No Acoustical Change” for Propeller-Driven Small Airplanes and Commuter Category Airplanes
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Sept. 12, 1950 W
Sept. 12, 1950 W. ANGST 2,522,337 MACH METER Filed Dec. 9, 1944 2 Sheets-Sheet. INVENTOR. M/2 2.7aar alwg,57. A77OAMA). Sept. 12, 1950 W. ANGST 2,522,337 MACH METER Filed Dec. 9, 1944 2. Sheets-Sheet 2 N 2 2 %/ NYSASSESSN S2,222,W N N22N \ As I, mtRumaIII-m- III It's EARAs i RNSITIE, 2 72/ INVENTOR, M247 aeawosz. "/m2.ATTORNEY. Patented Sept. 12, 1950 2,522,337 UNITED STATES ; :PATENT OFFICE 2,522,337 MACH METER Walter Angst, Manhasset, N. Y., assignor to Square D Company, Detroit, Mich., a corpora tion of Michigan Application December 9, 1944, Serial No. 567,431 3 Claims. (Cl. 73-182). is 2 This invention relates to a Mach meter for air plurality of posts 8. Upon one of the posts 8 are craft for indicating the ratio of the true airspeed mounted a pair of serially connected aneroid cap of the craft to the speed of sound in the medium sules 9 and upon another of the posts 8 is in which the aircraft is traveling and the object mounted a diaphragm capsuler it. The aneroid of the invention is the provision of an instrument s: capsules 9 are sealed and the interior of the cas-l of this type for indicating the Mach number of an . ing is placed in communication with the static aircraft in fight. opening of a Pitot static tube through an opening The maximum safe Mach number of any air in the casing, not shown. The interior of the dia craft is the value of the ratio of true airspeed to phragm capsule is connected through the tub the speed of sound at which the laminar flow of ing 2 to the Pitot or pressure opening of the Pitot air over the wings fails and shock Waves are en static tube through the opening 3 in the back countered. -
Brazilian 14-Xs Hypersonic Unpowered Scramjet Aerospace Vehicle
ISSN 2176-5480 22nd International Congress of Mechanical Engineering (COBEM 2013) November 3-7, 2013, Ribeirão Preto, SP, Brazil Copyright © 2013 by ABCM BRAZILIAN 14-X S HYPERSONIC UNPOWERED SCRAMJET AEROSPACE VEHICLE STRUCTURAL ANALYSIS AT MACH NUMBER 7 Álvaro Francisco Santos Pivetta Universidade do Vale do Paraíba/UNIVAP, Campus Urbanova Av. Shishima Hifumi, no 2911 Urbanova CEP. 12244-000 São José dos Campos, SP - Brasil [email protected] David Romanelli Pinto ETEP Faculdades, Av. Barão do Rio Branco, no 882 Jardim Esplanada CEP. 12.242-800 São José dos Campos, SP, Brasil [email protected] Giannino Ponchio Camillo Instituto de Estudos Avançados/IEAv - Trevo Coronel Aviador José Alberto Albano do Amarante, nº1 Putim CEP. 12.228-001 São José dos Campos, SP - Brasil. [email protected] Felipe Jean da Costa Instituto Tecnológico de Aeronáutica/ITA - Praça Marechal Eduardo Gomes, nº 50 Vila das Acácias CEP. 12.228-900 São José dos Campos, SP - Brasil [email protected] Paulo Gilberto de Paula Toro Instituto de Estudos Avançados/IEAv - Trevo Coronel Aviador José Alberto Albano do Amarante, nº1 Putim CEP. 12.228-001 São José dos Campos, SP - Brasil. [email protected] Abstract. The Brazilian VHA 14-X S is a technological demonstrator of a hypersonic airbreathing propulsion system based on supersonic combustion (scramjet) to fly at Earth’s atmosphere at 30km altitude at Mach number 7, designed at the Prof. Henry T. Nagamatsu Laboratory of Aerothermodynamics and Hypersonics, at the Institute for Advanced Studies. Basically, scramjet is a fully integrated airbreathing aeronautical engine that uses the oblique/conical shock waves generated during the hypersonic flight, to promote compression and deceleration of freestream atmospheric air at the inlet of the scramjet. -
Chapter 5 Dimensional Analysis and Similarity
Chapter 5 Dimensional Analysis and Similarity Motivation. In this chapter we discuss the planning, presentation, and interpretation of experimental data. We shall try to convince you that such data are best presented in dimensionless form. Experiments which might result in tables of output, or even mul- tiple volumes of tables, might be reduced to a single set of curves—or even a single curve—when suitably nondimensionalized. The technique for doing this is dimensional analysis. Chapter 3 presented gross control-volume balances of mass, momentum, and en- ergy which led to estimates of global parameters: mass flow, force, torque, total heat transfer. Chapter 4 presented infinitesimal balances which led to the basic partial dif- ferential equations of fluid flow and some particular solutions. These two chapters cov- ered analytical techniques, which are limited to fairly simple geometries and well- defined boundary conditions. Probably one-third of fluid-flow problems can be attacked in this analytical or theoretical manner. The other two-thirds of all fluid problems are too complex, both geometrically and physically, to be solved analytically. They must be tested by experiment. Their behav- ior is reported as experimental data. Such data are much more useful if they are ex- pressed in compact, economic form. Graphs are especially useful, since tabulated data cannot be absorbed, nor can the trends and rates of change be observed, by most en- gineering eyes. These are the motivations for dimensional analysis. The technique is traditional in fluid mechanics and is useful in all engineering and physical sciences, with notable uses also seen in the biological and social sciences. -
16.00 Introduction to Aerospace and Design Problem Set #3 AIRCRAFT
16.00 Introduction to Aerospace and Design Problem Set #3 AIRCRAFT PERFORMANCE FLIGHT SIMULATION LAB Note: You may work with one partner while actually flying the flight simulator and collecting data. Your write-up must be done individually. You can do this problem set at home or using one of the simulator computers. There are only a few simulator computers in the lab area, so not leave this problem to the last minute. To save time, please read through this handout completely before coming to the lab to fly the simulator. Objectives At the end of this problem set, you should be able to: • Take off and fly basic maneuvers using the flight simulator, and describe the relationships between the control yoke and the control surface movements on the aircraft. • Describe pitch - airspeed - vertical speed relationships in gliding performance. • Explain the difference between indicated and true airspeed. • Record and plot airspeed and vertical speed data from steady-state flight conditions. • Derive lift and drag coefficients based on empirical aircraft performance data. Discussion In this lab exercise, you will use Microsoft Flight Simulator 2000/2002 to become more familiar with aircraft control and performance. Also, you will use the flight simulator to collect aircraft performance data just as it is done for a real aircraft. From your data you will be able to deduce performance parameters such as the parasite drag coefficient and L/D ratio. Aircraft performance depends on the interplay of several variables: airspeed, power setting from the engine, pitch angle, vertical speed, angle of attack, and flight path angle. -
Cavitation Experimental Investigation of Cavitation Regimes in a Converging-Diverging Nozzle Willian Hogendoorn
Cavitation Experimental investigation of cavitation regimes in a converging-diverging nozzle Willian Hogendoorn Technische Universiteit Delft Draft Cavitation Experimental investigation of cavitation regimes in a converging-diverging nozzle by Willian Hogendoorn to obtain the degree of Master of Science at the Delft University of Technology, to be defended publicly on Wednesday May 3, 2017 at 14:00. Student number: 4223616 P&E report number: 2817 Project duration: September 6, 2016 – May 3, 2017 Thesis committee: Prof. dr. ir. C. Poelma, TU Delft, supervisor Prof. dr. ir. T. van Terwisga, MARIN Dr. R. Delfos, TU Delft MSc. S. Jahangir, TU Delft, daily supervisor An electronic version of this thesis is available at http://repository.tudelft.nl/. Contents Preface v Abstract vii Nomenclature ix 1 Introduction and outline 1 1.1 Introduction of main research themes . 1 1.2 Outline of report . 1 2 Literature study and theoretical background 3 2.1 Introduction to cavitation . 3 2.2 Relevant fluid parameters . 5 2.3 Current state of the art . 8 3 Experimental setup 13 3.1 Experimental apparatus . 13 3.2 Venturi. 15 3.3 Highspeed imaging . 16 3.4 Centrifugal pump . 17 4 Experimental procedure 19 4.1 Venturi calibration . 19 4.2 Camera settings . 21 4.3 Systematic data recording . 21 5 Data and data processing 23 5.1 Videodata . 23 5.2 LabView data . 28 6 Results and Discussion 29 6.1 Analysis of starting cloud cavitation shedding. 29 6.2 Flow blockage through cavity formation . 30 6.3 Cavity shedding frequency . 32 6.4 Cavitation dynamics . 34 6.5 Re-entrant jet dynamics . -
A Novel Full-Euler Low Mach Number IMEX Splitting 1 Introduction
Commun. Comput. Phys. Vol. 27, No. 1, pp. 292-320 doi: 10.4208/cicp.OA-2018-0270 January 2020 A Novel Full-Euler Low Mach Number IMEX Splitting 1, 2 2,3 1 Jonas Zeifang ∗, Jochen Sch ¨utz , Klaus Kaiser , Andrea Beck , Maria Luk´aˇcov´a-Medvid’ov´a4 and Sebastian Noelle3 1 IAG, Universit¨at Stuttgart, Pfaffenwaldring 21, DE-70569 Stuttgart, Germany. 2 Faculty of Sciences, Hasselt University, Agoralaan Gebouw D, BE-3590 Diepenbeek, Belgium. 3 IGPM, RWTH Aachen University, Templergraben 55, DE-52062 Aachen, Germany. 4 Institut f¨ur Mathematik, Johannes Gutenberg-Universit¨at Mainz, Staudingerweg 9, DE-55128 Mainz, Germany. Received 15 October 2018; Accepted (in revised version) 23 January 2019 Abstract. In this paper, we introduce an extension of a splitting method for singularly perturbed equations, the so-called RS-IMEX splitting [Kaiser et al., Journal of Scientific Computing, 70(3), 1390–1407], to deal with the fully compressible Euler equations. The straightforward application of the splitting yields sub-equations that are, due to the occurrence of complex eigenvalues, not hyperbolic. A modification, slightly changing the convective flux, is introduced that overcomes this issue. It is shown that the split- ting gives rise to a discretization that respects the low-Mach number limit of the Euler equations; numerical results using finite volume and discontinuous Galerkin schemes show the potential of the discretization. AMS subject classifications: 35L81, 65M08, 65M60, 76M45 Key words: Euler equations, low-Mach, IMEX Runge-Kutta, RS-IMEX. 1 Introduction The modeling of many processes in fluid dynamics requires the solution of the com- pressible Euler equations. -
AC 91-79A CHG 1 Appendix 1 APPENDIX 1
U.S. Department Advisory of Transportation Federal Aviation Administration Circular Subject: Mitigating the Risks of a Runway Date: 4/28/16 AC No: 91-79A Overrun Upon Landing Initiated by: AFS-800 Change: 1 1. PURPOSE. This advisory circular (AC) provides ways for pilots and airplane operators to identify, understand, and mitigate risks associated with runway overruns during the landing phase of flight. It also provides operators with detailed information that operators may use to develop company standard operating procedures (SOP) to mitigate those risks. 2. PRINCIPAL CHANGES. This change to the AC aligns the runway condition reported by airports with the runway condition reported to the pilots per the Runway Condition Assessment Matrix (RCAM) in Appendix 1. It also includes updates to Appendix 3, Tables 3-2 and 3-3 that provide an accurate mathematical process that yields the depicted values, clarifies in the table titles what the tables present, and deletes the Table 3-3 Note to remove redundancy. Additional minor corrections were made to the AC. PAGE CONTROL CHART Remove Pages Dated Insert Pages Dated Appendix 1, Pages 1 thru 4 9/17/14 Appendix 1, Pages 1 thru 3 4/28/16 Appendix 2, Page 2 9/17/14 Appendix 2, Page 2 4/28/16 Appendix 3, Page 2 9/17/14 Appendix 3, Page 2 4/28/16 Appendix 3, Page 5 9/17/14 Appendix 3, Page 5 4/28/16 Appendix 3, Pages 7 and 8 9/17/14 Appendix 3, Pages 7 and 8 4/28/16 Appendix 4, Page 1 9/17/14 Appendix 4, Page 1 4/28/16 ORIGINAL SIGNED by /s/ John Barbagallo Deputy Director, Flight Standards Service U.S. -
Compressible Flow in a Converging-Diverging Nozzle
Compressible Flow in a Converging-Diverging Nozzle Prepared by Professor J. M. Cimbala, Penn State University Latest revision: 19 January 2012 Nomenclature Symbols a speed of sound: a = (kRT)1/2 for an ideal gas A cross-sectional flow area A* critical cross-sectional flow area, at throat when the flow is choked Cp specific heat at constant pressure Cv specific heat at constant volume k ratio of specific heats: k = Cp/Cv (k = 1.4 for air) m mass flow rate through the pipe Ma Mach number: Ma = V/a n index of refraction P static pressure Q or V volume flow rate R specific ideal gas constant: for air, R = 287. m2/(s2K) t time T temperature V mean flow velocity V volume x flow direction y coordinate normal to flow direction, usually normal to a wall z elevation in vertical direction deflection angle for a light beam density of the fluid (for water, 998 kg/m3 at room temperature) Subscripts b back (downstream of converging-diverging nozzle) e exit (at the exit plane of the converging-diverging nozzle) i ideal (frictionless) t throat 0 or T stagnation or total (at a location where the flow speed is nearly zero); e.g. P0 = stagnation pressure Educational Objectives 1. Conduct experiments to illustrate phenomena that are unique to compressible flow, such as choking and shock waves. 2. Become familiar with a compressible flow visualization technique, namely the schlieren optical technique. Equipment 1. supersonic wind tunnel with a converging-diverging nozzle 2. Singer diaphragm flow meter, Model A1-800 3. -
Evaluation of V-22 Tiltrotor Handling Qualities in the Instrument Meteorological Environment
University of Tennessee, Knoxville TRACE: Tennessee Research and Creative Exchange Masters Theses Graduate School 5-2006 Evaluation of V-22 Tiltrotor Handling Qualities in the Instrument Meteorological Environment Scott Bennett Trail University of Tennessee - Knoxville Follow this and additional works at: https://trace.tennessee.edu/utk_gradthes Part of the Aerospace Engineering Commons Recommended Citation Trail, Scott Bennett, "Evaluation of V-22 Tiltrotor Handling Qualities in the Instrument Meteorological Environment. " Master's Thesis, University of Tennessee, 2006. https://trace.tennessee.edu/utk_gradthes/1816 This Thesis is brought to you for free and open access by the Graduate School at TRACE: Tennessee Research and Creative Exchange. It has been accepted for inclusion in Masters Theses by an authorized administrator of TRACE: Tennessee Research and Creative Exchange. For more information, please contact [email protected]. To the Graduate Council: I am submitting herewith a thesis written by Scott Bennett Trail entitled "Evaluation of V-22 Tiltrotor Handling Qualities in the Instrument Meteorological Environment." I have examined the final electronic copy of this thesis for form and content and recommend that it be accepted in partial fulfillment of the equirr ements for the degree of Master of Science, with a major in Aviation Systems. Robert B. Richards, Major Professor We have read this thesis and recommend its acceptance: Rodney Allison, Frank Collins Accepted for the Council: Carolyn R. Hodges Vice Provost and Dean of the Graduate School (Original signatures are on file with official studentecor r ds.) To the Graduate Council: I am submitting herewith a thesis written by Scott Bennett Trail entitled “Evaluation of V-22 Tiltrotor Handling Qualities in the Instrument Meteorological Environment”. -
Introduction
CHAPTER 1 Introduction "For some years I have been afflicted with the belief that flight is possible to man." Wilbur Wright, May 13, 1900 1.1 ATMOSPHERIC FLIGHT MECHANICS Atmospheric flight mechanics is a broad heading that encompasses three major disciplines; namely, performance, flight dynamics, and aeroelasticity. In the past each of these subjects was treated independently of the others. However, because of the structural flexibility of modern airplanes, the interplay among the disciplines no longer can be ignored. For example, if the flight loads cause significant structural deformation of the aircraft, one can expect changes in the airplane's aerodynamic and stability characteristics that will influence its performance and dynamic behavior. Airplane performance deals with the determination of performance character- istics such as range, endurance, rate of climb, and takeoff and landing distance as well as flight path optimization. To evaluate these performance characteristics, one normally treats the airplane as a point mass acted on by gravity, lift, drag, and thrust. The accuracy of the performance calculations depends on how accurately the lift, drag, and thrust can be determined. Flight dynamics is concerned with the motion of an airplane due to internally or externally generated disturbances. We particularly are interested in the vehicle's stability and control capabilities. To describe adequately the rigid-body motion of an airplane one needs to consider the complete equations of motion with six degrees of freedom. Again, this will require accurate estimates of the aerodynamic forces and moments acting on the airplane. The final subject included under the heading of atmospheric flight mechanics is aeroelasticity. -
7. Transonic Aerodynamics of Airfoils and Wings
W.H. Mason 7. Transonic Aerodynamics of Airfoils and Wings 7.1 Introduction Transonic flow occurs when there is mixed sub- and supersonic local flow in the same flowfield (typically with freestream Mach numbers from M = 0.6 or 0.7 to 1.2). Usually the supersonic region of the flow is terminated by a shock wave, allowing the flow to slow down to subsonic speeds. This complicates both computations and wind tunnel testing. It also means that there is very little analytic theory available for guidance in designing for transonic flow conditions. Importantly, not only is the outer inviscid portion of the flow governed by nonlinear flow equations, but the nonlinear flow features typically require that viscous effects be included immediately in the flowfield analysis for accurate design and analysis work. Note also that hypersonic vehicles with bow shocks necessarily have a region of subsonic flow behind the shock, so there is an element of transonic flow on those vehicles too. In the days of propeller airplanes the transonic flow limitations on the propeller mostly kept airplanes from flying fast enough to encounter transonic flow over the rest of the airplane. Here the propeller was moving much faster than the airplane, and adverse transonic aerodynamic problems appeared on the prop first, limiting the speed and thus transonic flow problems over the rest of the aircraft. However, WWII fighters could reach transonic speeds in a dive, and major problems often arose. One notable example was the Lockheed P-38 Lightning. Transonic effects prevented the airplane from readily recovering from dives, and during one flight test, Lockheed test pilot Ralph Virden had a fatal accident. -
Compressible Effects Modelling in Turbulent Cavitating Flows Jean Decaix, Eric Goncalvès Da Silva
Compressible effects modelling in turbulent cavitating flows Jean Decaix, Eric Goncalvès da Silva To cite this version: Jean Decaix, Eric Goncalvès da Silva. Compressible effects modelling in turbulent cav- itating flows. European Journal of Mechanics - B/Fluids, Elsevier, 2013, 39, pp.11-31. 10.1016/j.euromechflu.2012.12.001. hal-00768757 HAL Id: hal-00768757 https://hal.archives-ouvertes.fr/hal-00768757 Submitted on 12 Feb 2013 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. Compressible Effects Modelling in Turbulent Cavitating Flows Jean Decaix∗, Eric Goncalv`es∗ LEGI-Grenoble INP, 1025 rue de la Piscine, 38400 St Martin d’Heres, France Abstract A compressible, multiphase, one-fluid RANS solver has been developed to study turbulent cavitating flows. The interplay between turbulence and cav- itation regarding the unsteadiness and structure of the flow is complex and not well understood. This constitutes a determinant point to accurately sim- ulate the dynamic behaviour of sheet cavities. In the present study, different formulations including compressibility effects on turbulence are investigated. Numerical results are given for two partial cavities on Venturi geometries and comparisons are made with experimental data.