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The Physics of Baseball Alan M. Nathan University of Illinois ODU Colloquium, March 31, 2000. Introduction Hitting the Baseball The Flight of the Baseball Pitching the Baseball Summary. REFERENCES.
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The Physics of BaseballAlan M. Nathan University of IllinoisODU Colloquium, March 31, 2000 • Introduction • Hitting the Baseball • The Flight of the Baseball • Pitching the Baseball • Summary
REFERENCES • The Physics of Baseball, Robert K. Adair (Harper Collins, New York, 1990), ISBN 0-06-096461-8 • The Physics of Sports, Angelo Armenti (American Institute of Physics, New York, 1992), ISBN 0-88318-946-1 • www.npl.uiuc.edu/~a-nathan/pob
#521, September 28, 1960 Hitting the Baseball “...the most difficult thing to do in sports” --Ted Williams BA: .344 SA: .634 OBP: .483 HR: 521
Here’s Why….. (Courtesy of Bob Adair)
Description of Ball-Bat Collision • forces large (>8000 lbs!) • time is short (<1/1000 sec!) • ball compresses, stops, expands • kinetic energy potential energy • bat affects ball….ball affects bat • hands don’t matter! • GOAL: maximize ball exit speed vf vf 105 mph x 400 ft x/vf = 5 ft/mph What aspects of collision lead to large vf?
How to maximize vf? • What happens when ball and bat collide? • The simple stuff • conservation of momentum • conservation of angular momentum • energy dissipation in the ball (compression/expansion) • The really interesting stuff • vibrations of the bat
0.2 r recoil factor = “radius of gyration” The Simple Stuff: Rigid-Body Kinematics e Coefficient of Restitution 0.5 Vball,f = 0.25 Vball,i + 1.25 Vbat,i Conclusion: vbat much more important than vball
. . . CM z Translation Rotation Recoil Factor • Important Bat Parameters: • mbat, xCM, ICM • wood vs. aluminum 0.16 + 0.07 = 0.23 Conclusion: All things being equal, want mbat, Ibat large
Coefficient of Restitution (e) • “bounciness” of ball • Bounce ball off massive hard surface • e2= hf/hi • For baseball, e .5 • 3/4 energy lost! • Changing e by .05 changes V by 7 mph(35 ft!) Important Point: the bat matters too!
tennis ball/racket Effect of Bat on COR • Energy shared between ball and bat • Ball is inefficient: 25% returned • Wood Bat • kball/kbat ~ 0.02 • 80% restored • eeff = 0.50-0.51 • Aluminum Bat • kball/kbat ~ 0.10 • 80% restored • eeff = 0.55-0.58 • “trampoline effect” • Bat Proficiency Factor eeff/e • Claims of BPF 1.2 Ebat/Eball kball/kbat xbat/ xball >10% larger!
CM • vball,I= 90 mph • vbat,CM = 54 mph • bat,CM = 51 s-1 Aluminum bat more effective for inside pitches Rigid-Body Results
Beyond the Rigid Approximation: A Dynamic Model for the Bat-Ball collision • Collision excites bending vibrations in bat • Ouch!! Thud!! • Sometimes broken bat • Energy lost lower vf • Lowest modes easy to find by tapping • Location of nodes important • Modes with fn 1 excited Ref.: AMN, Am. J. Phys, submitted March 2000
y y z A Dynamic Model of the Bat-Ball Collision 20 • Solve eigenvalue problem for normal modes (yn, n) • Model ball-bat force F • Expand y in normal modes • Solve coupled equations of motion for ball, bat
In a bit more detail… impact point ball compression
f1 = 165 Hz f3 = 1177 Hz f2 = 568 Hz f4 = 1851 Hz Results: 1. Normal Modes Louisville Slugger R161 (34”, 31 oz) nodes Can be measured (modal analysis)
Results: 2. Low-speed collision Theory vs. Experiment (Rod Cross) (at 1 m/s) collision time 2.2 ms
Results: 3. High-speed collision CM nodes • Under realistic conditions… • 90 mph, 70 mph at 28” • no data (yet)…..
CM nodes 24” 27” 30” Results: 4. The “sweet spot” Possible “sweet spots” 1. Maximum of vf (28”) 2. Node of fundamental (27”) 3. Center of Percussion (27”)
Wood versus Aluminum • Length and weight “decoupled” • Can adjust shell thickness • Fatter barrel, thinner handle • More compressible • COR larger • Weight distribution more uniform • Easier to swing • Less rotational recoil • More forgiving on inside pitches • Less mass concentrated at impact point • Stiffer for bending • Less energy lost due to vibrations
How Would a Physicist Design a Bat? • Wood Bat • already optimally designed • highly constrained by rules! • a marvel of evolution! • Aluminum Bat • lots of possibilities exist • but not much scientific research • a great opportunity for ... • fame • fortune
Conclusions • The essential physics of ball-bat collision understood • bat can be well characterized • ball is less well understood • the “hands don’t matter” approximation is good • Vibrations play important role • Size, shape of bat far from impact point does not matter • Sweet spot has many definitions
Aerodynamics of a Baseball Forces on Moving Baseball • No Spin • Boundary layer separation • DRAG! • FD=½CDAv2 • With Spin • Ball deflects wake ==>Magnus force • FMRdFD/dv • Force in direction front of ball is turning
How Large are the Forces? =1800 RPM • Drag is comparable to weight • Magnus force < 1/4 weight)
The Flight of the Ball:Real Baseball vs. Physics 101 Baseball • Role of Drag • Role of Spin • Atmospheric conditions • Temperature • Humidity • Altitude • Air pressure • Wind Max @ 350 approxlinear
The Role of Friction • Friction induces spin for oblique collisions • Spin Magnus force • Results • Balls hit to left/right break toward foul line • Backspin keeps fly ball in air longer • Topspin gives tricky bounces in infield • Pop fouls behind the plate curve back toward field
The Home Run Swing • Ball arrives on 100 downward trajectory • Big Mac swings up at 250 • Ball takes off at 350 • The optimum home run angle!
“Hitting is timing. Pitching is upsetting timing” ---Warren Spahn vary speeds manipulate air flow orient stitches Pitching the Baseball
7 6 Vertical Position of Ball (feet) 5 90 mph Fastball 4 3 0 10 20 30 40 50 60 Distance from Pitcher (feet) 1.2 1 75 mph Curveball 0.8 0.6 Horizontal Deflection of Ball (feet) 0.4 0.2 0 0 10 20 30 40 50 60 Distance from Pitcher (feet) Let’s Get Quantitative!How Much Does the Ball Break? • Kinematics • z=vT • x=½(F/M)T2 • Calibration • 90 mph fastball drops 3.5’due to gravity alone • Ball reaches home plate in ~0.45 seconds • Half of deflection occurs in last 15’ • Drag: v -8 mph • Examples: • “Hop” of 90 mph fastball ~4” • Break of 75 mph curveball ~14” • slower • more rpm • force larger
Examples of Pitches Pitch V(MPH) (RPM) T M/W fastball 85-95 1600 0.46 0.10 slider 75-85 1700 0.51 0.15 curveball 70-80 1900 0.55 0.25 What about split finger fastball?
Effect of the Stitches • Obstructions cause turbulance • Turbulance reduces drag • Dimples on golf ball • Stitches on baseball • Asymmetric obstructions • Knuckleball • Two-seam vs. four-seam delivery • Scuffball and “juiced” ball
Example 1: Fastball 85-95 mph 1600 rpm (back) 12 revolutions 0.46 sec M/W~0.1
Example 2: Split-Finger Fastball 85-90 mph 1300 rpm (top) 12 revolutions 0.46 sec M/W~0.1
Example 3: Curveball 70-80 mph 1900 rpm (top and side) 17 revolutions 0.55 sec M/W~0.25
Example 4: Slider 75-85 mph 1700 rpm (side) 14 revolutions 0.51 sec M/W~0.15
Summary • Much of baseball can be understood with basic principles of physics • Conservation of momentum, angular momentum, energy • Dynamics of collisions • Excitation of normal modes • Trajectories under influence of forces • gravity, drag, Magnus,…. • There is probably much more that we don’t understand • Don’t let either of these interfere with your enjoyment of the game!
x2 x1 Sweet Spot #2: Center of Percussion • When ball strikes bat... • Linear recoil • conservation of momentum • Rotation about center of mass • conservation of angular momentum • When COP hit • The two motions cancel (at conjugate point) • No reaction force felt x1x2=Icm/M
bat speed vs mass ball speed vs mass But… • All things are not equal • Mass & Mass Distribution affect bat speed • Conclusion: • mass of bat matters….but probably not a lot