C & CD Nozzles for Jet Propulsion

Slides:



Advertisements
Similar presentations
Chapter Seven Compressible Fluid.
Advertisements

Example 3.4 A converging-diverging nozzle (Fig. 3.7a) has a throat area of m2 and an exit area m2 . Air stagnation conditions are Compute.
Chapter 17 Compressible Flow Study Guide in PowerPoint to accompany Thermodynamics: An Engineering Approach, 5th edition by Yunus A. Çengel and.
Choking Due To Friction The theory here predicts that for adiabatic frictional flow in a constant area duct, no matter what the inlet Mach number M1 is,
Gas Turbine Cycles for Aircraft Propulsion
Operating Characteristics of Nozzles P M V Subbarao Professor Mechanical Engineering Department I I T Delhi From Takeoff to cruising …… Realizing New.
Advanced Thermodynamics Note 6 Applications of Thermodynamics to Flow Processes Lecturer: 郭修伯.
Chapter 12: Compressible Flow
Isentropic Flow In A Converging Nozzle. M can equal 1 only where dA = 0 Can one find M > 1 upstream of exit? x = 0 Converging Nozzle M = 0.
Chap 5 Quasi-One- Dimensional Flow. 5.1 Introduction Good approximation for practicing gas dynamicists eq. nozzle flow 、 flow through wind tunnel & rocket.
16 CHAPTER Thermodynamics of High-Speed Gas Flow.
Chapter 17 COMPRESSIBLE FLOW
Department of Mechanical Engineering ME 322 – Mechanical Engineering Thermodynamics Lect 27b Jet Aircraft Propulsion.
Example 3.1 Air flows from a reservoir where P = 300 kPa and T = 500 K through a throat to section 1 in Fig. 3.4, where there is a normal – shock wave.
Lecture 5 Shaft power cycles Aircraft engine performance
Discovery of A Strong Discontinuity P M V Subbarao Associate Professor Mechanical Engineering Department I I T Delhi A Break Through Finding To Operate.
Assessment of Engine Breathing Capacity P M V Subbarao Professor Mechanical Engineering Department Measure of Filling & Emptying Effectiveness….
Breathing abilities are limited by throat size….
The Thrust Generator P M V Subbarao Professor Mechanical Engineering Department Another Passive Device…… An Obvious Concept for Generation of Motive Power.
Anatomy and SSSF Analysis of Ideal Turbo Jet Engine P M V Subbarao Professor Mechanical Engineering Department Features of A True Flying Machine Muscles.
Flow Measurement (Orifice meter)
MAE 4262: ROCKETS AND MISSION ANALYSIS
Chapter IV Compressible Duct Flow with Friction
Analysis of Thrust Equation for Ideal Turbo Jet Engine P M V Subbarao Professor Mechanical Engineering Department Understanding the Features of A True.
Compressible Flow.
Chapter II Isentropic Flow
Mass Flow Rate M 1 Flow rate out of a tank depends on tank temperature, pressure and size of throat.
Stagnation Properties P M V Subbarao Professor Mechanical Engineering Department I I T Delhi Capacity of A Resource…..
Choking Pressure Ratio Guidelines for Small Critical Flow Venturis
Analysis of A Disturbance in A Gas Flow P M V Subbarao Associate Professor Mechanical Engineering Department I I T Delhi Search for More Physics through.
Measurement of flowing fluids
Analysis of Expansion Waves P M V Subbarao Associate Professor Mechanical Engineering Department I I T Delhi Another Zero Cost Nozzle …..
Quasi - One Dimensional Flow with Heat Addition P M V Subbarao Professor Mechanical Engineering Department I I T Delhi A Gas Dynamic Model for Combustion.
Review of Components Analysis Aerospace Engineering, International School of Engineering (ISE) Academic year : (August – December, 2012) Jeerasak.
CP502 Advanced Fluid Mechanics Compressible Flow Lectures 5 and 6 Steady, quasi one-dimensional, isentropic compressible flow of an ideal gas in a variable.
One Dimensional Flow of Blissful Fluid -III P M V Subbarao Professor Mechanical Engineering Department I I T Delhi Always Start with simplest Inventions……..
The figure shows that the minimum area which can occur in a given isentropic duct flow is the sonic, or critical throat area. Choking For γ=1.4, this reduces.
One Dimensional Flow with Heat Addition
Gas Dynamics of Variable Area Ducts P M V Subbarao Professor Mechanical Engineering Department I I T Delhi Development of Efficient and Compact Passive.
Gas dynamics of Real Combustion in Turbo Combustor P M V Subbarao Professor Mechanical Engineering Department Make Sure that design is Acceptable to Gas.
Design of Supersonic Intake / Nozzle P M V Subbarao Associate Professor Mechanical Engineering Department I I T Delhi Meeting the Cruising Conditions…
Chapter 17 COMPRESSIBLE FLOW
First step in Understanding the Nature of Fluid Flow…. P M V Subbarao Professor Mechanical Engineering Department I I T Delhi Analysis of Simplest Flow.
MAE 4261: AIR-BREATHING ENGINES
Meghe Group of Institutions Department for Technology Enhanced Learning 1UNIT IV.
© Fox, Pritchard, & McDonald Introduction to Fluid Mechanics Chapter 13 Compressible Flow.
Design & Aerodynamics of Inlets & Nozzles P M V Subbarao Professor Mechanical Engineering Department Understanding of Real Flow Through Passive Devices…….
Parametric Study of Turbine Cascades P M V Subbarao Professor Mechanical Engineering Department Identification of New design Variables.……
Reflection of Oblique Shocks P M V Subbarao Professor Mechanical Engineering Department I I T Delhi A Train of Waves ….. Where to End ???
Gas Dynamics of Flow through Valves Method to Estimate the Flow Capacity of Valve Passage…. P M V Subbarao Professor Mechanical Engineering Department.
COMPRESSIBLE FLOW IN NOZZLES Alberto L. Pérez Dávila Est. # Thermal Engineering Laboratory WI-15-ME Prof. Eduardo Cabrera February
Chapter 7. Application of Thermodynamics to Flow Processes
Fanno Flow -1 School of Aerospace Engineering Copyright © 2001 by Jerry M. Seitzman. All rights reserved. AE3450 Fanno Flow - Thermodynamics Steady, 1-d,
Shock waves and expansion waves Rayleigh flow Fanno flow Assignment
Compressive Flow in Nozzles
CHAPTER 17 COMPRESSIBLE FLOW
Consequence Analysis 1.2.
Stagnation Properties
One Dimensional Flow of Blissful Fluid -III
Performance Characteristics of Turbo Jet Engines
Gas Dynamics for Design of Nozzles
Figure 2.9 T-s diagram for converging only nozzle
Design of Passive (Adiabatic) Control Volumes
Gas Dynamics for Study of Critically Off-Design Conditions
Gas Dynamics for Design of Intakes
Gas Dynamics for Study of Off-Design
For this type of flow, the stagnation temperature is constant, then
MAE 5380: ROCKETS AND MISSION ANALYSIS
Rocket Physics The Rocket Nozzle
Introduction to Fluid Mechanics
Presentation transcript:

C & CD Nozzles for Jet Propulsion P M V Subbarao Professor Mechanical Engineering Department Design Vs Off-Design Characteristics…..

Operational Characteristics of Isentropic C Nozzles A converging passage designed to accelerate the a gas flow is considered for study. The concern here is with the effect of changes in the upstream and downstream pressures on the nature of the flow and on the mass flow rate through a nozzle. Four different cases considered for analysis are: Converging nozzle with constant upstream conditions. Converging-diverging nozzle with constant upstream conditions. Converging nozzle with constant downstream conditions. Converging-diverging nozzle with constant downstream conditions.

Pressure Distribution in Under Expanded Nozzle pb=p0 p0 pb,critical<pb3<p0 pb,critical<pb2<p0 pb,critical<pb1<p0 Pb,critical At all the above conditions, the pressure at the exit plane of nozzle, pexit = pb.

Variation of Mass Flow Rate in Exit Pressure 1 1

Variation of in Exit Pressure 1 1

Variation of in Mass Flow Rate 1

Low Back Pressure Operation

Frictional Adiabatic Flow in A Variable Area Duct Sonic Point : M=1

Throat Conditions The capacity of Frictional throat is always lower than ideal throat!!!

The Real Nozzle for Sonic Flow It is impossible to get a sonic flow with real converging nozzle. The flow is always subsonic (transonic) at the throat. A compact real converging nozzle can produce transonic jet. A real nozzle for sonic exit is a CD Nozzle.

Ideal Convergent-Divergent Nozzle Under Design Conditions

Convergent-Divergent Nozzle with High Back Pressure pb1< p0 but > p* Pthroat > p*

Convergent-Divergent Nozzle with High Back Pressure When pb is very nearly the same as p0 the flow remains subsonic throughout. The flow in the nozzle is then similar to that in a venturi. The local pressure drops from p0 to a minimum value at the throat, pthroat , which is greater than p*. The local pressure increases from throat to exit plane of the nozzle. The pressure at the exit plate of the nozzle is equal to the back pressure. This trend will continue for a particular value of back pressure.

Convergent-Divergent Nozzle with High Back Pressure At all these back pressures the exit plane pressure is equal to the back pressure. pthroat> p*

Mass Flow Rate at Higher Back Pressures

Mass flow rate at high back pressure pb At throat with high back pressure pb

For a given value of high back pressure corresponding throat pressure can be calculated. As exit area is higher than throat area throat pressure is always less than exit plane pressure. A decreasing exit pressure produces lowering throat pressure

Variation of Mass Flow Rate in Exit Pressure 1 1

Variation of in Mass Flow Rate 1

Further Decrease the Back Pressure till the throat is just choked…. Define this back pressure as critical back pressure, pb.critical.

This generates choked condition at the throat. This is the back pressure which produces maximum flow rate Through the nozzle. Is this back pressure same as design back pressure? If not??????

Pexit = pb,critical Pthroat = p*

Variation of in Exit Pressure 1 1

Variation of in Throat Pressure 1 1

Variation of in Mass Flow Rate 1

What Next? What happens if back pressure is further reduced? Still the pressure at the exit plane is equal to the throat pressure? Further lower pressure at throat !?!?!

Convergent-Divergent Nozzle with High Back Pressure It is impossible to have a pressure lower than p* at the throat. However at any downstream location the pressure can reach p*. Pthroat = p* pb< pb,critical <p0 Pthroat< p*????

Find out the downstream location, x where p Find out the downstream location, x where p* can be achieved with lower back pressures. A=? pb < pb,critical <p0 Feasible solution Infeasible solution ? M<1 M<1

Convergent-Divergent Nozzle Under Off-Design Conditions

Normal Shock : A large discontinuity

Moving Shock Towards Exit

Flow Visualization Studies

Design Back Pressure

Steady Cruising Design Conditions

Back Pressure Lower than the design conditions

Back Pressure Lower than the design conditions

Back Pressure Lower than the design conditions