The ball in
motion- parabolic break down
Problem: Find the minimum force it takes to throw a
baseball from the
center field of wrigley field to home plate where a catcher will
receive the ball at the same height that the ball was released from the
outfielder's hand, a distance of 400 ft (123 m). The angle of
trajectory that an object will travel the farthest when released,
ignoring wind, is 45o
off the horizontal ground. The mass of an official MLB baseball is
between 5 and 5 1/4 ounces so we will use a 5 1/4 ounce baseball
(0.1488kg) since it is be the largest mass allowed by the MLB.
Remember the gravity of the earth accelerates objects at a rate of 9.81
m/sec^2. The arm span of the man throwing the ball is 8 ft (2.4 m)
There are two important parts to figuring this
problem out. First
finding the velocity at which the ball was released and then using the
man's arm span and the value for the velocity found in the first part
to
find the acceleration of the ball while in the mans possession this
value times the mass of the ball will give rise to the minimum force
required
for this man to throw a ball to home plate.
Step 1: The
X-component
Work
(from
picture,
vxi
=
vi * cos
(45) )
xf = xi + vxi
* deltat
+ ½ * ax * deltat2
xf = 0 + vxi * deltat
+
½
*
(0)
*
deltat2
xf = vxi
* deltat
xf =
vi
* cos (45) * deltat
Step 1: The
Y-component
Work (from
picture, vyi = vi * sin (45) )
yf = yi + vyi
* deltat
+ ½ * ay * deltat2
0 = 0 + vyi * deltat
+
½
*
ay
* deltat2
0 = vi * sin (45) * deltat
+
½
*
ay
* deltat2
Step 1: Manipulate
and Combine x-component and y-component
x:
xf
= vi
* cos (45) * deltat
manipulate
:
1.
0 = tan (45) * xf + ½ * ay * xf2
/
[vi2
* cos2 (45)]
y:
0
=
vi * sin (45) * deltat + ½ * ay
* deltat2
2.
-tan(45) * xf
= ½ * ay * xf2 /
[vi2
* cos2 (45)]
3. -2 tan(45) * xf / ay = xf2 /
[vi2
* cos2 (45)]
x:
deltat
=
xf / [vi * cos
(45)]
4. vi2 * cos2
(45) = -ay *
xf /[ 2tan(45)]
5. vi2 = -ay * xf /[ 2tan(45)
* cos2 (45)]
x into y: 0 = vi
*
sin (45) * xf / [vi * cos (45)] + ½ * ay
* [xf
/ (vi * cos (45))]2
6. vi
=
squrt(-ay * xf /[ 2tan(45) * cos2
(45)] )
vi is about 52 mph
Step 2: Finding the
force.
At this point in the problem we have
solved for the
initial velocity of the ball when it leaves the outfielders hand.
Now in order to find the force the man exerted on the ball we must find
the magnitude of the balls acceleration while in his possession.
We need this because F = ma and we know the mass because it is
given. To find the acceleration you can use one of the
equations provided on the previous link. It will be labeled
clearly below where, vo ,stands for velocity initial.
equation:
vf2 = vo2
+ 2a deltax
a
= (vf2
- vo2) / ( 2 deltax
)
known values:
Plug
in
known
values
to
find (a):
vf =
squrt(-ay
*
xf /[ 2tan(45) * cos2 (45)] )
vo = 0
m/sec
a =
(-ay
*
xf /[ 2tan(45) * cos2 (45)]
- 0) / ( 2 deltax )
deltax = 8.ft = 2.4m
m =
0.1488kg
a
= [9.81
* 123 /(
2tan(45)
*
cos2 (45)) ] / ( 2
* 2.4
)
ay = -9.81 m/sec^2
xf
= 400. ft = 123
m
a = 251.38 = 250
m/sec^2
Plug
in
values
to
find
force (F):
F = ma
F = (.1288) (251.38) = 32.38 = 32
kg*m/sec^2 = 32 Newtons = 32 N
Conclusion:
The minimum force required for this man to throw
the baseball is 32 N which will accelerate the ball 250 m/sec^2 and
will cause the ball to leave the outfielders hand at about 52 mph.