2. Aerodinamics Forces
Bernoulli’s Theorem
Bernoulli’s theorem states that the sum of kinetic energy
1/2qV2 and potential energy (pressure p) is constant and
which can be expresed as follows
1
2
qV2
+ p = constant , (1)
excluding the forces of gravity.
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4. Aerodinamics Forces
Bernoulli’s Theorem
The flows can be considered as two pipes, an upper one
T1 toward the ventral side of the plate and a lower one T2
toward the dorsal side.
In the dorsal part the airflow is forced to travel to rejoin the
exiting streamlines with an increase in speed and a loss of
pressure energy.
In the ventral part, the trajectories are shorter, due to lower
velocity, and the area Tv of local pressure is greater.
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6. Aerodinamics Forces
Nondimensional Coefficients
The component of the resultant parallel to airflow is the
drag R
CR = f (Re) =
R
1
2
qSV2
, (2)
with S the projected frontal area.
The component normal to the flow is the downforce −P
and its nondimensional coefficient −CP:
CP = f (Re) = −
P
1
2
qSV2
, (3)
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8. Aerodinamics Forces
Center of pressure
The point where the line of action of aerodinamics force F
encounters the body is called the center of pressure. It is
located at a distance XP from the leading edge, which
varies according to the angle of attack, so that the
nondimensional ratio Xp/C, with chord C, varies from 0 to
0.5 for angles to attack from 0
◦
to 90
◦
.
The curvature, in the plate, creates an angle j between the
slope of the tailing edge and the chord line.
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