P M V Subbarao Professor Mechanical Engineering Department I I T Delhi

Slides:



Advertisements
Similar presentations
Aerodynamic Characteristics of Airfoils and wings
Advertisements

Boudary Layer.
MAE 3241: AERODYNAMICS AND FLIGHT MECHANICS
Lecture # 3 Airfoil Aerodynamics.
Non-frictional Source of Entropy Generation… P M V Subbarao Professor Mechanical Engineering Department I I T Delhi Rotational Inviscid Flows.
Control on the ground ATC Chapter 2 & 3.
The Stall, Airfoil development, &Wing Lift and Span Effects
Gliding.
Basic Aerodynamic Theory
MAE 3241: AERODYNAMICS AND FLIGHT MECHANICS
Rocket Aerodynamics and Stability
Discovery of A Strong Discontinuity P M V Subbarao Associate Professor Mechanical Engineering Department I I T Delhi A Break Through Finding To Operate.
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.
Aerodynamic Shape Optimization in the Conceptual and Preliminary Design Stages Arron Melvin Adviser: Luigi Martinelli Princeton University FAA/NASA Joint.
Theory of Flight 6.05 Lift and Drag References:
Analysis of Blade Performance in Compressible Flows P M V Subbarao Professor Mechanical Engineering Department Enhanced Effects due to Flow with Snestive.
Aero Engineering 315 Lesson 12 Airfoils Part I. First things first…  Recent attendance  GR#1 review  Pick up handout.
Review Chapter 12. Fundamental Flight Maneuvers Straight and Level Turns Climbs Descents.
Introduction to Aeronautical Engineering
Basic Aerodynamic Theory and Drag
Two-Dimensional Gas Dynamics
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
MAE 1202: AEROSPACE PRACTICUM
MAE 3241: AERODYNAMICS AND FLIGHT MECHANICS
Introduction Aerodynamic Performance Analysis of A Non Planar C Wing using Experimental and Numerical Tools Mano Prakash R., Manoj Kumar B., Lakshmi Narayanan.
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.
MAE 3241: AERODYNAMICS AND FLIGHT MECHANICS
Aero Engineering 315 Lesson 20 Supersonic Flow Part II.
Introduction to Fluid Mechanics
Analysis of Expansion Waves P M V Subbarao Associate Professor Mechanical Engineering Department I I T Delhi Another Zero Cost Nozzle …..
Theory of Flight 6.05 Lift and Drag
2D Airfoil Aerodynamics
BIRD’S AERODYNAMICS.
MAE 3241: AERODYNAMICS AND FLIGHT MECHANICS
Lecture Leading Cadet Training Principles of Flight 3 Drag.
Compressible Frictional Flow Past Wings P M V Subbarao Professor Mechanical Engineering Department I I T Delhi A Small and Significant Region of Curse.
Theory of Flight All are demonstrated by the flight of the bird!
Thin Aerofoil Theory for Development of A Turbine Blade
Airfoils. Airfoil Any surface that provides aerodynamic force through interaction with moving air Moving air Airfoil Aerodynamic force (lift)
Lecture Leading Cadet Training Principles of Flight 2 Lift and Thrust.
Design & Aerodynamics of Inlets & Nozzles P M V Subbarao Professor Mechanical Engineering Department Understanding of Real Flow Through Passive Devices…….
Reflection of Oblique Shocks P M V Subbarao Professor Mechanical Engineering Department I I T Delhi A Train of Waves ….. Where to End ???
Aerodynamic Design of a Light Aircraft
High Speed Flight Chapter 7.
Airfoils, Lift and Bernoulli’s Principle
© 2009 Aviation Supplies & Academics, Inc. All Rights Reserved. The Pilot’s Manual – Ground School Aerodynamics Chapter 1 Forces Acting on an Airplane.
Review of Airfoil Aerodynamics
MAE 3241: AERODYNAMICS AND FLIGHT MECHANICS
Airfoil Any surface that provides aerodynamic force through interaction with moving air Aerodynamic force (lift) Moving air Airfoil.
Aerodynamic Forces Lift and Drag Aerospace Engineering
Airfoils, Lift and Bernoulli’s Principle
Theory of Flight 6.05 Lift and Drag References:
Boudary changed to Boundary Boundary Layer.
Gas Dynamics for Design of Intakes
WING LOADING (W/S), SPAN LOADING (W/b) AND ASPECT RATIO (b2/S)
Airfoils and Simulation
Aerodynamic Forces Lift and Drag Aerospace Engineering
Aerodynamics Lab 6A This lab tends to take a lot of time. For this reason, the lab lectures (aerodynamics and propulsion) are given during a normal class.
Irreversibilities in Propulsion Systems
P M V Subbarao Professor Mechanical Engineering Department
Airfoils.
Introduction to Aeronautical Engineering
Theory of Flight 6.05 Lift and Drag References:
Analysis of Hyperbolic SO-PDES
Airfoils and Simulation
Section 8, Lecture 1, Supplemental Effect of Pressure Gradients on Boundary layer • Not in Anderson.
Drag and Lift Elliott.
Presentation transcript:

P M V Subbarao Professor Mechanical Engineering Department I I T Delhi Supersonic Wings P M V Subbarao Professor Mechanical Engineering Department I I T Delhi An appropriate combination of Shocks & Expansion Waves…

Supersonic Flow Over Flat Plates at Angle of Attack

Review: Oblique Shock Wave Angle

Prandtl-Meyer Expansion Waves q<0 .. We get an expansion wave (Prandtl-Meyer)

• Compare to Flat Plate CD = 0

Wings At Zero Angle of Attack • Subsonic Wing in Subsonic Flow • Subsonic Wing in Supersonic Flow • Supersonic Wing in Subsonic Flow • Supersonic Wing in Supersonic Flow • Wings that work well sub-sonically generally Don’t work well supersonically, and vice-versa

Supersonic Airfoils • A leading edge in Supersonic Flow has a finite maximum wedge angle at which the oblique shock wave remains attached g=1.1 g=1.1 g=1.05 g=1.2 g=1.3 g=1.3 g=1.4 g=1.4 • Beyond that angle shock wave becomes detached from leading edge

Supersonic Flow Over an Airfoil g=1.1 Detached shock wave g=1.3 Localized normal shock wave • Normal Shock wave formed off the front of a blunt leading causes significant drag

Supersonic Airfoils • Double wedge or “diamond” Airfoil section • To eliminate this leading edge drag caused by detached bow wave Supersonic wings are typically quite sharp at the leading edge • Design feature allows oblique wave to attach to the leading edge eliminating the area of high pressure ahead of the wing. g=1.1 g=1.3 • Double wedge or “diamond” Airfoil section

Supersonic Airfoils : Positive Angle of Attack Dull Oblique Shock 2 4 1 6 3 5 Intense Oblique Shock

Supersonic Airfoils : Positive Angle of Attack • A supersonic airfoil at positive angle of attack : A dull shock at the top leading edge. An intense shock at the bottom. • The airflow over the top of the wing is now faster. • Further acceleration through the expansion fans. • The Expansion fan on the top is more intense than the one on the bottom. • Combined result is faster flow and lower pressure on the top of the airfoil. g=1.1 g=1.3 • We already have all of the tools we need to analyze the flow on this wing

Supersonic Airfoils : Negative Angle of Attack

• Result is the airflow over the top of the wing is now faster. •When supersonic airfoil is at negative angle of attack at the top leading edge there is a expansion fan and oblique shock at the bottom. • Result is the airflow over the top of the wing is now faster. • Airflow will also be accelerated through the expansion fans on both sides. • Result is much faster flow on top surface and therefore lower pressure on the top of the airfoil.

Supersonic Flow on Finite Thickness Wings at zero a • Symmetrical Diamond-wedge airfoil, zero angle of attack s i n ( e ) = t / 2 l D r a g = 2 b p l s i n ( e ) - 3 [ ] Þ p2 > p1 D r a g = b p 2 - 3 [ ] t

Supersonic Wave Drag • Finite Wings in Supersonic Flow have drag .. Even at zero angle of attack and no lift and no viscosity…. “wave drag” • Wave Drag coefficient is proportional to thickness ratio (t/c) • Supersonic flow over wings … induced drag (drag due to lift) + viscous drag + wave drag

Symmetric Double-wedge Airfoil … Drag Thickness ratio

• Look at mach number Effect on wave drag • Mach Number tends Increasing mach • Look at mach number Effect on wave drag • Mach Number tends to suppress wave drag Thickness ratio

+ = • How About The effect of angle of attack on drag Induced drag Wave drag + a=0 =

Total drag Mach constant Increasing t/c

The effect of angle of attack on Lift + Lift Coefficient Climbs Almost Linearly with a =

+ = • For Inviscid flow Supersonic Lift to drag ratio almost infinite for very thin airfoil t/c = 0.035 • But airfoils do not fly in inviscid flows + =

+ = t/c = 0.035 • Friction effects have small effect on Nozzle flow or flow in “large “ducts” • But contribute significantly to reduce the performance of supersonic wings + =

Disadvantages of Sharp Edged Wings • Problem with sharp leading edges is poor performance in subsonic flight. • Lead to very high stall speeds, poor subsonic handling qualities, and poor take off and landing performance for conventional aircraft

Wing Sweep Reduces Wave Drag • One way to augment the performance of supersonic aircraft is with wing sweep … • Lowers the speed of flow Normal to the wing … • Decreasing the strength Of the oblique shock wave • Result is a Decrease in wave Drag and enhanced L/D

Geometrical Description of Wing Sweep

Equivalent 2-D Flow on Swept Wing • Freestream Mach number resolved into 3 components i) vertical to wing … ii) in plane of wing, but tangent to leading edge iii) in plane of wing, but normal to leading edge

• Equivalent Mach Number normal to leading edge

• Equivalent angle of attack normal to leading edge

• Equivalent chord and span • Chord is shortened • Span is lengthened

• Equivalent 2-D Lift Coefficient

• Equivalent 2-D Drag Coefficient

• Solve for CL, CD, L/D

• Unswept Wing CL: 0.205 CD: 0.3606 L/D: 5.68441 • 30 Swept Wing CL: 0.2533 CD: 0.03909 L/D: 6.4799 • WOW! … 14% IMPROVEMENT IN PERFORMANCE

F-14 Tomcat The F-14's wing sweep can be varied between 20 and 68° in flight, and is automatically controlled by an air data computer. This maintains the wing sweep to give the optimum lift/drag ratio as the Mach number varies. The system can be manually overridden by the pilot if necessary. When the aircraft is parked, the wings can be swept to 75°, where they overlap the tail to save space on tight carrier decks.