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IJREAT International Journal of Research in Engineering & Advanced Technology, Volume 3, Issue 1, Feb-Mar, 2015
ISSN: 2320 – 8791 (Impact Factor: 1.479)
www.ijreat.org
www.ijreat.org
Published by: PIONEER RESEARCH & DEVELOPMENT GROUP (www.prdg.org) 158
Finite ElementAnalysis of Payload for SpaceApplicationFinite ElementAnalysis of Payload for SpaceApplicationFinite ElementAnalysis of Payload for SpaceApplicationFinite ElementAnalysis of Payload for SpaceApplicationssss
Pranav Mahamuni1
, Amol Kamthe2
, Rohit Cholke3
,
Sachin Velapure4
, Yash Parikh5
1, 2, 3, 4
Department of Mechanical Engineering, Sinhgad Institute of Technology and Science,
Pune, Maharashtra, India.
5
Department of Mechanical Engineering, Symbiosis Institute of Technology,
Pune, Maharashtra, India.
Abstract
For aircraft or launch vehicles, its carrying capacity is defined as
a Payload. It is usually measured in weights. For a rocket,
payload can be satellite or scientific instruments. The design of
the payload is a challenging task as it has to withstand space
environment and launch loads. Due to launch vibrations, there
are possibilities of failure of design of payload so it is very
important to reduce these vibrations by alternative techniques.
This paper studies the effect of different materials on the natural
frequency of payload which helps in the reduction of the natural
frequency of the payload and for safe functioning of satellite.
Keywords: Payload, Satellite, Launch Loads, Natural
frequency.
1. Introduction
Mechanical vibrations into the system can cause many
problems resulting in degradation of sensitive systems [1].
The static and dynamic unbalanced forces of rotary
equipments placed near payloads generate vibrations
which affect the pointing of precision payloads and devices
in space platforms [2]. In a Spacecraft, vibrations are
produced by on board equipments such as boosters,
electric motors, reaction wheels. They propagate through
the satellite structure towards payloads. Due to these
vibrations, there are possibilities of failure of the payload
due to fatigue stresses. So it becomes necessary payload to
withstand these vibrations so as to avoid the structural
failure of the payload.
The natural frequency of a payload changes with the
change in material [3], it becomes necessary to choose
such a material which will itself damp the vibrations and
also be light in weight so that it will reduce the payload
mass. As mass plays an important role in payload carrying
capacity of a space craft, it is necessary to reduce the mass
of a payload. With the reduction in the mass the propulsive
thrust required at the time of a launch is reduced thus
reducing the fuel for combustion.
In this article, Finite Element Analysis has been done to
see the effect of change in natural frequency as a result of
change in mass and material.
2. Design Requirements for Payload
Payload should fulfill following design requirements
1. It should have high strength in order to withstand
environmental and launch loads. The range of
Random Vibration is 20 Hz to 2000 Hz [4].
2. The natural frequency of it should be above 100
Hz. It should not couple with spacecraft structure
to avoid resonance [5].
3. The mass of the payload should be low to reduce
the fuel consumption or to increase the payload
carrying capacity of spacecraft.
3. Design of Payload
For aircraft or launch vehicles, its carrying capacity is
defined as a Payload. It is usually measured in weights. For
a rocket, payload can be satellite or scientific instruments.
The satellite consists of different subsystems like structural
subsystem, telemetry subsystem, power subsystem, thermal
control subsystem, altitude control subsystem and
communication payload [6].
The scope of this paper is limited to designing of payloads.
As mass plays an important role in the design of the
payload, which directly or indirectly affect the frequency
of the payload. This paper shows the effect of change in
IJREAT International Journal of Research in Engineering & Advanced Technology, Volume 3, Issue 1, Feb-Mar, 2015
ISSN: 2320 – 8791 (Impact Factor: 1.479)
www.ijreat.org
www.ijreat.org
Published by: PIONEER RESEARCH & DEVELOPMENT GROUP (www.prdg.org) 159
different material on frequency because the frequency of
an object changes with change in material.
To study this effect, an arbitrary model of transponder
casing was prepared using CAD software. The overall size
of payload is 250 mm * 175 mm * 122.2 mm (height). Fig.
1 shows the CAD layout of the model.
Fig. 1 CAD layout of the model
4. Simulation through Finite Element
Analysis
4.1 Finite Element Model of Casing (Payload)
Hypermesh has been used for Finite Element Analysis.
Combination of automesh and manual mesh has been taken
with “tria” and “quad” shell elements. Total number of
elements are17161 with 17328 nodes. Total number of
quad elements are 17153 while total number of tria
elements are 8. So, the number of tria elements is less than
5% of total elements. Total number of rigid elements are 4.
Fig. 2 shows the final meshed model.
Fig. 2 Final meshed model
In Fig. 2 different colours has been assigned to different
elements having different thickness. Green, Blue and red
colours have been assigned to elements having thickness
4.3mm, 6mm and 3.6 mm respectively.
4.2 Finite Element Analysis with Aluminium T6-
6061 as a Material
Aluminium T6-6061 has been selected for the model as it
is light in weight and has high strength.
The properties of Aluminium T6-6061 are as follows
Modulus of Elasticity – 70000 N/mm2
Poisson Ration – 0.33
Density – 2.7*10-9
Ton/mm3
After applying the material and properties the mass of the
payload obtain was 1719gm.
Fig. 3 Modal analysis result for first mode
IJREAT International Journal of Research in Engineering & Advanced Technology, Volume 3, Issue 1, Feb-Mar, 2015
ISSN: 2320 – 8791 (Impact Factor: 1.479)
www.ijreat.org
www.ijreat.org
Published by: PIONEER RESEARCH & DEVELOPMENT GROUP (www.prdg.org) 160
Fig. 3 shows the modal analysis result of model for the first
mode with aluminium T6-6061 as a material. The Table 1
shows the next modes obtained from the analysis.
Table 1: Modal analysis result
Mode Frequency (Hz)
1st
269.71
2nd
547.98
3rd
611.61
4th
788.17
5th
941.60
4.3 Finite Element Analysis with Titanium as a
Material
Titanium has been selected for model as it has high
strength, stiffness, toughness and resistance to corrosion.
The properties of Titanium are as follows
Modulus of Elasticity – 120000 N/mm2
Poisson Ration – 0.33
Density – 4.5*10-9
Ton/mm3
After applying the material and properties the mass of the
payload obtain was 2865gm.
Fig. 4 Modal analysis result for first mode
Fig. 4 shows the modal analysis result of model for the first
mode with Titanium as a material. The Table 2 shows the
next modes obtained from the analysis.
Table 2: Modal analysis result
Mode Frequency (Hz)
1st
273.54
2nd
555.75
3rd
620.28
4th
799.35
5th
954.59
4.4 Finite Element Analysis with Epoxy Carbon as a
Material
Epoxy Carbon has been selected for model as it has high
strength to weight ratio. They are extremely strong and
light in weight.
The properties of Epoxy Carbon are as follows
Modulus of Elasticity – 70000 N/mm2
Poisson Ration – 0.3
Density – 1.6*10-9
Ton/mm3
Here the material properties considered are of Epoxy
Carbon sheets. After applying the material and properties
the mass of the payload obtain was 1019gm.
Fig. 5 Modal analysis result for first mode
Fig. 5 shows the modal analysis result of model for the first
mode with Epoxy Carbon as a material. The Table 3 shows
the next modes obtained from the analysis.
IJREAT International Journal of Research in Engineering & Advanced Technology, Volume 3, Issue 1, Feb-Mar, 2015
ISSN: 2320 – 8791 (Impact Factor: 1.479)
www.ijreat.org
www.ijreat.org
Published by: PIONEER RESEARCH & DEVELOPMENT GROUP (www.prdg.org) 161
Table 3: Modal analysis result
Mode Frequency (Hz)
1st
350.36
2nd
711.85
3rd
794.50
4th
1023.87
5th
1223.18
4.5 Comparison of Frequencies for Different
Materials
From Finite Element Analysis, it is observed that natural
frequency modes changes with change in material of the
model. The first mode of the model having Aluminium T6-
6061 as a material is obtained at 269.71 Hz. The first mode
of the model having Titanium as a material is obtained at
273.54 Hz. The first mode of the model having an Epoxy
Carbon as a material is obtained at 35036 Hz.
Fig. 6 shows the comparison of modal analysis results for
different materials.
0
200
400
600
800
1000
1200
1400
Al Ti EC
Frequency(Hz)
Mode 1
Mode 2
Mode 3
Mode 4
Mode 5
Fig. 6 Comparison of frequencies for different materials
From Fig. 6, it can be seen that the first mode frequency
for Aluminium T6-6061 is least while it is maximum for
the Epoxy Carbon.
5. Conclusions
The different results obtained in this paper are hopeful and
from these results, it is clear that change of material lead to
change of frequencies. For these reasons, material
selection plays a vital role in designing of spacecraft
components. It is also observed that Aluminium T6-6061
is a suitable material for designing of payloads. This work
can give a hint for the researchers in the design of payloads.
Acknowledgments
The authors are grateful to Mr. Vinayak Shingare from
Designtech System Ltd., Faculty of Mechanical
Engineering in Sinhagad Institute of Technology and
Science, Pune and Symbiosis Institute of Technology,
Pune for providing support and encouragement for this
paper.
References
[1] R. G. Cobb, J. M. Sullivan, A. Das, L. P. Davis, T. T. Hyde,
T. Davis, Z. H. Rahaman, J. T. Spanos, “Vibration isolation
and suppression system for precision payloads in space”,
Smart Materials and Structures, 8 (1999) pp. 798-812.
[2] D. Kamesh, R. Pandiyan, A. Ghosal, “Modeling, design and
analysis of low frequency platform for attenuating micro-
vibration in spacecraft”, Journal of Sound and Vibration, 329
(2010) pp. 3431-3450.
[3] A. Boudjemai, R. Amri, A. Mankour, H. Salem, M. H.
Bouanane, D. Boutchicha, “Modal analysis and testing of
hexagonal plates used for satellite structural design”,
Materials and Design, 35 (2012) pp. 266-275
[4] Space shuttle program payload bay payload user’s guide,
Johnson space center, Texas, NSTS21492, December 2000,.
[5] D. Shah, V. R. Iyer, A. V. Pathak, “Simulation and
modification of microwave packaging for space
communication payload”, National conference on current
trends in technology, November 2009.
[6] http://www.nasa.gov/

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Finite Element Analysis of Payload for Space Applications

  • 1. IJREAT International Journal of Research in Engineering & Advanced Technology, Volume 3, Issue 1, Feb-Mar, 2015 ISSN: 2320 – 8791 (Impact Factor: 1.479) www.ijreat.org www.ijreat.org Published by: PIONEER RESEARCH & DEVELOPMENT GROUP (www.prdg.org) 158 Finite ElementAnalysis of Payload for SpaceApplicationFinite ElementAnalysis of Payload for SpaceApplicationFinite ElementAnalysis of Payload for SpaceApplicationFinite ElementAnalysis of Payload for SpaceApplicationssss Pranav Mahamuni1 , Amol Kamthe2 , Rohit Cholke3 , Sachin Velapure4 , Yash Parikh5 1, 2, 3, 4 Department of Mechanical Engineering, Sinhgad Institute of Technology and Science, Pune, Maharashtra, India. 5 Department of Mechanical Engineering, Symbiosis Institute of Technology, Pune, Maharashtra, India. Abstract For aircraft or launch vehicles, its carrying capacity is defined as a Payload. It is usually measured in weights. For a rocket, payload can be satellite or scientific instruments. The design of the payload is a challenging task as it has to withstand space environment and launch loads. Due to launch vibrations, there are possibilities of failure of design of payload so it is very important to reduce these vibrations by alternative techniques. This paper studies the effect of different materials on the natural frequency of payload which helps in the reduction of the natural frequency of the payload and for safe functioning of satellite. Keywords: Payload, Satellite, Launch Loads, Natural frequency. 1. Introduction Mechanical vibrations into the system can cause many problems resulting in degradation of sensitive systems [1]. The static and dynamic unbalanced forces of rotary equipments placed near payloads generate vibrations which affect the pointing of precision payloads and devices in space platforms [2]. In a Spacecraft, vibrations are produced by on board equipments such as boosters, electric motors, reaction wheels. They propagate through the satellite structure towards payloads. Due to these vibrations, there are possibilities of failure of the payload due to fatigue stresses. So it becomes necessary payload to withstand these vibrations so as to avoid the structural failure of the payload. The natural frequency of a payload changes with the change in material [3], it becomes necessary to choose such a material which will itself damp the vibrations and also be light in weight so that it will reduce the payload mass. As mass plays an important role in payload carrying capacity of a space craft, it is necessary to reduce the mass of a payload. With the reduction in the mass the propulsive thrust required at the time of a launch is reduced thus reducing the fuel for combustion. In this article, Finite Element Analysis has been done to see the effect of change in natural frequency as a result of change in mass and material. 2. Design Requirements for Payload Payload should fulfill following design requirements 1. It should have high strength in order to withstand environmental and launch loads. The range of Random Vibration is 20 Hz to 2000 Hz [4]. 2. The natural frequency of it should be above 100 Hz. It should not couple with spacecraft structure to avoid resonance [5]. 3. The mass of the payload should be low to reduce the fuel consumption or to increase the payload carrying capacity of spacecraft. 3. Design of Payload For aircraft or launch vehicles, its carrying capacity is defined as a Payload. It is usually measured in weights. For a rocket, payload can be satellite or scientific instruments. The satellite consists of different subsystems like structural subsystem, telemetry subsystem, power subsystem, thermal control subsystem, altitude control subsystem and communication payload [6]. The scope of this paper is limited to designing of payloads. As mass plays an important role in the design of the payload, which directly or indirectly affect the frequency of the payload. This paper shows the effect of change in
  • 2. IJREAT International Journal of Research in Engineering & Advanced Technology, Volume 3, Issue 1, Feb-Mar, 2015 ISSN: 2320 – 8791 (Impact Factor: 1.479) www.ijreat.org www.ijreat.org Published by: PIONEER RESEARCH & DEVELOPMENT GROUP (www.prdg.org) 159 different material on frequency because the frequency of an object changes with change in material. To study this effect, an arbitrary model of transponder casing was prepared using CAD software. The overall size of payload is 250 mm * 175 mm * 122.2 mm (height). Fig. 1 shows the CAD layout of the model. Fig. 1 CAD layout of the model 4. Simulation through Finite Element Analysis 4.1 Finite Element Model of Casing (Payload) Hypermesh has been used for Finite Element Analysis. Combination of automesh and manual mesh has been taken with “tria” and “quad” shell elements. Total number of elements are17161 with 17328 nodes. Total number of quad elements are 17153 while total number of tria elements are 8. So, the number of tria elements is less than 5% of total elements. Total number of rigid elements are 4. Fig. 2 shows the final meshed model. Fig. 2 Final meshed model In Fig. 2 different colours has been assigned to different elements having different thickness. Green, Blue and red colours have been assigned to elements having thickness 4.3mm, 6mm and 3.6 mm respectively. 4.2 Finite Element Analysis with Aluminium T6- 6061 as a Material Aluminium T6-6061 has been selected for the model as it is light in weight and has high strength. The properties of Aluminium T6-6061 are as follows Modulus of Elasticity – 70000 N/mm2 Poisson Ration – 0.33 Density – 2.7*10-9 Ton/mm3 After applying the material and properties the mass of the payload obtain was 1719gm. Fig. 3 Modal analysis result for first mode
  • 3. IJREAT International Journal of Research in Engineering & Advanced Technology, Volume 3, Issue 1, Feb-Mar, 2015 ISSN: 2320 – 8791 (Impact Factor: 1.479) www.ijreat.org www.ijreat.org Published by: PIONEER RESEARCH & DEVELOPMENT GROUP (www.prdg.org) 160 Fig. 3 shows the modal analysis result of model for the first mode with aluminium T6-6061 as a material. The Table 1 shows the next modes obtained from the analysis. Table 1: Modal analysis result Mode Frequency (Hz) 1st 269.71 2nd 547.98 3rd 611.61 4th 788.17 5th 941.60 4.3 Finite Element Analysis with Titanium as a Material Titanium has been selected for model as it has high strength, stiffness, toughness and resistance to corrosion. The properties of Titanium are as follows Modulus of Elasticity – 120000 N/mm2 Poisson Ration – 0.33 Density – 4.5*10-9 Ton/mm3 After applying the material and properties the mass of the payload obtain was 2865gm. Fig. 4 Modal analysis result for first mode Fig. 4 shows the modal analysis result of model for the first mode with Titanium as a material. The Table 2 shows the next modes obtained from the analysis. Table 2: Modal analysis result Mode Frequency (Hz) 1st 273.54 2nd 555.75 3rd 620.28 4th 799.35 5th 954.59 4.4 Finite Element Analysis with Epoxy Carbon as a Material Epoxy Carbon has been selected for model as it has high strength to weight ratio. They are extremely strong and light in weight. The properties of Epoxy Carbon are as follows Modulus of Elasticity – 70000 N/mm2 Poisson Ration – 0.3 Density – 1.6*10-9 Ton/mm3 Here the material properties considered are of Epoxy Carbon sheets. After applying the material and properties the mass of the payload obtain was 1019gm. Fig. 5 Modal analysis result for first mode Fig. 5 shows the modal analysis result of model for the first mode with Epoxy Carbon as a material. The Table 3 shows the next modes obtained from the analysis.
  • 4. IJREAT International Journal of Research in Engineering & Advanced Technology, Volume 3, Issue 1, Feb-Mar, 2015 ISSN: 2320 – 8791 (Impact Factor: 1.479) www.ijreat.org www.ijreat.org Published by: PIONEER RESEARCH & DEVELOPMENT GROUP (www.prdg.org) 161 Table 3: Modal analysis result Mode Frequency (Hz) 1st 350.36 2nd 711.85 3rd 794.50 4th 1023.87 5th 1223.18 4.5 Comparison of Frequencies for Different Materials From Finite Element Analysis, it is observed that natural frequency modes changes with change in material of the model. The first mode of the model having Aluminium T6- 6061 as a material is obtained at 269.71 Hz. The first mode of the model having Titanium as a material is obtained at 273.54 Hz. The first mode of the model having an Epoxy Carbon as a material is obtained at 35036 Hz. Fig. 6 shows the comparison of modal analysis results for different materials. 0 200 400 600 800 1000 1200 1400 Al Ti EC Frequency(Hz) Mode 1 Mode 2 Mode 3 Mode 4 Mode 5 Fig. 6 Comparison of frequencies for different materials From Fig. 6, it can be seen that the first mode frequency for Aluminium T6-6061 is least while it is maximum for the Epoxy Carbon. 5. Conclusions The different results obtained in this paper are hopeful and from these results, it is clear that change of material lead to change of frequencies. For these reasons, material selection plays a vital role in designing of spacecraft components. It is also observed that Aluminium T6-6061 is a suitable material for designing of payloads. This work can give a hint for the researchers in the design of payloads. Acknowledgments The authors are grateful to Mr. Vinayak Shingare from Designtech System Ltd., Faculty of Mechanical Engineering in Sinhagad Institute of Technology and Science, Pune and Symbiosis Institute of Technology, Pune for providing support and encouragement for this paper. References [1] R. G. Cobb, J. M. Sullivan, A. Das, L. P. Davis, T. T. Hyde, T. Davis, Z. H. Rahaman, J. T. Spanos, “Vibration isolation and suppression system for precision payloads in space”, Smart Materials and Structures, 8 (1999) pp. 798-812. [2] D. Kamesh, R. Pandiyan, A. Ghosal, “Modeling, design and analysis of low frequency platform for attenuating micro- vibration in spacecraft”, Journal of Sound and Vibration, 329 (2010) pp. 3431-3450. [3] A. Boudjemai, R. Amri, A. Mankour, H. Salem, M. H. Bouanane, D. Boutchicha, “Modal analysis and testing of hexagonal plates used for satellite structural design”, Materials and Design, 35 (2012) pp. 266-275 [4] Space shuttle program payload bay payload user’s guide, Johnson space center, Texas, NSTS21492, December 2000,. [5] D. Shah, V. R. Iyer, A. V. Pathak, “Simulation and modification of microwave packaging for space communication payload”, National conference on current trends in technology, November 2009. [6] http://www.nasa.gov/