- Open Access
- Total Downloads : 241
- Authors : E Madhu Babu, Srikanth Sikhakolli, S Srinivasa Prasad
- Paper ID : IJERTV3IS091027
- Volume & Issue : Volume 03, Issue 09 (September 2014)
- Published (First Online): 29-09-2014
- ISSN (Online) : 2278-0181
- Publisher Name : IJERT
- License: This work is licensed under a Creative Commons Attribution 4.0 International License
Analysis of Space Launch Vehicle
A Coupled Field Analysis
E. Madhu Babu
-
G. student, Aerospace Engineering
MLR Institute of Technology Hyderabad, India
Srikanth Sikhakolli Post Graduate, Aerospace Engineering
MLR Institute of Technology Hyderabad, India
Dr. S. Srinivasa Prasad Professor & Head, Department of Aeronautical Engineering
MLR Institute of Technology Hyderabad, India
Abstract Space launch vehicles are manufactured by thin metallic or composite shells. Such shells are vulnerable and prone to buckling due to internal pressures produced because of the combustion process of the solid propellant. The first stage of GSLV III solid booster stage is considered for the analysis. The cylinder will be modeled as an orthotropic cylinder and various thickness and orientations will be checked for the cylinder weather it can with stand those loads. Mathematical calculation will be used to calculate the appropriate thickness of each layer for orthotropic cylinder. Finite element analysis tool ANSYS 14.5 will be used to calculate the results for doing the static and buckling analysis.
Keywords Space launch vehicle ; Coupled field analysis; ANSYS; APDL.
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INTRODUCTION
Cylindrical shells are structures which find uses in a large number of applications. In the aerospace field, they are used extensively as rocket bodies and aircraft fuselage. As designers look for methods of further reducing the weight of such shell structures, fibre reinforced composite materials are finding wider usage [1]. Because of the thinness of these structures, buckling is often the controlling failure mode. It is therefore essential that their buckling behaviour be properly understood so that suitable design methods can be established
[2].In India, the launch vehicles development program began in the early 1970s. The first experimental Satellite Launch Vehicle (SLV-3) was developed in 1980. An Augmented version of this, ASLV, was launched successfully in 1992. India has made tremendous strides in launch vehicle technology to achieve self-reliance in satellite launch vehicle program with the operationalization of Polar Satellite Launch Vehicle (PSLV) and Geosynchronous Satellite Launch Vehicle (GSLV).
Figure 1. Launch vehicle family of INDIA
The primary objective of this paper is to do the optimum thickness calculations for the considered model of GSLV MK III space launch vehicle and apply the thermal as well as structural loads and study the behavior of the cylindrical shell. It is of interest to examine the behavior of the proposed launch vehicle models under thermal loads and internal pressure loading. The outer cases of launch vehicle are considered as orthotropic (composite) cylindrical shells. They are the main structures of interest in the stability analyses. ANSYS Parametric Design Language (APDL) will be used to compare the results for different thicknesses and lay-ups.
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OPTIMUM THICKNESS CALCULATIONS
The formula for calculating the optimum thickness based on the applied loading and radius is
Where,
P Applied pressure
R – Radius of the cylinder
Poissons ratio in XY and YZ directions respectively
EY Youngs modulus in Y direction
Figure 2. Multi-layered orthotropic cylindrical shell geometry
If we calculate the thicknesses for other ply- orientations with an applied pressure of 0.6 MPa [4], we are going to get the following values
Ply orientation
90
+10
-10
90
90
+45
-45
90
90
+85
-85
90
Modulus [Ey]
95753.26495
114752.4135
158831.1435
Thickness [t]
46.55955
43.83348
39.33218
Table-1 Thickness values for Different Ply-Orientations (P=0.6 MPa)
Similarly, if we calculate the thicknesses for other ply-orientations with an applied pressure of 6.2 MPa, we are going to get the following values
Ply orientation
90
+10
-10
90
90
+45
-45
90
90
+85
-85
90
Modulus [Ey]
95753.26495
114752.4135
158831.1435
Thickness [t]
101.41
95.47
85.67
Table-2Thickness values for Different Ply-Orientations (P=6.2 MPa)
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METHODOLOGY
The re-usable large solid booster of GSLV MK-III is modeled as an orthotropic cylinder. The formula for calculating the optimum thickness is provided in the previous session. The material properties of these composites are shown in the table 1.
S. NO.
Parameter
Value
1
EX
120000
2
EY
9000
3
EZ
9000
4
PRXY
0.25
5
PRYZ
0.32
6
PRXZ
0.25
7
GXY
3580
8
GYZ
4500
9
GXZ
3580
10
KXX
7e-3
11
DENS
1.7e-6
12
ALPX
2e-6
Table-3: Material Properties of CFRP
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FINITE ELEMENT MODELLING AND ANALYSIS
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Modeling
Outer radius = 1600 mm
Inner radius = 1249.36 mm
Length = 22000 mm
1
No. of layers = 4
VOLUMES TYPE NUM
JUN 8 2014
19:44:41
YZ X
Figure-3. Geometry of cylinder
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Analysis
Y
X
Z
Y
X
Z
The thermal and static analysis is done on the composite cylinder by applying composites. The thermal analysis is done by applying temperature of 1804 k on inner layers. The results obtained in the thermal analysis are applied for the space capsule in structural analysis and an internal pressures of 0.6 and 6.2 MPa are applied simultaneously.
1
V-A-E-L-K-N
JUN 8 2014
20:10:03
Y1Y1
X
Z
Figure-4: Applied Boundary Conditions
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RESULTS AND DISCUSSION
MN
1
The below figure shows the results of the nodal solution for the displacement vector sum and von-mises stress.
NODAL SOLUTION
STEP=1 SUB =1 TIME=1
USUM (AVG) RSYS=0
DMX =10.0997
SMX =10.0997
JUN 25 2014
13:06:13
MX
Y
11
Z X
0
1.12219 3.36656 5.61094 7.85531 10.0997
8.9775
6.73312
4.48875
2.24437
Figure-5: Displacement Vector sum for P = 0.6 MPa
Figure-6 Displacement vector sum vs. length of the cylinder
graph
NODAL SOLUTION
STEP=1 SUB =1 TIME=1
JUN 25 2014
13:12:46
DMX =10.0997
SMN =21.168
SMX =301.312
Y
11
Z MX X
21.168
52.2951 114.549 176.803 239.057 301.312
270.185
207.93
145.676
<>83.4221MN
(AVG)
SEQV
1
Figure-7 Von-mises stress for P=0.6 MPa
Figure-8 Vonmises stress Vs. length of the cylinder
The above results shows the displacement vector sum and von-mises stresses result. Figures 6 & 8 are showing the comparison for different lay-ups for the same applied load. The coupled field analysis results are tabulated in the below tables.
Applied pressure
(MPa)
0.6
Thickness (mm)
46.55
(90/10/-10/90)
43.83
(90/45/-45/90)
39.33
(90/85/-85/90)
Maximum
Displacement (mm)
11.5406
10.0997
10.7876
Maximum
Vonmises stress (MPa)
474.211
301.312
188.24
Table-4 Comparison of results between different orientations for P=0.6 MPa
Applied pressure
(MPa)
6.2
101.41
95.47
85.67
Thickness (mm)
(90/10/-
(90/45/-
(90/85/-
10/90)
45/90)
85/90)
Maximum
Displacement (mm)
11.0958
9.9479
12.316
Maximum Equivalent
stress (MPa)
640.812
489.059
340.288
Table-5 Comparison of results between different orientations for P=6.2MPa
From the results we can say that, as per the stiffness criterion the 90/45/-45/90 lay-up is best suitable. But as per the strength criterion, the 90/85/-85/90 lay-up is suitable. On the over-all consideration the 90/45/-45/90 lay-up is best suited for all kind of loading conditions.
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CONCLUSION
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Based on the results that we got from the analysis the following conclusions have been drawn:
-
The Composite cylinder designed is meeting the stipulated internal pressure. The procedure followed has worked out to be efficient in accurately predicting the structural response of composite components.
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It meets all the desired functional requirements.
REFERENCES
-
Jonathan E. Rich, Design Optimization Procedure for Monocoque Composite Cylinder Structures Using Response Surface Techniques,
September 12, 1997 Blacksburg, VA
-
Jin Guang Teng,Buckling of thin shells: Recent advances and trends
American Society of Mechanical Engineers, 1996
-
Reissner. E.,On the theory of bending of elastic plates, J. Math. Phys.,23, 1944.
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John. T. Dorsey, Structural analysis of the space shuttle solid rocket booster attached ring, NASA Technical Memorandum 100510, 1988.