MAE 3241: AERODYNAMICS AND FLIGHT MECHANICS

Slides:



Advertisements
Similar presentations
Aerodynamic Characteristics of Airfoils and wings
Advertisements

MAE 3241: AERODYNAMICS AND FLIGHT MECHANICS
MAE 3241: AERODYNAMICS AND FLIGHT MECHANICS
MAE 5130: VISCOUS FLOWS Introduction to Boundary Layers
MAE 3241: AERODYNAMICS AND FLIGHT MECHANICS
Effect of Different Nose Profiles on Subsonic Pressure Coefficients
MAE 1202: AEROSPACE PRACTICUM Lecture 12: Swept Wings and Course Recap April 22, 2013 Mechanical and Aerospace Engineering Department Florida Institute.
AE 1350 Lecture Notes #8. We have looked at.. Airfoil Nomenclature Lift and Drag forces Lift, Drag and Pressure Coefficients The Three Sources of Drag:
U5AEA15 AIRCRAFT STRUCTURES-II PREPARED BY Mr.S.Karthikeyan DEPARTMENT OF AERONAUTICALENGINEERING ASSISTANT PROFESSOR.
Flow Over Immersed Bodies
ME403 Chapter 3 Wing Aerodynamics
6.07 Stalls References: FTGU pages 18, 35-38
Lesson 13 Airfoils Part II
Analysis of Blade Performance in Compressible Flows P M V Subbarao Professor Mechanical Engineering Department Enhanced Effects due to Flow with Snestive.
Parts of an Aircraft Parts of an Aircraft Gateway To Technology®
AE 1350 Lecture Notes #7 We have looked at.. Continuity Momentum Equation Bernoulli’s Equation Applications of Bernoulli’s Equation –Pitot’s Tube –Venturi.
Lesson 2-2a Principles of Flight
Aerodynamic Forces Lift and Drag Aerospace Engineering
MAE 3241: AERODYNAMICS AND FLIGHT MECHANICS
Drag Lecture 6 Chapter 3.
MAE 3241: AERODYNAMICS AND FLIGHT MECHANICS
Ch9 Linearized Flow 9.1 Introduction
MAE 3241: AERODYNAMICS AND FLIGHT MECHANICS Compressible Flow Over Airfoils: Linearized Subsonic Flow Mechanical and Aerospace Engineering Department Florida.
MAE 3241: AERODYNAMICS AND FLIGHT MECHANICS Review: Bernoulli Equation and Examples Mechanical and Aerospace Engineering Department Florida Institute of.
Prof. Galal Bahgat Salem Aerospace Dept. Cairo University
Pharos University ME 253 Fluid Mechanics II
MAE 3241: AERODYNAMICS AND FLIGHT MECHANICS
MAE 1202: AEROSPACE PRACTICUM Lecture 11: Finite Wings April 15, 2013 Mechanical and Aerospace Engineering Department Florida Institute of Technology D.
Aero Engineering 315 Lesson 20 Supersonic Flow Part II.
P M V Subbarao Professor Mechanical Engineering Department I I T Delhi
Introduction to Fluid Mechanics
Incompressible Flow over Airfoils
Airfoil Terminology and Pressure Distribution Lecture 3 Chapter 2.
2D Airfoil Aerodynamics
Aerodynamic Forces Lift and Drag.
Introduction to Fluid Mechanics
1 MAE 3241: AERODYNAMICS AND FLIGHT MECHANICS Finite Wings: General Lift Distribution Summary April 18, 2011 Mechanical and Aerospace Engineering Department.
MAE 3241: AERODYNAMICS AND FLIGHT MECHANICS
Theory of Flight All are demonstrated by the flight of the bird!
CE 1501 Flow Over Immersed Bodies Reading: Munson, et al., Chapter 9.
Thin Aerofoil Theory for Development of A Turbine Blade
MAE 4261: AIR-BREATHING ENGINES
MAE 3241: AERODYNAMICS AND FLIGHT MECHANICS
External flow over immersed bodies If a body is immersed in a flow, we call it an external flow. Some important external flows include airplanes, motor.
Panel methods to Innovate a Turbine Blade -2 P M V Subbarao Professor Mechanical Engineering Department A Linear Mathematics for Invention of Blade Shape…..
Aerodynamic Design of a Light Aircraft
High Speed Flight Chapter 7.
Beard & McLain, “Small Unmanned Aircraft,” Princeton University Press, 2012, Chapter 4: Slide 1 Chapter 4 Forces and Moments.
CGS Ground School Principles Of Flight Drag © Crown Copyright 2012
6.01 Aircraft Design and Construction References: FTGU pages 9-14, 27
Review of Airfoil Aerodynamics
The concept of the airfoil (wing section)
Streamlined body - flow follows contours of body : Bluff body
P M V Subbarao Professor Mechanical Engineering Department
Airfoil Any surface that provides aerodynamic force through interaction with moving air Aerodynamic force (lift) Moving air Airfoil.
MAE 5380: AIR-BREATHING ENGINE INLETS
Aerodynamic Forces Lift and Drag Aerospace Engineering
DRAG REDUCTION OF AIRPLANES - INDUCED DRAG
Control of Boundary Layer Structure for Low Re Blades
MAE 3241: AERODYNAMICS AND FLIGHT MECHANICS
Airfoils, Lift and Bernoulli’s Principle
MAE 5360: Hypersonic Airbreathing Engines
c/Maj Christopher Greves
Subject Name: AIRCRAFT PROPULSION Subject Code: 10AE55
MAE 5360: Hypersonic Airbreathing Engines
Analysis of Boundary Layer flows
Aerodynamic Forces Lift and Drag Aerospace Engineering
Ch14 Transonic Flow -drag divergence phenomena, rapid shift of center of pressure unsteady and somewhat unpredictable effects of shock waves on the control.
Unit 2 Unmanned Aircraft
Section 8, Lecture 1, Supplemental Effect of Pressure Gradients on Boundary layer • Not in Anderson.
Presentation transcript:

MAE 3241: AERODYNAMICS AND FLIGHT MECHANICS Compressible Flow Over Airfoils: Linearized Supersonic Flow Mechanical and Aerospace Engineering Department Florida Institute of Technology D. R. Kirk

SMALL PERTURBATION VELOCITY POTENTIAL EQUATION Equation is a linear PDE and easy to solve Recall: Equation is no longer exact Valid for small perturbations Slender bodies Small angles of attack Subsonic and Supersonic Mach numbers Keeping in mind these assumptions equation is good approximation Nature of PDE: Subsonic: (1 - M∞2) > 0 (elliptic) Supersonic: (1 - M∞2) < 0 (hyperbolic)

SUPERSONIC APPLICATION Linearized small perturbation equation Re-write for supersonic flow Solution has functional relation May be any function of (x - ly) Perturbation potential is constant along lines of x – ly = constant

DERIVATION OF PRESSURE COEFFICIENT, CP Solutions to hyperbolic wave equation Velocity perturbations Eliminate f’ Linearized flow tangency condition at surface Linearized definition of pressure coefficient Combined result Positive q: measured above horizontal Negative q: measured below horizontal

KEY RESULTS: SUPERSONIC FLOWS Linearized supersonic pressure coefficient Expression for lift coefficient Thin airfoil or arbitrary shape at small angles of attack Expression for drag coefficient

EXAMPLE: FLAT PLATE

TRANSONIC AREA RULE Drag created related to change in cross-sectional area of vehicle from nose to tail Shape itself is not as critical in creation of drag, but rate of change in shape Wave drag related to 2nd derivative of volume distribution of vehicle

EXAMPLE: YF-102A vs. F-102A

EXAMPLE: YF-102A vs. F-102A

CURRENT EXAMPLES No longer as relevant today – more powerful engines F-5 Fighter Partial upper deck on 747 tapers off cross-sectional area of fuselage, smoothing transition in total cross-sectional area as wing starts adding in Not as effective as true ‘waisting’ but does yield some benefit. Full double-decker does not glean this wave drag benefit (no different than any single-deck airliner with a truly constant cross-section through entire cabin area)

SUPERCRITICAL AIRFOILS Supercritical airfoils designed to delay and reduce transonic drag rise, due to both strong normal shock and shock-induced boundary layer separation Relative to conventional, supercritical airfoil has: Reduced amount of camber Increased leading edge radius Small surface curvature on suction side Concavity in rear part of pressure side

SUPERCRITICAL AIRFOILS

SUPERCRITICAL AIRFOILS For given thickness, supercritical airfoil allows for higher cruise velocity For given cruise velocity, airfoil thickness may be larger Structural robustness, lighter weight, more volume for increased fuel capacity 757 wing