Hitting Home Runs:
How a Physicist Thinks About Baseball
Alan M. Nathan
University of Illinois at Urbana-Champaign a-nathan@uiuc.edu
http://www.npl.uiuc.edu/~a-nathan/pob
My day job…
experimental nuclear/particle physics
high-speed collisions between subatomic particles
Nights and weekends...
physics of baseball
high-speed collision between baseball and bat
Jefferson Laboratory Science Series March 28, 2002 Page 1
“...the most difficult thing in sports”
--Ted Williams
BA: .344
SA: .634
HR: 521
OBP: .483
#521, last at-bat
September 28, 1960
Jefferson Laboratory Science Series March 28, 2002 Page 2
90 mph fastball takes about 0.40 sec to reach batter
~ 0.20 sec needed to “observe, process, decide”
~ 0.15 sec needed for swing
half of “break” occurs in last 0.10 sec if batter mis-estimates speed by
1.5 mph (0.007 sec)
swing will be early/late by 1’
elevation of ball misjudged by
1”
backspin/topspin makes ball fall less/more
Warren Spahn (greatest lefthander?) said:
“Hitting is timing. Pitching is upsetting timing.”
30% success rate gets you in Hall of Fame!
Jefferson Laboratory Science Series March 28, 2002 Page 3
A violent collision!
forces large (>8000 lbs!)
time is short (<1/1000 sec!)
ball compresses, stops, expands
kinetic energy
potential energy
lots of energy dissipated
distortion of ball and bat
hands don’t matter!
Jefferson Laboratory Science Series March 28, 2002 Page 4
Large hit ball speed
v hit
105 mph
D
400 ft
each additional mph gives 4-5 ft
Proper takeoff angle
about 35 0
Lots of backspin
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The basic stuff (“kinematics”)
speed of pitched ball
speed of bat
weight and weight distribution of bat
The really interesting stuff (“dynamics”)
“bounciness” of ball
impact location on bat (“sweet spot”)
Jefferson Laboratory Science Series March 28, 2002 Page 6
My only formula v hit
ball
bat example: 90 + 70 gives 102 mph (~400”)
Bat speed matters much more!
Each mph of bat speed worth 5 ft
Each mph of pitch speed worth 1 ft
Collision is very inefficient
perfect efficiency: 0.2/1.2
1.0/2.0
Jefferson Laboratory Science Series March 28, 2002 Page 7
v hit
= 0.2 v ball
+ 1.2 v bat
CM recoil rotation
• For given bat speed, heavier bat is better
0.2/1.2
0.5/1.5
• But….
Jefferson Laboratory Science Series March 28, 2002 Page 8
COR measures “bounciness” of ball
Final speed/Initial speed
(from massive rigid surface)
For baseball, COR
0.5
h f
/h i
= 3/4
3/4 energy lost!
Is the ball “juiced ”?
10% change
30’
Jefferson Laboratory Science Series March 28, 2002 Page 9
Collision excites bending vibrations in bat
Ouch!! Thud!!
Sometimes broken bat
Energy lost
lower COR
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nodes Center of mass
“sweet spot” zone
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thin shell & added mass
mass, mass distribution, length independent
lighter and CG closer to hands
…easier to swing
fatter barrel, thinner handle
more forgiving on mis-hits
“trampoline” effect
golf drivers
tennis rackets
corked bats?
Net result: higher batted ball speed
Jefferson Laboratory Science Series March 28, 2002 Page 12
Forces on Moving Baseball
Without Spin:
Ball pushes air out of way
Low-pressure wake
DRAG!
Grows with square of velocity
With Spin:
Ball deflects wake
action/reaction
“Magnus force”
Force grows with rpm
Force in direction front of ball is turning
Jefferson Laboratory Science Series March 28, 2002 Page 13
The Flight of the Ball
Real Baseball vs. Physics 101 Baseball
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Friction between ball and bat
spin on ball
Bat undercuts ball
• ball goes up
• backspin
Jefferson Laboratory Science Series March 28, 2002 Page 15
Friction between ball and bat
spin on ball
Bat overcuts ball
• ball goes down
• topspin
Jefferson Laboratory Science Series March 28, 2002 Page 16
Friction between ball and bat
spin on ball
Swing early/late
• ball goes left/right
• sidespin
Jefferson Laboratory Science Series March 28, 2002 Page 17
Balls hit to left/right break toward foul line
Topspin gives tricky bounces in infield
Pop fouls behind the plate curve back toward field
Backspin keeps fly ball in air longer
Jefferson Laboratory Science Series March 28, 2002 Page 18
Backspin (RPM) optimum angle distance
0
500
36 0
35 0
355 ft
361 ft
1000
1500
2000
2500
34 0
32 0
31 0
29 0
368 ft
375 ft
382 ft
389 ft
Jefferson Laboratory Science Series March 28, 2002 Page 19
• Ball arrives on 8.5
o downward trajectory
• Big Mac swings up at 8.5
o
• Undercuts ball by ~1”
• Ball takes off at 35 o with lots of backspin
The optimum home run swing!
Jefferson Laboratory Science Series March 28, 2002 Page 20
Lots of physics in baseball
Knowledge of physics helps understanding of game
And it’s fun too….
Jefferson Laboratory Science Series March 28, 2002 Page 21