Buckling of laminated beam higher order discrete model-main
Thesis presentation
1. Analysis of Elastic Behaviour of Honeycombs and
Auxetic Materials with Variation in its Cell Geometry
MS THESIS PRESENTED BY
VISHWATEJ MANE
ADVISOR- PROF. MAEN ALKHADER
DEPARTMENT OF MECHANICAL ENGINEERING
STONY BROOK UNIVERSITY
2. Introduction
Honeycombs used as core in sandwich panels of lightweight structure
Progressive collapse with retaining functionality
Auxetic materials exhibits NPR
Auxetic material has improved Shear, indentation resistance and fracture toughness
Potential applications in defense and aerospace
Relative density
Outline of the study
3. Deformation mechanism and Theory
Flexure, stretching and hinging mechanism
Cell Geometry and General Mathematical model
“ I.G. Masters and K E Evans, ”Models for the elastic deformation of honeycombs”, composite
strucutres,0263-8223/96
5. FEA Model development
Development of Geometry for different cellular models
In Property module used Al 6061 as material
ρ=2700 kg/m3, E= 68950 MPa, ν= 0.3, plastic strain
Static, general analysis type
meshing - structured Quad shell elements (S4R)
Node Sets- TOP, BOTTOM, LEFT, RIGHT
6. BCs for Poisson’s ratio ν21
Hex30 model
U3=0
Bottom, U2=UR1=UR2=UR3=0
Top, UR1=UR2=UR3=0
U2= -2.5
7. BCs for Poisson’s ratio ν12
Hex30 model
U3= 0
LEFT, U1=UR1=UR2=UR3=0
RIGHT, UR1=UR2=UR3=0
U1= -2.5
8. FEA results and Trends for Honeycombs
Hex 30, t= 0.25mm Hex 10, t=0.3mm
9. Stress 22, Young’s Modulus E22 and Poisson’s ratio ν21 vs. Strain 22 for Hex05 model and Hex10 model
10. Stress 22, Young’s Modulus E22 and Poisson’s ratio ν21 vs. Strain 22 for Hex20 model and Hex30 model
11. FEA Results and Trends for Auxetics
Hex -05, t= 0.2mm Hex -10, t= 0.15mm
12. Stress 22, Young’s Modulus E22, Poisson’s ratio ν21 vs. Strain 22 for Hex-05 model and Hex-10 model
13. Stress 22, Young’s Modulus E22 and Poisson’s ratio ν21 vs. Strain 22 curve for Hex -20 model
14. FEA Results and Trends in honeycombs 11 direction
Hex30, t=0.3mm Hex20, t=0.25mm
15. Stress 11, Young’s Modulus E11 and Poisson’s ratio ν12 vs. Strain 11 for Hex 05 model and Hex10
model
16. Stress 11, Young’s Modulus E11 and Poisson’s ratio ν12 vs. Strain 11 for Hex20 model and Hex30
model
17. FEA Results and Trends in Auxetics
Hex-05, t=0.2mm Hex-10, t=0.15mm
18. Stress 11, Young’s Modulus E11 Poisson’s ratio ν12 vs. Strain 11 for Hex -05 model and Hex-10 model
19. Stress 11, Young’s Modulus E11 and Poisson’s ratio ν12 vs. Strain for Hex-20 model
20. Specifications of 3D printed models
MakerBot Replicator 2.0 3D printer
Sr No. Model by cell angle geometry
(wall thickness= 0.8mm)
Constant width= 15mm
Length
in mm
Height
in mm
1 -20 28.33 27.85
2 -10 24.94 25.45
3 -5 24.12 24.35
4 5 24.15 26.02
5 10 29.63 28.69
6 20 28.02 25.94
7 30 26.38 27.54
21. 3D printed Honeycombs test results
Stress vs Strain curves over entire period of compression test on MTS machine
0
5
10
15
20
25
0 0.1 0.2 0.3
StressY
Strain Y
Hex 05
0
2
4
6
8
10
12
14
16
18
0 0.05 0.1 0.15 0.2 0.25
StressY
Strain Y
Hex 10
0
1
2
3
4
5
6
7
0 0.1 0.2 0.3
StressY
Strain Y
Hex 20
0
1
2
3
4
5
6
7
8
0 0.1 0.2 0.3
StressY
Strain Y
Hex 30
37. Conclusions for honeycomb samples
FEA methods can be used to predict trends in elastic constants
E22 and E11 increases with increase in relative density
E22 increases with decrease in cell angle closer to zero
E11 increases with increase in angle closer to 30 degrees
Trends of ν21 and ν12 are linear and independent of relative density in elastic region
ν21 increase with decrease in cell angle closer to 0
ν12 increases with increase in cell angle closer to 30
Waviness in stress vs. strain trend in plastic region represents cell arrays collapse
38. Conclusions for Auxetic samples
E22 and E11 increases with relative density
Exhibits Negative Poisson’s ratio (NPR) property
Trends ν21 and ν12 independent of relative density in elastic region
ν21 increases with decrease in cell angle
ν12 decreases with increase in cell angle
Waviness in stress, Poisson’s ratio vs. strain trends represents cell arrays collapse
39. Young’s modulus 22 vs. cell angle
0
5000
10000
15000
20000
25000
30000
5 10 20 30 -5 -10 -20
Young'sModulusE22
Cell angle in degrees
t=0.15 mm t= 0.2 mm t= 0.25 mm t=0.3 mm
40. Poisson’s ratio 21 vs. cell angle
-6
-4
-2
0
2
4
6
5 10 20 30 -5 -10 -20
Poisson'sratioν21
Cell angle in degrees
t=0.15 mm t=0.2 mm t=0.25 mm t=0.3 mm
41. Young’s modulus 11 vs cell angle
0
500
1000
1500
2000
2500
3000
3500
5 10 20 30 -5 -10 -20
Young'sModulusE11
cell angles in degrees
t=0.15 mm t=0.2 mm t=0.25 mm t=0.3 mm
42. Poisson’s ratio12 vs cell angle
-0.4
-0.2
0
0.2
0.4
0.6
0.8
1
1.2
5 10 20 30 -5 -10 -20
Poisson'sratioν12
Cell angles in degrees
t=0.15 mm t=0.2 mm t=0.25 mm t=0.3 mm
43. Bibliography
I.G. Masters and K E Evans, “ Models for the elastic deformation of honeycombs”
composite structures,0263-8223/96
Q.Liu,” Literature Review: Material with Negative Poisson’s ratio and potential
applications to aerospace and defence” DSTO-GD-0472, August 2006
Yanping Liu and Hong Hu, “ A Review on Auxetic structures and polymeric materials”,
ISSN 1992-2248, May 2010
M. Bianchi, S. Frontoni, F. Scarpa, and C.W.Smith, “Density change during the
manufacturing process of PU-PE open cell Auxetic foams”, pssb.201083966, May 2010
Kim Alderson, Andrew Alderson, Naveen Ravirala, Virginia Simkins, and Philip Davies,
“Manufacture and characterization of thin flat and curved Auxetic foam sheets”,
pssb.201084215, March 2012