamlines and pressure distribution p   v2 n R where n co-ordinate normal to streamline R radius of streamline curvature If the streamlines are curved pressure increases perpendicular to them, outwards from the centre of curvature
  • 4. Aerodynamic forces and viscosity In case of inviscid flow =0 (no shear stresses exist) and   p dA 0 the resultant of pressure forces is 0 A . (In case of cylinder symmetrical flow field.) So Faer = 0 In case of viscous flow   0 (shear stresses exist) and (the resultant of pressure fA orcesis different from 0). In case of cylinder non- symmetrical flow field. So Faer  0 p dA  0
  • 5. Cause of drag forces at streamlined and bluff bodies Streamlined bodies are characterized by attached flow. The share of pressure forces in drag force (component of aerodynamic force parallel to undisturbed flow) is small. Drag is caused mainly by shear stresses. Since shear forces are small cD is relatively small. Bluff bodies are characterized by boundary layer separation and separation bubbles. Drag is caused mainly by pressure forces, since p-p0  cD is relatively big.
  • 6. Boundary layer (BL) separation On solid surface BL develops Adverse pressure gradient causes BL separation Adverse pressure gradient over the plate BL at accelerating and decelerating flow Separation bubble is confined by shear layer BL separation causes asymmetry in flow field
  • 7. Where to expect BL separation Between points a) 7-16 behind the leading edge, b) over the bonnet, in front of the windscreen c) 21-25 after the upper horizontal leading edge over the windscreen d) 1-35 behind the upper horizontal trailing edge, over the rear window Ad a) Ad b), d)
  • 8. Components of the drag of a brick shaped bluff body and their reduction Drag type % of cD Caused by Way of reduction and measures Forebody drag 65% Overpressure on the front face Reduction of overpressure by accelerating the flow: rounding up of upper horizontal and vertical leading edges, slanting the front face Base drag 34.9% Depression on the rear end Increase of pressure: boat-tailing, tapering the rear part of the body, rounding up of trailing edges Side wall, roof and under- body drag 0.1% Shear stresses over the walls, roof and underbody Decrease of shear stresses: reduction of roughness, decrease of the velocity in the underbody gap
  • 9. Reduction of forebody drag (decrease of overpressure on the front) 1 Boundary layer separation is a good indicator of high drag Rounding up of upper horizontal leading edge Rounding up of vertical leading edges
  • 10. Reduction of side wall, roof and underbody drag (decrease of shear stresses) Conclusions a)Roof and side wall drag can be reduced by reduction of roughness of the wall (no protruding parts, frames) b)Underbody drag can be reduced by reducing the roughness (covering) and reducing the velocity in underbody gap (tight underbody gap, front spoiler )
  • 11. Example: wind tunnel investigations aiming at reduction of aerodynamic drag of buses Wind tunnel: recirculating, 2.6 m x 5 m open test section, vmax= 50 m/s wind velocity, 6 component overhead balance, when necessary, ground simulation with moving belt, flow visualisation with oil smoke. Bus model: 1:5 scale bus models with rotating wheels, detailed underbody and interchangeable parts.
  • 12. Increase of driving stability 1 reducing aerodynamic lift Effect of the gap size on the lift Airfoils, side box provided with wing increase the negative lift: acp= v2/R = 2-3
  • 13. Experimental investigations of mud deposition on bus body Reduction of mud deposition an side walls and rear wall by using wind tunnel experiments • simulation of moving ground with moving belt • rotating wheels, detailed underbody • Measurement of mud deposition - with water of increased conductivity, introduced over the moving belt: measurement of conductivity - measurement of concentration of tracer gas - flow visualisation using oil smoke Conclusions Small changes in rear wall geometry reduces mud deposition on rear wall by 73%. The area of side walls covered by mud can be reduced considerably by reducing the deceleration of underbody flow.
  • 14. Numerical simulation of mud deposition on rear wall of buses Unfavourable flow conditions  extensive mud deposition on rear wall
  • 15. Conclusion Optimisation of vehicle bodies results in • considerable reduction of fuel consumption • improvement of comfort characteristics and • more favourable driving characteristics of ground vehicles. In optimisation besides wind tunnel investigations numerical simulation of flow field has become more and more important.