Fluid Mechanics Laboratory University of Kentucky Active Control of Separation on a Wing with Conformal Camber David Munday and Jamey Jacob Department.

Slides:



Advertisements
Similar presentations
Aerodynamic Characteristics of Airfoils and wings
Advertisements

Background Interest is in maximizing the maneuverability of flight vehicles changing lift vector – but it takes time for forces (lift) to change, even.
MAE 3241: AERODYNAMICS AND FLIGHT MECHANICS
Static Extended Trailing Edge for Lift Enhancement: Experimental and Computational Studies T. Liu, J. Montefort, W. Liou Western Michigan University Kalamazoo,
MAE 5130: VISCOUS FLOWS Introduction to Boundary Layers
Pharos University ME 352 Fluid Mechanics II
Separation Control with Nanosecond Pulse Driven Dielectric Barrier Discharge Plasma Actuators Lucio Cota Advisor: Jesse Little Department of Aerospace.
Flow Over Immersed Bodies
Dr. Laila Guessous Suresh Putta, M.S. Student Numerical Investigations of Pulsatile Flows To develop a better understanding of the characteristics of pulsating.
Engineering H191 - Drafting / CAD The Ohio State University Gateway Engineering Education Coalition Lab 4P. 1Autumn Quarter Transport Phenomena Lab 4.
MECH 221 FLUID MECHANICS (Fall 06/07) Chapter 9: FLOWS IN PIPE
Fluid Dynamics Introduction Section 0 Lecture 1 Slide 1 Lecture 21 Slide 1 INTRODUCTION TO Modern Physics PHYX 2710 Fall 2004 Physics of Technology—PHYS.
ME 388 – Applied Instrumentation Laboratory Wind Tunnel Lab
Theoretical & Industrial Design of Aerofoils P M V Subbarao Professor Mechanical Engineering Department An Objective Invention ……
Computation of FREE CONVECTION P M V Subbarao Associate Professor Mechanical Engineering Department IIT Delhi Quantification of Free …….
Synthetic Jet Actuators for Aerodynamic Control
Basic Aerodynamic Theory and Drag
Janusz Podliński, Artur Berendt, Jerzy Mizeraczyk Centre for Plasma and Laser Engineering The Szewalski Institute of Fluid-Flow Machinery Polish Academy.
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
Practical Aspects of using Pitot Tube
Lecture #17 Boundary Layer Measurements  Boundary layer Thickness  * Displacement Thickness  Momentum Thickness.
Laminar flow, turbulent flow and Reynold’s number
Drag Lecture 6 Chapter 3.
Steady control of laminar separation over airfoils with plasma sheet actuators Sosa Roberto Artana Guillermo Laboratorio de Fluidodinámica, Universidad.
Dynamically Variable Blade Geometry for Wind Energy
Prof. Galal Bahgat Salem Aerospace Dept. Cairo University
Lesson 21 Laminar and Turbulent Flow
Study of Oscillating Blades from Stable to Stalled Conditions 1 CFD Lab, Department of Aerospace Engineering, University of Glasgow 2 Volvo Aero Corporation.
Introduction to Fluid Mechanics
LOAD ALLEVIATION ON WIND TURBINE BLADES USING VARIABLE AIRFOIL GEOMETRY Thomas Buhl, Mac Gaunaa, Peter Bjørn Andersen and Christian Bak ADAPWING.
Study of Separated Flow Over Low-Pressure Turbine Blades and Automobiles Using Active Flow Control Strategies Michael Cline Junior Mechanical Engineering.
2D Airfoil Aerodynamics
Cavitation and Hydrodynamic Evaluation of a Uniquely Designed Hydrofoil for Application on Marine Hydrokinetic Turbines R. Phillips, W. Straka, A. Fontaine.
1 Fluidic Load Control for Wind Turbine Blades C.S. Boeije, H. de Vries, I. Cleine, E. van Emden, G.G.M Zwart, H. Stobbe, A. Hirschberg, H.W.M. Hoeijmakers.
REVOLUTIONARY AERODYNAMICS The Sinha- Deturbulator Sumon K. Sinha, Ph.D., P.E, SINHATECH, 3607 Lyles Drive Oxford, Mississippi
Convection in Flat Plate Boundary Layers P M V Subbarao Associate Professor Mechanical Engineering Department IIT Delhi A Universal Similarity Law ……
Laser Energy Deposition for Control of Turbulent Mixing Layers Liliana Saldana University of Arizona Advisor: Dr. Jesse Little Assistant Professor, Department.
Compressible Frictional Flow Past Wings P M V Subbarao Professor Mechanical Engineering Department I I T Delhi A Small and Significant Region of Curse.
Wind Energy Program School of Aerospace Engineering Georgia Institute of Technology Computational Studies of Horizontal Axis Wind Turbines PRINCIPAL INVESTIGATOR:
DNS of Surface Textures to Control the Growth of Turbulent Spots James Strand and David Goldstein The University of Texas at Austin Department of Aerospace.
Laminar flow Also known as streamline flow Occurs when the fluid flows in parallel layers, with no disruption between the layers The opposite of turbulent.
Physical analysis of the electroactive morphing effects around a supercritical wing at high Reynolds number by means of High-Speed PIV Supervised by: Prof.
Heat Transfer Su Yongkang School of Mechanical Engineering # 1 HEAT TRANSFER CHAPTER 6 Introduction to convection.
Aerodynamic Design of a Light Aircraft
GURNEY FLAP By: KASYAP T V S7 M
Control of Boundary Layer Separation and the Wake of an Airfoil Using ns-DBD Plasma Actuators Kenneth Decker Project Advisor: Dr. Jesse Little Department.
Review of Airfoil Aerodynamics
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.
Aerodynamic Forces Lift and Drag Aerospace Engineering
Aerodynamic Force Measurement
AUTHORS: PhD. Hernán Darío Cerón Muñoz. David Diaz Izquierdo
Control of Boundary Layer Structure for Low Re Blades
MAE 3241: AERODYNAMICS AND FLIGHT MECHANICS
Fluid Mechanics & Hydraulics
Delta-Wing Vortex Lift Enhancement Using Oblique Channel Distribution
Airfoils and Simulation
Flow Control over Trapezoidal-Wing Planforms with Sharp Edges
Aerodynamic Forces Lift and Drag Aerospace Engineering
Fundamentals of Convection
Analysis & Control of Profile Losses
Experimental and Numerical Investigation of Controlled, Small-Scale Motions in a Turbulent Shear Layer Bojan Vukasinovic, Ari Glezer Woodruff School of.
Airfoils and Simulation
Low-Re Separation Control by Periodic Suction Surface Motion
Airfoils and Simulation
Section 8, Lecture 1, Supplemental Effect of Pressure Gradients on Boundary layer • Not in Anderson.
Fundamentals of TRANSPORT MECHANISMs
Presentation transcript:

Fluid Mechanics Laboratory University of Kentucky Active Control of Separation on a Wing with Conformal Camber David Munday and Jamey Jacob Department of Mechanical Engineering University of Kentucky 8 January 2001 The 39 th Aerospace Sciences Meeting and Exhibit American Institute of Aeronautics and Astronautics

Fluid Mechanics Laboratory University of Kentucky Outline Motivation Flow Control Adaptive Airfoils Adaptive Wing Model Experimental results Conclusions Further work

Fluid Mechanics Laboratory University of Kentucky Motivation μAVs Re = UAVs Re = High Altitude Other atmospheres (Mars)

Fluid Mechanics Laboratory University of Kentucky Airfoil Performance L/D reduced by more than an order of magnitude as Re falls through 10 5 Figure from McMasters and Henderson

Fluid Mechanics Laboratory University of Kentucky Laminar Separation Bubble Adverse Pressure gradient on a laminar flow causes separation Transition occurs. Fluid is entrained and turbulent flow re-attaches Figure from Lissaman

Fluid Mechanics Laboratory University of Kentucky Flow Control Any method which can modify the flow Can be passive or active –Active flow control can respond to changes in conditions –Requires energy input Active flow control is not a mature technology Shows promise

Fluid Mechanics Laboratory University of Kentucky Active Flow Control Constant sucking or blowing Intermittent sucking and blowing (synthetic jets) –Wygnanski, Glezer –Suggests existence of “sweet spots” in frequency range Mechanical momentum transfer –Modi, V. J. Change of the shape of the wing (Adaptive Airfoils)

Fluid Mechanics Laboratory University of Kentucky Adaptive Airfoils Can change shape to adapt to flow Simple examples: Flaps, Slats, Droops –Move slowly, quasi-static –Change shape parameter (usually camber) to adapt to differing flight regimes Rapid Actuation –Can adapt to rapid changes in flow condition –May produce the same sort of “sweet spot” frequency response as synthetic jets

Fluid Mechanics Laboratory University of Kentucky Some Adaptive Wing Research DARPA smart wing –torsion control of entire wing using internal actuators DDLE wing –rapid change in leading edge radius using mechanical actuator micro Flaps - MITEs (Kroo et. al.) –multiple miniature trailing edge flaps with fixed displacement

Fluid Mechanics Laboratory University of Kentucky Piezoelectric Actuation Rapid actuation requires either large forces or light actuators Piezo-actuators are small and light They are a natural choice for μAV designs

Fluid Mechanics Laboratory University of Kentucky Previous Work Pinkerton and Moses A Feasibility Study To Control Airfoil Shape Using THUNDER, NASA TM 4767

Fluid Mechanics Laboratory University of Kentucky Adaptive Wing Construction NACA 4415 –well measured, room for internal actuator placement Modular (allows variation in aspect ratio) Multiple independent actuators Flexible insulating layer and skin

Fluid Mechanics Laboratory University of Kentucky Adaptive Wing Construction Airfoil Profiles –predicted prior to construction using given actuator placement and full range of actuator motion –actuator displacement increases maximum thickness and moves point of maximum thickness aft

Fluid Mechanics Laboratory University of Kentucky Wing Construction Base 4415 With Cutout With mount-block With Actuator With spars

Fluid Mechanics Laboratory University of Kentucky Adaptive Wing Module A Single Module

Fluid Mechanics Laboratory University of Kentucky Testing Overview Static model force measurements –L/D enhancement using fixed actuator locations Static model PIV –separation control using fixed actuator locations Dynamic model force measurements –L/D enhancement using oscillating actuator motion Dynamic model Flow Visualization –flow control using oscillating actuator motion

Fluid Mechanics Laboratory University of Kentucky Static Model Force Measurements Corrected for Blockage as per Barlow, Rae and Pope, 1999 Wind tunnel tests –L/D declines as actuator displacement decreases then increases as maximum displacement is reached at high AoA

Fluid Mechanics Laboratory University of Kentucky Static Model PIV Separation

Fluid Mechanics Laboratory University of Kentucky Dynamic Model Oscillating upper surface –scanning LDS at 1 inch/sec with 1 Hz oscillation Plot of displacement -vs- time as a distance transducer scans the model. Oscillations can be seen. Units are mV -vs- seconds.

Fluid Mechanics Laboratory University of Kentucky Dynamic Model Force Measurements So far we have only tested at a Re of 25,000 At this Re the forces are quite light They are lost in the noise We expect to have force measurements for higher Re Present model has protrusions on lower surface where the skin attaches Next generation model will have the attachment hardware recessed

Fluid Mechanics Laboratory University of Kentucky Dynamic Model Flow Visualization Flow Visualization is by the smoke wire technique –As described in Batill and Mueller (1981) –A wire doped with oil is stretched across the test section –The wire is heated by Joule heating and the oil evaporates making smoke trails Limited to low Re –Limit due to requirement for laminar flow over wire –Limited to a wire diameter based Re d < 50

Fluid Mechanics Laboratory University of Kentucky Dynamic Model Flow Visualization α = 0˚ Actuator Fixed Actuation 15 Hz

Fluid Mechanics Laboratory University of Kentucky Dynamic Model Flow Visualization α = 9˚ Actuator Fixed Actuation 45 Hz

Fluid Mechanics Laboratory University of Kentucky Conclusions Large static displacement of the actuator shows some improvement in L/D Oscillation of the actuator has a pronounced effect on the size of the separated flow The response to this oscillation does show a “sweet spot” where separation is reduced maximally –15 Hz for 0˚ –20 to 60 Hz for 9˚ with a maximum at 45 Hz

Fluid Mechanics Laboratory University of Kentucky Further Work Expand the range of Re Force measurements of Dynamic Mode –effect on L/D PIV measurements of Dynamic Mode –flow control Phase average PIV data Examine behavior with artificial turbulation Compare gains in performance with power required

Fluid Mechanics Laboratory University of Kentucky Questions?