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9.4 The maximum ball spe
speed.
ed when hitting the racket and the bouncing ball
Above calculations have been based on maximum b l speeds when
with the racket, which is equal to 210
al
colliding
km/h or 58.3 m/sec [14]. While flying
the maximum boundaries of the
court th
Y
e ball can travel over ≥23 meters
provi
ded it travels along a straight line
parallel to the length of the court and not
less that around 32 meters provided it
travels diagonally. The sp
eed of the bal
l is
Θ
reduc
ed during the flight due to the air
X
resistance; therefore its initial speed
ld b higher [14].
R
shou e
Fig. 14
We calculated the actual speed of the ball based on the theory of an object
(shell) flight in a resistance environment when shot at a certain angle from the surface
plane. – Figure 14.
The equation for movement in resistance environment is:
X = cosθ /b. h (Vo. cosθ /V cosθ),
0
0
(Eq. 45)
and from
aerodynamics
b
=
R
=
C
ρ
V 2
.
S
(Eq. 46)
x
x
2
where, Vo = Uo; V = U1; Rx = sir resistance
ρ = air density = 0.125 (at n
ormal temperature and humidity conditions and when
meas
ured at the level of the court);
S – cross sectional ar
ea of the ball (m2
);
b1 – ball diameter = 0.065 m;
nce coefficient, which depends on the shape ;
0.14 for Re3.8 . 105 = 380000
π/4 = 0.0033 m2
For spherical shape it is Cx =
S – cross sectional area of the ball = 0.0652
R
e
=
69000
b
1
V
(
V
=
U
1
)
forV
=
60
m
/
sec
R
e
=
69000
.
60
.
065
R
=
269100 <
380000
36
within
Cx – air resista
.
.
 
 

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