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Faculty of Process and System Engineering
Master Thesis Presentation
Influence of plate thickness on contact time at elastic, elastic-plastic, plastic
impact of brass sphere on thin glass plates
presented by
Tausif Patel
Matriculation # (206098)
Supervisors:-
Dr.Ing. Peter Mueller
M.Sc. Farhad Jebelisinaki Date:- 30. 09 .2016 Magdeburg
1
CONTENTS
Introduction
Objectives and task description
Experimental setup and methodology
Results and discussion
Summary and outlook 2
INTRODUCTION
What is contact deformation ?
Contact deformation :-
Three ranges of deformation behavior
can be identified elastic, elastic-plastic,
and fully plastic
 Normal impact :-
The center of mass of colliding bodies is on the common normal line passing through the impact point.
3
INTRODUCTION (CONTD.)
 What is coefficient of restitution ?
Ratio of relative velocity after the impact to relative velocity before the impact
𝜺 =
𝒗 𝟏,𝑹
𝒗 𝟏
𝜺 =
𝑾 𝒌𝒊𝒏,𝑹
𝑾 𝒌𝒊𝒏
ε = 1 (elastic)
ε = 0 (plastic)
0 < ε < 1 (elastic – plastic)
4
OBJECTIVES AND TASK DESCRIPTION
To investigate how the impact plate thickness influence the contact time at elastic, elastic-plastic and
plastic impact of brass spheres on thin glass plates.
 Brass spheres of (d = 3 to 8.731 mm).
 Coated and noncoated glass plates (H = 2, 4, 8, 12 mm).
 Fall heights (h = 50 to 150 mm) – to study the effect of impact velocities.
 40 single experiments per each adjustment.
 Comparison of experimental results with theoretical models from Hertz and Zener .
 Force-displacement curves using compression tests. 5
EXPERIMENTAL SETUP AND METHODOLOGY
6
Schematic representation of free fall apparatus
EXPERIMENTAL SETUP AND METHODOLOGY
7
The experimental setup has divided into two
steps
 Measurement of coefficient of restitution
 Measurement of contact time
 Measurement of coefficient of restitution
Method used in experiment to compute the
coefficient of restitution
𝑣 =
𝑔. ∆𝑡
2
𝜀 =
𝑡 𝑛 + 1
𝑡 𝑛
EXPERIMENTAL SETUP AND METHODOLOGY
 Measurement of contact time
Experimental setup has been modified for formation of electric current to measure contact time
For measurement of contact time only the first impact was considered.
8
EXPERIMENTAL SETUP AND METHODOLOGY
9
 Compression test
Material behavior has been studied using
single granule uniaxial compression tests until
primary fracture at a constant loading velocity
𝑣 𝐵 = 0.01 mm/min.
Test were repeated 10 times per series of
samples
RESULTS AND DISCUSSION
10
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8
Coefficientofrestitutionε
Impact velocity v (m/s)
6.350
3
6.350
3
Measurements
d = [mm]
Zener d = [mm]
CoR vs. impact velocity (glass plate, H = 2 mm) and theoretical curves according to the Zener model
RESULTS AND DISCUSSION
11
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8
Coefficientofrestitutionε
Impact velocity v (m/s)
3 6.35
8 8.731
3 6.35
8 8.731
Measurements
d = [mm]
Zener d = [mm]
CoR vs. impact velocity (glass plate, H = 4 mm) and theoretical curves according to the Zener model
RESULTS AND DISCUSSION
12
CoR vs. plate thickness on glass plate (𝑣 = 0.85 m/s) CoR vs. plate thickness on coated plate (𝑣 = 0.85 m/s)
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
0 2 4 6 8 10 12 14
Coefficientofrestitutionε
Plate thickness H mm
3 6.350
8 8.731
3 6.350
8 8.731
Zener d = [mm]
0.5
0.55
0.6
0.65
0.7
0.75
0.8
0.85
0.9
0.95
1
0 2 4 6 8 10 12 14
Coefficientofrestitutionε
Plate thickness H mm
3 6.35
8 8.731
3 6.35
8 8.731
Measurements
d = [mm]
Zener d = [mm]
Measurements
d = [mm]
RESULTS AND DISCUSSION
13
0.5
0.55
0.6
0.65
0.7
0.75
0.8
0.85
0.9
0.95
1
0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8
Coefficientofrestitutionε
Sphere diameter/plate thickness (d/H)
0.55
0.9
1.25
0.55
0.9
1.25
Measurements
v = [m/s]
Zener v= [m/s]
CoR vs. ratio of sphere diameter to plate thickness (d / H) and the theoretical curves according to the Zener
model
RESULTS AND DISCUSSION
14
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
0 1 2 3 4 5 6 7 8 9 10
Coefficientofrestitutionε
Sphere diameter d (mm)
0.55
0.9
1.6
Measurements
v =[m/s]
CoR vs. Particle diameter on gold coated plate (H = 4 mm)
RESULTS AND DISCUSSION
15
10
20
30
40
50
60
70
80
90
100
0 2 4 6 8 10 12 14
Contacttimeµs
Plate thickness H mm
3 6.350
8 8.731
3 6.350
8 8.731
Measurements d =[mm]
Zener d =[mm]
Contact time vs. plate thickness (𝑣 = 0.98 m/s) theoretical curves according to Zener model
RESULTS AND DISCUSSION
16
30
40
50
60
70
80
90
100
0.45 0.65 0.85 1.05 1.25 1.45 1.65 1.85
Contacttimeµs
Impact velocity v (m/s)
2 4
8 12
2 4
8 12
Contact time vs. Impact velocity at (d = 8 mm) the theoretical curves according to the Zener model
Measurements
H=[mm]
Zener H= [mm]
RESULTS AND DISCUSSION
17
10
15
20
25
30
35
40
45
50
55
0.4 0.6 0.8 1 1.2 1.4 1.6 1.8
Contacttimeµs
Impact velocity v (m/s)
3 6.35
8 8.731
3 6.35
8 8.731
Contact time vs. Impact velocity (H = 4 mm) and the theoretical curves as per Zener’s model
Measurements
d =[mm]
Measurements d =[mm]
Zener d =[mm]
RESULTS AND DISCUSSION
18
Contact time vs. sphere diameter at (H= 4 mm) an VA= 0.98, 1.65 and
theoretical curves as per Hertz & Zener model
Contact time vs. sphere diameter at (H= 12 mm) and VA= 0.98, 1.65
and theoretical curves as per Hertz & Zener model
0
10
20
30
40
50
60
0 2 4 6 8 10
Contacttimeμs
Sphere diameter d (mm)
Measurement VA = 0.98 (m/s)
Measurements VA=1.65 (m/s)
Zener VA = 0.98 (m/s)
Herz VA = 0.98 (m/s)
Zener VA= 1.65 (m/s)
Hertz VA =1.65 (m/s)
0
5
10
15
20
25
30
35
40
45
50
0 2 4 6 8 10
Contacttimeμs
Sphere diameter d (mm)
measurement VA=0.98
Measurements VA=1.65 (m/s)
Zener VA=0.98
Hertz VA=0.98
Zener VA=1.65 (m/s)
Hertz VA= 1.65 (m/s)
RESULTS AND DISCUSSION
19
0.00
5.00
10.00
15.00
20.00
25.00
30.00
35.00
40.00
45.00
50.00
0.0000 0.0100 0.0200 0.0300 0.0400 0.0500
Force(N)
Displacement (mm)
Experimental force N linear fit
0.00
10.00
20.00
30.00
40.00
50.00
60.00
70.00
80.00
0.0000 0.0100 0.0200 0.0300 0.0400 0.0500
Force(N) Displacement (mm)
Experimental force N linear fit
Force vs displacement behavior of (d= 3 mm) and (d = 6.350 mm) and approach
for linear relation in plastic regime
SUMARRY AND OUTLOOK
Coefficient of restitution is inversely proportional to impact velocity & sphere
diameter where as it is directly proportional to plate thickness
The Experimental values are lesser than values derived from Zener’s model
The measured values of the contact time on a plate of 2 mm thickness showed a
notable deviation from the theoretical model of Zener
Contact time increases with increasing the sphere diameter where as it decreases with
increasing the plate thickness & impact velocities
Experimental contact time values are slightly higher than values derived from Zener’s
model 20
THANK YOU
21
22
λ 0 0.5 1 1.5
ε 1 0.44 0.18 0.067
Intermediate values of CoR vs inelastic parameter
CoR vs the inelasticity parameter according to Zener’s model
23
Waves Propagation
Velocity (m/s)
Transverse
Time (µs)
H=2mm
Traverse Time
(µs)
H=4mm
Traverse Time
(µs)
H=8mm
Traverse Time
(µs)
H=12mm
Longitudinal
Waves
6196.77 0.6454 1.290 2.58 3.8724
Transverse
Waves
3577.70 1.11 2.22 4.44 6.66
24
25
0.6
0.65
0.7
0.75
0.8
0.85
0.9
0.95
1
0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8
Coefficientofrestitutionε
Impact velocity v (m/s)
3 6.350
8 8.731
3 6.350
8 8.731
Measurements d = [mm]
Zener d = [mm]
𝜆 =
𝜋
3
5
3
1
2
𝛾
2
2 𝑣 𝐴
𝐶𝐿,𝑃
1
5 𝜌1
𝜌2
3
5
𝐸1
(1 − 𝜈1
2
)
𝐸1
1 − 𝜈1
2 +
𝐸2
1 − 𝜈2
2
2
5
𝛾 =
𝑑
𝐻
Equation for inelasticity parameter
26
Plate
thickness H
[mm]
tL [µs] tTR [µs] Contact time
[µs] v=0.98
m/s
Contact time
[µs] v=1.32
m/s
Contact time
[µs] v=1.65
m/s
2 0.6454 1.11 44.7 43.54 42.41
4 1.290 2.22 33.65 30.375 29.285
8 2.58 4.44 32.39 29.63 28.21
12 3.8724 6.66 31.63 28.97 27.68
27

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Thesis Presentation presentation

  • 1. Faculty of Process and System Engineering Master Thesis Presentation Influence of plate thickness on contact time at elastic, elastic-plastic, plastic impact of brass sphere on thin glass plates presented by Tausif Patel Matriculation # (206098) Supervisors:- Dr.Ing. Peter Mueller M.Sc. Farhad Jebelisinaki Date:- 30. 09 .2016 Magdeburg 1
  • 2. CONTENTS Introduction Objectives and task description Experimental setup and methodology Results and discussion Summary and outlook 2
  • 3. INTRODUCTION What is contact deformation ? Contact deformation :- Three ranges of deformation behavior can be identified elastic, elastic-plastic, and fully plastic  Normal impact :- The center of mass of colliding bodies is on the common normal line passing through the impact point. 3
  • 4. INTRODUCTION (CONTD.)  What is coefficient of restitution ? Ratio of relative velocity after the impact to relative velocity before the impact 𝜺 = 𝒗 𝟏,𝑹 𝒗 𝟏 𝜺 = 𝑾 𝒌𝒊𝒏,𝑹 𝑾 𝒌𝒊𝒏 ε = 1 (elastic) ε = 0 (plastic) 0 < ε < 1 (elastic – plastic) 4
  • 5. OBJECTIVES AND TASK DESCRIPTION To investigate how the impact plate thickness influence the contact time at elastic, elastic-plastic and plastic impact of brass spheres on thin glass plates.  Brass spheres of (d = 3 to 8.731 mm).  Coated and noncoated glass plates (H = 2, 4, 8, 12 mm).  Fall heights (h = 50 to 150 mm) – to study the effect of impact velocities.  40 single experiments per each adjustment.  Comparison of experimental results with theoretical models from Hertz and Zener .  Force-displacement curves using compression tests. 5
  • 6. EXPERIMENTAL SETUP AND METHODOLOGY 6 Schematic representation of free fall apparatus
  • 7. EXPERIMENTAL SETUP AND METHODOLOGY 7 The experimental setup has divided into two steps  Measurement of coefficient of restitution  Measurement of contact time  Measurement of coefficient of restitution Method used in experiment to compute the coefficient of restitution 𝑣 = 𝑔. ∆𝑡 2 𝜀 = 𝑡 𝑛 + 1 𝑡 𝑛
  • 8. EXPERIMENTAL SETUP AND METHODOLOGY  Measurement of contact time Experimental setup has been modified for formation of electric current to measure contact time For measurement of contact time only the first impact was considered. 8
  • 9. EXPERIMENTAL SETUP AND METHODOLOGY 9  Compression test Material behavior has been studied using single granule uniaxial compression tests until primary fracture at a constant loading velocity 𝑣 𝐵 = 0.01 mm/min. Test were repeated 10 times per series of samples
  • 10. RESULTS AND DISCUSSION 10 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 Coefficientofrestitutionε Impact velocity v (m/s) 6.350 3 6.350 3 Measurements d = [mm] Zener d = [mm] CoR vs. impact velocity (glass plate, H = 2 mm) and theoretical curves according to the Zener model
  • 11. RESULTS AND DISCUSSION 11 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 Coefficientofrestitutionε Impact velocity v (m/s) 3 6.35 8 8.731 3 6.35 8 8.731 Measurements d = [mm] Zener d = [mm] CoR vs. impact velocity (glass plate, H = 4 mm) and theoretical curves according to the Zener model
  • 12. RESULTS AND DISCUSSION 12 CoR vs. plate thickness on glass plate (𝑣 = 0.85 m/s) CoR vs. plate thickness on coated plate (𝑣 = 0.85 m/s) 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 0 2 4 6 8 10 12 14 Coefficientofrestitutionε Plate thickness H mm 3 6.350 8 8.731 3 6.350 8 8.731 Zener d = [mm] 0.5 0.55 0.6 0.65 0.7 0.75 0.8 0.85 0.9 0.95 1 0 2 4 6 8 10 12 14 Coefficientofrestitutionε Plate thickness H mm 3 6.35 8 8.731 3 6.35 8 8.731 Measurements d = [mm] Zener d = [mm] Measurements d = [mm]
  • 13. RESULTS AND DISCUSSION 13 0.5 0.55 0.6 0.65 0.7 0.75 0.8 0.85 0.9 0.95 1 0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 Coefficientofrestitutionε Sphere diameter/plate thickness (d/H) 0.55 0.9 1.25 0.55 0.9 1.25 Measurements v = [m/s] Zener v= [m/s] CoR vs. ratio of sphere diameter to plate thickness (d / H) and the theoretical curves according to the Zener model
  • 14. RESULTS AND DISCUSSION 14 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 0 1 2 3 4 5 6 7 8 9 10 Coefficientofrestitutionε Sphere diameter d (mm) 0.55 0.9 1.6 Measurements v =[m/s] CoR vs. Particle diameter on gold coated plate (H = 4 mm)
  • 15. RESULTS AND DISCUSSION 15 10 20 30 40 50 60 70 80 90 100 0 2 4 6 8 10 12 14 Contacttimeµs Plate thickness H mm 3 6.350 8 8.731 3 6.350 8 8.731 Measurements d =[mm] Zener d =[mm] Contact time vs. plate thickness (𝑣 = 0.98 m/s) theoretical curves according to Zener model
  • 16. RESULTS AND DISCUSSION 16 30 40 50 60 70 80 90 100 0.45 0.65 0.85 1.05 1.25 1.45 1.65 1.85 Contacttimeµs Impact velocity v (m/s) 2 4 8 12 2 4 8 12 Contact time vs. Impact velocity at (d = 8 mm) the theoretical curves according to the Zener model Measurements H=[mm] Zener H= [mm]
  • 17. RESULTS AND DISCUSSION 17 10 15 20 25 30 35 40 45 50 55 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 Contacttimeµs Impact velocity v (m/s) 3 6.35 8 8.731 3 6.35 8 8.731 Contact time vs. Impact velocity (H = 4 mm) and the theoretical curves as per Zener’s model Measurements d =[mm] Measurements d =[mm] Zener d =[mm]
  • 18. RESULTS AND DISCUSSION 18 Contact time vs. sphere diameter at (H= 4 mm) an VA= 0.98, 1.65 and theoretical curves as per Hertz & Zener model Contact time vs. sphere diameter at (H= 12 mm) and VA= 0.98, 1.65 and theoretical curves as per Hertz & Zener model 0 10 20 30 40 50 60 0 2 4 6 8 10 Contacttimeμs Sphere diameter d (mm) Measurement VA = 0.98 (m/s) Measurements VA=1.65 (m/s) Zener VA = 0.98 (m/s) Herz VA = 0.98 (m/s) Zener VA= 1.65 (m/s) Hertz VA =1.65 (m/s) 0 5 10 15 20 25 30 35 40 45 50 0 2 4 6 8 10 Contacttimeμs Sphere diameter d (mm) measurement VA=0.98 Measurements VA=1.65 (m/s) Zener VA=0.98 Hertz VA=0.98 Zener VA=1.65 (m/s) Hertz VA= 1.65 (m/s)
  • 19. RESULTS AND DISCUSSION 19 0.00 5.00 10.00 15.00 20.00 25.00 30.00 35.00 40.00 45.00 50.00 0.0000 0.0100 0.0200 0.0300 0.0400 0.0500 Force(N) Displacement (mm) Experimental force N linear fit 0.00 10.00 20.00 30.00 40.00 50.00 60.00 70.00 80.00 0.0000 0.0100 0.0200 0.0300 0.0400 0.0500 Force(N) Displacement (mm) Experimental force N linear fit Force vs displacement behavior of (d= 3 mm) and (d = 6.350 mm) and approach for linear relation in plastic regime
  • 20. SUMARRY AND OUTLOOK Coefficient of restitution is inversely proportional to impact velocity & sphere diameter where as it is directly proportional to plate thickness The Experimental values are lesser than values derived from Zener’s model The measured values of the contact time on a plate of 2 mm thickness showed a notable deviation from the theoretical model of Zener Contact time increases with increasing the sphere diameter where as it decreases with increasing the plate thickness & impact velocities Experimental contact time values are slightly higher than values derived from Zener’s model 20
  • 22. 22 λ 0 0.5 1 1.5 ε 1 0.44 0.18 0.067 Intermediate values of CoR vs inelastic parameter CoR vs the inelasticity parameter according to Zener’s model
  • 23. 23
  • 24. Waves Propagation Velocity (m/s) Transverse Time (µs) H=2mm Traverse Time (µs) H=4mm Traverse Time (µs) H=8mm Traverse Time (µs) H=12mm Longitudinal Waves 6196.77 0.6454 1.290 2.58 3.8724 Transverse Waves 3577.70 1.11 2.22 4.44 6.66 24
  • 25. 25 0.6 0.65 0.7 0.75 0.8 0.85 0.9 0.95 1 0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 Coefficientofrestitutionε Impact velocity v (m/s) 3 6.350 8 8.731 3 6.350 8 8.731 Measurements d = [mm] Zener d = [mm]
  • 26. 𝜆 = 𝜋 3 5 3 1 2 𝛾 2 2 𝑣 𝐴 𝐶𝐿,𝑃 1 5 𝜌1 𝜌2 3 5 𝐸1 (1 − 𝜈1 2 ) 𝐸1 1 − 𝜈1 2 + 𝐸2 1 − 𝜈2 2 2 5 𝛾 = 𝑑 𝐻 Equation for inelasticity parameter 26
  • 27. Plate thickness H [mm] tL [µs] tTR [µs] Contact time [µs] v=0.98 m/s Contact time [µs] v=1.32 m/s Contact time [µs] v=1.65 m/s 2 0.6454 1.11 44.7 43.54 42.41 4 1.290 2.22 33.65 30.375 29.285 8 2.58 4.44 32.39 29.63 28.21 12 3.8724 6.66 31.63 28.97 27.68 27