1. The Physics of Hitting a Home Run ANL Colloquium September 20, 2002 Page 1 The Physics of Hitting a Home Run ANL Colloquium, September 20, 2002 Alan M. Nathan University of Illinois at Urbana-Champaign a-nathan@uiuc.edu http://www.npl.uiuc.edu/~a-nathan/pob l Introduction l Model for colinear ball-bat collisions  some applicatons l Beginners guide to aerodynamics l Model for oblique ball-bat collisions  some applications l Summary & Conclusions

2. The Physics of Hitting a Home Run ANL Colloquium September 20, 2002 Page 2 1927 Solvay Conference: Greatest physics team ever assembled Baseball and Physics 1927 Yankees: Greatest baseball team ever assembled MVP’s

3. The Physics of Hitting a Home Run ANL Colloquium September 20, 2002 Page 3 As smart as he was, Albert Einstein could not figure out how to handle those tricky bounces at third base.

4. The Physics of Hitting a Home Run ANL Colloquium September 20, 2002 Page 4 Philosophical Notes: “…the physics of baseball is not the clean, well-defined physics of fundamental matters but the ill-defined physics of the complex world in which we live, where elements are not ideally simple and the physicist must make best judgments on matters that are not simply calculable…Hence conclusions about the physics of baseball must depend on approximations and estimates….But estimates are part of the physicist’s repertoire…a competent physicist should be able to estimate anything...” --- Bob Adair in “The Physics of Baseball”, May, 1995 issue of Physics Today “The physicist’s model of the game must fit the game.” “Our aim is not to reform baseball but to understand it.”

5. The Physics of Hitting a Home Run ANL Colloquium September 20, 2002 Page 5 Hitting the Baseball “... the most difficult thing to do in sports” -- Ted Williams: 1918-2002 BA:.344 SA:.634 OBP:.483 HR: 521 #521, September 28, 1960

6. The Physics of Hitting a Home Run ANL Colloquium September 20, 2002 Page 6 Introduction: Description of Ball-Bat Collision l forces large (>8000 lbs!) l time short (<1/1000 sec!) l ball compresses, stops, expands  kinetic energy  potential energy  lots of energy lost l bat is flexible  hands don’t matter l to hit a home run...  large hit ball speed  optimum take-off angle  backspin

7. The Physics of Hitting a Home Run ANL Colloquium September 20, 2002 Page 7 The Ball-Bat Collision: Kinematics v f = e A v ball + (1+e A ) v bat Conclusion: v bat matters much more than v ball v ball v bat vfvf “Lab” Frame v rel e A v rel Bat Rest Frame e A  “Collision Efficiency” property of ball & bat weakly dependent on v rel Superball-wall: e A  1 Ball-Bat near “sweet spot”: e A  0.2  v f  0.2 v ball + 1.2 v bat

8. The Physics of Hitting a Home Run ANL Colloquium September 20, 2002 Page 8 What Does e A Depend On? Kinematics: recoil of bat (r) Dynamics: energy dissipation (e) Small r is best r  0.25 typical…depends on …. mass of bat mass distribution of bat impact location.. CM. b = + Heavier bat is better but….

9. The Physics of Hitting a Home Run ANL Colloquium September 20, 2002 Page 9 What is Ideal Bat Weight? Note: Batters seem to prefer lighter bats! Actually, Scaling with I knob better

10. The Physics of Hitting a Home Run ANL Colloquium September 20, 2002 Page 10  v BAT (6”) = 1.2 mph/(1000 oz-in 2) (  v f =1.5  0.3 mph) v bat  I -0.3 v bat  I -0.5

11. The Physics of Hitting a Home Run ANL Colloquium September 20, 2002 Page 11 Energy Dissipation: the ball-bat COR (e) Coefficient Of Restitution in CM frame: E f /E i = e 2 ball on hard floor: e 2 = h f /h i  0.25  e  0.5 (note: r=0.25, e=0.5  e A =0.2)  ~3/4 CM energy dissipated! depends (weakly) on impact speed the bat matters too!  vibrations  “trampoline” effect

12. The Physics of Hitting a Home Run ANL Colloquium September 20, 2002 Page 12 Aside: Effect of “Juiced” Ball MLB: e = 0.546  0.032 @ 58 mph on massive rigid surface 10% increase in COR  ~30-35 ft increase in distance

13. The Physics of Hitting a Home Run ANL Colloquium September 20, 2002 Page 13 l Collision excites bending vibrations in bat  Ouch!! Thud!! Sometimes broken bat  Energy lost  lower e, v f l Find lowest mode by tapping l Reduced considerably if  Impact is at a node  Collision time (~0.6 ms) > T N see AMN, Am. J. Phys, 68, 979 (2000) Accounting for Energy Dissipation: Dynamic Model for Ball-Bat Colllision

14. The Physics of Hitting a Home Run ANL Colloquium September 20, 2002 Page 14 Dynamic Model 20 y z y l Step 1: Solve eigenvalue problem for free vibrations l Step 2: Nonlinear lossy spring for F l Step 3: Expand in normal modes and solve

15. The Physics of Hitting a Home Run ANL Colloquium September 20, 2002 Page 15 Normal Modes of the Bat Louisville Slugger R161 (33”, 31 oz) f 1 = 177 Hz f 2 = 583 Hz f 3 = 1179 Hz f 4 = 1821 Hz Can easily be measured: Modal Analysis

16. The Physics of Hitting a Home Run ANL Colloquium September 20, 2002 Page 16 frequency barrel node Expt Calc 179 17726.526.6 582 58327.828.2 1181117929.029.2 1830182130.029.9 Measurements via Modal Analysis Louisville Slugger R161 (33”, 31 oz) Conclusion: free vibrations of bat can be well characterized FFT

17. The Physics of Hitting a Home Run ANL Colloquium September 20, 2002 Page 17 Theory vs. Experiment: Louisville Slugger R161 33-inch/31-oz. wood bat Conclusion: essential physics understood only lowest mode excited lowest 4 modes excited

18. The Physics of Hitting a Home Run ANL Colloquium September 20, 2002 Page 18 Time evolution of the bat   0.6 ms  hands don’t matter T= 0-1 ms T= 1-10 ms

19. The Physics of Hitting a Home Run ANL Colloquium September 20, 2002 Page 19 Effect of Bat on COR: Vibrations COR maximum near 2 nd node

20. The Physics of Hitting a Home Run ANL Colloquium September 20, 2002 Page 20 Putting Everything Together... “sweet spot” depends on collision efficiency *recoil factor *COR how bat is swung CM v f = e A v ball + (1+e A ) v bat

21. The Physics of Hitting a Home Run ANL Colloquium September 20, 2002 Page 21 Conclusion: ideal ball-bat collision can be simulated

22. The Physics of Hitting a Home Run ANL Colloquium September 20, 2002 Page 22 Wood versus Aluminum Kinematics Length, weight, MOI “decoupled” shell thickness, added weight fatter barrel, thinner handle weight distribution more uniform CM closer to handle less mass at contact point  easier to swing Dynamics Stiffer for bending Less vibrational energy More compressible COR larger

23. The Physics of Hitting a Home Run ANL Colloquium September 20, 2002 Page 23 The “Trampoline” Effect l Compressional energy shared between ball and bat  PE bat /PE ball = k ball /k bat << 1  PE ball mostly dissipated (75%) l Wood Bat  hard to compress  little effect on COR: “BPF”  1 l Aluminum Bat  compressible through “shell” modes  k ball /k bat ~ 0.10 (more or less)  PE bat mostly restored (more on this later)  COR larger: “ BPF”  1.1 (more or less)

24. The Physics of Hitting a Home Run ANL Colloquium September 20, 2002 Page 24 The Trampoline Effect: A Closer Look Bending Modes vs. Shell Modes k  R 4 : large in barrel  little energy stored f (170 Hz, etc) > 1/   energy goes into vibrations k  (t/R) 3 : small in barrel  more energy stored f (2-3 kHz) < 1/   energy mostly restored

25. The Physics of Hitting a Home Run ANL Colloquium September 20, 2002 Page 25 Wood versus Aluminum: Dynamics of “Trampoline” Effect “bell” modes: “ping” of bat Want k small to maximize stored energy Want  >>1 to minimize retained energy Conclusion: there is an optimum 

26. The Physics of Hitting a Home Run ANL Colloquium September 20, 2002 Page 26 Where Does the Energy Go?

27. The Physics of Hitting a Home Run ANL Colloquium September 20, 2002 Page 27 “Corking” a Wood Bat (illegal!) Drill ~1” diameter hole along axis to depth of ~10” Smaller mass larger recoil factor (bad) higher bat speed (good) Is there a trampoline effect?

28. The Physics of Hitting a Home Run ANL Colloquium September 20, 2002 Page 28 Not Corked DATA Corked COR: 0.445  0.005 0.444  0.005 Conclusions: no tramopline effect! corked bat is WORSE even with higher v bat Baseball Research Center, UML, Sherwood & amn, Aug. 2001 calculation

29. The Physics of Hitting a Home Run ANL Colloquium September 20, 2002 Page 29 Aerodynamics of a Baseball Forces on Moving Baseball No Spin  Boundary layer separation  DRAG!  F D =½ C D  Av 2 With Spin  Ball deflects wake ==>”lift”  F M ~  RdF D /dv  Force in direction front of ball is turning Drawing courtesty of Peter Brancazio

30. The Physics of Hitting a Home Run ANL Colloquium September 20, 2002 Page 30

31. The Physics of Hitting a Home Run ANL Colloquium September 20, 2002 Page 31 approx linear: The Flight of the Ball: Real Baseball vs. Physics 101 Baseball

32. The Physics of Hitting a Home Run ANL Colloquium September 20, 2002 Page 32 Summary of Aerodynamics l 108 mph  ~400 ft l each mph  ~5 ft l optimum angle ~35 0 l 2000 rpm backspin  Increases range ~27 ft  Decreases optimum angle ~3 0 l these number are only estimates!

33. The Physics of Hitting a Home Run ANL Colloquium September 20, 2002 Page 33 Oblique Collisions: The Role of Friction l Friction halts v T  spin, “lift” l 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

34. The Physics of Hitting a Home Run ANL Colloquium September 20, 2002 Page 34 Model for Oblique Collisions:  v N treated as before v Nf = e A (v ball +v bat ) N + v bat,N  Angular momentum conserved about contact point (!)  Friction reduces v T, increases   Rolls when v T = R   Horizontal: v Tf  (5/7)v T  Vertical: a bit more complicated  Not the way a superball works! vNvN vTvT vN|vN| vT|vT|

35. The Physics of Hitting a Home Run ANL Colloquium September 20, 2002 Page 35 Oblique Collisions: Horizontal Plane Initial takeoff angle down the line power alley

36. The Physics of Hitting a Home Run ANL Colloquium September 20, 2002 Page 36 Oblique Collisions: Vertical Plane optimum: D  0.75”  3000 rpm   33 0 Ball10 0 downward Bat 10 0 upward D = center-to-center offset

37. The Physics of Hitting a Home Run ANL Colloquium September 20, 2002 Page 37 Typical Trajectories Ball10 0 downward Bat 10 0 upward D = center-to-center offset

38. The Physics of Hitting a Home Run ANL Colloquium September 20, 2002 Page 38 Some Practical/Interesting Questions l Does more friction help? l Can a curveball be hit further than a fastball?

39. The Physics of Hitting a Home Run ANL Colloquium September 20, 2002 Page 39 Summary and Conclusions l Some aspects of baseball are amenable to physics analysis  Kinematic and dynamics of ball-bat collision  Trajectory of a ball with drag and lift l Can understanding these things improve our ability to play the game?  Almost surely NOT l Can understanding these things enhance our own enjoyment of the game  For me, a resounding YES  I hope for you also