Title: Physics 199BB The Physics of Baseball
1Physics 199BBThe Physics of Baseball
- Fall 2007 Freshman Discovery Course
- Alan M. Nathan
- 403 Loomis
- 333-0965
- a-nathan_at_uiuc.edu
- Week 2
2The Flight of a Baseball
- The goal to develop an understanding of the
trajectory of a baseball in flight - Pitched baseball
- Batted baseball
- Thrown baseball
- First step we need to go over some basic
physics concepts
3Position, Velocity, and Acceleration
- Position x,y,z
- Units of length (m, ft, )
- Trajectory completely known if we know the
position of an object at every instant of time
x(t),y(t),z(t) - Position is a vector with three components
4Position, Velocity, and Acceleration
- 2. Velocity vx,vy,vz
- Units of length/time (m/s, ft/s,mph,)
- Velocity is the rate of change of position
- Velocity is a vector with three components
5Position, Velocity, and Acceleration
- 3. Acceleration ax,ay,az
- Units of length/time2 (m/s2, ft/s2,)
- Acceleration is the rate of change of velocity
- Acceleration is a vector with three components
6Motion with Constant Acceleration
Special Case 1 a0
x x0 v0t v v0
7Special Case 2Two-dimensional projectile motion
with gravity
ax 0 (horizontal)ay -g (vertical)g
32.2 ft/s2 9.8 m/s2
- x x0 v0xt vx vx0 (constant)
- y y0 v0yt - ½gt2 vy v0y - gt
8Detailed example pitched baseball
- Suppose a pitcher throws a baseball with an
initial horizontal velocity of 90 mph at a height
of 6 ft above home plate. How long does the
pitch take to reach home plate? How much does
the pitch drop vertically?
x x0 v0xt x00 v0x 90 mph y y0
v0yt - ½gt2 y06 ft v0y0
9Detailed example pitched baseball
x x0 v0xt x00 v0x 90 mph y y0
v0yt - ½gt2 y06 ft v0y0
Want to find time T when x 60.5 ft. Use that T
to find y. But firstneed a consistent set of
units. Convert mph to f/s 90 mile/hour 90
(mile/hour)(5280 ft/mile)(1/3600
hour/sec) 901.467132.0 ft/s
10Useful thing to remember
- To convert mph to ft/s, multiply by 1.467
- To convert ft/s to mph, divide by 1.467
11Detailed example pitched baseball
x x0 v0xt x00 v0x 90 mph y y0
v0yt - ½gt2 y06 ft v0y0
Now solve to find T 60.5 ft 0 132T
ft/s T0.458 s Now solve to find y(T) Y 6 ft
0 -0.532.2 ft/s2(0.458)2 s2 6 ft 3.382
ft 2.618 ft Ball drops 3.4 ft!
12Using Excel to Compute the Trajectory
- divide up time into slices separate by dt
- suppose x,y,vx,vy are known at time t
- at time tdt
- x(tdt)x(t)vx(t)dt
- y(tdt)y(t)vy(t)dt
- vx(tdt)vx(t)ax(t)dt
- vy(tdt)vy(t)ay(t)dt
- for case at hand values known at t0
- x0,y0,v0x,v0y
- ax0 ay-g
13Detailed example batted baseball
- Suppose the baseball is hit at an initial height
of 3 ft off the ground at a speed of 100 mph and
an angle of 35o to the horizontal. - How far does it travel?
- How long is it in the air?
- How high does it go?
14Detailed example batted baseball
- Suppose the baseball is hit at an initial height
of 3 ft off the ground at a speed of 100 mph and
an angle of 35o to the horizontal.
v0 100 mph 146.7 ft/s ? 35o v0x v0
cos(?) v0y v0 sin(?)
y
v0
?
x
15Batted Ball Example
- x x0 v0xt x0 v0tcos(?)
- y y0 v0tsin(?) - ½gt2
- x00 y03 ft v0146.7 ft/s ?35o
First step How long T is ball in the
air? Trick when ball hits ground,
vy-v0y-v0sin(?) Use vyv0y-gT and solve for T,
with vy-voy. T2v0y/g2v0sin(?)/g2146.7sin(350
)/32.25.23 s
16Batted Ball Example
- x x0 v0xt x0 v0tcos(?)
- y y0 v0tsin(?) - ½gt2
- x00 y03 ft v0146.7 ft/s ?35o
Second step How far D did ball travel? Use D
v0Tcos(?) 146.75.23cos(35o) 628.5 ft
17Batted Ball Example
- x x0 v0xt x0 v0tcos(?)
- y y0 v0tsin(?) - ½gt2
- x00 y03 ft v0146.7 ft/s ?35o
Third step How high H did ball go? Maximum
height occurs at time tT/2 2.62 s. Plug into
equation for y, using tT/2 H 6
146.72.62sin(35o)-0.532.2(2.62)2 115.9 ft
18Now lets use Excel to solve(just like before)
- divide up time into slices separate by dt
- dt needs to be small
- suppose x,y,vx,vy are known at time t
- at time tdt
- x(tdt)x(t)vx(t)dt
- y(tdt)y(t)vy(t)dt
- vx(tdt)vx(t)ax(t)dt
- vy(tdt)vy(t)ay(t)dt
- for case at hand values known at t0
- x0,y0,v0x,v0y
- ax0 ay-g
19Some Useful Formulas(we wont use these for
anything)
- Maximum distance D v02sin(2?)/g
- Maximum height H v02sin2(?)/2g
- Time of flight T 2v0sin(?)/g
- D is largest when ?45o
- T and H are largest with ?90o
20Baseball Trajectories with Drag and Magnus Forces
- Some additional physics concepts
- Newtons First Law
- Objects at rest stay at rest and objects in
motion continue to move at constant velocity if
not acted upon by an external force - In other words, with no external force v is
constant in both magnitude and direction - Newtons Second Law
- Forces cause acceleration a F/m or
21Forces on a Baseball in Flight
- Gravity
- Already discussed
- Drag (air resistance) Force
- We will do this next
- Magnus Force
- We will do this later
22Baseball Trajectories with Drag
- Fdrag ½ CD?Av2
- ? is density of air
- 1.23 kg/m3 at normal temp and pressure
- A is cross sectional area of ball
- A ?R2 4.16 x 10-3 m2
- v speed of ball
- CD is drag coefficient
- A number between 0 and 1
- Approximately 0.5 for vlt50 mph
- See plot in Adair, p. 8, Fig. 2.1
- Direction of force is exactly opposite velocity
23Drag Coefficient from Adair
24Lets estimate size of drag force
- Let CD ½, v100 mph
- FD ½CD?Av2
- Convert mph to m/s 100 mph 44.7 m/s
- FD1/21/21.234.16x10-3(44.7)2
- FD 2.56 N 0.574 lb
- By comparison, weight of ball is 5.1 oz
- mg 0.319 lb
- We conclude that the drag is very important
last slide of Week 2