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KINEMATIC ANALYSIS OF A MOTORCYCLE AND RIDER IMPACT ON A
CONCRETE BARRIER UNDER DIFFERENT IMPACT AND ROAD CONDITIONS
A Thesis by
Shashikumar Ramamurthy
Bachelor of Engineering, Bangalore University, 2004
Submitted to the Department of Mechanical Engineering
and the faculty of the Graduate School ofWichita State University
in partial fulfillment of
Master of Science
December 2007
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Copyright 2007 by [Shashikumar Ramamurthy],
All Rights Reserved
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KINEMATIC ANALYSIS OF A MOTORCYCLE AND RIDER IMPACT ON A
CONCRETE BARRIER UNDER DIFFERENT IMPACT AND ROAD CONDITIONS
The following faculty members have examined the final copy of this thesis for form andcontent and recommend that it be accepted in partial fulfillment of the requirements for the
degree of Master of Science, with a major in Mechanical Engineering
_____________________________________________
Hamid M. Lankarani, Committee Chair
We haveread this thesis and recommend its acceptance:
_________________________________________________
Kurt Soschinske, Committee Member
___________________________________________________
Krishna Krishnan, Committee Member
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DEDICATION
To my parents and Chandra Mohans family members, who kept me continuously
motivated with their great support and encouragement throughout my MS program.
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ACKNOWLEDGEMENTS
I take this opportunity to extend my sincere gratitude and appreciation to many great
people who made this Masters possible. First I would likt to thank my academic advisor Dr.
Hamid M. Lankarani for all his valuable help and guidance. His constant encouragement and
motivation helped me a lot in the completion of this thesis and my masters.
I would like to thank my committee members Dr. Kurt Soschinske, Dr Krishna
Krishnan for being my committee and reviewing this report.
I would like to thank my mom and brothers who supported me throughout my life and
without their sacrifice and love I would not have achieved this goal.
I would like to thank Mr Chandra Mohan and Mrs Nirupa Mohan for their constant
motivation and of course my beloved friend Ms. Thejeswini Mohan serving as a back bone.
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ABSTRACT
In many countries, motorcycle crashes constitutes a significant proportion of all road
crash fatalities and injuries and safety measures can be successful only if much more
attention is devoted to this issue. Several Roadside guard systems such as concrete barriers,
wire rope barriers and steel guard rails are used to protect occupants of four wheels and heavy
trucks. Yet motorcycle riders are vulnerable to any crash scenario, resulting in major injuries.
Also the climatic conditions have a major impact on motorcyclists. Thousands of
motorcyclists are killed or injured in road accidents. The need to provide and improve crash
survival programs in collision environment is the subject matter of interest and research. In
this research, simulation of full scale crash tests of a motorcycle with rider driven in an
upright position and sliding on the road surface impacting on steel barriers and concrete
barriers are carried out by DEKRA Accident Research, to analyze real-world crashes. It is
most important to evaluate head injury risks as it causes a serious threat to life. The
motorcycle model with a rider are developed in MADYMO 6.3 and validated using the real
time barrier tests.
Under normal road conditions, the motorcycle driven in an upright position is
assumed to have a pre-crash velocity of 60km/h impacting at 12 on a concrete barrier. The
validation criteria used are: motorcycle kinematics, rider kinematics and the rider injury
criteria. The results obtained in this research are found to be in a reasonable correlation with
the experimental data. A parametric study is then conducted to investigate the crash for
various impact speeds (40 km/h, 60 km/h and 80 km/h) under different impact scenarios (6
impact, 8 impact, 12 impact, 24 impact, 45 impact, 60 impact and 90 impact).
An icy road condition is then studied. A study of kinematics and injury parameters
for a motorcycle rider is proven to be different under various impact speeds (40 km/h, 60
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km/h and 80 km/h) under different impact scenarios (6 impact, 8 impact, 12 impact, 24
impact, 45 impact, 60 impact and 90 impact).
Design of Experiments is conducted to study the contribution of the road condition,
impact angles, speed and the interaction of these factors. The result from this study helps in
understanding the factors affecting the crash and rider injuries. Design of Experiment also
provides a valuable knowledge about the contribution of factors chosen (road type, angle of
collision and speed) towards accidents.
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TABLE OF CONTENTS
CHAPTER PAGE
1 INTRODUCTION.........................................1
1.1 Importance of Motorcycle Accidents Study............1
1.2 Motorcycle Accidents Statistical Background21.2.1 Motorcycle Accidents Safety Programs ...3
1.3 Types of riding.........41.3.1 Rider training and licensing...5
1.4 Importance of Safety Barriers..........51.5 Effects of Safety Barriers on Motorcyclist..61.6 Literature Review71.7 Objectives......11
2 MATHEMATICAL MODELING PRINCIPLES...12
2.1 Importance of Computer Simulations........122.2 Introduction to MADYMO........12
2.3 Introduction to Multi-body Systems..142.4 Introduction to Kinematics Joints..14
2.4.1 Types of mechanical joints.......16
2.5 Introduction to Inertial Space and Null space Systems.....182.6 Introduction to Injury Biomechanics.202.7 Injury Parameters...........202.8 Injury criteria.212.9 Head Injury Criteria.......222.10 Neck Injury Criteria.......232.11 Thoracic Trauma Index.....242.12 Femur Force Criteria.25
3 MATHEMATICAL MODELING OF MOTORCYCLE AND BARRIER........26
3.1 Methodology..26
3.2 Rider modeling......27
3.3 Motorcycle modeling.....28
3.4 Concrete Barrier modeling....30
4 VALDATION OF MOTORCYLE AND MOTORCYCLE WITH RIDER...31
4.1 Validation of a Motorcycle....314.2 Validation of a Motorcycle with a rider....33
5 ANALYSIS OF MOTORCYCLE AND BARRIER IMPACT...38
5.1 Analysis of a Motorcycle-Concrete Barrier impact- Test matrix...385.1.1 Analysis of 12 deg / 40km/h / NRC .....405.1.2 Analysis of 12 deg / 80km/h / NRC......415.1.3 Analysis of 6 deg / 40km/h / NRC ...........425.1.4 Analysis of 6 deg / 60km/h / NRC ...........435.1.5 Analysis of 6 deg / 80km/h / NRC ...........445.1.6 Analysis of 8 deg / 40km/h / NRC ...455.1.7 Analysis of 8 deg / 60km/h / NRC ...........465.1.8 Analysis of 8 deg / 80km/h / NRC ...........47
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TABLE OF CONTENTS (CONTINUED)
CHAPTER PAGE
5.1.9 Analysis of 24 deg / 40km/h / NRC .485.1.10 Analysis of 24 deg / 60km/h / NRC ....49
5.1.11 Analysis of 24 deg / 80km/h / NRC ....505.1.12 Analysis of 45 deg / 40km/h / NRC ... 51
5.1.13 Analysis of 45 deg / 60km/h / NRC.... 52
5.1.14 Analysis of 45 deg / 80km/h / NRC ... 53
5.1.15 Analysis of 60 deg / 40km/h / NRC 54
5.1.16 Analysis of 60 deg / 60km/h / NRC 55
5.1.17 Analysis of 60 deg / 80km/h / NRC 56
5.1.18 Analysis of 90 deg / 40km/h / NRC 57
5.1.19 Analysis of 90 deg / 60km/h / NRC 58
5.1.20 Analysis of 90 deg / 80km/h / NRC 59
5.1.21 Analysis of 6 deg / 40km/h / IRC 60
5.1.22 Analysis of 6 deg / 60km/h / IRC 61
5.1.23 Analysis of 6 deg / 80km/h / IRC 625.1.24 Analysis of 8 deg / 40km/h/ IRC .63
5.1.25 Analysis of 8 deg / 60km/h / IRC 64
5.1.26 Analysis of 8 deg / 80km/h / IRC 65
5.1.27 Analysis of 12 deg / 40km/h / IRC ..66
5.1.28 Analysis of 12 deg / 60km/h / IRC ..67
5.1.29 Analysis of 12 deg / 80km/h / IRC ..68
5.1.30 Analysis of 24 deg / 40km/h / IRC ..69
5.1.31 Analysis of 24 deg / 60km/h / IRC ..70
5.1.32 Analysis of 24 deg / 80km/h / IRC ......71
5.1.33 Analysis of 45 deg / 40km/h / IRC ......72
5.1.34 Analysis of 45 deg / 60km/h / IRC ..73
5.1.35 Analysis of 45 deg / 80km/h / IRC ..74
5.1.36 Analysis of 60 deg / 40km/h / IRC ..........75
5.1.37 Analysis of 60 deg / 60km/h / IRC ..76
5.1.38 Analysis of 60 deg / 80km/h / IRC ..77
5.1.39 Analysis of 90 deg / 40km/h / IRC ..78
5.1.40 Analysis of 90 deg / 60km/h / IRC ..79
5.1.41 Analysis of 90 deg / 80km/h / IRC ......80
5.2 Discussion of Results...81
6 DESIGN OF EXPERIMENTS APPLIED TO THE SYSTEM...93
6.1 Principles of Design of Experiments.......93
6.2 Steps to be considered while implementing DOE.......................................946.3 Factors considered for Design of Experiments....... 94
6.4 Effects of the model.... 94
7 CONCLUSIONS AND RECOMMENDATIONS......98
7.1 Conclusions.................98
7.2 Recommendations.. 99
REFERENCES..................101
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LIST OF TABLES
TABLE PAGE
1.1 NHTSAs Motorcycle Safety Program..3
2.1 Standard typologies selected for Model generation.28
3.1 Standard MADYMO Hybrid III 50th
percentile dummy specification284.1 Dimensions of a Motorcycle28
5.1 Dimensions of a Concrete barrier30
6.1 Comparison of results between full-scale crash test and simulated
Experiment for 12 deg/ 60km/h/ NRC.37
7.1 Analysis of Motorcycle-Concrete Barrier impact under NRC.387.2 Analysis of Motorcycle-Concrete Barrier impact under IRC...388.1 Neck at 40 km/h-NRC..828.2 Neck at 60 km/h-NRC..848.3 Neck at 80 km/h-NRC..868.4 Neck at 40 km/h-IRC888.5 Neck at 60 km/h-IRC90
8.6 Neck at 80 km/h-IRC929.1 Effects of the model..95
9.2 ANOVA table for the model.....96
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LIST OF FIGURES
FIGURE PAGE
1.2 Statistical data of motorcyclists killed in the consecutive years...2
1.3 Statistical data indicating the ways motorcycles been utilized.4
1.3.1 Rider Training and Licensing...................................................................51.4 Median Barrier...............6
1.5 Motorcycle impacting safety barrier system.7
1.6.1 Motorcycle impacting safety barrier and car.........8
1.6.2 Motorcycle after the 90deg/32.2 km/h Barrier test and Motorcycle
trolley, including dummy support frame...9
1.6.3 Full simulation model of scooter type motorcycle and a car...10
1.6.4 Test where Motorcycle impacted the Barrier in an upright driving position..10
2.2 MADYMO structure........13
2.3 Example of single and multi-body systems with tree structure...14
2.4 Constraint load in a spherical joint..15
2.4.1(a)Revolute Joint..16
2.4.1(b)Translational Joint.......172.4.1(c)Speherical Joint...17
2.4.1(d)Universal Joint............18
2.5 Inertial space coordinate system.19
2.5.1 Null system Co-ordinate system.19
3.1 Methodology representing models.26
3.1(a) Methodology representing joints27
3.2 Rider modeling...27
3.3 Kawasaki ER 5 Twister..28
3.3.1 Three-dimensional Motorcycle model29
3.3.2 Three-dimensional Motorcycle model representing joints.29
3.4 Three-dimensional Concrete Barrier model...30
4.1 Motorcycle and Barrier modeled in MADYMO31
4.1(a) Simulated kinematics of the motorcycle for the 90 degree/32.2 km/h
Barrier test condition..32
4.1(b) Simulated resultant Acceleration Left of the CG for 90 degree/32.2 km/h.......33
4.2 Motorcycle with a rider..34
4.2(a) Full-scale crash test of a motorcycle impacting a concrete barrier
Protection system in an upright position prior to impact moving..34
4.2(b) Motorcycle and rider trajectories during 175 milliseconds after
Impacting the concrete barrier as determined from analysis of the
overhead-view Cameras......34
4.2(c) Motorcycle with a rider moving along the concrete barrier35
4.2(d) Simulated kinematics for12 deg/ 60km /h. / NRC for validation......364.2(e) Femur R Resultant Force (N)37
4.2(f) Neck flexion and extension....37
5.1.1 Simulated Kinematics for 12 deg/40 km/ h /NRC......40
5.1.2 Simulated Kinematics for 12 deg/80 km/ h /NRC.....41
5.1.3 Simulated Kinematics for 6 deg/40 km/ h /NRC.......42
5.1.4 Simulated Kinematics for 6 deg/60 km/ h /NRC.......43
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LIST OF FIGURES (CONTINUED)
FIGURE PAGE
5.1.5 Simulated Kinematics for 6 deg/80 km/ h /NRC.........44
5.1.6 Simulated Kinematics for 8 deg/40 km/ h /NRC.........45
5.1.7 Simulated Kinematics for 8 deg/60 km/ h /NRC.....465.1.8 Simulated Kinematics for 8 deg/80 km/ h /NRC.........47
5.1.9 Simulated Kinematics for 24 deg/40 km/ h /NRC.......48
5.1.10 Simulated Kinematics for 24 deg/60 km/ h /NRC.......49
5.1.11 Simulated Kinematics for 24 deg/80 km/ h /NRC...50
5.1.12 Simulated Kinematics for 45 deg/40 km/ h /NRC...51
5.1.13 Simulated Kinematics for 45 deg/60 km/ h /NRC...52
5.1.14 Simulated Kinematics for 45 deg/80 km/ h /NRC...53
5.1.15 Simulated Kinematics for 60 deg/40 km/ h /NRC...54
5.1.16 Simulated Kinematics for 60 deg/60 km/ h /NRC...55
5.1.17 Simulated Kinematics for 60 deg/80 km/ h /NRC...56
5.1.18 Simulated Kinematics for 90 deg/40 km/ h /NRC...57
5.1.19 Simulated Kinematics for 90 deg/60 km/ h /NRC....585.1.20 Simulated Kinematics for 90 deg/80 km/ h /NRC....59
5.1.21 Simulated Kinematics for 6 deg/40 km/ h /IRC...60
5.1.22 Simulated Kinematics for 6 deg/60 km/ h /IRC...61
5.1.23 Simulated Kinematics for 6 deg/80 km/ h /IRC...62
5.1.24 Simulated Kinematics for 8 deg/40 km/ h /IRC...63
5.1.25 Simulated Kinematics for 8 deg/60 km/ h /IRC...64
5.1.26 Simulated Kinematics for 8 deg/80 km/ h /IRC...65
5.1.27 Simulated Kinematics for 12 deg/40 km/ h /IRC.66
5.1.28 Simulated Kinematics for 12 deg/60 km/ h /IRC.67
5.1.29 Simulated Kinematics for 12 deg/80 km/ h /IRC.68
5.1.30 Simulated Kinematics for 24 deg/40 km/ h /IRC.69
5.1.31 Simulated Kinematics for 24 deg/60 km/ h /IRC.70
5.1.32 Simulated Kinematics for 24 deg/80 km/ h /IRC.71
5.1.33 Simulated Kinematics for 45 deg/40 km/ h /IRC.72
5.1.34 Simulated Kinematics for 45 deg/60 km/ h /IRC.73
5.1.35 Simulated Kinematics for 45 deg/80 km/ h /IRC.74
5.1.36 Simulated Kinematics for 60 deg/40 km/ h /IRC.75
5.1.37 Simulated Kinematics for 60 deg/60 km/ h /IRC.76
5.1.38 Simulated Kinematics for 60 deg/80 km/ h /IRC.77
5.1.39 Simulated Kinematics for 90 deg/40 km/ h /IRC.78
5.1.40 Simulated Kinematics for 90 deg/60 km/ h /IRC.79
5.1.41 Simulated Kinematics for 90 deg/80 km/ h /IRC.80
5.2.1 HIC at 40 km / h-NRC for different impact angles..815.2.2 Femur R at 40km/h-NRC.81
5.2.3 HIC at 60 km / h-NRC for different impact angles..83
5.2.4 Femur R at 60 km/h-NRC83
5.2.5 HIC at 80 km / h-NRC for different impact angles..85
5.2.6 Femur R at 80km/h-NRC.85
5.2.7 HIC at 40 km / h-IRC for different impact angles87
5.2.8 Femur R at 40 km/h-IRC..87
5.2.9 HIC at 60 km / h-IRC for different impact angles89
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LIST OF FIGURES (CONTINUED)
FIGURE PAGE
5.2.10 Femur R at 60km/h-IRC..89
5.2.11 HIC at 80 km / h-IRC for different impact angles....91
5.2.12 Femur R at 80km/h-IRC...916.4.1 Effects of angle of Collision on HIC966.4.2 Effects of speed on HIC976.4.3 Effects of road condition on HIC..98
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LIST OF ABBREVIATIONS
ABBREVIATION DESCRIPTION
NHTS National Highway Traffic Safety Administration
HHs Health and Human Services
HIC Head Injury Criterion
T0 Start time of the simulation
TE End time of the simulation
t1 Initial time of interval during which HIC attains maximum value
t2 Final time of interval during which HIC attains maximumvalue
FMVSS Federal Motor Vehicle Standards
NRC Normal Road Condition
IRC Ice Road Condition
COG Center of Gravity
GSI Gadd Severity Index
NIC Neck Injury Criteria
TTI Thoraic Trauma Index
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CHAPTER 1
INTRODUCTION
1.1 Importance of Motorcycle Accidents Study
Motorcycle accidents have become very popular yet a serious subject of matter in this
decade. According to the National Highway Traffic Safety Administration (NHTSA) about
2,100 motorcyclists were killed in 1997 and around 4500 motorcyclists in 2005 [1]. The
increase in the number of motorcycles on the road is one contributing factor to the rising
death toll; but, even with this increase taken into account, the number of crashes is up. It is
known that the motorcycles differ completely from cars in their design and handling. As a
result they have a complex behavior during the time of impact. The most important difference
between cars and motorcycles is that motorcycle has no passenger cubicle and the rider is
reserved to the motorcycle only by his grip on the handle bars. As a result, the rider is free to
move independently of the motorcycle during the impact and is separated from his vehicle in
most of the accidents. Exposure to collision environment and separation from the motorcycle
are simply facts of life in motorcycle accidents. Another important difference is that
motorcycle lose balance due to improper seating position, locking up brakes, speeding,
weather conditions which happens frequently just before collision. During accidents,
motorcycle is subjected to either yaw or lean or both at the time. At upright position,
Motorcycles usually collides front end first but when motorcycle is down sliding, any of its
parts like the front end, wheel, and tank collide with obstacles. The rider may be partially or
completely separated from the motorcycles before impact. Hence the impact threat to a
motorcyclist is Omni-directional. Due to small in size, motorcyclist is always in danger when
they collide to any hindrance [1].
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21002300
2550
29503200 3250
3900 40284553
0
500
1000
1500
2000
2500
3000
3500
4000
4500
5000
1997 1998 1999 2000 2001 2002 2003 2004 2005
1.2 Motorcycle Accidents Statistical Background
Motorcycle riding has become very popular from past two decades, attracting all age
groups. As Motorcycles become more popular, sales rise, so has the number of accidents and
fatalities [2]
Figure 1.2 Statistical data of Motorcyclists killed in the consecutive years[2]
In 2005, nearly 4,553 people died in motorcycle crashes, an increase of 13 percent from
4,028 in 2004[2].
Motorcycle fatalities have increased for eight consecutive years[2].
Motorcyclists were 34 more times likely than passenger car occupants to die in a crash in
2005 and 8 times more likely to be injured[2].
From 1997 to 2005, motorcycle fatalities are estimated to have risen 115 percent. In 2005,
87,000 riders were injured in accidents, up 14.5 percent from 76,000 in 2004 [2].
Motorcyclists accounted for 10.5 percent of total traffic fatalities, 13.8 percent of occupant
fatalities and 3.5 percent of all occupants injured [2].
47 percent of riders killed were 40 years of age and older [2].
Fatalities of riders 30 years of age and under dropped to 32 percent in 2005 compared to 50
percent in 1995 [2].
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Fatalities among riders 30 to 35 years of age also dropped 21 percent from 26 percent in
1995 [2].
34 percent of motorcyclists involved in fatal crashes were speeding compared to 26 percent
of passenger car drivers [2].
24 percent of riders involved in a fatal accident were riding without a valid license [2].
1.2.1 Motorcycle Accidents Safety Programs
Several efforts were put forth by NHTSA to prevent accident rates and to bring
awareness on safety programs. As a result of providing a greatest benefit of safety for
motorcyclists. The Motorcycle Safety Program covers major areas of concern which includes
causes for crashes, operator behavior and roadway design. The program also has a complete
approach that helps prevention of crash, lessen rider injury when collision occurs and to
provide rapid and appropriate emergency medical services response. The causes for crash
and the methods to prevent crash scenarios were organized according to the Haddon Matrix,
where crash event is divided into three phases namely: Pre-Crash, Crash and Post-Crash and
the factors influencing each of the crash time phases are Human Factors, Vehicle Role and
Environmental Conditions as shown in the table[2].
Table 1.1 NHTSAs Motorcycle Safety Program[2]
Human Factors Vehicle Role Environmental Conditions
Crash
Prevention
(Pre-Crash)
Rider Education/Licensing
Impaired Riding
Motorist Awareness
State Safety Programs
Brakes, Tires,and Controls
Lighting and
Visibility
Compliance
Testing and
Investigations
Roadway Design,Construction, Operationsand Preservation
Roadway Maintenance
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1.99
2.27
3.69
2.87
2.65
0 0.5 1 1.5 2 2.5 3 3.5 4
Casual Pleasure
Riding
Touring under 500
miles
Commuting &
Running Errands
Sport Riding
Touring over 500
miles
Injury
Mitigation
(Crash)
Use of Protective Gear OccupantProtection
Roadside Design,Construction, and
Preservation
Emergency
Response
(Post-Crash)
Automatic CrashNotification
Education and Assistanceto EMS
Bystander Care
Training for LawEnforcement
Data collection &analysis
1.3 Types of riding
National Transportation Safety Board conducted a survey by telephone using national
probability sample of HHs. around 300,000 households called in order to reach owing HHs.
A report summary consisted set of detailed reports and approximately 3,000 tables were
produced by research firm [3].
One of The statistical data indicates the types of Riding by people. It is seen from the graph
that most of the population preferred a casual pleasure ride than touring over 500 miles.
Most of the riders tend to ignore safety measures while casual pleasure riding.
Figure 1.3 Statistical data indicating the ways Motorcycles been utilized [3]
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NO
61.3
YES
37.6
1.3.1 Rider training and licensing
From the chart we can observe around 61.3 % of the population have not taken an Organized
Rider Education Class. Hence it is one of the causes for increase in Motorcycle accidents [3].
Figure 1.3.1 Rider training and licensing [3]
1.4 Importance of Safety Barriers
Safety barriers have become very popular from past two decades. An effort to
improve their performance so as to reduce accident rates is a latest trend of study. Rigid
barriers are used for the separation of opposite traffic [4]. They are designed especially for
the use on narrow medians, where little or no deflection could be tolerated. As vehicles
become more popular, sales rise, so has the number of accidents and fatalities. Rigid barriers
help preventing few fatalities. They are developed in a unique way to resist forces through
their own mass.
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Figure 1.4 Median Barrier [4]
The impact forces are transferred to ground through a foundation. Since the barriers
limit the impact deflection to minimal values sometimes no deflection. They should be
chosen based on their use and location. Rigid barriers are ideally used in the situations where
road side hazards are located immediately behind the barrier. Using rigid barriers are very
advantageous as they experience least impact damage and perform optimally in collisions
where the impact angle is less than 15degrees. Hence this reduces maintenance costs and also
reduces the traffic disturbances [4].
1.5 Effects of Safety Barriers on Motorcyclist
Road safety barriers are developed to reduce the accident rates by preventing errant
vehicles moving in opposite directions [5]. A conventional barrier system has proved to
perform well in protecting the occupants of passenger car. Yet, their usage is offending the
motorcyclists. Since information on motorcycle-barrier crash is inadequate and require more
procedures for crash testing, the interaction of motorcycle- barrier has become complex. The
most dangerous aspect of a barrier system with respect to motorcyclists is projected edges. As
barrier displays projected edge; the impact forces are concentrated, resulting in serious
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injuries to the rider. Motorcyclists can be catapulted over barrier systems if the barrier is too
low.
Figure 1.5 Motorcycle impacting safety barrier system [5]
The jagged edges of the wire mesh topped barrier systems can cause severe lacerations, thus
increasing rider injury risk. Exposure to collision environment the rider is simply separated
from the motorcycle. When knocked with such dangerous projection, a chance of survival is
very low [5].
1.6 Literature Review
Several motorcycle to car and motorcycle to barrier tests were conducted to study the
characteristics of the motorcycle and the behavior of the rider during collision. These
researches were undertaken at different areas of interest. Since the behavior of the rider
during accidents is complex, a comprehensive study of impacts at different angles is a subject
matter of current research.
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1.6.1 Motorcycle to car and Motorcycle to Barrier test
Seventeen staged motorcycle to car and motorcycle to barrier crash tests were
conducted at the World Reconstruction Exposition 2000 (WREX2000) held at College
Station, Texas on September 25-30, 2000 by Kelley S. Adamson, Peter Alexander, Ed L.
Robinson and Gary M. Johnson, Claude I. Burkhead, III, John McManus, Gregory C.
Anderson, Ralph Aronberg, J. Rolly Kinney and David W. Sallmann. The speed of
Motorcycle considered for impact was varied from 10 MPH and 49 MPH. The objective of
the tests was to evaluate the characteristics of a heavy motorcycle involved in collisions with
two stationary targets namely a rigid heavy concrete block, and an automobile [6].
Figure 1.6.1 Motorcycle impacting safety barrier system and car [6]
1.6.2 Motorcycle Crash Test Modeling
To objective of this research was develop and validate a three dimensional
mathematical model representing a motorcycle with a rider. As a part of this development,
several motorcycle to barrier tests was performed at the laboratories of the TNO Crash-Safety
Research Centre. Several measurements were carried out including measurements to
determine the inertia properties of the motorcycle segments. Results of two full scale tests
involving a passenger car were applied to validate the model [7]. The MADYMO model of
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Motorcycle consisted of 7 bodies linked to each other by joints and spring damper type
elements.
Figure 1.6.2 Motorcycle after the 90deg/32.2 km/h Barrier test and Motorcycle trolley,
including dummy support frame [7]
1.6.3 Simulation of Motorcycle-car Collision
In this research a scooter type motorcycle was developed for simulation. Comparison
was made between a full-scale test and the simulation using a basic impact configuration
recommended in ISO 13232. Motoaki Deguchi developed a Motorcycle-Car model to
examine the behavior of a rider during collision. The aim of simulation was to evaluate rider
protective devices and therefore to reduce rider injuries when an accident occurs. During
collision, the rider experiencing the secondary impact with the environment such as road was
considered [8]. The motorcycle modeled using MADYMO consisted of 21 rigid bodies, 12
movable joints and many surfaces such as ellipsoid, cylinder, plane and facet surfaces were
used.
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Figure 1.6.3 Full simulation model of scooter type motorcycle and a car [8]
1.6.4 Motorcycle impacting into Roadside Barriers
Two crash tests have been conducted to analyze impacts onto conventional Steel
guard rails and two tests to analyze impacts onto a Concrete Barrier. Two additional full scale
crash tests were carried out to analyze the behavior of a modified roadside protection system
made from steel. Full scale test was conducted at DEKRA and the computer simulations were
carried out at Monash Universitys Department of Civil Engineering. The simulation model
was validated when the motorcycle was driven in an upright position while moving at 60km/h
impacting concrete barrier at an angle of 12 degree [9].
Figure 1.6.4 Test where the Motorcycle impacted the Barrier in an upright driving
position [9]
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1.7 Objectives
The main objective of this study is the development and validation of a three
dimensional Motorcycle with a rider. Results from the Motorcycle-barrier impact tests
conducted at the laboratories of DEKRA Accident Research were used for validation of the
Motorcycle with a rider model. Further under normal road condition, Motorcycle is impacted
to Concrete Barrier at different speeds under various impact angles. Kinematics of the rider
and the Motorcycle was an important part of study. The Head injury of the rider under
different speeds and at a range of impact angles was studied.
The second part of this research deals with study of kinematics of the rider and the
Motorcycle impacting the Concrete Barrier under ice roads. The effect of change in
environmental conditions and impact angles under different speeds leading to difference in
injury levels was studied. Design of Experiments is conducted to study the contribution of the
road condition, impact angles, speed and the interaction of these factors.
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CHAPTER 2
MATHEMATICAL MODELING PRINCIPLES
2.1 Importance of Computer Simulations
The use of computer simulation is recognized as a powerful tool passive safety
research field. Computer simulations has two major advantages, one being reproducibility
and other being the fact of inexpensive. The latter means in full scale crash test involving a
motorcycle with a rider, only a very limited number of crash conditions like speed, impact
angle and position of a motorcycle can be assigned. Where as in computer simulations, any
number of parametric studies can be conducted demanding less amount of time. Since the
motorcycle crash exhibit a complex behavior computer simulations will be very helpful in
analyzing the impact at any point of time. Taking into account the diversity of collision
configurations and the length of analysis time, MADYMO is one such software which can be
very helpful to predict the crash and can be used as a basic simulation tool for occupant
safety research.
2.2 Introduction to MADYMO
MADYMO (MAthematical DYnamic MOdel) is simulation software, which has an
ability to simulate the dynamic behaviour of mechanical systems. Mainly focusing on the
analysis of impact and evaluating the injury parameters. While originally developed for
studying occupant behaviour during impacts, MADYMO is successively increasing to study
the active safety. Hence it has become sufficiently flexible to analyze any kind of crash. Due
to dramatic increase in the accident rates, safety programs have become an area of interest.
MADYMO provides a detailed assessment of the restraint factors [10]. Therefore it is used
extensively in design industries, research institutes etc. MADYMO combines in one
simulation program the capabilities offered by multi-body, for the simulation of the gross
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motion of systems of bodies connected by kinematical joints and finite element techniques
for the simulation of structural behaviour, the advantage of MADYMO is having the
capability of creating either a multi-body or finite element body or both. The figure below
explains a model can be created with only finite element models, or only multi-bodies, or
both [10].
Figure 2.2 MADYMO structure [10]
The multi-body algorithm in MADYMO yields the second time derivatives of the degrees of
freedom in an explicit form. The number of computer operations is linear in the number of
bodies if all joints have the same number of degrees of freedom. This leads to an efficient
algorithm for large systems of bodies. While starting with the integration, the initial state of
the systems of bodies has to be specified in terms of joint positions and velocities. Several
kinematic joint types are available with dynamic restraints to account for joint stiffness,
damping and friction. Joints can be locked, unlocked or removed based on user-defined
options. The finite element module provides a method for dividing the range into finite
volumes, surfaces or line segments. The range continuum is then analyzed as a complex
system, composed of relatively simple elements where continuity should be ensured along the
interface between elements. These elements are Inter-connected at a discrete number of
points, the nodes. The initial nodal positions and velocities, the connectivity, as well as the
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element properties such as material behaviour, must be specified at the start of the simulation
[10].
2.3 Introduction to Multi-body Systems
A Multi-body system is a system of bodies. Any pair of bodies in the same system can
be interconnected by one Kinematic joint. The MADYMO Multi-body formalism for
generating the equations of motion is suitable for systems of bodies with a tree structure as
shown in Figure 2.3 and systems with closed chains. Systems with closed chains are reduced
to systems with a tree structure by removing a Kinematic joint in every chain. Removed
joints are subsequently considered as closing joints. For each (reduced) system with a tree
structure, one body can be connected to the reference space by a Kinematic joint, or the
motion relative to the reference space of one body can be prescribed as a function of time
[10].
Figure 2.3 Example of Single and Multi-body systems with tree structure[10]
2.4 Introduction to Kinematic Joints
A Kinematic joint restricts the relative motion of the two bodies it connects. A
specific type of Kinematic joint is characterized by the way the relative motion of two bodies
is constrained. The relative motion allowed by a joint is described by quantities called joint
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degrees of freedom. The number depends on the type of joint. In MADYMO, the most
common joint types are available such as spherical joints, translational joints, revolute joints,
cylindrical joints, planar joints and universal joints [10].
A system of bodies is defined by:
The bodies: the mass, the inertia matrix and the location of the centre of gravity,
The kinematic joints: the bodies they connect, the type and
the location and the orientation, and
The initial conditions.
In addition, the shape of bodies may be needed for contact calculations or post-processing
purposes [10].
Figure 2.4 Constraint load in a Spherical Joint [10]
Two bodies can be connected by one kinematic joint. A kinematic joint constrains the
relative motion of this pair of bodies, so a translational joint allows only relative translation.
In The constraints imposed by a kinematic joint cause a load on the pair of interconnected
bodies, the constraint load. This load is such that the relative motion of the pair of bodies is
restricted to a motion that does not violate the constraints imposed by the kinematic joint. The
constraint loads on the separate bodies are equal but opposite loads as shown in the figure
2.4. Constraint loads can be used to assess the strength of the joint [10].
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2.4.1 Types of mechanical joints
A: Revolute joint
A Revolute joint constrains the relative motion of the interconnected bodies to a
rotation around the axes of the joint coordinate systems. The origins of the joint coordinate
systems remain coincident. The number of degrees of freedom of a revolute joint equals one
[10].
Figure 2.4.1 (a) Revolute joint [10]
B: Translational joint
A Translational joint (Figure 3.15) constrains the relative motion of the
interconnected bodies to a translation along the axes of the joint coordinate systems. The
axes are coincident and the () axes are parallel. The number of degrees of freedom of a
translational joint equals one. The joint position degree of freedom s is the coordinate of the
origin of the joint coordinate system on the child body in the joint coordinate system on the
parent body. The joint velocity degree of freedom is its first time derivative [10].
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Figure 2.4.1 (b) Translational joint [10]
C: Spherical joint
A spherical or ball joint constrains the relative motion of the interconnected bodies to
a rotation around the origins of the joint coordinate systems. The number of joint position
degrees of freedom of a spherical joint equals four. The number of joint velocity degrees of
freedom equals three [10].
Figure 2.4.1 (c) Spherical joint [10]
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D: Universal joint
A Universal joint constrains the relative motion of the interconnected bodies, starting
from the orientation for which the joint coordinate systems coincide, to a rotation around i
axis followed by a rotation around the j axis. The origins of the joint coordinate systems
remain coincident. The number of degrees of freedom of a universal joint equals two. The
joint velocity degrees of freedom are their first time derivatives [10].
Figure 2.4.1 (d) Universal joint [10]
2.5 Introduction to Inertial Space and Null Space Systems
A coordinate system (X, Y, Z) is connected to the inertial space as shown in figure 2.5
The origin and orientation of this inertial reference space coordinate system can be selected
arbitrarily. Usually the positive Z axis is chosen pointing upwards, that is, opposite to the
direction of gravity. The motion of all systems is described relative to this coordinate system.
Contact surfaces such as planes, ellipsoids and restraints as well as nodes of finite element
structures in MADYMO can be attached to the inertial space [10].
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Figure 2.5 Inertial Space Co-ordinate System [10]
Several auxiliary systems with known motion can be defined, for instance to represent
a vehicle for which the motion is known from experimental data, as shown in the figure 2.5.1.
However, the preferred way to model this is using a system of one body with a prescribed
motion [10].
Figure 2.5.1 Null System Co-ordinate System [10]
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Contact surfaces such as planes, ellipsoids, restraints, spring damper elements as well
as nodes of finite element structures can be attached to a null system. The motion of a null
coordinates of the null system origin O and quantities that define the orientation of the null
system coordinate system define this motion. If no motion is specified for a null system, its
coordinate system coincides with the inertial coordinate system. The time points at which the
position of the origin O is defined can differ from the points for which the orientation is
specified. This can be useful, for instance, in case the orientation of a null system changes
only slightly. Then the orientation can be specified at less time points than the position of the
origin in order to reduce the amount of input data [10].
2.6 Introduction to Injury Biomechanics
Injury Biomechanics describes the effect mechanical loads have on the human body,
particularly impact loads. Due to a mechanical load, a body region will experience
mechanical and physiological changes, the biomechanical response. Injury occurs if the
biomechanical response is so severe that the biological system deforms beyond a recoverable
limit, resulting in damage to anatomical structures and altering the normal function. The
mechanism involved is called injury mechanism, the severity of the resulting injury is
indicated by the expression injury severity [10].
2.7 Injury Parameters
An injury parameter is a physical parameter or a function of several physical
parameters that correlates well with the injury severity of the body region under
consideration. Many offers have been put forth for ranking and quantifying injuries.
Anatomical scales describe the injury in terms of its anatomical location, the type of injury
and its relative severity. The recognized accepted anatomical scale is the Abbreviated Injury
Scale (AIS) [10].
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The AIS distinguishes the following levels of injury:
0 no injury 5 critical
1 minor 6 maximum injury (causing death)
2 moderate 9 unknown.
3 serious
4 severe
The numerical values have no significance other than to designate order. Many injury
criterias are based on acceleration forces, displacements and velocities. MADYMO provides
these quantities with the standard feature. MADYMO offers possibilities to perform some of
these injury parameter calculations [10]. The following injury parameter calculations are
available:
Gadd Severity Index (GSI) Head Injury Criterion (HIC)
Neck Injury Criteria (NIC) 3 ms Criterion (3 MS)
Thoracic Trauma Index (TTI) Femur Loads
Injury parameter calculations for HIC, GSI, and 3 MS are carried out on the linear
acceleration signal of a selected body. The TTI calculation is carried out on the linear
acceleration signals of two selected bodies. These linear acceleration signals must have been
defined under the LINACC keyword [10].
2.8 Injury Criteria
An injury criterion can be defined as a biomechanical index of exposure severity, which
indicates the potential for impact induced injury by its magnitude. There are several reasons
why injury criteria are developed. The search for a valid criterion improves the understanding
of injury mechanisms and the situations in which they occur. An injury criteria also relates
loading conditions during impacts on human bodies to certain levels of injury scales as the
AIS scale. Another practical reason is that experiments with cadavers, animals, dummies
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provide only measurements of forces, displacements, velocities and accelerations and no
injuries. The injury criteria, based on data of these experiments or mathematical simulations,
can be used for an efficient analysis of motorcycle safety design and optimization. Most
injury criteria are based on accelerations, relative velocities or displacements, or joint
constraint forces. These quantities must be requested with standard output options. Most
injury criteria need some mathematical evaluation of a time history signal.
2.9 Head Injury Criterion (HIC)
Head Injury Criterion (HIC) is frequently the most challenging standard to meet.
J. Versace was the first to propose the Head Injury Criteria (HIC), and was later modified by
NHTSA. This criterion is based on the interpretation of the Gadd Severity Index. HIC is an
empirical formula based on experimental work. The HIC does not represent simply a data
value, but represents an integration of data over a varying time base. The HIC is based on
data obtained from three mutually perpendicular accelerometers installed in the head of the
ADT in accordance with the dummy specification. Head Injury Criterion (HIC) is developed
as an indicator of the likelihood of severs head injury and is determined by the relation[10].
(2.9)
Where:
T0: Starting time of the simulation
TE: End time of the simulation
t1: Initial time of interval during which HIC attains maximum value
t2: Final time of interval during which HIC attains maximum value[10].
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In automotive crash testing, HIC is calculating regardless of the presence of head contact,
according to the Federal Motor Vehicle Standards (FMVSS) and FAA regulations, the HIC
should not exceed 1000. If HIC is kept below 1000 serious injury is considered unlikely[10].
2.10 Neck Injury Criteria (NIC)
Neck injury is often assessed by peak forces and moments in the upper and lower neck.
Usually in crashes, the loading on the neck due ti head contact force is a combination of an
axial load or shear load with bending. Bending loads are almost always present and the
degree of axial or shear force is dependent upon the location and direction of the contact
force. For impact near the crown of the head, compressive forces predominate. If the impact
is principally in the transverse plane, there is less compression and more shear. Bending can
occur in any direction because impacts can come from any angle around the head [10].
2.10.1 Predicting neck injury ( Nij )
The biomechanical neck injury predictor is a measure of the injury due to the load transferred
through the occipital condyles[10]. This injury parameter combines the neck axial force and
the flexion/extension moment about the occipital condyles. The injury calculation is applied
to joint constraint load signals. It is assumed that the coordinate systems of this bracket joint
are oriented because as axial force, the component of the constraint force in the joint -
direction is used, as shear force Fx, the component of the constraint force in the joint -
direction is used and as bending moment, the component of the constraint moment M y1about
the joint -axis is used. This bending moment is, in general, not about the occipital condyles.
The moment about the occipital condyles My is obtained from the following equation
(2.10.1) where e is the distance between the occipital condyle and the joint in the positive
joint -direction. Four injury predictors is the collective name of four injury predictors
corresponding to different combinations of axial force and bending moment[10]:
- Tension-extension (NTE),
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- Tension-flexion (NTF),
- Compression-extension (NCE), and
- Compression-flexion (NCF).
The equation for the calculation of is given by
My= My1- eFx (2.10.1)
The equation for the calculation of Nij is given by
Nij= +
(2.10.2)
Where Fzc and Myc are constants that depend on the dummy and on the neck loading
condition like compression, tension, flexion, extension. Each predictor pocess a value equal
to or lesser than one [10].
2.11 Thoracic Trauma Index (TTI)
Thoracic Trauma Index (TTI) was proposed to predict the probability of serious injury
to the hard thorax as a result of blunt lateral impact [10]. The TTI is an acceleration criterion
based on the accelerations of the lower thoracic spine and the ribs. It also incorporates the
weight and the age of the human model. The formulation was derived from a large
biomechanical database consisting of 84 cadaver tests. The occurrence of injuries to the hard
thorax, including the ribs and the internal organs protected by the ribs, is strongly related to
the average of the peak lateral acceleration experienced by the impacted side of the rib cage
and the lower thoracic spine. The TTI can be used as an indicator for the side impact
performance of passenger cars. The specific benefit of the TTI is that it can be used to
address the entire population of vehicle occupants because the age and the weight of the
cadaver are included [10].
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2.12 Femur Force Criteria (FFC)
The Femur Force Criterion (FFC) is a measure of injury to the femur. It is the
compression force transmitted axially on each femur of the dummy as it is measured by the
femur load cell [10]. The FFC injury calculation is applied to the joint constraint force in the
bracket joint located at a femur load cell. It is assumed that the coordinate systems of this
joint are oriented because as axial force, the component of the constraint force in the joint -
direction is used. A duration curve of this time history signal is made. The resulting femur
axial force duration curve must not exceed the values shown in Figure 2.12 [10].
Figure 2.12 Femur force performance criterion [10]
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CHAPTER 3
MATHEMATICAL MODELING OF MOTORCYCLE AND BARRIER
The MADYMO model consisted of four distinct systems; the road, the motorcycle,
the barrier and the rider. The road is considered as an inertial space over which the
motorcycle, barrier and rider is operated.
3.1 Methodology
Physical model of a Motorcycle MADYMO model of a Motorcycle
Motorcycle-Barrier test validation at 90deg Motorcycle-rider Model
/32.2 km/h
Parametric Studies
Motorcycle-rider impacting a Concrete Barrier
model validation at 12 deg/60km/h
Figure 3.1 Methodology representing models
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Figure 3.1 (a) Methodology representing steps
3.2 Rider Modeling
Figure 3.2 Hybrid III 50th
percentile dummy model [10]
A wide range of two dimensional and three dimensional ATD models are available in
MADYMO. The standard models of adult and child Hybrid III dummies are: the 5th
percentile female, the 50th
percentile male, the 95th
percentile male, 3 year old child and 6
year old child. The Hybrid III 50th
percentile male dummy is widely used for most of the
crash testing. It represents the average size and weight of adult male population in United
States. The above model is made of ellipsoids only consisting of 37 bodies [10].
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Table 2.1 Standard typologies selected for model generation [10]
Parameter Selected options
Gender Male Female Very tall
Length (standing) Very short Medium Large waist
Corpulence Slim waist Medium waist Long torso
Proportion Short torso Medium torso
Table 3.1 Standard MADYMO Hybrid III 50th
percentile dummy specification [10]
MADYMO model Size Length (m) Mass (kg)
Hybrid III 50th percentile dummy Medium 1.72 77
3.3 Motorcycle Modeling
Kawasaki ER 5 Twister was used for crash study. The required dimensions were
obtained from the Kawasaki manufactures handbook [11]. Few dimensions such as the
overall length, overall width, overall height, seat height, wheel base, minimum ground
clearance, weight were taken into account. The table bellow provides the details of the
motorcycle.
Figure 3.3 Kawasaki ER 5 Twister [11]
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MADYMO model of a Motorcycle
The motorcycle is modeled using ellipsoids. It consists of 6 bodies representing the
frame, seat, two wheels, suspensions and the handle. The frame is considered a parent body
over which the other bodies are connected through respective joints. Revolute joint is used to
connect the wheels and handle. Bracket joint is used to connect the seat to frame. Kelvin
elements are introduced for the suspensions. Since the front portion of the motorcycle
impacts on barrier, Special attention is given to describe the front wheel and front suspension
characteristics. The stiffness data for front wheel, front suspensions, seat and inertial
properties are obtained from Raphael Grzebieta, Roger Zou, Monash University, Australia
[9].
Figure 3.3.1 Three-dimensional Motorcycle model
Figure 3.3.2 Three-dimensional Motorcycle model representing joints
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Specifications
Body
Mass
(Kgs) COG Inertia
Frame 70 0 0.05 0.4 40 26 18 0 0 0
Handle 6 0
-
0.015 -0.071 1.1 0.60.3
8 0 0 0
Front wheel 22 0 0
0.0629
5 3 2 1.2 0 0 0
Rear wheel 25
-
0.315 0
0.0629
5 2.1 1.6 1.1 0 0 0
Seat 9 0 -0.25 0.086
0.4
1
0.3
80.2
2 0 0 0
Front
fork(Suspension) 8 0 -0.41 0.26 1.1
0.9
7 0.9 0 0 0
Engine 40 0 0.05 0.15 9 7.6 6.8 0 0 0
3.4 Concrete Barrier Modeling
Concrete barriers are used to prohibit the entries of errant vehicles. They are widely used on
the roadside, since they show no aggressive behavior when compared to steel guards.
Currently there are four types of barriers used in America namely [9];
1. New Jersey concrete barrier 3.The F shape concrete barrier
2. The Single-slope barrier 4. The Vertical concrete barrier
MADYMO model of a Concrete Barrier
The concrete barrier assuming as a single ellipsoid is modeled using MADYMO. The
following parameters are considered while modeling [9].
Table 5.1 Dimensions of a Concrete Barrier
Figure 3.4 Three-dimensional Concrete Barrier model
Height 800 mm
Width 200 mm
Length 10 m
Material density 2,500 kg/m3
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CHAPTER 4
VALDATION OF MOTORCYLE AND MOTORCYCLE WITH RIDER
4.1 Validation of a Motorcycle
A Motorcycle model was developed using MADYMO. Simulations and experimental
results were compared for a Barrier test condition. A comparison was made for the
kinematics of the Motorcycle and Motorcycle Acceleration [7]. The barrier test condition
considered was a Motorcycle moving with a velocity of 32.2 km / h and colliding at an angle
of 90 degrees as shown in the figure 4.1
.
Figure 4.1 Motorcycle and Barrier modeled in MADYMO
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0 ms 200 ms
250 ms 300 ms
350 ms 400 ms
Figure 4.1(a) simulated kinematics of the Motorcycle for the 90 degree/ 32.2 km / h
Barrier test condition.
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From the simulation experiment, it was observed that the kinematics of the motorcycle were
in good correlation with the real time barrier test. The Acceleration generated during the time
of impact is high around 38 g as shown in the figure 4.1(b). As a result the Motorcycle model
is good for further research.
0
5
10
15
20
25
30
35
40
45
50
0 50 100 150 200
Time (msec)
LeftCGA
cce
leration(g)
experimental
simulated
Figure 4.1(b) Simulated resultant Acceleration Left of the CG for 90 deg/ 32.2 km /h test
4.2 Validation of Motorcycle with a rider
A mathematical multi-body model rider and motorcycle is developed to simulate the
impact on concrete barrier. The motorcycle- barrier model is created for simulation using
MADYMO. The performance of this model is evaluated by correlating the obtained results
with those from the data of full-scale crash test and also from the data of a computer
simulation study conducted by Raphael Grzebieta and Roger Zou at Monash University,
Australia.
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Figure 4.2 Motorcycle with a rider
In order to verify the Motorcycle- Barrier model with the experimental data, all
parameters are applied as assumed by Raphael Grzebieta and Roger Zou for the simulations.
The response from the model, such as the rider behavior during impact and Accelerations of
the head for a specific test configuration are compared with experimental data obtained from
Raphael Grzebieta and Roger Zou.
Figure 4.2(a) Full-scale crash test of a motorcycle impacting a concrete barrier
protection system in an upright position prior to impact moving [9]
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The trajectories of Motorcycle and a rider are shown in the figure 4.5(b). When the
Motorcycle is impacting at an angle of 12 degrees and at a speed of 60 km/hr. the rider is
separated from his machine and lands up on the other side of the barrier.
Figure 4.2(b) Motorcycle and rider trajectories during 175 milliseconds after impactingthe concrete barrier as determined from analysis of the overhead-view cameras[9]
Validation for the MADYMO model is made based on the above principles. Kinematics of
the Motorcycle and rider play a very important role to determine the injury parameters.
Hence kinematics of the full scale crash test and the simulated kinematics were matched in
order to meet the validation criteria. Head injury and femur load during collision also helps in
validation of a motorcycle with a rider impacting concrete barrier at 12 deg/60km/h.
Figure 4.2 (c) Motorcycle with a rider moving along the concrete barrier
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100 ms 430 ms
530 ms 750 ms
1060 ms 1140 ms
Figure 4.2(d) Simulated kinematics for 12 deg / 60 km /hr / NRC for validation:
The kinematics of the simulated experiment appears to be satisfactory when compared to the
full-scale crash test. The head injury obtained from the simulation and full-scale test is as
shown in the figure 4.2(d).
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Figure 4.2(e) Femur R Resultant Force (N) Figure 4.2(f) Neck flexion and extension
Table 6.1 Comparison of results between full-scale crash test and simulated experiment
for 12 deg / 60km/h / NRC [9]
Full scale crash test Simulation
HIC 36ms 164 HIC 36ms 168.3
Femur R (N) 4500 Femur R (N) 3529
As seen from the graph, load acting on the right Femur and HIC obtained from the simulated
experiment is very close to the full-scale crash test. The HIC from simulation is 168.3 as
compared to the HIC of 164 from full scale crash test [7]. Femur R loads also showed a good
result. Therefore the Motorcycle with a rider has been validated under 12 degree impact/ 60
km / hr / NRC.
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CHAPTER 5
ANALYSIS OF MOTORCYCLE AND BARRIER IMPACT
This aim of this part of research is to predict the kinematics of Motorcycle and a rider and the
Head Injury Suffered by the rider. Several velocities impacting at various angles are taken in
to an account for analysis. The behavior of rider is seemed to be relatively different during
different crash scenarios. There are several factors namely speed, angle of impact and
environmental conditions affecting the kinematics of Motorcycle and a rider. Ice road is
considered as one such hindrance caused due to climatic changes. The analysis is carried out
to examine the behavior of the rider under different speeds impacting at different angles
under icy road conditions. Later the percentages of contribution of three factors namely
change in road contribution, speeds and different angles are calculated using the Design of
Experiments.
5.1 Analysis of Motorcycle-Concrete Barrier impact considered for a parametric study
Table7.1 Analysis of Motorcycle and Barrier impact under Normal Road Condition
Road type Angle of collision Speed
40 km/h
NRC 6 degree 60 km/h
80 km/h
40 km/h
NRC 8 degree 60 km/h
80 km/h
40 km/h
NRC 12 degree 60 km/h
80 km/h
40 km/h
NRC 24 degree 60 km/h
80 km/h
40 km/h
NRC 45 degree 60 km/h
80 km/h
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40 km/h
NRC 60 degree 60 km/h
80 km/h
40 km/h
NRC 90 degree 60 km/h
80 km/h
Table7.2 Analysis of Motorcycle and Barrier impact under Icy Road Condition
Road type Angle of collision Speed
40 km/h
IRC 6 degree 60 km/h
80 km/h
40 km/h
IRC 8 degree 60 km/h
80 km/h
40 km/h
IRC 12 degree 60 km/h
80 km/h
40 km/h
IRC 24 degree 60 km/h
80 km/h
40 km/h
IRC 45 degree 60 km/h
80 km/h
40 km/h
IRC 60 degree 60 km/h
80 km/h
40 km/h
IRC 90 degree 60 km/h
80 km/h
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100 ms 400 ms
800 ms 910 ms
1090 ms 1490 ms
Figure 5.1.1 Simulated Kinematics for 12deg/ 40km /h / NRC
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100 ms 350 ms
540 ms 740 ms
950 ms 1150 ms
Figure 5.1.2 Simulated Kinematics for 12deg/ 80km /h / NRC
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0 ms 450 ms
630 ms 920 ms
1140 ms 1540 ms
Figure 5.1.3 Simulated Kinematics for 6deg/ 40km /h / NRC
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0 ms 410 ms
560 ms 770 ms
930 ms 1600 ms
Figure 5.1.4 Simulated Kinematics for 6deg/ 60km /h / NRC
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0 ms 370 ms
510 ms 620 ms
840 ms 1200 ms
Figure 5.1.5 Simulated Kinematics for 6deg/ 80km /h / NRC
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0 ms 380 ms
550 ms 760 ms
1070 ms 1620 ms
Figure 5.1.6 Simulated Kinematics for 8deg/ 40km /h / NRC
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0 ms 400 ms
510 ms 610 ms
910 ms 1380 ms
Figure 5.1.7 Simulated Kinematics for 8deg/ 60km /h / NRC
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0 ms 480 ms
780 ms 1050 ms
1210 ms 1320 ms
Figure 5.1.8 Simulated Kinematics for 8deg/ 80km /h / NRC.
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0 ms 260 ms
560 ms 700 ms
1030 ms 1540 ms
Figure 5.1.9 Simulated Kinematics for 24deg/ 40km /h / NRC
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0 ms 210 ms
400 ms 600 ms
1110 ms 1410 ms
Figure 5.1.10 Simulated Kinematics for 24deg/ 60km /h / NRC
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0 ms 200 ms
350 ms 490 ms
790 ms 1200 ms
Figure 5.1.11 Simulated Kinematics for 24deg/ 80km /h / NRC
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0 ms 220 ms
550 ms 810 ms
1140 ms 1550 ms
Figure 5.1.12 Simulated Kinematics for 45 deg/ 40km /h / NRC
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0 ms 240 ms
410 ms 510 ms
630 ms 990 ms
Figure 5.1.13 Simulated Kinematics for 45 deg/ 60km /h / NRC
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.
0 ms 240 ms
390 ms 460 ms
610 ms 940 ms
Figure 5.1.14 Simulated Kinematics for 45 deg/ 80km /h / NRC
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0 ms 320 ms
640 ms 910 ms
1020 ms 1370 ms
Figure 5.1.15 Simulated Kinematics for 60 deg/ 40km /h / NRC
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0 ms 290 ms
480 ms 590 ms
770 ms 1080 ms
Figure 5.1.16 Simulated Kinematics for 60 deg/ 60km /h / NRC
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0 ms 190 ms
440 ms 520 ms
660 ms 970 ms
Figure 5.1.17 Simulated Kinematics for 60 deg/ 80km /h / NRC
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0 ms 340 ms
750 ms 940 ms
1410 ms 2000 ms
Figure 5.1.18 Simulated Kinematics for 90 deg/ 40km /h / NRC
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0 ms 310 ms
400 ms 520 ms
640 ms 1260 ms
Figure 5.1.19 Simulated Kinematics for 90 deg/ 60km /h / NRC
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0 ms 230 ms
440 ms 530 ms
760 ms 1110 ms
Fig 5.1.20: Simulated Kinematics for 90 deg/ 80km /h / NRC
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0 ms 230 ms
500 ms 780 ms
1330 ms 1900 ms
Figure 5.1.21 Simulated Kinematics for 6deg/ 40km /h / IRC
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0 ms 380 ms
530 ms 830 ms
1080 ms 1390 ms
Figure 5.1.22 Simulated Kinematics for 6 deg / 60km/h / IRC
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0 ms 350 ms
530 ms 690 ms
1020 ms 1180 ms
Figure 5.1.23 Simulated Kinematics for 6 deg / 80km/h / IRC
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0 ms 420 ms
560 ms 690 ms
860 ms 1360 ms
Figure 5.1.24 Simulated Kinematics for 8 deg / 40km/h / IRC
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0 ms 370 ms
520 ms 680 ms
980 ms 1390 ms
Figure 5.1.25 Simulated Kinematics for 8 deg / 60km/h / IRC
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0 ms 360 ms
580 ms 870 ms
1280 ms 1390 ms
Figure 5.1.26 Simulated Kinematics for 8 deg / 80km/h / IRC
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100 ms 470 ms
510 ms 890 ms
1160 ms 1260 ms
Figure 5.1.28 Simulated Kinematics for 12 deg / 60km/h / IRC
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100 ms 430 ms
540 ms 630 ms
1000 ms 1260 ms
Figure 5.1.29 Simulated Kinematics for 12 deg / 80km/h / IRC
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0 ms 430 ms
660 ms 930 ms
1420 ms 1500 ms
Figure 5.1.30 Simulated Kinematics for 24 deg / 40km/h / IRC
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0 ms 380 ms
530 ms 790 ms
1000 ms 1230 ms
Figure 5.1.31 Simulated Kinematics for 24 deg / 60km/h / IRC
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0 ms 370 ms
460 ms 670 ms
870 ms 1120 ms
Figure 5.1.32 Simulated Kinematics for 24 deg / 80km/h / IRC
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0 ms 320 ms
620 ms 910 ms
1200 ms 1760 ms
Figure5.1.33 Simulated Kinematics for 45 deg / 40km/h / IRC
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0 ms 430 ms
570 ms 850 ms
1120 ms 1320 ms
Figure 5.1.34 Simulated Kinematics for 45 deg / 60km/h / IRC
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0 ms 380 ms
550 ms 680 ms
800 ms 930 ms
Figure 5.1.35 Simulated Kinematics for 45 deg / 80km/h / IRC
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0 ms 310 ms
510 ms 690 ms
1320 ms 1760 ms
Figure 5.1.36 Simulated Kinematics for 60 deg / 40km/h / IRC
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0 ms 310 ms
440 ms 650 ms
920 ms 1170 ms
Figure 5.1.37 Simulated Kinematics for 60 deg / 60km/h / IRC
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0 ms 230 ms
400 ms 480 ms
600 ms 1100 ms
Figure 5.1.38 Simulated Kinematics for 60 deg / 80km/h / IRC
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0 ms 470 ms
710 ms 850 ms
1100 ms 1480 ms
Figure 5.1.39 Simulated Kinematics for 90 deg / 40km/h / IRC
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0 ms 440 ms
520 ms 610 ms
910 ms 1150 ms
Figure 5.1.40 Simulated Kinematics for 90 deg / 60km/h / IRC
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0 ms
0 ms 300 ms
400 ms 500 ms
670 ms 910 ms
Figure 5.1.41 Simulated Kinematics for 90 deg / 80km/h / IRC
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406.9
6.6 44.9
51.1
189162.7
164
0
100
200
300
400
500
600
700
800
900
1000
40 km / h-NRC
HIC
6 degree impact
8 degree impact
12 degree impact
24 degree impact
45 degree impact
60 degree impact
90 degree impact
5.2 Discussion of Results
Figure 5.2.1 HIC at 40 km /h-NRC for different impact angles
Figure 5.2.2 Femur R at 40 km /h- NRC
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Table 8.1 Neck at 40 km /h- NRC
40 km/h-NRC
Angle of collision Flexion (Nm) Extension (Nm)
6 degree 25.5 29.7
8 degree 26.1 20.7
12 degree 31.2 50.4
24 degree 56.8 24.1
45 degree 21.5 11.2
60 degree 80.6 150.7
90 degree 86.3 26.2
The results were obtained when a Motorcycle is moving at 40 km /h, colliding at different
angles is as shown in the above figure. Under normal road condition the HIC is
comparatively high at an impact angle of 90 degree than 60 degree. Injury on Femur
decreases as the angle of collision is increased. We also observe a high neck extension when
a Motorcycle is impacting at 60 degree/ 40 km/h.
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473.3
1290.6
344.1
340.1
168.8
293.7
161.2
0
100
200
300
400
500
600
700
800
900
1000
1100
1200
1300
1400
1500
60 km / h -NRC
HIC
6 degree impact
8 degree impact
12 degree impact
24 degree impact
45 degree impact
60 degree impact
90 degree impact
Figure 5.2.3 HIC at 60 km /h-NRC for different impact angles
Figure 5.2.4 Femur R at 60 km /h- NRC
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Table 8.2 Neck at 60 km /h- NRC
60 km/h-NRC
Angle of collision Flexion (Nm) Extension (Nm)
6 degree 206.2 34.5
8 degree 55.8 65.2
12 degree 56.1 46.6
24 degree 22.1 12.1
45 degree 22.1 11.7
60 degree 32.6 13.9
90 degree 91.9 138.7
The results were obtained when a Motorcycle is moving at 60 km / h, colliding at different
angles is as shown in the above figure. Under normal road condition the HIC is very high at
an impact angle of 90 degree, the chances of survival is very low. Other impact angles also
have an effect on Motorcyclist. Femur load is very high at 6 degree/ 60km/h.
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1260
96.8
505.4
808.6
521.9
132.4
153
0
100
200
300
400
500
600
700
800
900
1000
1100
1200
1300
1400
80 km / h- NRC
HIC
6 degree impact
8 degree impact
12 degree impact
24 degree impact
45 degree impact
60 degree impact
90 degree impact
Figure 5.2.5 HIC at 80 km / h-NRC for different impact angles
Figure 5.2.6 Femur R at 80 km /h- NRC
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Table 8.3 Neck at 80 km /h- NRC
80 km/h-NRC
Angle of collision Flexion (Nm) Extension (Nm)
6 degree 127.1 48.3
8 degree 48.5 62.9
12 degree 22.1 31.3
24 degree 127.6 13.9
45 degree 12.8 17.2
60 degree 10.4 26.3
90 degree 79.6 46.1
The results were obtained when a Motorcycle is moving at 80 km / h, colliding at different
angles is as shown in the above figure. Under normal road condition the HIC is very high at
an impact angle of 24 degree, since the Motorcyclist head is in direct contact with the road. It
is seen from the graph that HIC is very low at an impact angle of 90 degree. This is because
the Motorcyclists body hits the road prior to his head contact. Other impact angles also have
major effect on Motorcyclist. Femur suffers sever injury.
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4.3
707.7
295
83.369
355.9
151.5
0
100
200
300
400
500
600
700
800
900
1000
40 km / h-IRC
HIC
6 degree impact
8 degree impact
12 degree impact
24 degree impact
45 degree impact
60 degree impact
90 degree impact
Figure 5.2.7 HIC at 40 km /h-IRC for different impact angles
Figure 5.2.8 Femur R at 40 km /h- IRC
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Table 8.4 Neck at 40 km /h- IRC
40 km/h-IRC
Angle of collision Flexion (Nm) Extension (Nm)
6 degree 29.1 10.4
8 degree 33.9 38.7
12 degree 58.3 68.3
24 degree 50.6 14.1
45 degree 46.1 32.1
60 degree 210.3 31.9
90 degree 37.7 66.1
Under icy road condition when a Motorcycle moving at 40 km/h impacting the Concrete
Barrier at different angles have relatively less effect on the rider as shown in the above figure.
As in most of the crashes the riders head does not hit the ground yet his femur is injured
severely so as his arms. The rider is ejected brutally while impacting at an angle of 8 degree.
Therefore maximum Head injury is observed at this angle of impact.
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5.6
621.3
199.9
321.1
1037.1
643 645.4
0
100
200
300
400
500
600
700
800
900
1000
1100
60 km / h-IRC
HIC
6 degree impact8 degree impact
12 degree impact
24 degree impact
45 degree impact
60 degree impact
90 degree impact
Figure 5.2.9 HIC at 60 km /h-IRC for different impact angles
Figure 5.2.10 Femur R at 60 km / h- IRC
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Table 8.5 Neck at 60 km /h- IRC
60 km/h-IRC
Angle of collision Flexion (Nm) Extension (Nm)
6 degree 18.1 14.1
8 degree 398.1 70.4
12 degree 140.2 27.9
24 degree 36.3 12.1
45 degree 16.2 13.9
60 degree 248.6 26.7
90 degree 98.1 257.3
It is observed from the above figure that a Motorcycle is moving at 60 km / h under icy road
condition; the rider sustains severe Head impact. While examining the kinematics of the
rider, it is found the Head comes in direct contact with the road in most of the collisions.
Death may be seen as the rider collides at 90 degree impact angle. Femur has a severe impact
at most of the impacts.
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272.3
1050.1
542.5
32.1
1139
348.74
237.9
0
100
200
300
400
500
600
700
800
9001000
1100
1200
1300
1400
80 km / h-IRC
HIC
6 degree impact
8 degree impact
12 degree impact
24 degree impact
45 degree impact
60 degree impact
90 degree impact
Figure 5.2.11 HIC at 80 km / h-IRC for different impact angles
Figure 5.2.12 Femur R at 80 km / h- IRC
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Table 8.6 Neck at 80 km /h- IRC
80 km/h-IRC
Angle of collision Flexion (Nm) Extension (Nm)
6 degree 123.3 62.2
8 degree 28.4 15.6
12 degree 23.1 22.1
24 degree 18.1 34.8
45 degree 25.2 20.7
60 degree 161.1 31.7
90 degree 98.1 26.6
Under icy road condition when a Motorcycle moving at 80 km/h impacting the Concrete
Barrier at different angles have a very high effect on the rider as shown in the above figure.
The rider is at a very high risk while colliding at certain angles. As a result many death
causes could be seen particularly at 80 km/h. Hence it is advisable to slow down during such
impacts so that the rider is saved for life.
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CHAPTER 6
DESIGN OF EXPERIMENTS APPLIED TO THE SYSTEM
Design of experiments are statistically designed experiments which refer to the
process of planning the experiments where the data collected are appropriate to be
statistically analyzed resulting in valid and objective conclusions. They are used to study the
effect of the various controllable variables on any desired response in a process. There are
three basic principles in an experimental design namely randomization, replication and
blocking. Randomization means that the experimental material and the order of performance
of the individual run in an experiment need to be allocated randomly. The effects of certain
extraneous factors which might be present are averaged out by this method. Replication is the
repeat of all possible combinations between the factors. Blocking improves the preciseness in
the comparisons among various factors of interest and it reduces or completely eliminates the
variability transmitted to the responses due to the nuisance factors. There are certain
sequential guidelines to be followed for designing experiments. The first phase is the pre-
experimental planning which includes the recognition and statement of the problem, selection
of the response variables and the choice of factors, levels and ranges. The sequence of steps
after the first phase is choice of an experimental design, performing the experiment, statistical
analysis of the data, conclusions and recommendations [12].
6.1 Principles of Design of Experiments
To understand the need of experiments
Understand different strategies of experimentation
To know what a factorial experiment is and
To recognize the information it can provide
Identify advantages and disadvantages of different strategies [12]
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Table 9.1 Effects of the Model
Term DOF Sum Square % Contribution
Require Intercept
Error A 1 33583.0 0.66
Model B 6 1192306.3 23.29
Model C 2 823676.5 16.09
Model AB 6 282383.2 5.52
Error AC 2 8823.84 0.17
Model BC 12 1180746.3 23.06
Model ABC 12 1598081.6 31.21
Where:
A: Road conditions, two road conditions are used namely normal road condition and ice
road condition.
B: Angle of Collision, different impact angles is considered namely 6 degree, 8 degree, 12
degree, 24 degree, 45 degree, 60 degree and 90 degree.
C: Speed, three speeds are assumed namely 40 km/ h, 60 km/h and 80 km/h.
AB: Interaction of road conditions and angle of collision contributing to severity of Head
injury.
AC: Interaction of road conditions and speed contributing to severity of Head injury
ABC: Interaction of all three factors namely road conditions, angle of collision and the speed
contributing to severity of Head injury.
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From the effects table we can see that factors B (angle of collision), C (speed) and
interactions BC and ABC have significant effect on the response (HIC). ANOVA table is
derived by selecting these factors to find if the model is significant or not.
Table 9.2 ANOVA table for the model
Sum of Mean F
Source Squares DF Square Value Prob > F
Model 5077194.1 38 133610.3 9.4 0.04 significant
B 1192306.3 6 198717.7 14.0 0.02
C 823676.5 2 411838.2 29.1 0.01
AB 282383.2 6 47063.8 3.3 0.17
BC 1180746.3 12 98395.5 6.9 0.06
ABC 1598081.6 12 133173.4 9.4 0.04
Residual 42406.9 3 14135.6
Cor Total 5119601.0 41
The Model F-value of 9.45 implies the model is significant. There is only a 4.38% chance
that a "Model F-Value" this large could occur due to noise. Values of "Prob > F" less than
0.0500 indicate model terms are significant. In this case B, C, ABC are significant model
terms. Values greater than 0.1000 indicate the model terms are not significant.
Figure 6.4.1 Effects of Angle of Collision on HIC
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As seen from the table 9.1, Angle of Collision contributes to 23.29 % for the HIC. Increase in
the impact angle increases the risk of survival for the Motorcyclist. Hence it is always
preferred to have a low angle impact
Figure 6.4.2 Effects of Speed on HIC
As seen from the table 9.1, change in road condition contributes to 16.09 % for the HIC.
Increase in speed also has a high impact on Motorcyclist. Therefore it is important to slow
down Motorcycle before colliding on the obstacle.
Figure 6.4.3 Effects of road condition on HIC
As seen from the table 9.1, change in Speed contributes to 0.66 % for the HIC. As a result
this change has a very least effect on the road condition. Therefore the rider is safe from any
changes in the road condition except for the speed and angle of collision.
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CHAPTER 7
CONCLUSIONS AND RECOMMENDATIONS
7.1 Conclusions
The objective of this research was to study the kinematics and potential injury to a
rider. A motorcycle model with the rider was developed using the MADYMO crash
analysis software. Concrete Barrier was modeled according to the data provided by Zou
and Grzebieta. Motorcycle-Barrier test was conducted at 90deg/ 32.2 km/h for validation.
The following conclusions were made from the research
The motorcycle model alone impacting the wall generated reasonable acceleration
compared to actual test.
The kinematics and acceleration values of the model were in good correlation with the
experimental values.
The Motorcycle with a rider model impacting at an angle of 12 degrees, at a speed of
60 km/h, was validated with the full scale crash test data.
Parametric study was conducted at various speeds (40 km/h, 60km/h, 80 km/h),
impacting Concrete Barrier at different angles (6 degree, 8 degree, 12 degree, 24
degree, 45 degree, 60 degree, 90 degree) under Normal Road Condition and Icy Road
Condition.
HIC values obtained were useful to asses the severity on rider.
HIC at 6 degree impact/ 40 km/h-NRC resulted in a very low injury
HIC at 90 degree impact/ 40 km/h-NRC was with in the threshold limit
HIC at 90 degree impact/ 60 km/h-NRC was above the threshold limit, the rider
suffers death
HIC appeared to be very high when a Motorcycle is moving an 80 km/h while
impacting at 24 degree impact; Death can be seen at this point.
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During 90 degree impact/ 80 km/h, the rider flies away from barrier resulting in a low
HIC.
Femur injury increases as the impact angle decreases at the normal road condition.
At Icy road condition, Femur R injury is maximum at 12deg/60km/h-IRC and low at
90deg/40 km/h-IRC
Design of Experiments showed the percentage contribution of three factors related to
injuries to rider as shown below:
Angle of collision was 23%.
Contribution of road condition was very low (0.66%) towards the crash.
Change in speed contributed to 16% of overall crash.
The interaction of three factors plays a very important role during crash (31.2%).
7.2 Recommendations
The rider kinematics, injury parameters under different configurations was studied in
this research. Some of the recommendations that can be followed to improve upon study
are presented below:
Similar kind of tests can be conducted for steel guard barriers, and wire rope barriers.
As they are aggressive in nature during the time of impact, the behavior of
Motorcycle and rider would be different.
Spring damper barriers can be used to study the impact analysis. The behavior of rider
kinematics may change due to energy absorbed by the barriers.
Effect of Temporary Concrete Barrier system (University of Nebraska-Lincoln)
can be used to study the behavior of rider kinematics during collision.
Effect of helmet in the head injuries can be evaluated during collision.
Multiple occupants seating can be considered for the same test configurations. Hence
to observe the kinematics of rider and pillion and their injuries.
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Motorcycles with crash guards implemented also helps in preventing the rider to
suffer severe injuries.
A finite element model for the motorcycle can be developed which would be helpful
in studying the structural responses during impact.
Other passengers such as female or children can be introduced to study the kinematic
analysis and injury parameters
Kinematic analysis can be performed when the Motorcycle hits the obstacle during
sliding position
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REFERENCES
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LIST OF REFERENCES
[1] Schneider H., An Analysis of Motorcycle Crashes 1996 to 2002, Louisiana State
University; May 2003.
[2] Statistical background of Motorcycle Accidents, U.S. National Highway Traffic
Safety Administration (NHTSA), 2005.
[3] MIC Motorcycle Survey- Trends and Safety Statistics, National Transportation
Safety board, 2003
[4] Chandrakumaran C, Road design and Road side Safety, New Zealand, 1999.
[5] Duncan C., Corben B., Truedsson N. and Tingvall C., Motorcycle and Safety Barrier
Crash-Testing: Feasibility Study Accident Research Centre, Monash University,
2000.
[6] Adamson S. K., Alexander P, Robinson L. E., Johnson M. G., Burkhead I. C.,
McManus J, Anderson C. G., Aronberg R, Kinney J, Sallmann W. D, SeventeenMotorcycle Crash Tests into Vehicles and a Barrier, College Station, Texas, 2000.
[7] Niieboer J. J.