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Aerodynamics Material - Taylor & Francis
CopyrightAerodynamics material - Taylor & Francis ______________________________________________________________________ 257 Aerodynamics Symbol List Symbol Definition Units a speed of sound ⁄ a speed of sound at sea level ⁄ A area aspect ratio ‐‐‐‐‐‐‐‐ b wing span c chord length c Copyrightmean aerodynamic material chord- Taylor & Francis specific heat at constant pressure of air · root chord tip chord specific heat at constant volume of air · / quarter chord total drag coefficient ‐‐‐‐‐‐‐‐ , induced drag coefficient ‐‐‐‐‐‐‐‐ , parasite drag coefficient ‐‐‐‐‐‐‐‐ , wave drag coefficient ‐‐‐‐‐‐‐‐ local skin friction coefficient ‐‐‐‐‐‐‐‐ lift coefficient ‐‐‐‐‐‐‐‐ , compressible lift coefficient ‐‐‐‐‐‐‐‐ compressible moment ‐‐‐‐‐‐‐‐ , coefficient , pitching moment coefficient ‐‐‐‐‐‐‐‐ , rolling moment coefficient ‐‐‐‐‐‐‐‐ , yawing moment coefficient ‐‐‐‐‐‐‐‐ ______________________________________________________________________ 258 Aerodynamics Aerodynamics Symbol List (cont.) Symbol Definition Units pressure coefficient ‐‐‐‐‐‐‐‐ compressible pressure ‐‐‐‐‐‐‐‐ , coefficient , critical pressure coefficient ‐‐‐‐‐‐‐‐ , supersonic pressure coefficient ‐‐‐‐‐‐‐‐ D total drag induced drag Copyright material - Taylor & Francis parasite drag e span efficiency factor ‐‐‐‐‐‐‐‐ L lift pitching moment · rolling moment · yawing moment · M mach number ‐‐‐‐‐‐‐‐ critical mach number ‐‐‐‐‐‐‐‐ free stream mach number ‐‐‐‐‐‐‐‐ P static pressure ⁄ total pressure ⁄ free stream pressure ⁄ q dynamic pressure ⁄ R -
Overview of Pressure Coefficient Data in Building Energy Simulation and Airflow Network Programs
PREPRINT: Costola D, Blocken B, Hensen JLM. 2009. Overview of pressure coefficient data in building energy simulation and airflow network programs. Building and Environment. In press. Overview of pressure coefficient data in building energy simulation and airflow network programs D. Cóstola*, B. Blocken, J.L.M. Hensen Building Physics and Systems, Eindhoven University of Technology, the Netherlands Abstract Wind pressure coefficients (Cp) are influenced by a wide range of parameters, including building geometry, facade detailing, position on the facade, the degree of exposure/sheltering, wind speed and wind direction. As it is practically impossible to take into account the full complexity of pressure coefficient variation, Building Energy Simulation (BES) and Air Flow Network (AFN) programs generally incorporate it in a simplified way. This paper provides an overview of pressure coefficient data and the extent to which they are currently implemented in BES-AFN programs. A distinction is made between primary sources of Cp data, such as full- scale measurements, reduced-scale measurements in wind tunnels and computational fluid dynamics (CFD) simulations, and secondary sources, such as databases and analytical models. The comparison between data from secondary sources implemented in BES-AFN programs shows that the Cp values are quite different depending on the source adopted. The two influencing parameters for which these differences are most pronounced are the position on the facade and the degree of exposure/sheltering. The comparison of Cp data from different sources for sheltered buildings shows the largest differences, and data from different sources even present different trends. The paper concludes that quantification of the uncertainty related to such data sources is required to guide future improvements in Cp implementation in BES-AFN programs. -
Upwind Sail Aerodynamics : a RANS Numerical Investigation Validated with Wind Tunnel Pressure Measurements I.M Viola, Patrick Bot, M
Upwind sail aerodynamics : A RANS numerical investigation validated with wind tunnel pressure measurements I.M Viola, Patrick Bot, M. Riotte To cite this version: I.M Viola, Patrick Bot, M. Riotte. Upwind sail aerodynamics : A RANS numerical investigation validated with wind tunnel pressure measurements. International Journal of Heat and Fluid Flow, Elsevier, 2012, 39, pp.90-101. 10.1016/j.ijheatfluidflow.2012.10.004. hal-01071323 HAL Id: hal-01071323 https://hal.archives-ouvertes.fr/hal-01071323 Submitted on 8 Oct 2014 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. I.M. Viola, P. Bot, M. Riotte Upwind Sail Aerodynamics: a RANS numerical investigation validated with wind tunnel pressure measurements International Journal of Heat and Fluid Flow 39 (2013) 90–101 http://dx.doi.org/10.1016/j.ijheatfluidflow.2012.10.004 Keywords: sail aerodynamics, CFD, RANS, yacht, laminar separation bubble, viscous drag. Abstract The aerodynamics of a sailing yacht with different sail trims are presented, derived from simulations performed using Computational Fluid Dynamics. A Reynolds-averaged Navier- Stokes approach was used to model sixteen sail trims first tested in a wind tunnel, where the pressure distributions on the sails were measured. -
Investigation of Sailing Yacht Aerodynamics Using Real Time Pressure and Sail Shape Measurements at Full Scale
18th Australasian Fluid Mechanics Conference Auckland, New Zealand 3-7 December 2012 Investigation of sailing yacht aerodynamics using real time pressure and sail shape measurements at full scale F. Bergsma1,D. Motta2, D.J. Le Pelley2, P.J. Richards2, R.G.J. Flay2 1Engineering Fluid Dynamics,University of Twente, Twente, Netherlands 2Yacht Research Unit, University of Auckland, Auckland, New Zealand Abstract VSPARS for sail shape measurement The steady and unsteady aerodynamic behaviour of a sailing yacht Visual Sail Position and Rig Shape (VSPARS) is a system that is investigated in this work by using full-scale testing on a Stewart was developed at the YRU by Le Pelley and Modral [7]; it is 34. The aerodynamic forces developed by the yacht in real time designed to measure sail shape and can handle large perspective are derived from knowledge of the differential pressures across the effects and sails with large curvatures using off-the-shelf cameras. sails and the sail shape. Experimental results are compared with The shape is recorded using several coloured horizontal stripes on numerical computation and good agreement was found. the sails. A certain number of user defined point locations are defined by the system, together with several section characteristics Introduction such as camber, draft, twist angle, entry and exit angles, bend, sag, Sail aerodynamics is an open field of research in the scientific etc. All these outputs are then imported into the FEPV system and community. Some of the topics of interest are knowledge of the appropriately post-processed. The number of coloured stripes used flying sail shape, determination of the pressure distribution across is arbitrary, but it is common practice to use 3-4 stripes per sail. -
Richard Lancaster [email protected]
Glider Instruments Richard Lancaster [email protected] ASK-21 glider outlines Copyright 1983 Alexander Schleicher GmbH & Co. All other content Copyright 2008 Richard Lancaster. The latest version of this document can be downloaded from: www.carrotworks.com [ Atmospheric pressure and altitude ] Atmospheric pressure is caused ➊ by the weight of the column of air above a given location. Space At sea level the overlying column of air exerts a force equivalent to 10 tonnes per square metre. ➋ The higher the altitude, the shorter the overlying column of air and 30,000ft hence the lower the weight of that 300mb column. Therefore: ➌ 18,000ft “Atmospheric pressure 505mb decreases with altitude.” 0ft At 18,000ft atmospheric pressure 1013mb is approximately half that at sea level. [ The altimeter ] [ Altimeter anatomy ] Linkages and gearing: Connect the aneroid capsule 0 to the display needle(s). Aneroid capsule: 9 1 A sealed copper and beryllium alloy capsule from which the air has 2 been removed. The capsule is springy Static pressure inlet and designed to compress as the 3 pressure around it increases and expand as it decreases. 6 4 5 Display needle(s) Enclosure: Airtight except for the static pressure inlet. Has a glass front through which display needle(s) can be viewed. [ Altimeter operation ] The altimeter's static 0 [ Sea level ] ➊ pressure inlet must be 9 1 Atmospheric pressure: exposed to air that is at local 1013mb atmospheric pressure. 2 Static pressure inlet The pressure of the air inside 3 ➋ the altimeter's casing will therefore equalise to local 6 4 atmospheric pressure via the 5 static pressure inlet. -
Introduction to Aerospace Engineering
Introduction to Aerospace Engineering Lecture slides Challenge the future 1 Introduction to Aerospace Engineering Aerodynamics 11&12 Prof. H. Bijl ir. N. Timmer 11 & 12. Airfoils and finite wings Anderson 5.9 – end of chapter 5 excl. 5.19 Topics lecture 11 & 12 • Pressure distributions and lift • Finite wings • Swept wings 3 Pressure coefficient Typical example Definition of pressure coefficient : p − p -Cp = ∞ Cp q∞ upper side lower side -1.0 Stagnation point: p=p t … p t-p∞=q ∞ => C p=1 4 Example 5.6 • The pressure on a point on the wing of an airplane is 7.58x10 4 N/m2. The airplane is flying with a velocity of 70 m/s at conditions associated with standard altitude of 2000m. Calculate the pressure coefficient at this point on the wing 4 2 3 2000 m: p ∞=7.95.10 N/m ρ∞=1.0066 kg/m − = p p ∞ = − C p Cp 1.50 q∞ 5 Obtaining lift from pressure distribution leading edge θ V∞ trailing edge s p ds dy θ dx = ds cos θ 6 Obtaining lift from pressure distribution TE TE Normal force per meter span: = θ − θ N ∫ pl cos ds ∫ pu cos ds LE LE c c θ = = − with ds cos dx N ∫ pl dx ∫ pu dx 0 0 NN Write dimensionless force coefficient : C = = n 1 ρ 2 2 Vc∞ qc ∞ 1 1 p − p x 1 p − p x x = l ∞ − u ∞ C = ()C −C d Cn d d n ∫ pl pu ∫ q c ∫ q c 0 ∞ 0 ∞ 0 c 7 T=Lsin α - Dcosα N=Lcos α + Dsinα L R N α T D V α = angle of attack 8 Obtaining lift from normal force coefficient =α − α =α − α L Ncos T sin cl c ncos c t sin L N T =cosα − sin α qc∞ qc ∞ qc ∞ For small angle of attack α≤5o : cos α ≈ 1, sin α ≈ 0 1 1 C≈() CCdx − () l∫ pl p u c 0 9 Example 5.11 Consider an airfoil with chord length c and the running distance x measured along the chord. -
Calculation of Optimum Angle of Attack to Determine Maximum Lift To
Journal of Multidisciplinary Engineering Science and Technology (JMEST) ISSN: 3159-0040 Vol. 2 Issue 5, May - 2015 Calculation of Optimum Angle of Attack to Determine Maximum Lift to Drag Ratio of NACA 632-215 Airfoil Haci Sogukpinar Ismail Bozkurt Department of Energy Systems Engineering, Department of Mechanical Engineering, Faculty of Technology, University of Adiyaman, Faculty of Engineering, University of Adiyaman, Adiyaman 02040, Turkey, Adiyaman 02040, Turkey. [email protected] [email protected] Abstract—Wind energy is an important source examined. Gharali and Johnson [4] simulated an to meet future energy needs. Therefore, oscillating free stream over a stationary S809 airfoil investigations on wind power technology are numerically by using ANSYS Fluent for comparison the progressing rapidly. In this study, numerical laminar-turbulent transition with the realizable k–, simulation of airfoil was conducted to determine SST and k–w models. Thumthae and Chitsomboon [5] optimum angle of attack for horizontal axis wind investigated the numerical simulation of horizontal axis turbine. This study simulates air flow around wind turbines with untwisted blade to determine the inclined NACA 632-215 airfoil using SST optimal angle of attack that produces the highest turbulence model. Lift, drag coefficient, lift to drag power output. The computational results of the 12⁰ ratio and power coefficient around the airfoil were pitch was compared favorably with the field calculated and compared with different velocity. experimental data of The National Renewable With the increasing of wind velocity, lift and drag Laboratory. Lee et. al. [6] evaluated the performance coefficient increases and maximum lift to drag of a blade with blunt airfoil which was adapted at the ratio starts to increase then degreases again. -
Potential Equations and Pressure Coefficient For
International Journal of Theoretical & Applied Sciences, 9(1): 35-42(2017) ISSN No. (Print): 0975-1718 ISSN No. (Online): 2249-3247 Potential Equations and Pressure Coefficient for Compressible Flow: Comparison between Compressible and Incompressible Flow in Aerodynamics Menka Yadav * and Santosh Kumar Yadav ** *Research Scholar, J.J.T. University. Rajasthan, India ** Director (A&R), J.J.T. University, Rajasthan, India (Corresponding author: (Corresponding author: Menka Yadav) (Received 02 March, 2017 accepted 05 April, 2017) (Published by Research Trend, Website: www.researchtrend.net) ABSTRACT: We derive the potential equation for slender bodies and seek to understand the flow field equations for subsonic, supersonic and transonic flow in framework of small perturbation. Large amount of heat and mass can be transferred in a efficient way between the surface and fluid when flow is released against the surface. When aircraft passes through several distinct regions, the flow develops a velocity and pressure profile. In stagnation-region large scale turbulent flow affects transfer coefficient. At the face of object total pressure is higher than behind the object. Profile slopes shows that compressible and incompressible flows are related via certain equations. Zero Mach number incompressible medium causes pressure disturbances to move uniformly in all directions. Flow of heat and mass transfer is strongly affected by the geometry of the device. Keywords: Mach number, Pressure drag, Shock wave, Slender bodies, Velocity profile. I. INTRODUCTION called lift, which acts on the wing. Velocity varies along the wing chord and in the direction normal to its surface. Flow having significant changes in fluid density are The region adjacent to the wall, where the velocity known as compressible flow or flow with Mach number increases from zero to freestream value is known as the greater than 0.3 is treated as compressible. -
TOTAL ENERGY COMPENSATION in PRACTICE by Rudolph Brozel ILEC Gmbh Bayreuth, Germany, September 1985 Edited by Thomas Knauff, & Dave Nadler April, 2002
TOTAL ENERGY COMPENSATION IN PRACTICE by Rudolph Brozel ILEC GmbH Bayreuth, Germany, September 1985 Edited by Thomas Knauff, & Dave Nadler April, 2002 This article is copyright protected © ILEC GmbH, all rights reserved. Reproduction with the approval of ILEC GmbH only. FORWARD Rudolf Brozel and Juergen Schindler founded ILEC in 1981. Rudolf Brozel was the original designer of ILEC variometer systems and total energy probes. Sadly, Rudolph Brozel passed away in 1998. ILEC instruments and probes are the result of extensive testing over many years. More than 6,000 pilots around the world now use ILEC total energy probes. ILEC variometers are the variometer of choice of many pilots, for both competition and club use. Current ILEC variometers include the SC7 basic variometer, the SB9 backup variometer, and the SN10 flight computer. INTRODUCTION The following article is a summary of conclusions drawn from theoretical work over several years, including wind tunnel experiments and in-flight measurements. This research helps to explain the differences between the real response of a total energy variometer and what a soaring pilot would prefer, or the ideal behaviour. This article will help glider pilots better understand the response of the variometer, and also aid in improving an existing system. You will understand the semi-technical information better after you read the following article the second or third time. THE INFLUENCE OF ACCELERATION ON THE SINK RATE OF A SAILPLANE AND ON THE INDICATION OF THE VARIOMETER. Astute pilots may have noticed when they perform a normal pull-up manoeuvre, as they might to enter a thermal; the TE (total energy) variometer first indicates a down reading, whereas the non-compensated variometer would rapidly go to the positive stop. -
Flight Evaluation of a Simple Total Energy-Rate System with Potential Wind-Shear Application
I NASA TP 1854 c.1 ,! NASA Technical Paper 1854 Flight Evaluation of a Simple Total Energy-Rate System With Potential Wind-Shear Application Aaron J. Ostroff, Richard M. Hueschen, R. F. Hellbaum, and J. F. Creedon MAY 1981 - Ill TECH LIBRARY KAFB, NM I llllll lllll lllll lllll lllll Ill#lllll1111 Ill 00b77b7 NASA Technical Paper 1854 Flight Evaluation of a Simple Total Energy-Rate System With Potential Wind-Shear Application Aaron J. Ostroff, Richard M. Hueschen, R. F. Hellbaum, and J. F. Creedon LaizgIey Research Ceizter Hrtinptoiz, Virgiizia NASA National Aeronautics and Space Administration Scientific and Technical Information Branch 1981 I SUMMARY Wind shears can create havoc during aircraft terminal area operations and have been cited as the primary cause of several major aircraft accidents. A simple sensor, potentially having application to the wind-shear problem, has been developed to rapidly measure aircraft total energy relative to the air mass. Combining this sensor with either a variometer or a rate-of-climb indi- cator provides a total energy-rate system which has been successfully applied in soaring flight. The measured rate of change of aircraft energy can poten- tially be used on display/control systems of powered aircraft to reduce glide- slope deviations caused by wind shear. This paper describes the experimental flight configuration and evaluations of the energy-rate system. Two mathematical models are developed: the first describes operation of the energy probe in a linear design region and the second model is for the nonlinear region. The calculated total energy rate is compared with measured signals for many different flight tests. -
Fluid Mechanics Policy Planning and Learning
Science and Reactor Fundamentals – Fluid Mechanics Policy Planning and Learning Fluid Mechanics Science and Reactor Fundamentals – Fluid Mechanics Policy Planning and Learning TABLE OF CONTENTS 1 OBJECTIVES ................................................................................... 1 1.1 BASIC DEFINITIONS .................................................................... 1 1.2 PRESSURE ................................................................................... 1 1.3 FLOW.......................................................................................... 1 1.4 ENERGY IN A FLOWING FLUID .................................................... 1 1.5 OTHER PHENOMENA................................................................... 2 1.6 TWO PHASE FLOW...................................................................... 2 1.7 FLOW INDUCED VIBRATION........................................................ 2 2 BASIC DEFINITIONS..................................................................... 3 2.1 INTRODUCTION ........................................................................... 3 2.2 PRESSURE ................................................................................... 3 2.3 DENSITY ..................................................................................... 4 2.4 VISCOSITY .................................................................................. 4 3 PRESSURE........................................................................................ 6 3.1 PRESSURE SCALES ..................................................................... -
Bernoulli? Perhaps, but What About Viscosity?
Volume 6, Issue 1 - 2007 TTTHHHEEE SSSCCCIIIEEENNNCCCEEE EEEDDDUUUCCCAAATTTIIIOOONNN RRREEEVVVIIIEEEWWW Ideas for enhancing primary and high school science education Did you Know? Fish Likely Feel Pain Studies on Rainbow Trout in the United Kingdom lead us to conclude that these fish very likely feel pain. They have pain receptors that look virtually identical to the corresponding receptors in humans, have very similar mechanical and thermal thresholds to humans, suffer post-traumatic stress disorders (some of which are almost identical to human stress reactions), and respond to morphine--a pain killer--by ceasing their abnormal behaviour. How, then, might a freshly-caught fish be treated without cruelty? Perhaps it should be plunged immediately into icy water (which slows the metabolism, allowing the fish to sink into hibernation and then anaesthesia) and then removed from the icy water and placed gently on ice, allowing it to suffocate. Bernoulli? Perhaps, but What About Viscosity? Peter Eastwell Science Time Education, Queensland, Australia [email protected] Abstract Bernoulli’s principle is being misunderstood and consequently misused. This paper clarifies the issues involved, hypothesises as to how this unfortunate situation has arisen, provides sound explanations for many everyday phenomena involving moving air, and makes associated recommendations for teaching the effects of moving fluids. "In all affairs, it’s a healthy thing now and then to hang a question mark on the things you have long taken for granted.” Bertrand Russell I was recently asked to teach Bernoulli’s principle to a class of upper primary students because, as the Principal told me, she didn’t feel she had a sufficient understanding of the concept.