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International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 06 Issue: 05 |May 2019 www.irjet.net p-ISSN: 2395-0072
© 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 7180
A Study on the Behaviour of Double Layer Steel Braced Barrel Vaults
Sayali Jadhav1, Dr. P.S. Patil2
1M. Tech. student, Dept. of Civil-structural Engineering, RIT, Maharashtra, India
2Professor, Dept. of Civil-structural Engineering¸ RIT, Maharashtra, India
---------------------------------------------------------------------***----------------------------------------------------------------------
Abstract –The computer analysis of Double Layer steel
braced barrel vault is presented. In this work four types of
geometries of double layer braced barrel vault trusses are
modeled and their behavior is studied. Axial force and
deflection for top layer are compared and best geometry is
suggested. Modeling and analysis is done using finite
element software STAAD-PRO.
Key Words: Modeling, Double layer grid geometries,
behaviour, axial forces, deflection, STAAD-PRO.
1. INTRODUCTION
1.1 Introduction
The braced double layer barrel vaultiscomposedofmember
elements arranged on a cylindrical surface. The basic curve
is a circular segment; occasionally, a parabola, ellipse or
funicular line may also be used. Double-layer grids, or flat
surface space frames, consist of two planar networks of
members forming top and bottom-layers parallel to each
other and interconnected by vertical and inclined web
members. Double-layer grids are characterized by pinned
joints with no moment or torsional resistance; therefore, all
members can only resist tension or compression. Several
types of double-layer grids can be formed by these basic
elements. They are developed by varying thedirectionofthe
top and bottom-layers with respect to eachotherandalsoby
the positioning of the top-layer nodal points with respect to
the bottom- layer nodal points. Additional variations can be
introduced by changing the size of the top-layer grid with
respect to the bottom-layer grid. Thus,internal openingscan
be formed by omitting every second element in a normal
configuration.
Fig 1 Double layer steel braced barrel vault structure
2. Study of behaviour of double layer barrel vaults.
The structural behavior of double layer grid steel braced
barrel vaults depends on the various factors such as type of
patterns used for the geometry formation, types of support,
aspect ratio, type of connection used at the joint, Type of
sections, material used, type of bracings etc
To study the behavior of double layer grid steel braced
barrel vaults,4 different types of geometric patterns are
modeled and analyzed in Staad pro software and results for
maximum nodal deflection and axial forces in members for
particular group of elements are compared.
2.1 Common types of geometries used in double layers
Fig. 2 Different types of geometries.
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 06 Issue: 05 |May 2019 www.irjet.net p-ISSN: 2395-0072
© 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 7181
Alsodepending ontheir behaviortheycanbeclassifiedaslong
shells and short shells and it can be explained from L/R ratio
where L is the distance between the supports in longitudinal
direction and R is the radius of curvature of the transverse
curve.
1) Beam action - . If the distance between the supports is long
andusually edgebeamsareused in thelongitudinaldirection,
the primary response will be beam action. For 1.67 < L/R< 5 ,
the barrel vaults arecalledlongshells,whichcanbevisualized
as beams with curvilinear cross-sections. If L/R>3, beam
theorywithlinear stress distributioncanbeappliedforbarrel
vaultswithuniformcrosssectionandunderuniformloading..
This class of barrel vault will have longitudinal compressive
stresses near the crown of the vault, longitudinal tensile
stresses towards the free edges, and shear stresses towards
the supports.
2) Arch action - When distance between supports goes on
decreasing i.e when 0 . 25< L/R >1.67 , then the primary
response will be arch action in the transverse direction. Then
the barrel vaults are called short shells. Their structural
behavior is rather complex and dependent on their
geometrical proportions. The force distribution in the
longitudinal direction is no longer linear, but in a curvilinear
manner, trusses or arches are usually used as the transverse
supports.
3) Parallel arches – When L/R ratio becomes very small i.e.,
<25, theforcesare carried directly in thetransversedirection
to the edge supports. Displacement in the radial direction is
resisted by circumferential bending stiffness. Such type of
barrel vault can be applied to buildings such as airplane
hangars or gymnasia where the wall and roof are combined
together
3. MODELLING AND ANALYSIS
3.1Geometric details of models
 Span - 30m
 Height - 15m
 Length – 30m
 Span to height ratio - 2
 No of divisions - 20
 Size of module – 2.355m
3.2 Data used for analysis
 Type of section – pipe
 Size of section – PIP483L-48.3mm-2.9mm
 Loading – 1)self weight (from software)
2) DL – 4kN (Nodal load)
3.3 Types of geometries considered for study
 Square on square
 Lattice structure (Two way grid)
 Diagonal on diagonal
 Square on diagonal
3.4 Modelling and analysis of barrel vault structures in
STAAD pro.
In this section the modelling and analysis of barrel vault
structure in STAAD pro is explained in brief. The steps
followed are also explained.
3.5Types of geometries created in STAAD Pro
1) Square on Square
Fig. 3 Square on square geometry
2)Lattice structure (Two way grid)
Fig. 4 Two way grid geometry
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 06 Issue: 05 |May 2019 www.irjet.net p-ISSN: 2395-0072
© 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 7182
3) Diagonal on diagonal
Fig. 5 Diagonal on Diagonal geometry
4) Square on diagonal
Fig. 6 Square on diagonal geometry
3.5.2 Material properties and section assignment
After modelling next part is creating and assigning material
and section properties. Steel material having young's
modulus 2x10^5 N/mm^2 and poisons ratio 0.3 is created
and assigned. Then circular steel pipe section of Indian
standard is assigned to whole structure.
3.5.3 Support conditions
Pinned support is created and assigned to the bottom nodes.
3.5.4 Loads definations and combinations
Here, only dead load case is considered so DL case is defined
and self weight and nodal load of 4kN is assigned to the
model.
3.5.5 Analysis
For analysis finite element software STAAD-PRO is used.
4. RESULTS AND DISCUSSION
4.1 Maximum nodal displacement
Table 1 Maximum nodal deflection in mm
Member
No.
Type 1 Type 2 Type 3 Type 4
1 1.1176 2.3114 302.4124 241.3000
2 1.1938 0.7366 235.6866 243.3574
3 0.9144 2.0828 199.5678 205.5114
4 0.5588 4.0386 214.4268 194.8688
5 0.4318 5.2578 194.3862 183.3118
6 0.8636 5.6896 144.4498 113.0300
7 1.2700 5.4356 114.7064 98.7806
8 1.6256 4.5974 110.3630 154.7876
9 1.8542 3.2766 114.6302 167.1574
10 1.9558 1.6256 87.5538 162.1790
11 1.8796 1.6256 87.5538 170.2054
12 1.6764 3.2512 114.6556 156.9974
13 1.3462 4.5720 110.3884 141.4018
14 0.9398 5.4356 114.7318 112.014
15 0.5080 5.6896 144.4752 135.4328
16 0.5080 5.2578 194.3862 203.6064
17 0.8382 4.0386 214.4268 208.5848
18 1.1176 2.0828 199.5678 219.075
19 1.0668 0.7620 235.6866 245.7958
20 1.0000 2.4130 302.4124 241.3000
Graph 1 Maximum nodal deflection
Above graph shows that square on square (type 1) and
latticed structure (type 2) geometry is stable having almost
negligible nodal deflections. While, type 3 and type 4
geometries i.e., diagonal on diagonal and square on diagonal
have large nodal deflections.
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 06 Issue: 05 |May 2019 www.irjet.net p-ISSN: 2395-0072
© 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 7183
4.2 Maximum axial forces in members
Table 2 Maximum axial force in kN
Membe
r No.
Type 1 Type 2 Type 3 Type 4
1 -11.859 -4.0645 -4.02946 -6.6002
2 -16.7115 -14.198 -7.5893 -6.6902
3 -15.9881 -17.8071 -11.4203 -10.518
4 -11.2538 -16.3102 2.49055 2.74696
5 -4.00375 -11.1746 -0.80748 -0.54851
6 4.32688 -3.84741 18.0204 20.0548
7 12.3935 4.31984 15.6291 17.6653
8 19.1006 12.1052 30.8225 35.7392
9 23.5980 18.5155 29.5624 34.4794
10 25.3465 22.8017 34.1503 41.3263
11 25.5832 22.8017 34.1503 41.3275
12 24.1528 18.5156 29.5626 32.6525
13 20.1700 12.1054 30.8227 33.9137
14 13.8974 4.3197 15.6292 15.2432
15 6.14695 -3.84753 18.0204 17.6329
16 -2.01009 -11.1753 -0.80798 -2.88158
17 -9.27413 -16.3103 2.49005 0.41250
18 -14.2011 -17.8057 -11.419 -10.6332
19 -15.2925 -14.1966 -7.58801 -6.80682
20 -11.0393 -4.07153 -4.02946 -6.60682
Graph 2 Maximum axial load
Chart 2: Maximum axial forces in members
Above graph clearly illustrates that, in barrel vault truss as
we go from support to central peak axial forces goes on
increasing. Here, square on square(type 1) and latticed
truss(type 2) shows less axial force as compared to diagonal
on diagonal(type 3) and square on diagonal(type 4).
5. CONCLUSIONS
From modeling and analysis of different types of double
layer barrel vault truss the following conclusionsaredrawn.
1. The square on square and latticed truss geometries
shows very less nodal deflections.
2. variation in axial forces in diagonal on diagonal and
square on square geometries is nearly 63%
3. The square on square geometry (type 1) and
latticed truss (type 2) has minimum deflection and
axial forces. Hence they are optimun.
ACKNOWLEDGEMENT
I extend my sincerest gratitude to my parents, my Guides,
head of program, head of dept., and my well-wishers who
helped me in all situations whenever needed during this
project completion.
REFERENCES
[1] Balkanlou V. Sadeghi, Karimi M. Reza Bagerzadeh,
Azar B. Bagheri, and Alaeddin Behravesh (2013)
"Evaluating effects of viscous dampers on,, Camp,
Charles V. "Design of space trusses using Big
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Structural Engineering133, no. 7 (2007):999-1008.
[2] Camp, Charles V., and Barron J. Bichon. "Design of
space trusses using ant colony
optimization." Journal of Structural
Engineering 130, no. 5 (2004): 741-751.
[3] Dizangian, Babak, and Mohammad Reza Ghasemi.
"Border-search and jump reduction method for
size optimization of spatial truss
structures." Frontiers of Structural and Civil
Engineering: 1-12.
[4] Grande, Ernesto, Maura Imbimbo, and Valentina
Tomei. "Role of global buckling in the
optimization process of grid shells: Design
strategies." Engineering Structures 156 (2018):
260-270.
[5] Grigorian, Mark. "Performance control for
efficient design of double-layer grids under
uniform loading." International Journal of
Advanced Structural Engineering (IJASE) 6, no. 1
(2014): 52.
[6] Kaveh, A., and M. Moradveisi. "Size and Geometry
Optimization of Double-Layer Grids Using CBO
and ECBO Algorithms." Iranian Journal of Science
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 06 Issue: 05 |May 2019 www.irjet.net p-ISSN: 2395-0072
© 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 7184
and Technology, Transactions of Civil
Engineering 41, no. 2 (2017): 101-112.
[7] Kaveh, A., and S. Mahjoubi. "Optimum Design of
Double-layer Barrel Vaults by Lion Pride
Optimization Algorithm and a Comparative
Study." In Structures, vol. 13, pp. 213-229.Elsevier,
2018.
[8] Li, Lei, and Kapil Khandelwal. "Topology
optimization of geometrically nonlinear trusses
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Salajegheh, and Mohammad Javad Fadaee.
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[10] Shin, Jiuk, Kihak Lee, Gee-Cheol Kim, Chan-Woo
Jung, and Joo-Won Kang. "Analytical and
experimental studies on seismic behavior of
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113-125.
[11] Arnout, Saartje, Geert Lombaert, Geert Degrande,
and Guido De Roeck. "The optimal design of a
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[12] Roudsari, M. Tahamouli, M. Gordini, H.Fazeli,andB.
Kavehei. "Probability analysis of double layer
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simultaneously." International Journal of Steel
Structures 17, no. 3 (2017): 939-948.
[13] Sheidaii, M. R., S. Bayrami, and M. Babaei. "Collapse
behavior of single-layer space barrel vaults
under non-uniform support
settlements." International Journal of Steel
Structures13, no. 4 (2013): 723-730.
BIOGRAPHIES
Miss. Sayali S. Jadhav , PG Student,
M.Tech, Structural Engineering, at
Rajarambapu Institute of
Technology, Rajaramnagar.
Graduated from Savitribai Phule
Pune University, Pune.
Dr.P.S.Patil is presently workingas
HOP Structural engg. Department
at Rajarambapu Institute of
Technology, Rajaramnagar.

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IRJET- A Study on the Behaviour of Double Layer Steel Braced Barrel Vaults

  • 1. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 05 |May 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 7180 A Study on the Behaviour of Double Layer Steel Braced Barrel Vaults Sayali Jadhav1, Dr. P.S. Patil2 1M. Tech. student, Dept. of Civil-structural Engineering, RIT, Maharashtra, India 2Professor, Dept. of Civil-structural Engineering¸ RIT, Maharashtra, India ---------------------------------------------------------------------***---------------------------------------------------------------------- Abstract –The computer analysis of Double Layer steel braced barrel vault is presented. In this work four types of geometries of double layer braced barrel vault trusses are modeled and their behavior is studied. Axial force and deflection for top layer are compared and best geometry is suggested. Modeling and analysis is done using finite element software STAAD-PRO. Key Words: Modeling, Double layer grid geometries, behaviour, axial forces, deflection, STAAD-PRO. 1. INTRODUCTION 1.1 Introduction The braced double layer barrel vaultiscomposedofmember elements arranged on a cylindrical surface. The basic curve is a circular segment; occasionally, a parabola, ellipse or funicular line may also be used. Double-layer grids, or flat surface space frames, consist of two planar networks of members forming top and bottom-layers parallel to each other and interconnected by vertical and inclined web members. Double-layer grids are characterized by pinned joints with no moment or torsional resistance; therefore, all members can only resist tension or compression. Several types of double-layer grids can be formed by these basic elements. They are developed by varying thedirectionofthe top and bottom-layers with respect to eachotherandalsoby the positioning of the top-layer nodal points with respect to the bottom- layer nodal points. Additional variations can be introduced by changing the size of the top-layer grid with respect to the bottom-layer grid. Thus,internal openingscan be formed by omitting every second element in a normal configuration. Fig 1 Double layer steel braced barrel vault structure 2. Study of behaviour of double layer barrel vaults. The structural behavior of double layer grid steel braced barrel vaults depends on the various factors such as type of patterns used for the geometry formation, types of support, aspect ratio, type of connection used at the joint, Type of sections, material used, type of bracings etc To study the behavior of double layer grid steel braced barrel vaults,4 different types of geometric patterns are modeled and analyzed in Staad pro software and results for maximum nodal deflection and axial forces in members for particular group of elements are compared. 2.1 Common types of geometries used in double layers Fig. 2 Different types of geometries.
  • 2. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 05 |May 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 7181 Alsodepending ontheir behaviortheycanbeclassifiedaslong shells and short shells and it can be explained from L/R ratio where L is the distance between the supports in longitudinal direction and R is the radius of curvature of the transverse curve. 1) Beam action - . If the distance between the supports is long andusually edgebeamsareused in thelongitudinaldirection, the primary response will be beam action. For 1.67 < L/R< 5 , the barrel vaults arecalledlongshells,whichcanbevisualized as beams with curvilinear cross-sections. If L/R>3, beam theorywithlinear stress distributioncanbeappliedforbarrel vaultswithuniformcrosssectionandunderuniformloading.. This class of barrel vault will have longitudinal compressive stresses near the crown of the vault, longitudinal tensile stresses towards the free edges, and shear stresses towards the supports. 2) Arch action - When distance between supports goes on decreasing i.e when 0 . 25< L/R >1.67 , then the primary response will be arch action in the transverse direction. Then the barrel vaults are called short shells. Their structural behavior is rather complex and dependent on their geometrical proportions. The force distribution in the longitudinal direction is no longer linear, but in a curvilinear manner, trusses or arches are usually used as the transverse supports. 3) Parallel arches – When L/R ratio becomes very small i.e., <25, theforcesare carried directly in thetransversedirection to the edge supports. Displacement in the radial direction is resisted by circumferential bending stiffness. Such type of barrel vault can be applied to buildings such as airplane hangars or gymnasia where the wall and roof are combined together 3. MODELLING AND ANALYSIS 3.1Geometric details of models  Span - 30m  Height - 15m  Length – 30m  Span to height ratio - 2  No of divisions - 20  Size of module – 2.355m 3.2 Data used for analysis  Type of section – pipe  Size of section – PIP483L-48.3mm-2.9mm  Loading – 1)self weight (from software) 2) DL – 4kN (Nodal load) 3.3 Types of geometries considered for study  Square on square  Lattice structure (Two way grid)  Diagonal on diagonal  Square on diagonal 3.4 Modelling and analysis of barrel vault structures in STAAD pro. In this section the modelling and analysis of barrel vault structure in STAAD pro is explained in brief. The steps followed are also explained. 3.5Types of geometries created in STAAD Pro 1) Square on Square Fig. 3 Square on square geometry 2)Lattice structure (Two way grid) Fig. 4 Two way grid geometry
  • 3. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 05 |May 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 7182 3) Diagonal on diagonal Fig. 5 Diagonal on Diagonal geometry 4) Square on diagonal Fig. 6 Square on diagonal geometry 3.5.2 Material properties and section assignment After modelling next part is creating and assigning material and section properties. Steel material having young's modulus 2x10^5 N/mm^2 and poisons ratio 0.3 is created and assigned. Then circular steel pipe section of Indian standard is assigned to whole structure. 3.5.3 Support conditions Pinned support is created and assigned to the bottom nodes. 3.5.4 Loads definations and combinations Here, only dead load case is considered so DL case is defined and self weight and nodal load of 4kN is assigned to the model. 3.5.5 Analysis For analysis finite element software STAAD-PRO is used. 4. RESULTS AND DISCUSSION 4.1 Maximum nodal displacement Table 1 Maximum nodal deflection in mm Member No. Type 1 Type 2 Type 3 Type 4 1 1.1176 2.3114 302.4124 241.3000 2 1.1938 0.7366 235.6866 243.3574 3 0.9144 2.0828 199.5678 205.5114 4 0.5588 4.0386 214.4268 194.8688 5 0.4318 5.2578 194.3862 183.3118 6 0.8636 5.6896 144.4498 113.0300 7 1.2700 5.4356 114.7064 98.7806 8 1.6256 4.5974 110.3630 154.7876 9 1.8542 3.2766 114.6302 167.1574 10 1.9558 1.6256 87.5538 162.1790 11 1.8796 1.6256 87.5538 170.2054 12 1.6764 3.2512 114.6556 156.9974 13 1.3462 4.5720 110.3884 141.4018 14 0.9398 5.4356 114.7318 112.014 15 0.5080 5.6896 144.4752 135.4328 16 0.5080 5.2578 194.3862 203.6064 17 0.8382 4.0386 214.4268 208.5848 18 1.1176 2.0828 199.5678 219.075 19 1.0668 0.7620 235.6866 245.7958 20 1.0000 2.4130 302.4124 241.3000 Graph 1 Maximum nodal deflection Above graph shows that square on square (type 1) and latticed structure (type 2) geometry is stable having almost negligible nodal deflections. While, type 3 and type 4 geometries i.e., diagonal on diagonal and square on diagonal have large nodal deflections.
  • 4. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 05 |May 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 7183 4.2 Maximum axial forces in members Table 2 Maximum axial force in kN Membe r No. Type 1 Type 2 Type 3 Type 4 1 -11.859 -4.0645 -4.02946 -6.6002 2 -16.7115 -14.198 -7.5893 -6.6902 3 -15.9881 -17.8071 -11.4203 -10.518 4 -11.2538 -16.3102 2.49055 2.74696 5 -4.00375 -11.1746 -0.80748 -0.54851 6 4.32688 -3.84741 18.0204 20.0548 7 12.3935 4.31984 15.6291 17.6653 8 19.1006 12.1052 30.8225 35.7392 9 23.5980 18.5155 29.5624 34.4794 10 25.3465 22.8017 34.1503 41.3263 11 25.5832 22.8017 34.1503 41.3275 12 24.1528 18.5156 29.5626 32.6525 13 20.1700 12.1054 30.8227 33.9137 14 13.8974 4.3197 15.6292 15.2432 15 6.14695 -3.84753 18.0204 17.6329 16 -2.01009 -11.1753 -0.80798 -2.88158 17 -9.27413 -16.3103 2.49005 0.41250 18 -14.2011 -17.8057 -11.419 -10.6332 19 -15.2925 -14.1966 -7.58801 -6.80682 20 -11.0393 -4.07153 -4.02946 -6.60682 Graph 2 Maximum axial load Chart 2: Maximum axial forces in members Above graph clearly illustrates that, in barrel vault truss as we go from support to central peak axial forces goes on increasing. Here, square on square(type 1) and latticed truss(type 2) shows less axial force as compared to diagonal on diagonal(type 3) and square on diagonal(type 4). 5. CONCLUSIONS From modeling and analysis of different types of double layer barrel vault truss the following conclusionsaredrawn. 1. The square on square and latticed truss geometries shows very less nodal deflections. 2. variation in axial forces in diagonal on diagonal and square on square geometries is nearly 63% 3. The square on square geometry (type 1) and latticed truss (type 2) has minimum deflection and axial forces. Hence they are optimun. ACKNOWLEDGEMENT I extend my sincerest gratitude to my parents, my Guides, head of program, head of dept., and my well-wishers who helped me in all situations whenever needed during this project completion. REFERENCES [1] Balkanlou V. Sadeghi, Karimi M. Reza Bagerzadeh, Azar B. Bagheri, and Alaeddin Behravesh (2013) "Evaluating effects of viscous dampers on,, Camp, Charles V. "Design of space trusses using Big Bang–Big Crunch optimization." Journal of Structural Engineering133, no. 7 (2007):999-1008. [2] Camp, Charles V., and Barron J. Bichon. "Design of space trusses using ant colony optimization." Journal of Structural Engineering 130, no. 5 (2004): 741-751. [3] Dizangian, Babak, and Mohammad Reza Ghasemi. "Border-search and jump reduction method for size optimization of spatial truss structures." Frontiers of Structural and Civil Engineering: 1-12. [4] Grande, Ernesto, Maura Imbimbo, and Valentina Tomei. "Role of global buckling in the optimization process of grid shells: Design strategies." Engineering Structures 156 (2018): 260-270. [5] Grigorian, Mark. "Performance control for efficient design of double-layer grids under uniform loading." International Journal of Advanced Structural Engineering (IJASE) 6, no. 1 (2014): 52. [6] Kaveh, A., and M. Moradveisi. "Size and Geometry Optimization of Double-Layer Grids Using CBO and ECBO Algorithms." Iranian Journal of Science
  • 5. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 05 |May 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 7184 and Technology, Transactions of Civil Engineering 41, no. 2 (2017): 101-112. [7] Kaveh, A., and S. Mahjoubi. "Optimum Design of Double-layer Barrel Vaults by Lion Pride Optimization Algorithm and a Comparative Study." In Structures, vol. 13, pp. 213-229.Elsevier, 2018. [8] Li, Lei, and Kapil Khandelwal. "Topology optimization of geometrically nonlinear trusses with spurious eigenmodes control." Engineering Structures 131 (2017): 324-344. [9] Mashayekhi, Mostafa, Eysa Salajegheh, Javad Salajegheh, and Mohammad Javad Fadaee. "Reliability-based topology optimization of double layer grids using a two-stage optimization method." Structural and Multidisciplinary Optimization 45, no. 6 (2012): 815-833. [10] Shin, Jiuk, Kihak Lee, Gee-Cheol Kim, Chan-Woo Jung, and Joo-Won Kang. "Analytical and experimental studies on seismic behavior of double-layer barrel vault systemswith different open angles." Thin-Walled Structures 54 (2012): 113-125. [11] Arnout, Saartje, Geert Lombaert, Geert Degrande, and Guido De Roeck. "The optimal design of a barrel vault in the conceptual design stage." Computers & Structures 92 (2012): 308- 316. [12] Roudsari, M. Tahamouli, M. Gordini, H.Fazeli,andB. Kavehei. "Probability analysis of double layer barrel vaults considering the effect of initial curvature and length imperfections simultaneously." International Journal of Steel Structures 17, no. 3 (2017): 939-948. [13] Sheidaii, M. R., S. Bayrami, and M. Babaei. "Collapse behavior of single-layer space barrel vaults under non-uniform support settlements." International Journal of Steel Structures13, no. 4 (2013): 723-730. BIOGRAPHIES Miss. Sayali S. Jadhav , PG Student, M.Tech, Structural Engineering, at Rajarambapu Institute of Technology, Rajaramnagar. Graduated from Savitribai Phule Pune University, Pune. Dr.P.S.Patil is presently workingas HOP Structural engg. Department at Rajarambapu Institute of Technology, Rajaramnagar.