IYPT 2010 Austria, I. R. Iran Reporter: Ali Farajollahi 1.

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IYPT 2010 Austria, I. R. Iran IYPT 2010 Austria, I. R. Iran Problem No. STEEL BALLS Reporter: Ali Farajollahi 3 1

Transcript of IYPT 2010 Austria, I. R. Iran Reporter: Ali Farajollahi 1.

Page 1: 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

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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.

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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

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Initial Observations

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Initial Observation

Deformation

Waves

Radial rupture

Burning

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Initial Observation

Aluminum

Tissue

Styrofoam

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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

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Material Strength Background

• Stress & Strain

• Poisson’s Ratiol

lA

F

F

F

l

Δl

x yy

x

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Static Loaded Balls• To be able to simulate the

collision…• Finding the deformation of two

steel balls under a specific load

FF

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Static Loaded Balls

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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

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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

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Different Strains• By assuming that the thickness of

sheet is negligible, we are able to find different strains in the sheet.

FF

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Different Strains

r

Top

r

r+Δr

After collision

Before collisionθ

Δr

Before Collision

Side

x

zMaximum Collision

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Tensile Stress

r

r+Δr

P0 : Initial perimeterP1 : Perimeter after collisionr : Initial radius r+Δr : Increased radiusεx : Deformation through x-Axis

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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

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Two Kinds of Behaviors

Critical Pressure

Pressing stress

m/s

m/s

m/s

m/s

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Two Kinds of Behaviorsσ

y

m/s

m/s

m/s

Tensile stress

Critical Pressure

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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)

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Theory Comparison• Paper• Tensile stress radius

Tensile Stress

Velocity (m/s)

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Theory Comparison• Balsa Wood• Pressing Stress Radius

Pressing Stress

Velocity (m/s)

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Theory Comparison• Balsa Wood• Tensile stress radius

Tensile Stress

Velocity (m/s)

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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

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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.

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IYPT 2010 Austria, I. R. IranIYPT 2010 Austria, National team of I. R. Iran

Thank you for your attention