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International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 05 Issue: 04 | Apr-2018 www.irjet.net p-ISSN: 2395-0072
© 2018, IRJET | Impact Factor value: 6.171 | ISO 9001:2008 Certified Journal | Page 1978
NUMERICAL ANALYSIS OF NOSE LANDING GEAR SYSTEM
SWARNAKIRAN.S1 , ROHITH.S2
1,2 Assistant Professor, Dept. of Mechanical Engineering, ATME College of Engineering, Mysore, Karnataka, India
---------------------------------------------------------------------***---------------------------------------------------------------------
Abstract -An aircraft landing gear system must absorb the
kinetic energy produced by a landing impact and excitations
caused by the aircraft travelling over an uneven runway
surface. This is the necessary requirement of a successfully
designed landing system. The oleo-pneumaticshockisthemost
common type of shock absorber landing gear system used in
aircrafts. It dissipates the kinetic energy produced by impacts
arising when an airplane lands at high speed but also offers a
comfortable ride to passengers when the airplanetaxiesatlow
speed. The objective of this project is to determine the stress
behavior and the displacement of a nose gear of an aircraft
during landing using structural finite element analysis. The
nose gear was first modeled using computer-aided design
software and then imported into finite element software. The
external forces were determined analytically and the
interactions between components were carefully modeled
using contact analysis.
Key Words: Oleo pneumatic, Nose landing gear, Finite
element analysis, Stress analysis, Normal modal analysis.
1. INTRODUCTION
The landing gear is that portion of the aircraft that
supports the weight of the aircraft while it is on the ground.
The landing gear containscomponentsthatarenecessaryfor
taking off and landing the aircraft safely. Some of these
components are landing gear struts that absorb landing and
taxing shocks; brakes that are used to stop the aircraft; nose
wheel steering for steering the aircraft.
An aircraft landing gear system must absorb the
kinetic energy produced by a landing impact and excitation
caused by an aircraft travelling over an uneven runway
surface. This is the necessary requirement of a successfully
designed landing system. The oleo-pneumatic shock strut is
the most common type of shock absorber landing gear
system used in aircrafts. It dissipates the kinetic energy
produced by impacts arising when an airplane lands at high
speed but also offers a comfortable ride to passengerswhen
the airplane taxies at low speed. The strut behaves in a
strongly nonlinear manner, which influences the
performance of the landing system. Investigations involving
real-time feedback of the ground input to the landingsystem
have shown that active control greatly reduces impact and
fatigue loads experienced by the aircraft as well as vertical
displacements. This is achieved by adjusting the system’s
stiffness and damping.
The landing gear is the interface of airplane to ground,
so that all the ground loads are transmitted by it to an
aircraft structure. There is a high influence of the landing
gear on the local structure, which must be taken intoaccount
in the initial design stage. The system must then have
considerable mechanical resistance, which means ingeneral
that its mass is significant. Depending on aircraft category,
this can range from 3 to 7% of the aircraft total mass.
Fig.1.1 Landing gear system.
The landing gear is necessary for the aircraft to
take-off and land on a runway, to relocate itself on anairport
and to support the weight of an aircraft when parked on the
platform. Once landed, the landing gear is equipped with
multiple systemsto bring an aircraft to a safe stop. Whenthe
speed of the aircraft is reduced, the aircraft will land to the
platform. When the aircraft is in flight, the landing gear will
be retracted and the doors will be closed. This gives the
aircraft better aerodynamic characteristics. When the
aircraft is approaching the runway, the landing gear will be
extended and locked.
The landing gear is the structure that supports an
aircraft on the ground and allows it to taxing, take-off and
land. In fact, landing gear design tends to have several
interferences with the aircraft structural design.
The landing gear system includes:
1 Strut.
2 Shock absorber.
3 Extraction/retraction mechanism.
4 Brakes.
5 Wheel.
6 Tyre.
2. LITERATURE
The survey of literature devoted to the most commonly
applied landing gear system, such aslanding gearsequipped
with hydraulic-pneumatic shock absorbers. Reviewing the
literature, in particular attention will be paid to the way in
which the dynamic properties of wheel, shock absorber and
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 05 Issue: 04 | Apr-2018 www.irjet.net p-ISSN: 2395-0072
© 2018, IRJET | Impact Factor value: 6.171 | ISO 9001:2008 Certified Journal | Page 1979
aircraft structures are taken into account, and to the way in
which the loads due the landing impacts are calculated.
V. d. Neut et.al.[2] is a very extensive investigation in the
field of symmetrical landing impact loads and is devoted in
particular to the problem of defining critical loading cases
for nose wheel landing gears. The tyre-shock absorber
combination of the nose wheel landing gear is represented
by a linear spring, but for the main wheel landing gear the
shock absorber damping characteristics are represented by
velocity squared damping forces. The unstrung mass is
neglected while wheel and shock absorber spring
characteristics are represented by linear springs. Further,
the drop test interpretation problem of how to take into
account static lift forces is already recognized.
With regard to the analytic approach to the problem in the
USA, first of all the work of E. G. Keller [3] should be
mentioned. This investigation formulates in an appropriate
way the equations of motion of wheel and shock absorber,
and calculates the vertical landing gear loads of a rigid
aircraft. It is described how in an elastic structure the
accelerations have to be calculated when the landing gear
forces are known as a function of time.
Jerzy Malachowski[4] his research on the most effective
methods of aircrafts’ landing gears design as well as the
evaluation of the gear’s condition during utilization period
and possibilities of extending itsdurability are the subjectof
numerous studies, including the ones by leading worldwide
aviation companies and national scientific centers. It is
indicated in these studies that numerical analysis of the
strength of the construction elements of the examined
aircraft’spart (beside experimental research) is a necessary
stage of proper methodology of aviation research, in
particular in programming and reliability evaluation and
development of methods of increasing durability in case of
solutions already used in practice.
Yang Yang [5] he conducted project on FW-11 cooperated
between Aviation Industry Corporation of China (AVIC) and
Cranfield University. His group designed a new conceptual
design and the target of it is to develop a flying wing
commercial airliner. Asa part of AVIC MSc program, theFW-
11 project is constructed by three phases: conceptualdesign
phase, preliminary design phase, and detail design phase.
The author was involved in the conceptual design phase
which was divided into three steps: derivation of
requirements, design a conventional aircraft as baseline
aircraft and design FW-11 comparing with the baseline
aircraft. The main objective of this thesiswasto buildasetof
diagnosis, prognosis and healthmanagementmethodswhich
are suitable for the aircraft landing gear extension and
retraction control system. FMEA and FTA for the system
were conducted. From the FHA, each of the catastrophic
events of the landing gear extension/retraction control
system was identified. The architecture of the rule-based
expert system, the acquisition of comprehensive domain
expert knowledge is in the most important factor.
Amit Goyal [7] he conducted this project in MSRIT School of
Advanced Studies (SAS), INDIA. He present an approach for
“Design Analysis; of a Nose Landing Gear of an Aircraft”
made of advanced compositesmaterialsusingadvancedCAE
tools and techniques. First of all, functional specification of
the part has been specified. General principles of composite
design were followed in arriving at suitable designs. In the
design phase using the FEA tool ANSYS 5.7, starting form
shape and wall construction, choosing a proper element
type, loadings, constraints, materialsand behaviormodeling
hasbeen done. Variousconstantsandlaminationparameters
were used to define the element.
3. METHODOLOGY
In this project, Finite Element analyses were used to
determine the characteristics of the nose landing gear. All
methodology principlesand theoriesdiscussedwereutilized
to achieve the project’s objectives. The combinationofallthe
analysis results were used to develop virtual model created
using FEM tools and the model was updated based on the
correlation process. The literature review of the nose
landing gear was carried out to obtain basic understanding
of the project. Information like typical natural frequency
values of nose landing gear, excitation sources and mode
shape of nose landing gear were searched and reviewed.For
the purpose of this study, the Landing gear was modeled
using CATIAV5-R17 software accordingtotheoriginalsizeof
structures. The model wasthen importedintoFiniteElement
preprocessing software Hypermeshforthemeshinganalysis,
8 noded hexa element, 6 nodded penta elements and rigid
elements were chosen to model the chassis. The model was
then imported into Finite Element solver software MSC
Nastran, Hyperview software is used for post processingthe
results.
4. FINITE ELEMENT METHOD
The Finite Element Method is a numerical approximation
method, investing the behavior of complex structures by
breaking them down into smaller pieces, simpler pieces and
these smaller pieces are called finite elements. The elements
are connected to each other at nodes. The finite element
method is also known as the matrix method of structural
analysis in the literature because it uses matrix algebra to
solve the system of simultaneous equations and it is
becoming the primary analysis tool for designers and
analysts.
The finite element method is based on two concepts:
1. Transformation of the original problem into an
equivalent integral formulation (weighted residual or
variation).
2. Approximation of the field variable distributionsandthe
geometry of the continuum domain in terms of a set of
shape functions, which are locally, defined within small
sub domains(finite elements) of the continuumdomain.
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 05 Issue: 04 | Apr-2018 www.irjet.net p-ISSN: 2395-0072
© 2018, IRJET | Impact Factor value: 6.171 | ISO 9001:2008 Certified Journal | Page 1980
Through the application of the element concept, the original
problem of determining field variable distributions in a
continuum domain is approximately transformed into a
problem of determining the field variables at some discrete
nodal positions within each element. This transformation
results in a set of algebraic equations, for which numerical
solution procedures are readily available.
Finite element analysis has been widely used in noise,
vibration and harshness, (NVH) simulation especially in the
fast growing automotive industries. Engineers were given
the power and ability to predict and assess structure-borne
noise in engine by high advanced computer software and
hardware. Validation of the finite element model itself has
become automated and more reliable. The finite element
models are often correlated with experimental modal
analysis results in order to achieve a high degree of
confidence in the finite element analysis.
Basic steps in finite element method, they are:
1. Discretize.
2. Deriving governing equations for each element.
3. Assemble global governing equations.
4. Apply loads and boundary conditions.
5. Solve for primary unknowns.
6. Calculate derived variables.
5. DESIGN DETAILS
The physical component of Landing Gear was modelled by
collecting various literature survey. These dimensional data
was used to build CATIA part model by using CATIA V5R17.
CATIA started as an in-house development in 1977 by
French aircraft manufacturer Avions Marcel Dassault,atthat
time customer of the CAD/CAMCAD software to develop
Dassault's Mirage fighter jet, then was adopted in the
aerospace, automotive, shipbuilding, and other industries.
Initially named CATI (Conception Assistive
Tridimensionnelle Interactive — French for Interactive
Aided Three-dimensional Design) — it was renamed CATIA
in 1981, when Dassault created a subsidiary to develop and
sell the software, and signed a non-exclusive distribution
agreement with IBM.
Fig.5.1 CATIA Model of nose landing gear system.
Fig.5.2 Isometric View of nose landing gear system.
5.1 CREATION OF FINITE ELEMENT MODEL:
After creation of CAD model in CATIAV5R17 to carry out
further pre-processing process the CATIA model part was
imported in Hypermesh during this processsome geometric
deviation will occur that needs to be corrected (geometric
clean up) in Hypermesh. Nose landing gear system
component modelled by using linear first-order (6-or 8-
noded) elements. Solid elements are Hexahedral and
Pentagon elements.
Meshing is done using Altair Hyperworksv10 pre-processor.
There are three options in the “create mesh” sub-panel of
Hypermesh. The switch allows one to choose from the
interactive, automatic, and QI optimized selections. The
interactive option is used to auto mesh multiple surfaces or
elements with user-controlled parameters.
Here global element size 2mm is maintained and the
minimum edge length is 0.5mm.
Fig.5.2 Finite Element Model of an Landing Gear system.
5.1.1 MESHING PARAMETERS:
Table 5.1 Landing Gear System Finite Element Model Data.
Meshing Size
Type
Of
Mesh
Type Of
Element
Used
Number
Of
Nodes
Number
Of
Elements
Fine
mesh(10mm)
solid Hexa, penta 319358
289486
Tetra mesh
(15mm)
solid Tetra 21821
83054
Average mesh
(20mm)
solid Hexa, penta 44065
36191
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 05 Issue: 04 | Apr-2018 www.irjet.net p-ISSN: 2395-0072
© 2018, IRJET | Impact Factor value: 6.171 | ISO 9001:2008 Certified Journal | Page 1981
5.1.2 ELEMENT QUALITY PARAMETERS:
For accurate results and numericalstability,elementsshould
be cleared for the quality criteria mentioned.
Table 5.2 Quality Criteria for 3 Dimensional Elements.
PARTICULAR UPPER LIMIT PARTICULAR UPPER
LIMIT
Warpage 30 degree Length* 0.5mm
Aspect 5mm Jacobian 0.6
Skew 60 degree Tria min angle 30 degree
Quad min angle 45 degree Tria max angle 120 degree
Quad max angle 135 degree
*length may vary from component to component.
5.1.3 MATERIAL PROPERTIES:
Material details of nose landing gear system.
Components Material Young’s
Modulus
[E]
N/mm2
Poissoin’s
Ratio [Nu]
Density
[Rho]
Tonne/mm3
Mass
[M]
Tonne
wheels Rubber 70 0.45 6.5E-9 6.9E-2
piston Steel 2.47E5 0.29 7.86E-9 11.16E-2
Upper mass Aluminium 7.17E4 0.33 2.82E-9 7.05E-2
Wheel hub Magnesium 4.48E3 0.35 1.8E-9 2.0E-3
Cylinder Aluminium 7.17E4 0.33 2.82E-9 2.948E-2
Piston rod Steel 2.47E5 0.29 7.86E-9 11.16E-2
Table 5.3 Material Properties of nose landing Gear system.
5.2 BOUNDARY CONDITIONS:
Finite element analysis wascarried out to evaluate thestatic
analysis and dynamic behavior such as eigen values and
eigen vectors. To execute the finite element analysis,
different boundary conditions were used depending up on
the nature of result to be evaluated.
5.2.1 BOUNDARY CONDITIONS FOR STATIC AND
DYNAMIC ANALYSIS:
The analysis was carried out to predict the mode shapesand
first few natural frequencies of nose landing gear system.
The mode shapes required for the study of dynamic
behaviour, were generally the lower mode shapes of the
structure.
Fixed in All Degree of freedom.
Fig.5.5 Finite Element Model of nose landing gear system
with Boundary Conditions.
5.3 POST-PROCESSING:
5.3.1 LINEAR STATIC ANALYSISRESULTSFORFINEMESH
SIZE 10mm:
Stress and displacement contours for loadinydirection:
The stress and displacement contours have been obtained
for the load casesmentioned above, following figuresshows
the Stress and displacement contours for load case. The
Figure shows the Displacement contour for the first load
case.
It is found that maximum displacement occurs at the wheel
hub which can be visualized from the red colored portion
indicating maximum value as shown in the figure below.
5.3.1.1 LOAD CASE 1 EMPTY WEIGHT OF AIRCRAFT
(10.5KN):
Displacement contour for load case-I
Stress contour for load case-I
5.3.2 NORMAL MODAL ANALYSIS-RESULTS:
The natural frequencies obtained from the finite element
modal analysis are tabulated below. Here the frequency
range of interest of an Landing gear system is between 0 to
300Hz.
First mode shape of Landing gear system.
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 05 Issue: 04 | Apr-2018 www.irjet.net p-ISSN: 2395-0072
© 2018, IRJET | Impact Factor value: 6.171 | ISO 9001:2008 Certified Journal | Page 1982
Second mode shape of Landing gear system.
Third mode shape of Landing gear system.
Fourth mode shape of Landing gear system.
Fifth mode shape of Landing gear system.
6. RESULTS OF LINEAR STATIC ANALYSIS:
As the material is ductile, maximum. Distortion energy
theory (Von mises theory) is considered for determiningthe
criterion for failure. Taking a factor of safety of 2.0, the
allowable stress for the material is 205 MPa, based on Y.S of
410 MPa.
It is concluded that, the maximum stressof163MPa(forboth
of above load cases, over the entire landing gearassembly)is
well within the allowable limit.
6.1.1 Graphs of stress v/s loading condition for nose
landing gear model.
Graph 6.1 - Stress v/s Load in fine mesh (10mm) model.
0.00E+00
2.00E+01
4.00E+01
6.00E+01
8.00E+01
1.00E+02
1.20E+02
Empty
weight(10.5KN)
Landing
weight(15.6KN)
Take off
weight(18.6KN)
Minimum stress(N/mm2)
Maximum stress(N/mm2)
Graph 6.2 - Stress v/s Load in Tetra mesh (15mm) model.
Graph 6.3 - Stress v/s Load in Average mesh (20 mm)
model.
6.1.2 Graphs of Displacement v/s varying Meshing size
for nose landing gear model.
0
2
4
6
Fine
mesh(10mm)
Tetra
mesh(15mm)
Average
mesh(20mm)
Empty
weight(KN)
Landing
weight(KN)
Graph 6.7- Displacement (mm) v/s varying mesh size.
0.00E+00
1.00E+01
2.00E+01
3.00E+01
4.00E+01
5.00E+01
6.00E+01
7.00E+01
Empty
weight(10.5KN)
Landing
weight(15.6KN)
Take off
weight(18.69KN)
Minimum stress(N/mm2)
Maximum stresss(N/mm2)
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 05 Issue: 04 | Apr-2018 www.irjet.net p-ISSN: 2395-0072
© 2018, IRJET | Impact Factor value: 6.171 | ISO 9001:2008 Certified Journal | Page 1983
6.1.3 Graphs of Stress v/s varying Meshing size for nose
landing gear model.
Graph - 6.8 Stress (N/mm2) v/s varying mesh size.
6.1.4 GRAPHS OF FREQUENCY V/S MESH SIZE FOR NOSE
LANDING GEAR MODEL.
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
FINE
MESH(10mm)
TETRA
MESH(15mm)
AVERAGE
MESH(20mm)
EMPTY WEIGHT
LANDING WEIGHT
TAKE OFF WEIGHT
Graph 6.11 Frequency v/s mesh size in first modal shape.
Graph 6.12 Frequency v/s mesh size in second modal
shape.
0
2
4
6
8
10
12
14
16
18
20
FINE MESH(10mm)TETRA MESH(15mm)AVERAGE MESH(20mm)
EMPTY WEIGHT
LANDING WEIGHT
TAKE OFF WEIGHT
Graph 6.13 Frequency v/s mesh size in third modal shape.
From the modal analysis graph it is observed that
tetra mesh results are greatly reduces when compare with
average mesh and fine mesh. Hence it is recommended that
to avoid the tetrahedral elements for dynamic analysis.
CONCLUSION
This analysis demonstrated several important factors in
analysing a nose landing gear. First, the function of the nose
landing gears must be understood. A CAD model of nose
landing gear was designed and discretized in to finite
element mesh using HYPERMESH. Designloadswereapplied
through RBE3 connection in respective directions.Staticand
Normal Modal analysis were conducted in MSC NASTRAN.
In static analysis the obtained stresses are much lesser than
the allowable stresses of the material. The obtained
magnitudesof maximum stressare less than the yield stress
and ultimate stress so we conclude that material in elastic
limit and not yet started yielding and initial crack. FE
analysis will allow them to make design alterations prior to
manufacturing and testing, which in turn can savethemtime
and money. This analysis can be performed on the Twin
Otter nose landing gear to predict failure. Future research
can be implemented from this analysis, such as
incorporating the tyre into the analysis, performing non-
linear and dynamics stress analysis at the time the tyre
contacts with the runway until the aircraft stop, and
performing physical testing for validation purposes.
In normal modal analysis predict the dynamic characteristic
of nose landing gear system such as the natural frequency
and mode shape. Basically, natural frequency and mode
shape are important parameters in design. That is because
damage can be occurred if the nose landing gear is excitedat
the natural frequency during operation. As conclusion, this
project has achieved its core objectives. The dynamic
characteristic such as the natural frequencies and mode
shapesof the nose landing gear wasdetermined analytically.
The result indicating that the FE model shows a good
correlation with the experimental model for themodeshape
but not for the natural frequencies. The FE model presented
an average of 10% higher frequencies than the nose landing
gear. This fact is due to the perfection of the model and the
imperfection of the real structure. For instance, in the FE
model the welds are perfect but in reality these can have
defects that lead to a smaller structural stiffness.
REFERENCES:
[1] Haitao wang, J.T.Xing, W.G.Price,Weiji Li,“An
investigation of an active landing gear system to reduce
aircraft vibrations caused by landing impacts and
runway excitations”.
[2] A.v.d.Neut - F.J. Plantema "Belastingen op
neuswielonderstellen tijdens landingen".
[3] (Nose wheel loads at landing impacts )Nat. Aeron.
Research Institute, Amsterdam. Rep. S-244, S-245 and
S-304 1941.
[4] E.G.Keller"Some present non-linear problems of the
electrical and aeronautical industries". Quarterly of
Applied Mathematics. Vol 11 p. 72 1944.
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 05 Issue: 04 | Apr-2018 www.irjet.net p-ISSN: 2395-0072
© 2018, IRJET | Impact Factor value: 6.171 | ISO 9001:2008 Certified Journal | Page 1984
[5] Jerzy Malachowski “DyanamicalanalysisofLandinggear
for critical work conditions”, 2010.
[6] Yang Yang,”Aircraft Landing Gear Extension And
Retraction Control” February 2012.
[7] Ying xing,“The Strength Analysis of the Diagonal Stay of
Aircraft Landing Gear Based on ANSYS”,2012.
[8] Amit Goyal “Light Aircraft Main Landing Gear Design
and Development”, SAS Tech journals pp. 45-50, 2012.
[9] JACOB IJFF, “Analysis of dynamic aircraft landing loads
and a proposal for rational design landing load
requirements”.
[10] Shkarayev, S. 2006, Preliminary design of landing gear,
University of Arizona, viewed 2nd September.
[11] Lee, H.C., Hwang, Y.H., Kim, T., 2003. “Failure Analysis of
Nose Landing Gear Assembly”, Engineering Failure
Analysis, Vol. 10, pp. 77-84.
[12] Malachowski, J., Wesolowski, M., Krason, W., 2006.
“Computational Study of Transport Aircraft Landing
Gear during Touchdown”, Journal of kones Power train
and Transport, Vol. 13, pp. 187-195.
[13] Strength Analysis of 3D Landing Gear Model with
Failure, WIESLAW KRASON, JERZY MALACHOWSKI,
Department of Mechanics and Applied Computer
Science, Military University of Technology
BIOGRAPHIES
Swarnakiran S received the B.E.
Mechanical Engineering from
Vidya vardhaka college of
engineering in 2013 and M.tech
degree from Don Bosco Instituteof
Technology in 2015. Presently
working as Assistant professor at
ATME college of Engineering.

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IRJET- Numerical Analysis of Nose Landing Gear System

  • 1. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 05 Issue: 04 | Apr-2018 www.irjet.net p-ISSN: 2395-0072 © 2018, IRJET | Impact Factor value: 6.171 | ISO 9001:2008 Certified Journal | Page 1978 NUMERICAL ANALYSIS OF NOSE LANDING GEAR SYSTEM SWARNAKIRAN.S1 , ROHITH.S2 1,2 Assistant Professor, Dept. of Mechanical Engineering, ATME College of Engineering, Mysore, Karnataka, India ---------------------------------------------------------------------***--------------------------------------------------------------------- Abstract -An aircraft landing gear system must absorb the kinetic energy produced by a landing impact and excitations caused by the aircraft travelling over an uneven runway surface. This is the necessary requirement of a successfully designed landing system. The oleo-pneumaticshockisthemost common type of shock absorber landing gear system used in aircrafts. It dissipates the kinetic energy produced by impacts arising when an airplane lands at high speed but also offers a comfortable ride to passengers when the airplanetaxiesatlow speed. The objective of this project is to determine the stress behavior and the displacement of a nose gear of an aircraft during landing using structural finite element analysis. The nose gear was first modeled using computer-aided design software and then imported into finite element software. The external forces were determined analytically and the interactions between components were carefully modeled using contact analysis. Key Words: Oleo pneumatic, Nose landing gear, Finite element analysis, Stress analysis, Normal modal analysis. 1. INTRODUCTION The landing gear is that portion of the aircraft that supports the weight of the aircraft while it is on the ground. The landing gear containscomponentsthatarenecessaryfor taking off and landing the aircraft safely. Some of these components are landing gear struts that absorb landing and taxing shocks; brakes that are used to stop the aircraft; nose wheel steering for steering the aircraft. An aircraft landing gear system must absorb the kinetic energy produced by a landing impact and excitation caused by an aircraft travelling over an uneven runway surface. This is the necessary requirement of a successfully designed landing system. The oleo-pneumatic shock strut is the most common type of shock absorber landing gear system used in aircrafts. It dissipates the kinetic energy produced by impacts arising when an airplane lands at high speed but also offers a comfortable ride to passengerswhen the airplane taxies at low speed. The strut behaves in a strongly nonlinear manner, which influences the performance of the landing system. Investigations involving real-time feedback of the ground input to the landingsystem have shown that active control greatly reduces impact and fatigue loads experienced by the aircraft as well as vertical displacements. This is achieved by adjusting the system’s stiffness and damping. The landing gear is the interface of airplane to ground, so that all the ground loads are transmitted by it to an aircraft structure. There is a high influence of the landing gear on the local structure, which must be taken intoaccount in the initial design stage. The system must then have considerable mechanical resistance, which means ingeneral that its mass is significant. Depending on aircraft category, this can range from 3 to 7% of the aircraft total mass. Fig.1.1 Landing gear system. The landing gear is necessary for the aircraft to take-off and land on a runway, to relocate itself on anairport and to support the weight of an aircraft when parked on the platform. Once landed, the landing gear is equipped with multiple systemsto bring an aircraft to a safe stop. Whenthe speed of the aircraft is reduced, the aircraft will land to the platform. When the aircraft is in flight, the landing gear will be retracted and the doors will be closed. This gives the aircraft better aerodynamic characteristics. When the aircraft is approaching the runway, the landing gear will be extended and locked. The landing gear is the structure that supports an aircraft on the ground and allows it to taxing, take-off and land. In fact, landing gear design tends to have several interferences with the aircraft structural design. The landing gear system includes: 1 Strut. 2 Shock absorber. 3 Extraction/retraction mechanism. 4 Brakes. 5 Wheel. 6 Tyre. 2. LITERATURE The survey of literature devoted to the most commonly applied landing gear system, such aslanding gearsequipped with hydraulic-pneumatic shock absorbers. Reviewing the literature, in particular attention will be paid to the way in which the dynamic properties of wheel, shock absorber and
  • 2. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 05 Issue: 04 | Apr-2018 www.irjet.net p-ISSN: 2395-0072 © 2018, IRJET | Impact Factor value: 6.171 | ISO 9001:2008 Certified Journal | Page 1979 aircraft structures are taken into account, and to the way in which the loads due the landing impacts are calculated. V. d. Neut et.al.[2] is a very extensive investigation in the field of symmetrical landing impact loads and is devoted in particular to the problem of defining critical loading cases for nose wheel landing gears. The tyre-shock absorber combination of the nose wheel landing gear is represented by a linear spring, but for the main wheel landing gear the shock absorber damping characteristics are represented by velocity squared damping forces. The unstrung mass is neglected while wheel and shock absorber spring characteristics are represented by linear springs. Further, the drop test interpretation problem of how to take into account static lift forces is already recognized. With regard to the analytic approach to the problem in the USA, first of all the work of E. G. Keller [3] should be mentioned. This investigation formulates in an appropriate way the equations of motion of wheel and shock absorber, and calculates the vertical landing gear loads of a rigid aircraft. It is described how in an elastic structure the accelerations have to be calculated when the landing gear forces are known as a function of time. Jerzy Malachowski[4] his research on the most effective methods of aircrafts’ landing gears design as well as the evaluation of the gear’s condition during utilization period and possibilities of extending itsdurability are the subjectof numerous studies, including the ones by leading worldwide aviation companies and national scientific centers. It is indicated in these studies that numerical analysis of the strength of the construction elements of the examined aircraft’spart (beside experimental research) is a necessary stage of proper methodology of aviation research, in particular in programming and reliability evaluation and development of methods of increasing durability in case of solutions already used in practice. Yang Yang [5] he conducted project on FW-11 cooperated between Aviation Industry Corporation of China (AVIC) and Cranfield University. His group designed a new conceptual design and the target of it is to develop a flying wing commercial airliner. Asa part of AVIC MSc program, theFW- 11 project is constructed by three phases: conceptualdesign phase, preliminary design phase, and detail design phase. The author was involved in the conceptual design phase which was divided into three steps: derivation of requirements, design a conventional aircraft as baseline aircraft and design FW-11 comparing with the baseline aircraft. The main objective of this thesiswasto buildasetof diagnosis, prognosis and healthmanagementmethodswhich are suitable for the aircraft landing gear extension and retraction control system. FMEA and FTA for the system were conducted. From the FHA, each of the catastrophic events of the landing gear extension/retraction control system was identified. The architecture of the rule-based expert system, the acquisition of comprehensive domain expert knowledge is in the most important factor. Amit Goyal [7] he conducted this project in MSRIT School of Advanced Studies (SAS), INDIA. He present an approach for “Design Analysis; of a Nose Landing Gear of an Aircraft” made of advanced compositesmaterialsusingadvancedCAE tools and techniques. First of all, functional specification of the part has been specified. General principles of composite design were followed in arriving at suitable designs. In the design phase using the FEA tool ANSYS 5.7, starting form shape and wall construction, choosing a proper element type, loadings, constraints, materialsand behaviormodeling hasbeen done. Variousconstantsandlaminationparameters were used to define the element. 3. METHODOLOGY In this project, Finite Element analyses were used to determine the characteristics of the nose landing gear. All methodology principlesand theoriesdiscussedwereutilized to achieve the project’s objectives. The combinationofallthe analysis results were used to develop virtual model created using FEM tools and the model was updated based on the correlation process. The literature review of the nose landing gear was carried out to obtain basic understanding of the project. Information like typical natural frequency values of nose landing gear, excitation sources and mode shape of nose landing gear were searched and reviewed.For the purpose of this study, the Landing gear was modeled using CATIAV5-R17 software accordingtotheoriginalsizeof structures. The model wasthen importedintoFiniteElement preprocessing software Hypermeshforthemeshinganalysis, 8 noded hexa element, 6 nodded penta elements and rigid elements were chosen to model the chassis. The model was then imported into Finite Element solver software MSC Nastran, Hyperview software is used for post processingthe results. 4. FINITE ELEMENT METHOD The Finite Element Method is a numerical approximation method, investing the behavior of complex structures by breaking them down into smaller pieces, simpler pieces and these smaller pieces are called finite elements. The elements are connected to each other at nodes. The finite element method is also known as the matrix method of structural analysis in the literature because it uses matrix algebra to solve the system of simultaneous equations and it is becoming the primary analysis tool for designers and analysts. The finite element method is based on two concepts: 1. Transformation of the original problem into an equivalent integral formulation (weighted residual or variation). 2. Approximation of the field variable distributionsandthe geometry of the continuum domain in terms of a set of shape functions, which are locally, defined within small sub domains(finite elements) of the continuumdomain.
  • 3. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 05 Issue: 04 | Apr-2018 www.irjet.net p-ISSN: 2395-0072 © 2018, IRJET | Impact Factor value: 6.171 | ISO 9001:2008 Certified Journal | Page 1980 Through the application of the element concept, the original problem of determining field variable distributions in a continuum domain is approximately transformed into a problem of determining the field variables at some discrete nodal positions within each element. This transformation results in a set of algebraic equations, for which numerical solution procedures are readily available. Finite element analysis has been widely used in noise, vibration and harshness, (NVH) simulation especially in the fast growing automotive industries. Engineers were given the power and ability to predict and assess structure-borne noise in engine by high advanced computer software and hardware. Validation of the finite element model itself has become automated and more reliable. The finite element models are often correlated with experimental modal analysis results in order to achieve a high degree of confidence in the finite element analysis. Basic steps in finite element method, they are: 1. Discretize. 2. Deriving governing equations for each element. 3. Assemble global governing equations. 4. Apply loads and boundary conditions. 5. Solve for primary unknowns. 6. Calculate derived variables. 5. DESIGN DETAILS The physical component of Landing Gear was modelled by collecting various literature survey. These dimensional data was used to build CATIA part model by using CATIA V5R17. CATIA started as an in-house development in 1977 by French aircraft manufacturer Avions Marcel Dassault,atthat time customer of the CAD/CAMCAD software to develop Dassault's Mirage fighter jet, then was adopted in the aerospace, automotive, shipbuilding, and other industries. Initially named CATI (Conception Assistive Tridimensionnelle Interactive — French for Interactive Aided Three-dimensional Design) — it was renamed CATIA in 1981, when Dassault created a subsidiary to develop and sell the software, and signed a non-exclusive distribution agreement with IBM. Fig.5.1 CATIA Model of nose landing gear system. Fig.5.2 Isometric View of nose landing gear system. 5.1 CREATION OF FINITE ELEMENT MODEL: After creation of CAD model in CATIAV5R17 to carry out further pre-processing process the CATIA model part was imported in Hypermesh during this processsome geometric deviation will occur that needs to be corrected (geometric clean up) in Hypermesh. Nose landing gear system component modelled by using linear first-order (6-or 8- noded) elements. Solid elements are Hexahedral and Pentagon elements. Meshing is done using Altair Hyperworksv10 pre-processor. There are three options in the “create mesh” sub-panel of Hypermesh. The switch allows one to choose from the interactive, automatic, and QI optimized selections. The interactive option is used to auto mesh multiple surfaces or elements with user-controlled parameters. Here global element size 2mm is maintained and the minimum edge length is 0.5mm. Fig.5.2 Finite Element Model of an Landing Gear system. 5.1.1 MESHING PARAMETERS: Table 5.1 Landing Gear System Finite Element Model Data. Meshing Size Type Of Mesh Type Of Element Used Number Of Nodes Number Of Elements Fine mesh(10mm) solid Hexa, penta 319358 289486 Tetra mesh (15mm) solid Tetra 21821 83054 Average mesh (20mm) solid Hexa, penta 44065 36191
  • 4. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 05 Issue: 04 | Apr-2018 www.irjet.net p-ISSN: 2395-0072 © 2018, IRJET | Impact Factor value: 6.171 | ISO 9001:2008 Certified Journal | Page 1981 5.1.2 ELEMENT QUALITY PARAMETERS: For accurate results and numericalstability,elementsshould be cleared for the quality criteria mentioned. Table 5.2 Quality Criteria for 3 Dimensional Elements. PARTICULAR UPPER LIMIT PARTICULAR UPPER LIMIT Warpage 30 degree Length* 0.5mm Aspect 5mm Jacobian 0.6 Skew 60 degree Tria min angle 30 degree Quad min angle 45 degree Tria max angle 120 degree Quad max angle 135 degree *length may vary from component to component. 5.1.3 MATERIAL PROPERTIES: Material details of nose landing gear system. Components Material Young’s Modulus [E] N/mm2 Poissoin’s Ratio [Nu] Density [Rho] Tonne/mm3 Mass [M] Tonne wheels Rubber 70 0.45 6.5E-9 6.9E-2 piston Steel 2.47E5 0.29 7.86E-9 11.16E-2 Upper mass Aluminium 7.17E4 0.33 2.82E-9 7.05E-2 Wheel hub Magnesium 4.48E3 0.35 1.8E-9 2.0E-3 Cylinder Aluminium 7.17E4 0.33 2.82E-9 2.948E-2 Piston rod Steel 2.47E5 0.29 7.86E-9 11.16E-2 Table 5.3 Material Properties of nose landing Gear system. 5.2 BOUNDARY CONDITIONS: Finite element analysis wascarried out to evaluate thestatic analysis and dynamic behavior such as eigen values and eigen vectors. To execute the finite element analysis, different boundary conditions were used depending up on the nature of result to be evaluated. 5.2.1 BOUNDARY CONDITIONS FOR STATIC AND DYNAMIC ANALYSIS: The analysis was carried out to predict the mode shapesand first few natural frequencies of nose landing gear system. The mode shapes required for the study of dynamic behaviour, were generally the lower mode shapes of the structure. Fixed in All Degree of freedom. Fig.5.5 Finite Element Model of nose landing gear system with Boundary Conditions. 5.3 POST-PROCESSING: 5.3.1 LINEAR STATIC ANALYSISRESULTSFORFINEMESH SIZE 10mm: Stress and displacement contours for loadinydirection: The stress and displacement contours have been obtained for the load casesmentioned above, following figuresshows the Stress and displacement contours for load case. The Figure shows the Displacement contour for the first load case. It is found that maximum displacement occurs at the wheel hub which can be visualized from the red colored portion indicating maximum value as shown in the figure below. 5.3.1.1 LOAD CASE 1 EMPTY WEIGHT OF AIRCRAFT (10.5KN): Displacement contour for load case-I Stress contour for load case-I 5.3.2 NORMAL MODAL ANALYSIS-RESULTS: The natural frequencies obtained from the finite element modal analysis are tabulated below. Here the frequency range of interest of an Landing gear system is between 0 to 300Hz. First mode shape of Landing gear system.
  • 5. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 05 Issue: 04 | Apr-2018 www.irjet.net p-ISSN: 2395-0072 © 2018, IRJET | Impact Factor value: 6.171 | ISO 9001:2008 Certified Journal | Page 1982 Second mode shape of Landing gear system. Third mode shape of Landing gear system. Fourth mode shape of Landing gear system. Fifth mode shape of Landing gear system. 6. RESULTS OF LINEAR STATIC ANALYSIS: As the material is ductile, maximum. Distortion energy theory (Von mises theory) is considered for determiningthe criterion for failure. Taking a factor of safety of 2.0, the allowable stress for the material is 205 MPa, based on Y.S of 410 MPa. It is concluded that, the maximum stressof163MPa(forboth of above load cases, over the entire landing gearassembly)is well within the allowable limit. 6.1.1 Graphs of stress v/s loading condition for nose landing gear model. Graph 6.1 - Stress v/s Load in fine mesh (10mm) model. 0.00E+00 2.00E+01 4.00E+01 6.00E+01 8.00E+01 1.00E+02 1.20E+02 Empty weight(10.5KN) Landing weight(15.6KN) Take off weight(18.6KN) Minimum stress(N/mm2) Maximum stress(N/mm2) Graph 6.2 - Stress v/s Load in Tetra mesh (15mm) model. Graph 6.3 - Stress v/s Load in Average mesh (20 mm) model. 6.1.2 Graphs of Displacement v/s varying Meshing size for nose landing gear model. 0 2 4 6 Fine mesh(10mm) Tetra mesh(15mm) Average mesh(20mm) Empty weight(KN) Landing weight(KN) Graph 6.7- Displacement (mm) v/s varying mesh size. 0.00E+00 1.00E+01 2.00E+01 3.00E+01 4.00E+01 5.00E+01 6.00E+01 7.00E+01 Empty weight(10.5KN) Landing weight(15.6KN) Take off weight(18.69KN) Minimum stress(N/mm2) Maximum stresss(N/mm2)
  • 6. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 05 Issue: 04 | Apr-2018 www.irjet.net p-ISSN: 2395-0072 © 2018, IRJET | Impact Factor value: 6.171 | ISO 9001:2008 Certified Journal | Page 1983 6.1.3 Graphs of Stress v/s varying Meshing size for nose landing gear model. Graph - 6.8 Stress (N/mm2) v/s varying mesh size. 6.1.4 GRAPHS OF FREQUENCY V/S MESH SIZE FOR NOSE LANDING GEAR MODEL. 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 FINE MESH(10mm) TETRA MESH(15mm) AVERAGE MESH(20mm) EMPTY WEIGHT LANDING WEIGHT TAKE OFF WEIGHT Graph 6.11 Frequency v/s mesh size in first modal shape. Graph 6.12 Frequency v/s mesh size in second modal shape. 0 2 4 6 8 10 12 14 16 18 20 FINE MESH(10mm)TETRA MESH(15mm)AVERAGE MESH(20mm) EMPTY WEIGHT LANDING WEIGHT TAKE OFF WEIGHT Graph 6.13 Frequency v/s mesh size in third modal shape. From the modal analysis graph it is observed that tetra mesh results are greatly reduces when compare with average mesh and fine mesh. Hence it is recommended that to avoid the tetrahedral elements for dynamic analysis. CONCLUSION This analysis demonstrated several important factors in analysing a nose landing gear. First, the function of the nose landing gears must be understood. A CAD model of nose landing gear was designed and discretized in to finite element mesh using HYPERMESH. Designloadswereapplied through RBE3 connection in respective directions.Staticand Normal Modal analysis were conducted in MSC NASTRAN. In static analysis the obtained stresses are much lesser than the allowable stresses of the material. The obtained magnitudesof maximum stressare less than the yield stress and ultimate stress so we conclude that material in elastic limit and not yet started yielding and initial crack. FE analysis will allow them to make design alterations prior to manufacturing and testing, which in turn can savethemtime and money. This analysis can be performed on the Twin Otter nose landing gear to predict failure. Future research can be implemented from this analysis, such as incorporating the tyre into the analysis, performing non- linear and dynamics stress analysis at the time the tyre contacts with the runway until the aircraft stop, and performing physical testing for validation purposes. In normal modal analysis predict the dynamic characteristic of nose landing gear system such as the natural frequency and mode shape. Basically, natural frequency and mode shape are important parameters in design. That is because damage can be occurred if the nose landing gear is excitedat the natural frequency during operation. As conclusion, this project has achieved its core objectives. The dynamic characteristic such as the natural frequencies and mode shapesof the nose landing gear wasdetermined analytically. The result indicating that the FE model shows a good correlation with the experimental model for themodeshape but not for the natural frequencies. The FE model presented an average of 10% higher frequencies than the nose landing gear. This fact is due to the perfection of the model and the imperfection of the real structure. For instance, in the FE model the welds are perfect but in reality these can have defects that lead to a smaller structural stiffness. REFERENCES: [1] Haitao wang, J.T.Xing, W.G.Price,Weiji Li,“An investigation of an active landing gear system to reduce aircraft vibrations caused by landing impacts and runway excitations”. [2] A.v.d.Neut - F.J. Plantema "Belastingen op neuswielonderstellen tijdens landingen". [3] (Nose wheel loads at landing impacts )Nat. Aeron. Research Institute, Amsterdam. Rep. S-244, S-245 and S-304 1941. [4] E.G.Keller"Some present non-linear problems of the electrical and aeronautical industries". Quarterly of Applied Mathematics. Vol 11 p. 72 1944.
  • 7. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 05 Issue: 04 | Apr-2018 www.irjet.net p-ISSN: 2395-0072 © 2018, IRJET | Impact Factor value: 6.171 | ISO 9001:2008 Certified Journal | Page 1984 [5] Jerzy Malachowski “DyanamicalanalysisofLandinggear for critical work conditions”, 2010. [6] Yang Yang,”Aircraft Landing Gear Extension And Retraction Control” February 2012. [7] Ying xing,“The Strength Analysis of the Diagonal Stay of Aircraft Landing Gear Based on ANSYS”,2012. [8] Amit Goyal “Light Aircraft Main Landing Gear Design and Development”, SAS Tech journals pp. 45-50, 2012. [9] JACOB IJFF, “Analysis of dynamic aircraft landing loads and a proposal for rational design landing load requirements”. [10] Shkarayev, S. 2006, Preliminary design of landing gear, University of Arizona, viewed 2nd September. [11] Lee, H.C., Hwang, Y.H., Kim, T., 2003. “Failure Analysis of Nose Landing Gear Assembly”, Engineering Failure Analysis, Vol. 10, pp. 77-84. [12] Malachowski, J., Wesolowski, M., Krason, W., 2006. “Computational Study of Transport Aircraft Landing Gear during Touchdown”, Journal of kones Power train and Transport, Vol. 13, pp. 187-195. [13] Strength Analysis of 3D Landing Gear Model with Failure, WIESLAW KRASON, JERZY MALACHOWSKI, Department of Mechanics and Applied Computer Science, Military University of Technology BIOGRAPHIES Swarnakiran S received the B.E. Mechanical Engineering from Vidya vardhaka college of engineering in 2013 and M.tech degree from Don Bosco Instituteof Technology in 2015. Presently working as Assistant professor at ATME college of Engineering.