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ISSN: 2321-9653
Estd : 2013
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Ijraset Journal For Research in Applied Science and Engineering Technology

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Feasibility of a Thrust Control Mechanism by Regulating the Flow at the Engine

Authors: Deepak Kataria, Er. Ashok Kumar

DOI Link: https://doi.org/10.22214/ijraset.2022.44533

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Abstract

This work is focused on performance analysis of a turbojet engine with an inlet flow control mechanism for same thrust values. Developed a real-time turbojet engine integrating aerothermodynamics of engine components, principles of jet propulsion and inter component volume dynamics represented in 1-D non-linear unsteady equations. Performance parameters of the engine are analyzed with the increase in compressor pressure ratio. Specific fuel consumption, specific thrust, component pressure ratios, thermal and propulsive efficiencies are the performance parameters of the engine that are analyzed on the model with reduced inlet pressure. All simulations will be done on MATLAB Tool.

Introduction

I. INTRODUCTION

Jet  engines  are  noticeably  non-linear  flowers  with  a  complex  range  of  operation defined  through  a  flight  envelope.  Altitude  and  Mach  amount  defines  the  operational  set elements for the engine. The important venture for these structures is the manufacturing of properly enough thrust whilst  maintaining  safe  and  strong  operation.  Performance  requirements  for  the  engines vary  in accordance  to  challenge  characteristics.

Civil  plane  operation  requires  minimum jogging and  renovation fees.

A  complete mathematical description of a gas  turbine engine is especially complex  and  in particular  nonlinear.  The  manage  synthesis  system  is  primarily based  on  the selection  of  a  set  of  format  fashions  that  may also  be  used  to  formulate  a  manage  regulation for  software  at some point of  the  engine  running  variety.  Therefore  a  crucial  step inside the manage  design  way is  the era  of tractable  layout  models.  Linear  fashions  are  one  elegance  of  such  layout  models  and  can  be  effectively integrated to offer a nonlinear manage feature.

A.  Model  Reduction

Once nonlinear engine dynamics has been linearised,  some approach may be required to investigate the linear models and set up much less complex layout fashions which consist of great dynamic factors crucial to the favoured control feature. Without such simplification, design can also want to bring about pretty complex and parameter sensitive controlled systems.

B.  Control  Mode and Structure Analysis

Once nonlinear engine dynamics has been linearised,  some approach may be required to investigate the linear models and set up much less complex layout fashions which consist of great dynamic factors crucial to the favored control feature. Without such simplification, design can also want to bring about pretty complex and parameter sensitive controlled systems. 

In Survey, Turbofan Power Ratio have become used as thrust parameter in turbofan engines with ordinary consistent nozzle production, and the writer confirmed the applicability of this parameter to turbojet engines with steady exhaust, therefore, it became a herbal sequel to research the variable nozzle configuration. The author finished measurements on a turbojet engine geared up with variable exhaust nozzle, and the facts confirmed distinct linear correlation between thrust and TPR relying on actual nozzle function putting.

Because the particular definition of TPR caused unbiased capabilities as opposed to a single expression, the author has evolved a manner to gain an equal overall performance parameter that adjustments linearly with thrust output of the engine and it's miles independent of the real situation of the nozzle.

This work is introduced as pursues. In Section II, It defines the function of turbojet engine. Section III portrays the proposed methodology of system. The performance parameters are described in Section IV. The results are explained in Section V. At last, conclusion is clarified in Section VI.

II. TURBOJET ENGINE

Jet Engine  is  the  gas turbine application for aircraft propulsion. Basic principle in a jet engine is to accelerate a mass of fluid within the path opposite to motion and thereby propelling the aircraft beforehand via using the thrust generated. Schematic variations the various Turbojets, Turbofans and Turboprop/Turbo shaft Engines are defined here. Turbojet  is  the  earliest  and  only  shape  of  jet  engines  and  produce  thrust  by using significantly  accelerating  a  small  mass  of  fluid.  Figure  1  indicates  a  conventional  unmarried  spool turbojet above the centre line, and one with the  addition of an afterburner, convergent–divergent consumption, and nozzle underneath the centre line. Ambient air passes from unfastened flow to the flight consumption  predominant component and the air hastens from unfastened flow if the engine is static, at the same time as at high flight Mach wide range it diffuses from the unfastened movement, ram situations. Usually, it then diffuses inside the flight intake earlier than passing through the engine consumption to the compressor face  with  a small  loss  in widespread pressure.  The  compressor  then  will increase  both  the  stress  and  temperature  of  the  gas. Work  input  is  required  to  benefit  the  pressure  ratio;  the  related  temperature  rise relies upon at the performance  of the compressor.

The compressor exit diffuser  passes the air to  the  combustor.  Here,  gasoline  is  injected  and  burnt  to  enhance  exit  fuel  temperature.  The diffuser and combustor every impose a small standard stress loss. The heat, excessive stress gasoline is  then  expanded  via  the  turbine  in which  art work  is  extracted  to  produce  shaft  electricity; each temperature and strain are reduced. The shaft power is that  required to electricity the compressor  and  any  engine  auxiliaries.  On  leaving  the  turbine,  the  fuel  is  nevertheless  at  a stress  commonly  at  least   times  that  of  ambient.  This  results  from  the  higher  inlet temperature  to  the  turbine.  Downstream  of  the  turbine  the  fuel  diffuses  in  the  jet  pipe.

This is a brief duct that  transforms the glide direction from annular to a complete circle at get admission to to the  propelling  nozzle.  The  jet  pipe  imposes  a  small  total  strain  loss.  The  propelling nozzle is a convergent duct that  quickens the drift to provide the immoderate velocity jet to create the thrust. Engine cooling system uses the pretty cool air from the compression system  that  bypasses the  combustor through air device waft paths  to relax the  turbine nozzle guide  vanes  and  blades  to  ensure  best  steel  temperatures  at  prolonged  fuel temperatures.

For high flight Mach amount programs an afterburner is frequently employed, which gives  produces higher  thrust from the identical  configuration. This is also referred to as reheat, and involves burning  gasoline in a further combustor downstream of the jet pipe.  Turbojets are  pretty  inefficient  in assessment  to  exclusive  engine  sorts  at  decrease  Mach  numbers  but  has dominant feature for the supersonic flight modes and navy applications. Turbofans  are  widely  used  engines  for  the  contemporary  civil-aircraft  propulsion.  A turbofan  engine  is  based totally definitely  on  the  principle  that  for  the  equal  strength,  a  large  volume  of slower-moving  air  will  produce  extra  thrust  than  a  small  quantity  of  speedy-moving  air. Turbofan  engines  are  of  the  types  separate  jets  turbofan  and  combined  turbofan  with afterburner.  Figure  2  indicates  the  configuration  of  the  separate  jets  turbofan  above  the centre line and combined turbofan with afterburner beneath the centre line.

III. PROPOSED METHODOLOGY

The main objective of this work is to analyze the feasibility of a thrust control mechanism by regulating the flow at the engine inlet. For the proper jet engine,  paintings executed on the turbine is thought to be same to the compressor work and the techniques in the diffuser, the compressor, the turbine and the nozzle are assumed to be isentropic. So the internet artwork carried out in a turbojet engine is 0. However,  for  the  real  cycle  assessment,  the  irreversibility  related  within  the compressor,  turbine,  nozzle  and  diffuser  ought to  be  considered.  Therefore,  in  a  consistent united states operation of the jet engine, the turbine and the compressor paintings have to be same. Any distinction in those parameters runs engine into the transient mode of operation.

A mathematical model, based on the lumped parameter technique is used from the  unsteady one dimensional conservation laws defined via a set of first-order differential and algebraic equations.

A.  Surrounding Atmosphere Model

The air flowing into the engine diffuser is taken from the out of doors surroundings. Ambient air temperature and strain are decided through the altitude.

B.  Inlet

Intake diffuser is used to hold the loose flow into air into the engine. It does not paintings at the glide and publications the flow to the compressor. However, the overall performance of the inlet is  defines  through  the  stress  healing  from  the  loose  flow into  to  the  engine. An  isentropic technique  is  assumed  for  the  air  go together with the glide  in  the  inlet  diffuser.  Heat  transfer  and  the  friction among the air and the diffuser walls are not considered. Also the go with the flow in the diffuser is modelled as a quasi consistent country and so the dynamic conduct of the air inside the diffuser isn't always considered.

C.  Compressor

The reason of a compressor is to growth the overall stress of the gas waft to that  required  through  the  engine  at the same time as  absorbing  the  minimum  shaft  power  feasible. Temperature  of  the  incoming  air  additionally  will increase  with  stress  in  the  compressor.  The  artwork completed via  the compressor at the gasoline is  extracted from the turbine.  In the reference engine model, the compressor is an axial compressor  with eight levels. But while modelling the engine in Simulink, compressor is modelled as a unmarried block with the useful resource of stacking all of the stages of the compressor right into a unmarried block. The  pressure  ratio  and performance are normally regarded up from a tabulated compressor overall performance map, however they also can be assigned right away inside the model. Compressor general overall performance maps deliver pressure  ratio  and  efficiency  as  capabilities  of  corrected  air  go together with the go with the flow  and  corrected  shaft velocity.

D.  Compressor Map

Compressor normal overall performance maps are acquired from the real rig take a look at of the engines and plotting the results on the map.  Compressor map are plotted among the corrected drift parameter and stress ratio with corrected velocity lines. Efficiency contours might be at the identical plot or separated onto any other plot among overall performance and pressure ratio with corrected velocity strains.

E.  Combustor

The  Burner  detail  calculates  standard overall performance  of  a  general  gasoline  turbine burner/combustor. This element accepts an air movement from the compressor and a gasoline move from the Fuel Start element as established in Fig 2.

The  Duct  element  calculates  strain  and  warmness  losses through ducts as validated in Fig 3. Pressure  and  warmth  losses  are  each  enter  as  person-defined  fractional  losses  or via character described calculation capabilities. The warm temperature loss thru the duct is idea to be negligible.

G. Turbine

The Turbine element  (Figure 4) expands  and extracts paintings from the core go with the flow of the fuel turbine. As  with  the  Compressor  element,  the  pressure  ratio  and  efficiency  for  the turbine  are  either  regarded  up  in  a  tabulated  turbine  overall performance  map  or  assigned right away  through  the  consumer.

H. Nozzle Element

The Nozzle detail calculates  the overall performance of the gasoline turbine’s nozzle. This  element  determines  overall performance  tendencies  for  excellent  nozzle geometries  (convergent,  convergent-divergent,  fixed,  or  variable  geometry).  In  on design mode, if the nozzle isn't always choked,  the nozzle exit region is  calculated  such  that  the  calculated  exhaust  static  stress  equals  the specified  exhaust  static  strain.

IV. PERFORMANCE PARAMETERS

The universal overall performance parameters for an aero-engine are defined on this phase. Each parameter has explains the significance associated with turbojet engine.

A.  Specific Thrust

This is the quantity of output thrust in line with unit of mass waft getting into the engine.  It is mainly crucial to maximize specific thrust in packages  wherein engine weight or quantity  is  crucial  for  plane  that  fly  at  excessive  Mach  numbers  wherein  the  drag  in keeping with  unit frontal vicinity is excessive.

B.  Specific Fuel Consumption

This is the mass of gasoline burnt in step with unit time consistent with unit of output energy or thrust. It is vital  to reduce SFC for packages in which the load and/or value of the gas are big. When specifying the  SFC values,  it's far  crucial to state  whether or no longer the decrease or better calorific charge of the gas is used.

C.  Thermal Efficiency

Thermal  performance  for  jet  engines  is  defined  as  the  price  of  addition  of  kinetic electricity  to  the  air  divided  with the useful resource of  the  price  of  gasoline  power  furnished,  commonly  ex pressed  as  a percent.

D.  Propulsive Efficiency

Propulsive  performance  for  jet  engines  is  defined  as  the  useful  propulsive  power produced  by way of way of  the  engine  divided  with the aid of  the  fee  of  kinetic  energy  addition  to  the  air,  once more commonly expressed as a percent. The net thrust is proportional to the difference within the  jet  and  flight  velocities. 

V. RESULTS & DISCUSSION

Ambient Air

Inlet

Compressor

Combustor

Turbine

Nozzle

Figure 5: Turbojet Engine Modelling

Although  the  solver  configuration  is  exclusive  among  the  first  and  2D layout instances, it's miles essential to notice that the converged answers are the identical. The input  parameters  for  both  layout  instances  are  defined  in  the  following  phase.  The design case parameters are described for full throttle operation.  The enter values of ambient stress, ambient temperature,  engine velocity,  thrust,  Mach wide variety, compressor strain ratio, fuel waft price, burner pressure loss, and turbine stress ratio  are  decided  experimentally.

A.  Results with Converging Nozzle

It  is critical to word that the engine version  is fixed for the off-layout evaluation in line with  the  converged  answer  of  the  design  evaluation.  This  manner  performance  is calculated  using  the  identical  rapid machinery  overall performance  maps  and  geometric  engine parameters for every case. The purpose of a compressor is to boom the full strain of the fuel flow to that  required  through  the  engine  even as  absorbing  the  minimal  shaft  energy  possible. Temperature  of  the  incoming  air  also  will increase  with  strain  in  the  compressor.  The  work carried out by  the compressor at the fuel is  extracted from the turbine.

B.  Results with Mixing Turbofan after Burner

In the temporary procedure,  the compressor is modelled as a blending extent wherein the mass and power may be accumulated. The fuel dynamics associated inside the compressor degrees  are  calculated  by using  applying  the  continuity,  power  and  Ideal  gas  equations  to  the inter element extent between the compressor and the combustor. Table 1 indicates the Input Parameters of System after Burner.

Table 1: Input Parameters of System after Burner

Parameter

Air

Burner

After Burner

Ratio of Specific Heat

1.4

1.33

1.3

Specific Heat at Constant Pressure

1004

1156

1243

Fuel Lower Heating Value

0

42000

42000

Unlike  the  theoretical  combustion  technique  where  the  inlet  pressure  and  outlet strain  of  the  chamber  are  same,  there  is  a  pressure  drop  in  the  combustion  for  the actual method. 

A convergent nozzle is considered in modelling the engine. The partly accelerated gas coming from the turbine at a especially high pressure is improved to a excessive velocity inside the nozzle. Finally, the gases extend to the ambient strain and offer the thrust to propel the aircraft.

Conclusion

With the known values of the altitude, the working Mach and decided on values of the shaft rotational pace, mass float parameter for the compressor, values for the compressor stress ratio, efficiency is cited from the values of the performance map. Overall performance of the turbojet engine decreases with reduced compressor inlet stress for the equal thrust if the engine is operated constantly with this mechanism. But has big importance for packages in which a certain amount of efficiency might be spent for the electricity demands. Performance parameters of the engine are analyzed with the increase in compressor pressure ratio. Specific fuel consumption, specific thrust, component pressure ratios, thermal and propulsive efficiencies are the performance parameters of the engine that are analyzed on the model with reduced inlet pressure

References

[1] L. Baoan, Z. Fan, (2012), \"Modeling and Simulation of Small Turbojet Engine Ground Starting Process\", International Conference on Instrumentation & Measurement, Computer, Communication and Control, pp. 28-32. [2] Z. Katolický, B. Bušov and M. Bartlová, (2014), \"Turbojet Engine Innovation and TRIZ\", IEEE, pp. 01-08. [3] L. Nyulászi, L. Madarász, (2014), \"Experimental Identification of the Small Turbojet Engine MPM-20\", IEEE International Symposium on Computational Intelligence and Informatics, pp. 497-501. [4] Ján Hrabovský, Rudolf Andoga, Ladislav Fozo, (2015), \"A Conceptual Method For Implementation of Anytime Algorithms For A Small Turbojet Engine \", IEEE International Symposium on Computational Intelligence and Informatics, pp. 113-116. [5] D. Klein, C. Abeykoon, (2015), \"Modeling of a Turbojet Gas Turbine Engine \", IEEE, pp. 200-206. [6] N. Mubarak, S. Farooq, (2015), \"Feasibility to Adapt Modifications in the Extant Turbojet Engine Test Bed for the Ground Test Run of Turbofan Engine\", IEEE, pp. 01-06. [7] D.Bai, Q. Zheng, (2017), \" Influence of Wet Compression on Operating Performance and Exhausts of Turbojet Engine\", International Conference on Computation of Power, Energy, Information and Communication, pp. 477-485. [8] V. Kuz\'michev, A. Tkachenko, (2017), \"Optimization of Working Process Parameters of Small-scale Turbojet for Unmanned Aircraft\", International Conference on Mechanical, System and Control Engineering, pp. 125-129. [9] O. Turan, A. Hepbasli, (2017), \"Investigating the Effect of Turbine Inlet Temperature on the Exergetic Improvement Potential of a Small Turbojet Engine\", International Conference on Mechanical and Aerospace Engineering, pp. 301-304. [10] K. Yuan, C. Chun, (2018), \"Performance Calculation and Integrated Mission Assessment of High Speed Turbojet-Scramjet Combined Engine\", International Conference on Mechanical and Aerospace Engineering, pp. 168-172. [11] I. Goryunov, M. Muraeva, (2018), \"Mathematical Modelling of In-turbine Isothermal Expansion in the Gas Turbine Engine\", International Russian Automation Conference, pp. 01-05. [12] J. Xiang, C. Chun, (2019), \"Adaptive Simulation of Micro-Turbojet Engine Component Characteristics\", IEEE International Conference on Mechanical & Aerospace Engineering, pp. 147-152. [13] I. A. Krivosheev, A. E. Kishalov, (2019), \"Analysis of Options for Converting Aviation Two Spool Turbojet Engines with Afterburner when Developing Gas–Turbine–Driven Compressor Plant for Gas–Compressor Unit\", International Russian Automation Conference, pp. 01-06. [14] A. Shehata, M. Khalil, (2020), \"Controller Design for Micro Turbojet Engine\", IEEE, pp. 436-440. [15] Flyur Ismagilov, Vyacheslav Vavilov, (2020), \"Design of the “Integrated Into An Aircraft Engine Starter-Generator- Dual-Flow Turbojet Engine” System As A Part Of The Electrified Aircraft Engine\", IEEE Explore, pp. 01-06. [16] K. Beneda, (2021), \"Investigation of Novel Thrust Parameters to Variable Geometry Turbojet Engines\", IEEE World Symposium on Applied Machine Intelligence and Informatics, pp. 339-341.

Copyright

Copyright © 2022 Deepak Kataria, Er. Ashok Kumar. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

IJRASET44533

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Authors : Deepak Kataria

Paper Id : IJRASET44533

Publish Date : 2022-06-19

ISSN : 2321-9653

Publisher Name : IJRASET

DOI Link : Click Here

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