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AAPT Philadelphia Meeting: The Science of Sports January 23, 2002 Page 1
A Comparative Study ofA Comparative Study ofWood and Aluminum Baseball BatsWood and Aluminum Baseball Bats
Alan M. NathanAlan M. NathanUniversity of Illinois at Urbana-ChampaignUniversity of Illinois at Urbana-Champaign
[email protected]@uiuc.eduhttp://www.npl.uiuc.edu/~a-nathan/pobhttp://www.npl.uiuc.edu/~a-nathan/pob
Introduction
Some Basics
Wood vs. Aluminum
Some Examples
Summary/Conclusions
AAPT Philadelphia Meeting: The Science of Sports January 23, 2002 Page 2
Introduction: Introduction: Description of Ball-Bat CollisionDescription of Ball-Bat Collision
violent collision forces large (>8000 lbs!)
time is short (<1/1000 sec!)
bat compresses ball kinetic energy potential energy
lots of energy dissipated
ball deforms bat vibrations!
performance metric: ball exit speed vf
AAPT Philadelphia Meeting: The Science of Sports January 23, 2002 Page 3
• vball and vbat
• “Collision efficiency” (eA)
* For superball on massive, rigid bat … eA 1
* For baseball on typical bat … eA 0.2
+ Recoil of bat
+ Energy dissipated in ball and bat
vball vbat
vf
What Does vf Depend On?
vf = eA vball + (1+eA) vbat
AAPT Philadelphia Meeting: The Science of Sports January 23, 2002 Page 4
Recoil Energy of Bat: m/MRecoil Energy of Bat: m/Meffeff
Bat recoil depends on….
• mass M
• mass distribution
* location of CM
* MOI ICM
• impact location (z)
Translation: Rotation:
1/Meff = 1/M + z2/ICM
. .CM
z
.
AAPT Philadelphia Meeting: The Science of Sports January 23, 2002 Page 5
Energy Dissipation: The COREnergy Dissipation: The COR
Coefficient Of Restitution: “bounciness” of ball
• in CM frame: Ef/Ei = COR2
• massive rigid surface: COR2 = hf/hi 0.25
COR 0.5
~3/4 CM energy dissipated!
• depends (weakly) on impact speed
• depends on surface
the bat matters too!
AAPT Philadelphia Meeting: The Science of Sports January 23, 2002 Page 6
0 5 10 15 20 25 30 35
f1 = 177 Hz
f2 = 583 Hz
Effect of Bat on COR: Vibrations
nodes
0
0.1
0.2
0.3
0.4
0.5
0 2 4 6 8 10 12 14distance from tip (inches)
CORCM
COR depends strongly on impact location
AAPT Philadelphia Meeting: The Science of Sports January 23, 2002 Page 7
Putting Everything Together...
“sweet spot” depends on•collision efficiency
*recoil factor*COR
•how bat is swung
20
40
60
80
100
0.00
0.05
0.10
0.15
0.20
0.25
0 2 4 6 8 10 12 14
eAv (mph)
distance from tip (inches)
vf
eA
vbat
CM
vf = eA vball + (1+eA) vbat
AAPT Philadelphia Meeting: The Science of Sports January 23, 2002 Page 8
Aluminum vs. Wood
• Inertial Effects: mass and mass distribution* recoil* bat swing
• Dynamic Effects* COR: the trampoline effect
AAPT Philadelphia Meeting: The Science of Sports January 23, 2002 Page 9
direct comparision
3.6% larger vbat
Generic Wood-Aluminum Comparison
60
70
80
90
100
2 3 4 5 6 7 8 9
vf (mph)
distance from knob (inches)
woodaluminum
Conclusion: Inertial effects seem to favor wood
AAPT Philadelphia Meeting: The Science of Sports January 23, 2002 Page 10
Compressional energy shared between ball and bat
Ball very inefficient (~25% restored)
Wood Bat hard to compress little effect on COR
Aluminum Bat
compressible through “shell” modes COR larger
The “Trampoline” Effect
AAPT Philadelphia Meeting: The Science of Sports January 23, 2002 Page 11
direct comparision
3.6% larger vbat
3.6% larger vbat + 10% larger COR
Generic Wood-Aluminum Comparison
60
70
80
90
100
2 3 4 5 6 7 8 9
vf (mph)
distance from knob (inches)
woodaluminum
Conclusion: Trampoline effect favors aluminum
AAPT Philadelphia Meeting: The Science of Sports January 23, 2002 Page 12
The Trampoline Effect: A Closer LookThe Trampoline Effect: A Closer Look
Bending Modes vs. Shell Modes
k R4: 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
AAPT Philadelphia Meeting: The Science of Sports January 23, 2002 Page 13
Tracking the Energy
0
50
100
150
200
250
300
350
400
0 0.2 0.4 0.6 0.8 1
Wood Bat
Ball KE
Ball PE
Bat Recoil KE
Bat Vibrational E
Energy (J)
t (ms)
0
50
100
150
200
250
300
350
400
0 0.2 0.4 0.6 0.8 1
Aluminum Bat
Ball KE
Ball PE
Bat Recoil KE
Bat Vibrational E
Energy (J)
t (ms)
AAPT Philadelphia Meeting: The Science of Sports January 23, 2002 Page 14
Example 1: Effect of Wall Thicknessk t3 t
make wall thinner add mass to keep CM, ICM fixed
100
105
110
115
0.08 0.09 0.10 0.11 0.12
vf (mph)
t (in)
Conclusion:thinner is better!
AAPT Philadelphia Meeting: The Science of Sports January 23, 2002 Page 15
Example 2: Redistributing the Mass
make wall thinner add mass at different locations
Conclusion:barrel loading better!
80
85
90
95
100
105
2 3 4 5 6 7 8 9 10
vf (mph)
distance from barrel (inches)
d=6"
d=0"
d=33"
d=12"
AAPT Philadelphia Meeting: The Science of Sports January 23, 2002 Page 16
Example 3:
“Corking” a Wood Bat “Corking” a Wood Bat (illegal!)(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?
AAPT Philadelphia Meeting: The Science of Sports January 23, 2002 Page 17
Not Corked DATA Corked COR: 0.445 0.005 0.444 0.005
Conclusions:
• no tramopline effect!
• corked bat is WORSE even with higher vbat
Bat Research Center, UML, Sherwood & amn, Aug. 2001
70
80
90
2 3 4 5 6 7 8 9
vf (mph)
distance from knob (inches)
uncorked
corked
calculation
AAPT Philadelphia Meeting: The Science of Sports January 23, 2002 Page 18
Example 4: Ash vs. Maple Ash vs. Maple (legal!)(legal!) (maple) 1.085 (ash)
• equal mass Rmaple = Rash/1.042
• k ~ R4 kmaple = 0.92 kash
more compression energy stored in maple
Conclusion: B2 had no real
advantage!
70
75
80
85
90
95
100
2 3 4 5 6 7 8 9
vf (mph)
z (inches)
Ash
Maple
AAPT Philadelphia Meeting: The Science of Sports January 23, 2002 Page 19
Summary and ConclusionsSummary and Conclusions
The physics of ball-bat collision is well understood
There are significant differences between wood and aluminum mass distribution trampoline effect
Wood bats cannot easily duplicate trampoline effect
Aluminum bats work better!