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IYPT 2010 Austria, I. R. Iran Reporter: Ali Farajollahi 1.
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Transcript of IYPT 2010 Austria, I. R. Iran Reporter: Ali Farajollahi 1.
IYPT 2010 Austria, I. R. IranIYPT 2010 Austria, I. R. Iran
Problem No.
1
STEEL BALLS
Reporter: Ali Farajollahi
3
IYPT 2010 Austria, I. R. Iran2
The Question
• Colliding two large steel balls with a thin sheet of material (e.g. paper) in between may "burn" a hole in the sheet.
• Investigate this effect for various materials.
IYPT 2010 Austria, I. R. Iran3
Contents• Initial Observations• Theoretical background
– Burning or Physical Rupture?– Material Background
• Theory: The balls– Static loaded balls– Balls collision simulation
• Theory: The sheet– Different strains
• Experiments– Setup– Comparison with Theory– Different Materials & Behaviors
• Conclusion
IYPT 2010 Austria, I. R. Iran4
Initial Observations
IYPT 2010 Austria, I. R. Iran5
Initial Observation
Deformation
Waves
Radial rupture
Burning
IYPT 2010 Austria, I. R. Iran6
Initial Observation
Aluminum
Tissue
Styrofoam
IYPT 2010 Austria, I. R. Iran7
Burning (Chemical) or Rupture (Physical)?
– Temperature rises because of sheet deflection
– Not enough energy to start flaming– Not enough Oxygen in the contact
point
• Burning occurs incompletely, but the burnt amount is too low
• Main Happening: Physical Rupture
IYPT 2010 Austria, I. R. Iran8
Material Strength Background
• Stress & Strain
• Poisson’s Ratiol
lA
F
F
F
l
Δl
x yy
x
IYPT 2010 Austria, I. R. Iran9
Static Loaded Balls• To be able to simulate the
collision…• Finding the deformation of two
steel balls under a specific load
FF
IYPT 2010 Austria, I. R. Iran10
Static Loaded Balls
IYPT 2010 Austria, I. R. Iran11
Static Loaded Balls• According to references, Contact
mechanics and Hertz theory, the force and shape of two steel balls can be calculated as follows:
r : Distance between a plot and center of contactδ : Maximum length of deformationα : Radius of contactR : Half of the radius of the ballsE* : Young’s modulusP0 : Pressure in the middle of contactF : Force
IYPT 2010 Austria, I. R. Iran12
Dynamic collision simulation• Simulating the system considering
to be quasi-static– F will be calculated as explained
– Euler method was used
Updating time
Calculating
forces
Finding accelera
tion
Updating
positions
at
x
m
F
2
2
IYPT 2010 Austria, I. R. Iran13
Different Strains• By assuming that the thickness of
sheet is negligible, we are able to find different strains in the sheet.
FF
IYPT 2010 Austria, I. R. Iran14
Different Strains
r
Top
r
r+Δr
After collision
Before collisionθ
Δr
Before Collision
Side
x
zMaximum Collision
IYPT 2010 Austria, I. R. Iran15
Tensile Stress
r
r+Δr
P0 : Initial perimeterP1 : Perimeter after collisionr : Initial radius r+Δr : Increased radiusεx : Deformation through x-Axis
IYPT 2010 Austria, I. R. Iran16
Two Kinds of Behaviors• Materials may rip because of
tensile or pressing stress
– σz: Pressing
– σy: Tensile
r
dr
r
dr
r
dx zzr
y
Δr
z
x
IYPT 2010 Austria, I. R. Iran17
Two Kinds of Behaviors
Critical Pressure
Pressing stress
m/s
m/s
m/s
m/s
IYPT 2010 Austria, I. R. Iran18
Two Kinds of Behaviorsσ
y
m/s
m/s
m/s
Tensile stress
Critical Pressure
IYPT 2010 Austria, I. R. Iran19
Experimental Setup
Holding the balls
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Experimental Setup
Using two electronic magnets to hold and release the balls on time
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Experiments• Changing the release height,
calculating the velocity
• Scanning the holes, developing a program with MATLAB to calculate the area and radius of holes
• Compare with theory
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Experiments• Paper, thickness of 0.2mm
• Released from different heights
5cm 10cm 15cm 20cm 40cm30cm
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Experiments
0 5 10 15 20 25 30 35 40 450
0.1
0.2
0.3
0.4
0.5
0.6
0.7
Release Height (cm)
Hole
Rad
ius (
cm)
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Experiments
• Paper thickness 0.1 mm
10cm 15cm 20cm 30cm 40cm
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Experiments
Release Height (cm)
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Experiments
• Balsa Wood 2.5mm Thick
10cm 15cm 20cm 30cm
40cm
25cm
35cm
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Experiments
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Comparison with Theory
• There are 2 main Causes,– Pressure Stress– Tensile Stress
• Calibrating the Critical Stress in Both Causes
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Theory Comparison• Paper 0.2 mm thick• The Maximum contact area is smaller than the
experiments radius
Pressing Stress
Velocity (m/s)
IYPT 2010 Austria, I. R. Iran30
Theory Comparison• Paper• Tensile stress radius
Tensile Stress
Velocity (m/s)
IYPT 2010 Austria, I. R. Iran31
Theory Comparison• Balsa Wood• Pressing Stress Radius
Pressing Stress
Velocity (m/s)
IYPT 2010 Austria, I. R. Iran32
Theory Comparison• Balsa Wood• Tensile stress radius
Tensile Stress
Velocity (m/s)
IYPT 2010 Austria, I. R. Iran33
Conclusion• Most of the phenomena happens
because of stresses in the sheet
• Burning is negligible in describing the phenomena, although it exists.
• Materials are different in the stresses they stand– Paper is weak in tensile stress– Balsa wood is weak in pressing stress
IYPT 2010 Austria, I. R. Iran34
References• Mechanics of Materials, Egor P. Popov, 2nd
Edition, 1976.• Contact mechanics, K.L. Johnson, Cambridge
University press, 1985.• Halliday Fundamentals of physics, Halliday-
Resnic-Walker, 1945.• A First Course in Numerical Analysis, Anthony
Ralston-Philip Rabinowitz, 2nd Edition, 2001.
IYPT 2010 Austria, I. R. IranIYPT 2010 Austria, National team of I. R. Iran
Thank you for your attention