- Open Access
- Total Downloads : 1928
- Authors : V.Veeraragavan
- Paper ID : IJERTV1IS10053
- Volume & Issue : Volume 01, Issue 10 (December 2012)
- Published (First Online): 28-12-2012
- ISSN (Online) : 2278-0181
- Publisher Name : IJERT
- License: This work is licensed under a Creative Commons Attribution 4.0 International License
Effect Of Temperature Distribution In 10c4/60c50 Gas Turbine Blade Model Using Finite Element Analysis
V.Veeraragavan
Lecturer in Mechanical Engineering
Eritrea Institute of Technology, Asmara, Eritrea, N.E.Africa
Abstract
In this research paper is mainly apprehensive with aircraft gas turbine engine. Turbine blade is an important part of aircraft gas turbine engine. The research focus of 10 C4 / 60 C 50 turbine blade model, because of its common use in all types of aircraft engines. Investigate used, Pro-e model and ANSYS tools. Present research was focused on using Finite element methods (FEM) to predict the location of possible temperature areas on turbine blades. The conventional alloys such as titanium, zirconium, molybdenum, super alloys are chosen for analysis. Initially the model is created with the help of Pro-e and then it is imported to Ansys.The static analysis of solid model is carried out by applying temperature from external circumference tip of turbine blade to root of the blade and the temperature distribution is plotted. At that time measured the maximum temperature withstood capacity in gas turbine blade. Finally the entire four alloy materials are compared with respect to temperature distribution to found out of the best one. Then suggested to which material is better performing in gas turbine engine applications.
Keywords: Gas turbine, Titanium, Temperature Distribution, Turbine blade, Rotor.
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Introduction
Gas turbines play an important role in aviation and industrial applications. There is a growing tendency to use higher temperatures at the inlet of the turbine to improve the efficiency of the
gas turbine engine. Consequently the heat load on the turbine components increases, especially in the high pressure turbine section. This heat load is caused by the exposure of an enormous heat flux of the burnt gas from the combustion chamber. Turbine blades are one of the most important components in a gas turbine application. There are components across which flow of high pressure gases takes place to produce work. A blade can be defined as the medium of transfer of energy from the gases to the turbine rotor. For turbine blades, however, stresses due to aerodynamic forces are typically much less important than stresses due to centrifugal loads. The same is not necessarily true to thermal stresses. If blade temperature is non- uniform (as it may well be, if exposed to a gas 400°C to 500°C better than the blade and subject to intense inner cooling through a distribution of air passages), it can suffer fairly large thermal stresses. A gas turbine is similar to the steam turbine but gas is used to run the turbine. It is mainly used in the aircraft engines, electric power generation, marine propulsion etc. Damage to turbine blades is of critical importance in aircraft engines. The irregular movements of throttle settings are a mandatory requirement for the pilots to perform various air combat maneuvers. This leads to excessive stresses on engine compressor and turbine blades in various flight regimes. The aircraft are also required to fly in varying atmospheric conditions ranging from negative temperature in icing conditions to over 50 degree Celsius in summers. These factors in addition to operations from deserts and tropical weathers also add to the variety of conditions that an aircraft engine is exposed.
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Materials
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Titanium Alloys
Table-1: Composition
Composition
Weight Percentage
Aluminum (A1)
8
Molybdenum (M0)
1
Titanium (Ti)
90
Vanadium (VD)
1
Table-2: Properties
Density
4370 kg/m3
Yield Strength
1070 Mpa
Ultimate Strength
1180 Mpa
Poisson Ratio
0.32
Youngs Modules
120 Gpa
Melting Pont
15400 C
Thermal Expansion
0.000010/m0 C
Thermal Conductivity
600 W/mk
Specific Heat
502 J/Kg k
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Zirconium Alloys
Table-3: Composition
Composition
Weight Percentage
Iron + Chromium
( Fe + Cr )
0.2
Hafinium (Hf )
Max 4.5
Niobium (Nb)
2.5
Oxygen (O)
0.18
Zirconium (Zr)
Min 95.5
Table-4: Properties
Density
6640 Kg/m3
Yield Strength
582 Mpa
Ultimate Strength
750 MPa
Poisson Ratio
0.33
Youngs Modules
97.9 Gpa
Melting Pont
17400 C
Thermal Expansion
0.0000063 /m0 C
Thermal Conductivity
17 W/ m k
Specific Heat
285 J/Kg0 C
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Molybdenum Alloys
Table-5: Composition
Composition
Weight Percentage
Molybdenum (Mo)
52.5%
Rhenium (Rh)
47.5%
Table-6: Properties
Density
9320 Kg/m3
Yield Strength
845 Mpa
Ultimate Strength
1180 Mpa
Youngs Modules
365 Gpa
Poisson Ratio
0.285
Thermal Expansion (at 10000C)
6.45 m/m0C
Thermal Conductivity
36.8 W/ m k
Specific Heat
255 J/Kg0 C
Melting Point
24500C
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Super Alloys
Table-7: Composition
Composition
Weight Percentage
Nickel Base (Ni)
78%
Chromium (Cr)
20%
Titanium (Ti)
0.4%
Carbon (c)
0.12%
Table-8: Properties
Density
8526 Kg/m3
Yield Strength
855 Mpa
Youngs Modules
220 Gpa
Poisson Ratio
0.33
Melting Pont
8700 C
Thermal Expansion
15.8 micron/m.k
Thermal Conductivity
24.9 W/ m k
Specific Heat
525 J/Kg0 k
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Modeling and Analysis
Pro/Engineer is a solid modeling software and it develops models as solid, allowing to work in a three dimensional environment. These models have volume and surface area, so you can calculate the mass propertis directly from the geometry that you can create and manipulate their display on the screen, the models remain as solids. To truly
appreciate the power of Pro/ Engineer as a solid modeling tool, you must a quire an understanding of the following concepts: feature based, associative and parametric modeling. Then after creating a model, imported to ansys and mesh the model. After that applying all properties of materials in ansys and temperature graph plotted.
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Results and Discussion
Fig-1. Temperature Propagation for Titanium Alloy.
Fig-1 shows show that, blue color curve to represent the temperature from root of the blade. The red color curve to represent the external circumference tip of turbine blade.Hence,during that time of 20 seconds corresponding to the temperature will reaches 140° C in root of the blade and 390 ° C in external circumference tip of turbine blade respectively.
Fig-2. Temperature Propagation for Zirconium Alloy.
Fig-2 shows show that, blue color curve to represent the temperature from root of the blade. The red color curve to represent the external circumference tip of turbine
blade.Hence,during that time of 20 seconds corresponding to the temperature will reaches 290° C in root of the blade and 450 ° C in external circumference tip of turbine blade respectively.
Fig-3. Temperature Propagation for Molybdenum Alloy
Fig-3 shows show that, blue color curve to represent the temperature from root of the blade. The red color curve to represent the external circumference tip of turbine blade.Hence,during that time of 20 seconds corresponding to the temperature will reaches 35° C in root of the blade and 190 ° C in external circumference tip of turbine blade respectively.
Fig-4.Temperature Propagation for Super Alloy.
Fig-4 shows show that, blue color curve to represent the temperature from root of the blade. The red color curve to represent the external circumference tip of turbine blade.Hence,during that time of 20 seconds corresponding to the temperature will reaches 345° C in root of the blade and 460 ° C in external circumference tip of turbine blade respectively.
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Conclusion
The comparisons of temperature distribution of four alloys graphs are shows that, a first one titanium alloy temperature at 20 sec to reached temperature at 390°C.Second one zirconium alloy temperature at 20 sec to reached temperature at 450°C.Third one molybdenum alloy temperature at 20 sec to reached temperature at 190°C.Fourth one super alloys temperature at 20 sec to reached temperature reached at 460°C. Hence, these four alloys temperature comparatives are state that molybdenum alloys are a good temperature withstand. A second one-titanium alloy is a best one. Finally concluded by molybdenum alloy is a best suited for design and manufacture in aircraft engines.
References:
[1]. Mohanty A.K, Raghavachar T.S and NandaR.S (1977),Heat Transfer from Rotating Short Radial Blades, International Journal of Heat and Mass Transfer, Volume.20, 1977, P.1417. [2]. Allen J.M (1982), Effect of Temperature Dependent Mechanical Properties on Thermal Stress in cooled Turbine Blades, Journal of Engineering Power, ASME Volume.104, P.349. [3]. Bahree R. Sharan A.M. and Rao J.S. (1989),The Design of Rotor Blades due to the Combined Effects of Vibratory and Thermal Loads, Journal of Engineering Power and Gas Turbines, ASME Volume.111,P.610. [4]. V.J.Parks, R.J Sanford and J.Cernosek, "Analyis of Blades using a rapid three dimensional photo elastic method," Journal of Aircraft, AIAA 81-4078, Vol 10, No.3, pp 213 -219, March 1981. [5]. L. He, V. Menshikova and B.R. Haller, Effect of hot streak counts on turbine blade heat load and forcing Journal of propulsion and power, Vol. 23, No.6, pp 1235 -1241, November-December2007.
[6]. E. Couch, J. Christophel, E. Holfeld, K.A. Thole and F. J. Cunha, Comparison of measurements and predictions for blowing from a turbine blade tip Journal of propulsion and power, Vol. 21, No. 2,. pp 335- 343, March- April 2005.
[7]. Ronald S. Bunker, Axial turbine blade tips: Funtion, Design and Durability Journal of propulsion and power, Vol. 22, No. 2, pp 271- 285, March-April 2006. [8]. R. G Alderson, M.A. Tani, D.J. Tree andR.J. Hill Three dimensional optimization of a gas turbine disk and blade attachment Journal of Aircraft, Vol. 13, No. 12, pp 994- 999, December 1976.
[9]. M. J. Holland and T. F. Thake, Rotor blade cooling in high pressure turbines Journal of Aircraft, Vol. 17, No. 6, pp 412561, June 1980
[10]. Philip H. Snyder and Richard J. Roelke, Design of an air cooled matellic high temperature radial turbine Journal of propulsion and power,, Vol. 6, No. 3. pp 283- 288, May- June 1990. [11]. R. H. Mao, S.A. Meguid and T. Y. Ng, Finite element modeling of a bird striking an engine fan blade Journal of Aircraft, Vol. 44, No. 2, pp 583- 596, March- April2007.
[12]. A. Hamed, Y. Sheoran and W. Tabakoff, Stress analysis study in cooled radial inflow turbine Journal of Aircraft, Vol. 15, No. 12,. pp 803- 804, December 1978. [13]. D. N. Duhl and E. R. Thompson,Directional structures for advanced aircraft turbine blades, Journal of Aircraft, Vol. 14, No. 6, pp 521- 526,June 1977.
[14]. Kasra Daneshkah and Wahid Ghaly, Aerodynamic inverse design for viscous flow in turbo machinery blading Journal of propulsion and power, Vol. 23, No. 4, pp 814 820, July- August 2007. [15]. M. L. Roberts Engine life, usage, and cycle selection Journal of Aircraft, Vol. 15, No. 4, pp 240 245, April 1978. [16]. Zhijiang He, Bogdan I. Epueanu and Christophe Pierre, Fluid structural coupling effects on the dynamics of mistuned bladed disks, AIAA Journal,Vol. 45, No. 3, pp 552 418, March 2007
[17]. Goldstein R.J,Eckert E.R.G, Wang H.P and Olson S.J (1996), Effects of Blade profile on Turbine Blade Heat (Mass) Transfer, A symposium Paper in November 16. [18]. Yahya S.M (1996), Turbines, Compressors and Fans,Tata McGraw-Hill Publishing Company Limited. [19]. Ganesan.V (1999), Gas Turbines,Tata McGraw-Hill Publishing Company Limited. [20]. Sarvanamuttoo HIH, Rogers GFC and Cohen H,(2001), Gas Turbine Theory, Low Price Edition. [21]. BATHIE W.William, (1995),Fundamentals of Gasturbines, John Wiley & Sons, Inc.
[22]. Jack D. Mattingly, (1996), Elements of Gas Turbine Propulsion, McGraw-Hill International Editions. [23]. George F. Titterton,(1941), Aircraft Materials and Process, Pitman.
[24]. Kenneth G. Budinski, (1992), Engineering Materials,Properties and Selection,Prrentice Hall. [25]. Singiresu S.Rao, (2001), The Finite Element Method in Engineering, Butterworth Heinemann. [26]. Segerlind L.J (1976),Applied Finite Element Analysis, John Wiley and Sons. [27]. ANSYS Verification Manual, Version 6.0. [28]. ANSYS Command and Theory Manual, Version 6.0.AUTHOR PROFILE
Mr.V.Veeraragavan has received the Master of Engineering from Anna University in 2004. Currently he is working as a Lecturer in Mechanical Engineering, Eritrea Institute of Technology, Ministry of
Education, Eritrea. He has blended his wide experience of 12 years in teaching and research in the field of Mechanical Engineering. He has published a number of international journal papers. His areas of research interest include Heat and Mass Transfer, I.C.Engines and Power Plant Engineering.