Parametric Cycle Analysis of Real Turbofan

Similar documents
The Turbofan cycle. Chapter Turbofan thrust

6.1 Propellor e ciency

Preliminary Design of a Turbofan Engine

CONTENTS Real chemistry e ects Scramjet operating envelope Problems

Contents. Preface... xvii

Civil aeroengines for subsonic cruise have convergent nozzles (page 83):

Quiz 2 May 18, Statement True False 1. For a turbojet, a high. gives a high thermodynamic efficiency at any compression ratio.

Jet Aircraft Propulsion Prof. Bhaskar Roy Prof. A.M. Pradeep Department of Aerospace Engineering

Jet Aircraft Propulsion Prof. Bhaskar Roy Prof A M Pradeep Department of Aerospace Engineering Indian Institute of Technology, Bombay

Section 4.1: Introduction to Jet Propulsion. MAE Propulsion Systems II

ANALYSIS OF TURBOFAN ENGINE DESIGN MODIFICATION TO ADD INTER-TURBINE COMBUSTOR

ME 440 Aerospace Engineering Fundamentals

DESIGN AND DEVELOPMENT OF A SIMULATION TOOL FOR AIRCRAFT PROPULSION SYSTEMS

ÂF = Ù. ı s. Ù u(ru) nds PRODUCTION OF THRUST. For x-component of vectors:

Performance Trends of High-Bypass Civil Turbofans

Propulsion Thermodynamics

SPC 407 Sheet 5 - Solution Compressible Flow Rayleigh Flow

TURBINE BURNERS: Engine Performance Improvements; Mixing, Ignition, and Flame-Holding in High Acceleration Flows

AKEY goal of conceptual aircraft design is to quantify basic

Simulation And Cycle Analyses For High Bypass Turbofan Engine A Comparative Study

Turbomachinery & Turbulence. Lecture 2: One dimensional thermodynamics.

Turbofan Engine Sizing and Tradeoff Analysis via Signomial Programming. Martin A. York

UNIFIED ENGINEERING Fall 2003 Ian A. Waitz

A Thermodynamic Analysis of a Turbojet Engine ME 2334 Course Project

ME Thermodynamics I

Contents. 2 Basic Components Aerofoils Force Generation Performance Parameters xvii

Results from SP2, Analysis of the Westinghouse J-30 Turbojet using Gasturb. Kevin Hoopes

AME 436. Energy and Propulsion. Lecture 11 Propulsion 1: Thrust and aircraft range

AME 436. Energy and Propulsion. Lecture 7 Unsteady-flow (reciprocating) engines 2: Using P-V and T-s diagrams

AIR FORCE INSTITUTE OF TECHNOLOGY

Please welcome for any correction or misprint in the entire manuscript and your valuable suggestions kindly mail us

+ m B1 = 1. u A1. u B1. - m B1 = V A. /v A = , u B1 + V B. = 5.5 kg => = V tot. Table B.1.

I. (20%) Answer the following True (T) or False (F). If false, explain why for full credit.

Direct Integration of Axial Turbomachinery Preliminary Aerodynamic Design Calculations in Engine Performance Component Models

UNIT 1 COMPRESSIBLE FLOW FUNDAMENTALS

PARAMETRIC AND PERFORMANCE ANALYSIS OF A HYBRID PULSE DETONATION/TURBOFAN ENGINE SIVARAI AMITH KUMAR

c The Society shall not be responsible for statements or opinions advanced in

Turbine D P. Example 5.6 Air-standard Brayton cycle thermal efficiency

R c = g c-1. c pc R t = g t-1. g c. c pt. g t. a 0 = g c R c g c T 0. t r = 1+ g c-1 2. p r = t c êhg c -1L r. c pc T 0.

Journal of Robotics and Mechanical Engineering Research

MONTANA STATE UNIVERSITY DEPARTMENT OF MECHANICAL ENGINEERING. EMEC 426 Thermodynamics of Propulsion Systems. Spring 2017

Dynamic Modeling and Simulation on GE90 Engine

AME 436. Energy and Propulsion. Lecture 15 Propulsion 5: Hypersonic propulsion

ME6604-GAS DYNAMICS AND JET PROPULSION. Prepared by C.Thirugnanam AP/MECH TWO MARK QUESTIONS AND ANSWERS UNIT I ISENTROPIC FLOW

THE FIRST LAW APPLIED TO STEADY FLOW PROCESSES

SECOND ENGINEER REG. III/2 APPLIED HEAT

Lecture 35: Vapor power systems, Rankine cycle

MODELING PROPULSION SYSTEM OF A SUBSONIC CIVIL JET AIRCRAFT FOR MULTIDISCIPLINARY CONCEPTUAL DESIGN OPTIMIZATION

Multipoint Variable Cycle Engine Design Using Gradient-based Optimization

Nonlinear Aircraft Engine Model for Future Integrated Power Center Development

MAHALAKSHMI ENGINEERING COLLEGE

THERMODYNAMICS, FLUID AND PLANT PROCESSES. The tutorials are drawn from other subjects so the solutions are identified by the appropriate tutorial.

Chapter Two. Basic Thermodynamics, Fluid Mechanics: Definitions of Efficiency. Laith Batarseh

3. Write a detailed note on the following thrust vector control methods:

Overall Performance Design of Ramjet for Combined Engine

Minimizing and maximizing compressor and turbine work respectively

CRANFIELD INSTITUTE OF TECHNOLOGY

Modeling and Analysis of Dynamic Systems

NUMERICAL INVESTIGATION OF TURBOJET ENGINE THRUST CORRELATED WITH THE COMBUSTION CHAMBER'S PARAMETERS

REVERSE ENGINEERING OF A MICRO TURBOJET ENGINE. Onur Tuncer and Ramiz 0mür İçke Istanbul Technical University Istanbul, Turkey

Dynamic Modeling and Simulation of a Variable Cycle Turbofan Engine with Controls

Performance Assessment of a Boundary Layer Ingesting Distributed Propulsion System at Off-Design

Compressible Duct Flow with Friction

Hydraulic modeling assessment Copyright 2010, Optimized Technical Solutions, LLC

UBMCC11 - THERMODYNAMICS. B.E (Marine Engineering) B 16 BASIC CONCEPTS AND FIRST LAW PART- A

10 minutes reading time is allowed for this paper.

Gasdynamics 1-D compressible, inviscid, stationary, adiabatic flows

Review of Fundamentals - Fluid Mechanics

Derivation and Application of a New Equation for Design and Analysis of Triple Spool Mixed Turbofan Jet Engines with Verification

Lecture with Numerical Examples of Ramjet, Pulsejet and Scramjet

STATISTICAL REPRESENTATION OF TURBOFAN OPERATIONAL CHARACTERISTICS BY THRUST PARAMETER

Turbomachinery. Hasan Ozcan Assistant Professor. Mechanical Engineering Department Faculty of Engineering Karabuk University

First Law of Thermodynamics

Prof. Dr.-Ing. F.-K. Benra. ISE Bachelor Course

CRUISE FLIGHT OPTIMIZATION OF A COMMERCIAL AIRCRAFT WITH WINDS. A Thesis. presented to. the Faculty of the Graduate School

The ramjet cycle. Chapter Ramjet flow field

3 Energy Exchange in Turbomachines

Aerodynamic Evaluation of Nacelles for Engines with Ultra High Bypass Ratio. Master s thesis in Applied Mechanics ANDREAS PETRUSSON

EDEXCEL NATIONAL CERTIFICATE/DIPLOMA. PRINCIPLES AND APPLICATIONS of THERMODYNAMICS NQF LEVEL 3 OUTCOME 2 -ENERGY TRANSFER

SIMULATING INDIRECT THRUST MEASUREMENT METHODS FOR HIGH BYPASS TURBOFANS. J. D. Stevenson and H. 1. H. Saravanamuttoo

Aircraft Turbofan Engine Health Estimation Using Constrained Kalman Filtering. Funded by the NASA Aviation Safety Program June 16, 2003

EFFICIENCY ANALYSIS OF A TURBOFAN ENGINE. GRADUATION PROJECT Yıldırım Burak KILINÇ. Department of Astronautical Engineering

THE INFLUENCE OF MULTI-ROLE AIRCRAFT MISSION TYPE ON THE LOW BYPASS ENGINE PERFORMANCE PARAMETERS

Fig. 1. Field of the Mach number and streamlines (cruise, М = 0.8)

Lecture 38: Vapor-compression refrigeration systems

Gas Dynamics and Propulsion Dr. Babu Viswanathan Department of Mechanical Engineering Indian Institute of Technology - Madras. Lecture 01 Introduction

Answers to questions in each section should be tied together and handed in separately.

ME Thermodynamics I

Gas Dynamics and Jet Propulsion

FPR= TSFC BPR FPR= Dfan/Dfan, BPR=

Lecture 43: Aircraft Propulsion

Effects of Large-Scale Transient Loading and Waste Heat Rejection on a Three Stream Variable Cycle Engine

Chapter 5. Mass and Energy Analysis of Control Volumes. by Asst. Prof. Dr.Woranee Paengjuntuek and Asst. Prof. Dr.Worarattana Pattaraprakorn

PARAMETRIC IDEAL CYCLE ANALYSIS OF A SCRAMJET ENGINE AT A CONSTANT COMBUSTION MACH NUMBER. An Undergraduate Honors Thesis Project

PART 2 POWER AND PROPULSION CYCLES

OPTIMAL PATH PLANNING OF AN UNMANNED COMBAT AERIAL VEHICLE WITH OBSTACLE AVOIDANCE. A Thesis. presented to. the Faculty of the Graduate School

AEROSPACE ENGINEERING DEPARTMENT. Second Year - Second Term ( ) Fluid Mechanics & Gas Dynamics

MONTANA STATE UNIVERSITY DEPARTMENT OF MECHANICAL ENGINEERING. EMEC 426 Thermodynamics of Propulsion Systems. Spring 2018

Design of Radial Turbines & Turbochargers

Unified Propulsion Quiz May 7, 2004

Transcription:

Parametric Cycle Analysis of Real Turbofan Introduction Parametric cycle analysis of a real turbofan The behaviour of a turbofan operating at optimum bypass ratio

Cycle Analysis of Real Turbofan Assumptions : Upstream of main burner: perfect gas with constant properties γ c, R c, c pc, etc. Downstream of main burner: perfect gas with constant properties γ t, R t, c pt, etc. All components are adiabatic (turbine cooling is neglected) Constant polytropic efficiencies e f, e c, e t for fan, compressor, and turbine Source: Real Turbofan Input:,,,,,,,,,,,,,,,,,,,,, Output:,,,,,,, Source:

Real Turbofan T-s Diagram for Turbofan Engine with Losses Source: Real Turbofan Equations = 1 = 1 = = =1+ 1 2 = =1 for 1 =1 0.075 1. for >1 = Source:

Real Turbofan Equations = = = 1 1 = = 1 1 = 1 =1 1+ 1+ 1 = = 1 1 Source: Real Turbofan Equations = = 2 1 1 = = = = 2 1 1 = Source:

Real Turbofan Equations Source: Cycle Analysis of Real Turbofan = 216.7 K = 0.98 = 0.90 Baseline = 1.4 = 0.98 : 0.91 = 0.9 = 1.004 kj/(kg. K) = = 0.98 = 0.88 = 24 = 1.35 = 0.99 = 42,800 kj/kg = 2 = 1.096 kj/(kg. K) = 0.98 = 1670 K Turbofan with Losses: Specific Thrust vs Comp Pressure Ratio Turbofan with Losses: Fuel-air Ratio vs Comp Pressure Ratio Source: Example 7.7

Cycle Analysis of Real Turbofan As α increases, difference in S between real engine cycle and ideal engine cycle increases: Due mainly to the much higher f for the "real" engine. Turbofan with Losses: Thrust Specific Fuel Consumption vs Comp Pressure Ratio Source: Example 7.7 Cycle Analysis of Real Turbofan Specific thrust is reduced more than that of ideal engine at high M 0 because of increasing inlet total pressure loss Limiting M 0 is much lower for real engine than for ideal engine. Turbofan with Losses: Specific Thrust vs Mach Number Turbofan with Losses: TSFC vs Mach Number Source: Example 7.7

Optimum BPR, a* Turbofan Optimum bypass ratio, in a turbofan with losses, that gives the minimum thrust specific fuel consumption Source: Optimum BPR, a* Turbofan An optimum-bypass-ratio turbofan engine has the following characteristics: π c has very little effect on the specific thrust Increasing theπ f increases the specific thrust α* increases with π c and decreases with π f Specific fuel consumption decreases with increasing π c Specific fuel consumption increases with increasing π f Specific thrust decreases with M 0 up to a critical value before increasing again. Specific fuel consumption increases with increasing M 0 Optimum bypass ratio decreases with increasing M 0 Adapted:

Optimum BPR, a* Turbofan = 216.7 K = 0.98 Baseline = 1.4 = 0.98 = 0.9 = 1.004 kj/(kg. K) = = 0.98 = 24 = 1.35 = 0.99 = 2 = 1.096 kj/(kg. K) = 0.98 = 0.90 : 0.91 = 0.88 = 42,800 kj/kg = 1670 K = 1 = 1 π c has very little effect on the specific thrust Optimum Bypass Ratio Turbofan: Specific Thrust and α* vs Comp Pres Ratio Increasing theπ f increases the specific thrust α* increases with π c and decreases with π f Source: Example 7.8 Optimum BPR, a* Turbofan Specific fuel consumption decreases with increasing π c Specific fuel consumption increases with increasing π f Optimum Bypass Ratio Turbofan: Thrust Specific Fuel Consumption vs Comp Pres Ratio Source: Example 7.8

Optimum BPR, a* Turbofan Specific thrust decreases with M 0 to a critical value before increasing again. Optimum bypass ratio decreases with increasing M 0 Optimum Bypass Ratio Turbofan: Specific Thrust and a* vs Mach Number Source: Example 7.8 Optimum BPR, a* Turbofan Specific fuel consumption increases with increasing M 0 Optimum Bypass Ratio Turbofan: Thrust Specific Fuel Consumption vs Mach Number Source: Example 7.8

Summary Parametric cycle analysis of a real turbofan Consideration for losses More real-world assumptions Comparison with ideal turbofan Evaluating a turbofan operating at optimum bypass ratio Reflection Question What is defined as a turbofan engine with optimum bypass ratio, and what are the characteristics of such an engine?