Flight Loads Analysis of a Maneuvering Transport Aircraft
|
|
- Jennifer Edwards
- 5 years ago
- Views:
Transcription
1 Flight Loads Analysis of a Maneuveing Tanspot Aiaft Hui hang, a, Jie Li, b, Qiong Liu, Shool of Aeonautis, Nothesten Polytehnial Univesity, China Univesidad Politénia de Madid, Spain a hanghui_@6.o, b lijieuihao@63.o, iong@tooja.dt.up.es Keyods: flight load; dynai deivative; dynai aneuves; doublet lattie ethod; ontol sufae Abstat: The pape povides a ethod appliable fo the deteination of flight loads fo aneuveing aiaft, in hih aeodynai loads ae alulated based on doublet lattie ethod, hih ontains thee piay steps. Fistly, non-diensional stability and ontol deivative oeffiients ae obtained though solving unsteady aeodynais in subsoni flo based on a doublet lattie tehnial. These stability and ontol deivative oeffiients ae used in seond step. Seondly, the siulation of aiaft dynai aneuves is opleted utiliing fouth ode Runge-Kutta ethod to solve otion euations in diffeent aneuves to gain esponse paaetes of aiaft due to the otion of ontol sufaes. Finally, the esponse esults alulated in the seond step ae intodued to the alulation of aeodynai loads. Thus, total loads and loads distibution on diffeent oponents of aiaft ae obtained. Aoding to the above ethod, abupt pithing aneuves, olling aneuves and yaing aneuves ae investigated espetively. Intodution Flight loads inluding aeodynai loads and inetia loads ae the oiginal data of aiaft stutue design. Only unde the athe auate stutue loads the designed aiaft an satisfy the given aiaft iteia suh as flight uality iteia, stength iteia. Theefoe the auate pedition of stutue loads is a key fato fo aiaft stutue design hih ipats dietly on the eight of a aiaft, the apaity of aneuveability and the safety of flight. When a pilot anipulates the ontol sufae to ake it otate aoding to an expeting ule, the esponse of aiaft suh as pith, oll o ya ill stat. To deteine loads duing aneuves, the flight ehanis euations of otion need to be solved to obtain the esponse haateistis of the aiaft. On the othe hand, it is neessay to onside the flexible effets on aneuve loads alulation, espeially fo oe highly flexible aiaft [,, 3]. Thus stutual ehanis euations have to be taken into aount siultaneously. Theefoe the auate pedition of aneuve flight loads need to siulate aneuveing aiaft by aeodynai, flight ehanis, and stutual ehanis oupling [, 5]. Hoeve these advaned siulation ethod ay be oplex and involve the use of lage digital oputes, and a ass of alulation tie has to be ost fo a aneuveing flight siulation on the uent opute ondition. Moeove, the agnitude of the nube of load points and onditions ay be investigated fo the aiaft stutue stength design, leading to the teendous diffiulty in deteining the loads fo aneuveing aiaft by opletely using the oupled ethod. In fat, it is the ost ost tie to solve Eule/Navie-Stokes to obtain the unsteady aeodynai loads in the oupled ethod. If this potion of alulation tie an be edued, the above diffiulty ill be oveoe. The alulation tie of solving unsteady aeodynai loads an be geatly edued based on doublet lattie ethod [6, 7]. Of ouse, the auay of solution based on doublet lattie ethod ill dop opae ith Eule/ Navie-Stokes. Wheeas the auay of
2 solution an satisfy the engineeing euieent in initial aiaft design stages. In addition, even fo the detailed design stage the aneuve loads an be deteined though doublet lattie ethod fistly then validating the esults fo Eule/ Navie-Stokes euations. The ethod disussed in the pape is appliable fo the deteination of flight loads fo aneuveing aiaft, in hih aeodynai loads ae alulated based on doublet lattie ethod. Dynai Deivative Coputations The definitions of longitudinal stability deivatives ae given in the euations fo the lift oeffiient and oent oeffiient C = C + C + C + C V V C = C + C + C + C V V h i t Haoni plunging ith aplitude h is onsideed, then i e ω = ω, and E. and E. beoe V h i ω C = ikc k C e t (3) h C = ikc k C e () i ω t In addition, based on a doublet lattie tehnial one an obtain C ( ) i t = Ce ω and C i t = Ce ω, Thus h C = ikc k C (5) h C = ikc k C (6) ( ) Siilaly, if haoni pithing ith aplitude is next onsideed, one an obtain C = C + ik C + C () () (7) C = C + ik C + C (8) Obviously, obining E.5 though E.8 and the esults fo a doublet lattie tehnial, longitudinal stability deivatives ill be obtained. The alulation of lateal-dietional deivatives is siila to that fo the longitudinal deivatives illustated above, in hih haoni sideslip oll and ya otions ae espetively onsideed. In the sae ay, ontol sufaes stability deivatives ith thei angle veloity ill be deteined though haoni otions of ontol sufaes. Dynai Maneuves The euations of otion fo both pithing aneuves and olling aneuves ae deived fo the ok of Jan R. Wight and Jonathan E. Coope in Ref., hih ae epeated espetively as follo. Ue δ δ I + y = M M Mδ (9)
3 Whee, Mδ ρv SC M δ = ρvsc, =. = ρvsc, δ = ρv SC δ, I p L p = L δ δ x p a a M = ρvscm, M = ρvs CM, () Whee, L ρ p = VSb CLp, Lδ = ρv SbC a L δ. a E.9 ay be solved to deteine the esponse oesponding to a patiula elevato input, and E. ay be used to deteine the esponse to any aileon input. The euations of otion fo yaing aneuves ae deived fo Ref.. dβ dt Y Y Y β β δ = δ d Nβ N + Nδ dt [ ( β ) +Δ ] gs gs W β W Lv xcg β S Wb Lv β +ΔxCG AW β Whee, Yβ = CY, Y = C Y +, N = Cn + SW CY, v, WV WV IV V I gsw δ S ( Wb δ S ) W Lv δ +ΔxCG δ Yδ = C Y, Nδ = C n + CY. WV I I E. ay be used to deteine the esponse to any udde input. E.9 to E. ae solved by using fouth ode Runge-Kutta ethod to deteine the tie histoy of aiaft load fato and elated paaetes suh as pith veloity, oll veloity, ya veloity, angle of attak, oll angle and side angle. () The Deteination of Flight Loads fo Maneuveing Aiaft Aoding to the ethod disussed in the pape, the alulation of flight loads fo a aneuveing aiaft is deonstated as follos. Desiption of the Calulation Model. The aeodynai odel is given in Fig., hih inludes the efeene hod of.9, span of.5, Wing, hoiontal tail and vetial tail idealied as lifting sufaes, hile fuselage idealied as slende body and intefeene body. Non-diensional stability and ontol deivative oeffiients ae alulated at Mah nube of.3, the dynai pessue of 637Pa, and listed in Table. The total eight of the aiaft is kg, the ente of gavity is. foad of the intesetion of the fuselage and ing elasti axis, and the entoidal oent of inetia in pith, oll and ya ae 9 kg, 536 kg and 533 kg espetively. Fig. Aeodynai odel Abupt Pith Maneuve. Fo abupt pith aneuve, the initial ondition is Steady level flight, in hih load fato is. Afte aiplane is tied, elevato is defleted ith the axiu available ate, and the deflet angle is deteinate hen load fato beoes the design value in the hole aneuve. The input of elevato angle depited in Fig. (a) is applied to the aiplane, and the
4 esponse esults of pith ate, angle of attak, and load fato ae also desibed in Fig. (a). The oesponding aeodynai loads on diffeent oponents of aiaft vaiation ith tie ae given in Fig.3 (a). The sevee load states of oponents of aiplane on the above ondition an be obtained. Beause abupt pith aneuve is often the itial load ondition of hoiontal tail, elevato and aft fuselage, thei axiu load values have to be onsideed hee. Hoiontal tail load gets a negative axiu value, -67N, at. seond, and a plus axiu value, 7565N, at.89 seond. The esults indiate that hoiontal tail load hange extensively in abupt pith aneuve, even ith ontay dietions. In addition, elevato and fuselage load eah the axiu value, -583N and 59N, at. and.87 seond espetively. Table Non-diensional stability and ontol deivative oeffiients C CM C C M M C C N -. L β C.69 N β C Yp C Lp C Np C Y Y -.3 L.363 N Y a -.8 C -.36 C L.7 Y β C -.9 N δ a Roll Maneuve. Fo oll aneuve, the aileons ae defleted ith the axiu available ate in oll aneuve. When the pesibed angle of oll is eahed, the aileons etun to stop the aneuve. The input of aileon angle depited in Fig. (b) is applied to the aiplane, the esponse esults of oll ate, angle of oll ae desibed in Fig. (b). The oesponding aeodynai loads on ing and aileon of aiaft vaiation ith tie ae given in Fig.3 (b). Tie histoy of aeodynai loads on ing and aileon sho that ight ing load beoe iniu hen left ing load eah the axiu value, and that aileon behave the sae poess as ing. Right ing load is 69799N hen left ing load eah 5N, and ight ing load is 5967N hen left ing beoe 67N. Maxiu left aileon load is N hen ight one is -55N. Ya Maneuve. Fo ya aneuve the udde is defleted ith the axiu available ate in ya aneuve. When the steady angle of side is eahed, the udde etuns to stop the aneuve. The input of udde angle depited in Fig. () is applied to the aiplane, the esponse esults of angle of side and lateal aeleation ae desibed in Fig. (). The oesponding aeodynai loads on vetial tail and udde of aiaft vaiation ith tie ae given in Fig.3 (). The axiu loads of vetial tail and udde ae espetively 95N and 7N. L a. 3 n(g) Delt(deg) Alpha(deg) pith ate(deg/s) 8 oll ate(deg/s) Delta(deg) oll angle(deg) Bny(g) Delty(deg) Beta(deg).8 6. deg g (a) Abupt pith aneuve (b) Roll aneuve () Ya aneuve Fig. Response paaetes vaiation ith tie
5 F_tail(N) F_WFP(N) F_Elevato(N) F_Fuselage(N) 6 F_Ring(N) F_Ling(N) F_LAileon(N) F_RAileon(N) Fy_Vtail(N) Fy_Rudde(N) (a) Abupt pith aneuve (b) Roll aneuve () Ya aneuve Fig.3 Aeodynai loads on diffeent oponents of aiaft vaiation ith tie Suay Flight loads on diffeent oponents of aiplane in diffeent aneuve an be obtained uikly and effetively using the ethod intodued in the pape. Subseuently the sevee load states of oponents of aiplane ae found, hih should be onsideed in stutue design. And the distibution of flight loads on oponents of aiplane auied an be dietly applied to the finite odel in intensity hek of aiaft. In addition, the uent eseahes only onen the alulation of flight loads fo igid odel. Atually, aiaft elastiity has an ipotant ipat on analysis esults and the distibution of flight loads. Aodingly, the alulation of flight loads fo flexible odel ill be aied out subseuently. Aknoledgents This ok as suppoted by the National Siene Foundation of China (Gant No. 9867, 778, 7,). The authos ould like to thank Pofesso LI Fengei fo any insightful tehnial disussions. Refeenes [] Jan R. Wight, and Jonathan E. Coope, Intodution to Aiaft Aeoelastiity and Loads, John Wiley & Sons, Ltd, 7, 66-69, [] Aiaft Design Manual, the 9th Volue: Loads Stength and Stiffness, Bei Jing: Aviation Industy Publishing House,, 8-3. [3] Loax, T.L. Stutue Loads Analysis fo Coeial Tanspot Aiaft: Theoy and patie, AIAA Eduation Seies, 996. [] Andeas Shutte, Gunna Einasson. Nueial Siulation of Maneuveing Aiaft by Aeodynai, Flight Mehanis, and Stutue Mehanis Coupling, Jounal of Aiaft, Vol.6, No., 9. [5] Li Xile, Yang Yong, Nueial Siulation of the Fee Rolling Motion of a Delta Wing Configuation ith Aileon Defletion, Ata Aeonautia et Astonautia Sinia, Vol.33, No.3,. [6] Gay, W.L, and Shenk, K.M., A ethod fo Calulating the Subsoni Steady-State Loading on an Aiplane Wing of Abitay Plan Fo and Stiffness, NACA TN 33,De [7] Albino, E. and Rodden, W.P. A doublet-lattie Method fo Calulating lift distibution on osillating sufaes in subsoni flos. AIAA Jounal, 7().
Determine the Stress Calculating Mode of Sliding Failure of Soil Mass under the Push-Extend Multi-under-Reamed Pile
Engineeing, 014, 6, 54-59 Published Online Apil 014 in SiRes. http://www.sip.og/jounal/eng http://dx.doi.og/10.436/eng.014.6509 Deteine the Stess Calulating Mode of Sliding Failue of Soil Mass unde the
More informationExtra Examples for Chapter 1
Exta Examples fo Chapte 1 Example 1: Conenti ylinde visomete is a devie used to measue the visosity of liquids. A liquid of unknown visosity is filling the small gap between two onenti ylindes, one is
More informationOBSTACLE DETECTION USING RING BEAM SYSTEM
OBSTACLE DETECTION USING RING BEAM SYSTEM M. Hiaki, K. Takamasu and S. Ozono Depatment of Peision Engineeing, The Univesity of Tokyo 7-3-1 Hongo, Bunkyo-ku, Tokyo, Japan Abstat: In this pape, we popose
More informationRecitation PHYS 131. must be one-half of T 2
Reitation PHYS 131 Ch. 5: FOC 1, 3, 7, 10, 15. Pobles 4, 17, 3, 5, 36, 47 & 59. Ch 5: FOC Questions 1, 3, 7, 10 & 15. 1. () The eloity of a has a onstant agnitude (speed) and dietion. Sine its eloity is
More informationFrom E.G. Haug Escape Velocity To the Golden Ratio at the Black Hole. Branko Zivlak, Novi Sad, May 2018
Fom E.G. Haug Esape eloity To the Golden Ratio at the Blak Hole Banko Zivlak, bzivlak@gmail.om Novi Sad, May 018 Abstat Esape veloity fom the E.G. Haug has been heked. It is ompaed with obital veloity
More informationAutodesk Robot Structural Analysis Professional - Verification Manual for Italian Codes
Autodesk Robot Stutual Analysis Pofessional VERIFICATIO MAUAL FOR ITALIA CODES Mah 2014 ITRODUCTIO... 1 COCRETE... 2 1. DM 9/1/96 RC COLUMS... 3 VERIFICATIO EXAMPLE 1 - COLUM SUBJECTED TO AXIAL LOAD AD
More informationRed Shift and Blue Shift: A realistic approach
Red Shift and Blue Shift: A ealisti appoah Benhad Rothenstein Politehnia Uniesity of Timisoaa, Physis Dept., Timisoaa, Romania E-mail: benhad_othenstein@yahoo.om Coina Nafonita Politehnia Uniesity of Timisoaa,
More informationSimulation of a Shielded Thermocouple
ISSN 1014-4874 DOI : http://dx.doi.og/10.4314/j.v27i1.1 Siulation of a Shielded Theoouple Fedik Bentsson 1, Fidèle Ndahayo, Yves Nyalihaa and, Jean Maie Vianney Munyeshyaka 2 1 Linköping Univesity, S-581
More informationThermodynamic and Kinetic Modeling of Phase Transitions for CH4/CO2 Hydrates
Reent Advanes in Meanis, eat & Mass Tansfe and Biology Teodynai and Kineti Modeling of Pase Tansitions fo C/CO ydates BJØRN KAMME, KURAM BAIG, MUAMMAD QASIM, JORDAN BAUMAN Depatent of Pysis and Tenology
More informationRevised Newtonian Formula of Gravity and Equation of Cosmology in Flat Space-Time Transformed from Schwarzschild Solution
Intenational Jounal of Astonomy and Astophysis,,, 6-8 http://dx.doi.og/.46/ijaa.. Published Online Mah (http://www.sip.og/jounal/ijaa) evised Newtonian Fomula of Gavity and Equation of Cosmology in Flat
More informationNon-Ideal Gas Behavior P.V.T Relationships for Liquid and Solid:
hemodynamis Non-Ideal Gas Behavio.. Relationships fo Liquid and Solid: An equation of state may be solved fo any one of the thee quantities, o as a funtion of the othe two. If is onsideed a funtion of
More informationKhmelnik S.I. Mathematical Model of Dust Whirl
Khmelnik S.I. Mathematial Model of Dust Whil Abstat The question of the soue of enegy in a dust whil is onsideed. Atmosphei onditions annot be the sole soue of enegy, as suh dust whils exist on Mas, whee
More informationGRAVITOELECTROMAGNETISM AND NEWTON S LAW OF UNIVERSAL GRAVITATION
GAVITOELECTOMAGNETIM AND NEWTON LAW O UNIVEAL GAVITATION Antoine Ake etied Pofesso, Depatent Industial ienes Uniesity Collee Kaho int-lieen Gent - Beliu ant.ake@skynet.be Abstat In this atile it is shown
More information4) Magnetic confinement of plasma
4) Magneti onfineent of plasa Due to the shielding in the plasa, thee is alost no ontol with eleti fields. A ontol is possible with agneti fields, as patiles ae bound to the field lines. This is alled
More information(conservation of momentum)
Dynamis of Binay Collisions Assumptions fo elasti ollisions: a) Eletially neutal moleules fo whih the foe between moleules depends only on the distane between thei entes. b) No intehange between tanslational
More informationGeneralized Vapor Pressure Prediction Consistent with Cubic Equations of State
Genealized Vapo Pessue Pedition Consistent with Cubi Equations of State Laua L. Petasky and Mihael J. Misovih, Hope College, Holland, MI Intodution Equations of state may be used to alulate pue omponent
More informationDARK MATTER AND THE DYNAMICS OF GALAXIES: A NEWTONIAN APPROACH 1. INTRODUCTION
DARK MATTER AND THE DYNAMICS OF GALAXIES: A NEWTONIAN APPROACH Mugu B. RĂUŢ Coesponding autho: Mugu RĂUŢ, E-mail: m_b_aut@yahoo.om Abstat In this pape I popose a oetion to the well-known Newtonian gavitational
More informationNEW ROTATIONAL DYNAMICS
NEW OTATIONAL DYNAMICS haate of statis Inetia toque piniple and the foe oent the GuagSan Yu ( Habin Mao Dynais Institute. 50066, P.. China ) E-ail:sxzyu5@hotail.o ( 04.8.7 04.9.0 ) Abstat: Textual point
More informationdp p v= = ON SHOCK WAVES AT LARGE DISTANCES FROM THE PLACE OF THEIR ORIGIN By Lev D. Landau J. Phys. U.S.S.R. 9, 496 (1945).
ON SHOCK WAVES AT LARGE DISTANCES FROM THE PLACE OF THEIR ORIGIN By Lev D. Landau J. Phys. U.S.S.R. 9, 496 (1945). It is shown that at lage distanes fom the body, moving with a. veloity exeeding that of
More information1121 T Question 1
1121 T1 2008 Question 1 ( aks) You ae cycling, on a long staight path, at a constant speed of 6.0.s 1. Anothe cyclist passes you, tavelling on the sae path in the sae diection as you, at a constant speed
More informationSAMPLE LABORATORY SESSION FOR JAVA MODULE B. Calculations for Sample Cross-Section 2
SAMPLE LABORATORY SESSION FOR JAVA MODULE B Calulations fo Sample Coss-Setion. Use Input. Setion Popeties The popeties of Sample Coss-Setion ae shown in Figue and ae summaized below. Figue : Popeties of
More informationTORSIONAL VIBRATIONS IN THE SAW UNIT OF A KIND OF CIRCULAR SAW. NUMERICAL INVESTIGATIONS OF THE NATURAL FREQUENCIES AND MODE SHAPES
TRIESKOVÉ A BEZTRIESKOVÉ OBRÁBANIE DREVA, 8(): 7 78, Zvolen, Tehniká univezita vo Zvolene, ISBN 978-8-8-85- 7 TORSIONAL VIBRATIONS IN THE SAW UNIT OF A KIND OF CIRCULAR SAW NUMERICAL INVESTIGATIONS OF
More informationGRAVITOELECTROMAGNETISM AND NEWTON S LAW OF UNIVERSAL GRAVITATION
GAVITOELECTOMAGNETIM AND NEWTON LAW O UNIVEAL GAVITATION Antoine Ake etied Pofesso, Depatent Industial ienes Uniesity Collee Kaho int-lieen Gent - Beliu ant.ake@skynet.be Abstat Takin into aount the kineatis
More informationTHEORETICAL AND EXPERIMENTAL STUDY ON DROPWISE CONDENSATION IN PLATE HEAT EXCHANGERS
Abstat THEORETICAL AND EXPERIMENTAL STUDY ON DROPWISE CONDENSATION IN PLATE HEAT EXCHANGERS V. Bendt, S. Zunft and H. Mülle-Steinhagen Geman Aeospae Cente (DLR), Stuttgat, Gemany This pape desibes the
More informationTime Dilation in Gravity Wells
Time Dilation in Gavity Wells By Rihad R. Shiffman Digital Gaphis Asso. 038 Dunkik Ave. L.A., Ca. 9005 s@isi.edu This doument disusses the geneal elativisti effet of time dilation aused by a spheially
More informationTidal forces. m r. m 1 m 2. x r 2. r 1
Tidal foces Befoe we look at fee waves on the eath, let s fist exaine one class of otion that is diectly foced: astonoic tides. Hee we will biefly conside soe of the tidal geneating foces fo -body systes.
More informationSuppose you have a bank account that earns interest at rate r, and you have made an initial deposit of X 0
IOECONOMIC MODEL OF A FISHERY (ontinued) Dynami Maximum Eonomi Yield In ou deivation of maximum eonomi yield (MEY) we examined a system at equilibium and ou analysis made no distintion between pofits in
More informationeighteen steel construction: column design ELEMENTS OF ARCHITECTURAL STRUCTURES: FORM, BEHAVIOR, AND DESIGN DR. ANNE NICHOLS SPRING 2019 lecture
ELEMENTS OF ARCHITECTURAL STRUCTURES: FORM, BEHAVIOR, AND DESIGN DR. ANNE NICHOLS SPRING 2019 letue eighteen steel onstution: olumn design Co-Ten Steel Sulptue By Rihad Sea Museum of Moden At Fot Woth,
More informationMacroelement Modelling of Laterally Loaded Piles and Pile-groups
1 st Intenational Confeene on Natual Hazads & Infastutue 8-30 June, 016, Chania, Geee Maoelement Modelling of Lateally Loaded Piles and Pile-goups Nikos Geolymos 1 National Tehnial Univesity of Athens
More informationFinite Difference Solution of Mixed Convective Heat Transfer Transient Flow along a Continuously Moving Cooled Plate
Annals of Pue and Applied Mathematis Vol 7, No, 14, 18-6 ISSN: 79-87X (P), 79-888(online) Published on 7 August 14 eseahmathsiog Annals of Finite Diffeene Solution of Mixed Convetive Heat Tansfe Tansient
More information2. Equation of generalized Dynamics. Let rectangular right hand coordinate triple is fixed in three-dimensional Euclidian space.
Genealized Dynamis about Foes Ating on Chage Moving in Capaito and Solenoid. J.G. Klyushin, Ph. D. Aademy of Civil Aviation, hai of applied mathematis; e-mail: klyushin@shaping.og; mail: Intenational Club
More informationChapter 4. Sampling of Continuous-Time Signals
Chapte 4 Sampling of Continuous-Time Signals 1 Intodution Disete-time signals most ommonly ou as epesentations of sampled ontinuous-time signals. Unde easonable onstaints, a ontinuous-time signal an be
More information7.2.1 Basic relations for Torsion of Circular Members
Section 7. 7. osion In this section, the geomety to be consideed is that of a long slende cicula ba and the load is one which twists the ba. Such poblems ae impotant in the analysis of twisting components,
More informationAN ELECTROMAGNETIC LAUNCH SYSTEM FOR UAVs
Tehnial Sienes and Applied athematis AN ELECTROAGNETIC LAUNCH SYSTE FOR UAVs Lauian GHERAN Depatment of Eletonis and Infomatis, Faulty of Aeonautial anagement, Heni Coandă Ai Foe Aademy, Basov, Romania
More informationGame Study of the Closed-loop Supply Chain with Random Yield and Random Demand
, pp.105-110 http://dx.doi.og/10.14257/astl.2014.53.24 Gae Study of the Closed-loop Supply Chain with ando Yield and ando Deand Xiuping Han, Dongyan Chen, Dehui Chen, Ling Hou School of anageent, Habin
More informationPhysics Courseware Modern Physics
Physis Cousewae oden Physis Enegy and oentu Relatiisti oentu: p γ Kineti enegy: K. E. ( γ ) Auxiliay equation: E + 4 p whee is the est ass and E is total enegy. Poble.- What has oe ass at est: i) A sodiu
More informationA second order system
The Link Between The Phase Magin And The Convete Tansient Response Chistophe BASSO ON Seionduto 4, ue Paul Mesplé BP535-335 TOULOUSE Cedex - Fane When designing a losed-loop syste, a swith-ode powe supply
More informationPhotographing a time interval
Potogaping a time inteval Benad Rotenstein and Ioan Damian Politennia Univesity of imisoaa Depatment of Pysis imisoaa Romania benad_otenstein@yaoo.om ijdamian@yaoo.om Abstat A metod of measuing time intevals
More informationChapter 2 Lecture 5 Longitudinal stick fixed static stability and control 2 Topics
hapter 2 eture 5 ongitudinal stik fied stati stability and ontrol 2 Topis 2.2 mg and mα as sum of the ontributions of various omponent 2.3 ontributions of ing to mg and mα 2.3.1 orretion to mα for effets
More informationPLEASE DO NOT REMOVE THIS PAGE
Thank you fo downloading this doument fom the RMIT ReseahR Repositoy Citation: Davy, J, Mahn, J, Kaji, L, Waeing, R and Pease, J 205, 'Compaison of theoetial peditions of adiation effiieny with expeimental
More information1 Fundamental Solutions to the Wave Equation
1 Fundamental Solutions to the Wave Equation Physial insight in the sound geneation mehanism an be gained by onsideing simple analytial solutions to the wave equation. One example is to onside aousti adiation
More informationATMO 551a Fall 08. Diffusion
Diffusion Diffusion is a net tanspot of olecules o enegy o oentu o fo a egion of highe concentation to one of lowe concentation by ando olecula) otion. We will look at diffusion in gases. Mean fee path
More informationExperiment 1 Electric field and electric potential
Expeiment 1 Eleti field and eleti potential Pupose Map eleti equipotential lines and eleti field lines fo two-dimensional hage onfiguations. Equipment Thee sheets of ondutive papes with ondutive-ink eletodes,
More informationGain-Scheduled Controller Design: An Analytic Framework Directly Incorporating Non-Equilibrium Plant Dynamics
Gain-Sheduled Contolle Design: An Analyti Fameok Dietly Inopoating Non-Equilibium Plant Dynamis D.J.Leith W.E.Leithead Abstat Depatment of Eletoni & Eletial Engineeing, Univesity of Stathlyde, GLASGOW
More informationAnswers to Coursebook questions Chapter 2.11
Answes to Couseook questions Chapte 11 1 he net foe on the satellite is F = G Mm and this plays the ole of the entipetal foe on the satellite, ie mv mv Equating the two gives π Fo iula motion we have that
More informationPlanck Quantization of Newton and Einstein Gravitation
Plank Quantization of Newton and Einstein Gavitation Espen Gaade Haug Nowegian Univesity of Life Sienes Mah 0, 06 Abstat In this pape we ewite the gavitational onstant based on its elationship with the
More informationThe Research of AQI Index Changing Regularity Mainly in Tianjin Ziyu Guo
nd Intenational Confeene on Eduation Tehnology, Management and Humanities Siene (ETMHS 06 The Reseah of AQI Index Changing Regulaity Mainly in Tianjin Ziyu Guo Shool of Institute of Eletial and Eletoni
More informationModeling of Vector Controlled Induction Motor in Different Reference Frames
ISSN (Online) : 39-8753 ISSN (Pint) : 347-67 Intenational Jounal of Innovative Reseah in Siene, Engineeing and Tehnology Volume 3, Speial Issue 3, Mah 4 4 Intenational Confeene on Innovations in Engineeing
More informationJournal of Theoretics
Jounal of Theoetis Volume 6-1, Feb-Mah 4 An Altenative Exlanation of the Cosmologial Redshift by the Tahyon Plasma Field in Integalati Sae Takaaki Musha musha@jda-tdi.go.j, musha@jg.ejnet.ne.j MRI, -11-7-61,
More information1 Fundamental Solutions to the Wave Equation
1 Fundamental Solutions to the Wave Equation Physial insight in the sound geneation mehanism an be gained by onsideing simple analytial solutions to the wave equation One example is to onside aousti adiation
More informationmomentum change via particle gain/
Letue 6 asi plasa dynais Ou fluid euations that we developed befoe ae: f ( n n )+ v v n + v v M v f P+ n E+ v 3 4 34 oentu lost via ollisions oentu hange via patile gain/ loss We have looked ollisions
More informationOn Rotating Frames and the Relativistic Contraction of the Radius (The Rotating Disc)
On Rotating Fames and the Relativisti Contation of the Radius (The Rotating Dis) Pantelis M. Pehlivanides Atlanti IKE, Athens 57, Geee ppexl@teemail.g Abstat The elativisti poblem of the otating dis o
More informationCHAPTER 5: Circular Motion; Gravitation
CHAPER 5: Cicula Motion; Gavitation Solution Guide to WebAssign Pobles 5.1 [1] (a) Find the centipetal acceleation fo Eq. 5-1.. a R v ( 1.5 s) 1.10 1.4 s (b) he net hoizontal foce is causing the centipetal
More informationDissolution of Solid Particles in Liquids: A Shrinking Core Model
Wold Aademy of Siene, Engineeing and Tehnology 5 9 Dissolution of Solid Patiles in Liquids: A Shining oe Model Wei-Lun Hsu, Mon-Jyh Lin, and Jyh-Ping Hsu Astat The dissolution of spheial patiles in liquids
More informationAn analytic calculation method on air gap flux in permanent magnet. brushless DC motor with ironless rotor
Intenational Confeene on Enegy and Envionmental Potetion ICEEP 6 An analyti alulation method on ai gap flux in pemanent magnet bushless DC moto with ionless oto Xinghua Wang,Yaolong Sheng andshugang Zhao,,
More informationOptimum Settings of Process Mean, Economic Order Quantity, and Commission Fee
Jounal of Applied Science and Engineeing, Vol. 15, No. 4, pp. 343 352 (2012 343 Optiu Settings of Pocess Mean, Econoic Ode Quantity, and Coission Fee Chung-Ho Chen 1 *, Chao-Yu Chou 2 and Wei-Chen Lee
More information3D Doublet Panel Method
3D Doublet Pal Method V An Issue With Doublet Pals Conside a ut though the body sufae no flow Pals appea as a ies of dite voties with stengths equal to the diffee between adjaent pal stengths. At the ontol
More informationEffect of MFD Viscosity on the Onset of Ferromagnetic Fluid Layer Heated from Below and Cooled from Above with Constant Heat Flux
478/v48-9--x MEASUEMENT SCIENCE EVIEW Volume 9 No 3 9 Effet of MFD Visosity on the Onset of Feomagneti Fluid Laye Heated fom Below and Cooled fom Above with Constant Heat Flux C E Nanjundappa I S Shivakumaa
More informationAnalysis of Heat and Mass Transfer of an Inclined Magnetic Field Pressure-driven Flow Past a Permeable Plate
Available at http://pvamuedu/aam Appl Appl Math ISSN: 1- ol 1 Issue 1 (June 01) pp 1-00 Appliations and Applied Mathematis: An Intenational Jounal (AAM) Analysis of Heat and Mass ansfe of an Inlined Magneti
More informationAdvanced Problems of Lateral- Directional Dynamics!
Advanced Poblems of Lateal- Diectional Dynamics! Robet Stengel, Aicaft Flight Dynamics! MAE 331, 216 Leaning Objectives 4 th -ode dynamics! Steady-state esponse to contol! Tansfe functions! Fequency esponse!
More informationEquivalency of Momentum and Kinetic Energy and Pythagorean Conservation of Mass and Energy
Intenational Jounal of Applied Physis and Matheatis, Vol., No. 4, July quivaleny of Moentu and Kineti negy and Pythagoean Consevation of Mass and negy Mohsen Lutey Abstat Aepted equations in the ehanis
More informationNumerical Modeling in Biomedical Systems
Numeial Modeling in Biomedial Systems BME 15:35 Letue 7 9/6/17 Nonlinea Systems Dunn Chapte 5 Nonlinea equations Root finding Baketing methods Open methods Gaphial Bisetion False Position Newton s method
More informationNOTE. Some New Bounds for Cover-Free Families
Jounal of Combinatoial Theoy, Seies A 90, 224234 (2000) doi:10.1006jcta.1999.3036, available online at http:.idealibay.com on NOTE Some Ne Bounds fo Cove-Fee Families D. R. Stinson 1 and R. Wei Depatment
More informationTest 2 phy a) How is the velocity of a particle defined? b) What is an inertial reference frame? c) Describe friction.
Tet phy 40 1. a) How i the velocity of a paticle defined? b) What i an inetial efeence fae? c) Decibe fiction. phyic dealt otly with falling bodie. d) Copae the acceleation of a paticle in efeence fae
More informationUniaxial Concrete Material Behavior
COMPUTERS AND STRUCTURES, INC., JULY 215 TECHNICAL NOTE MODIFIED DARWIN-PECKNOLD 2-D REINFORCED CONCRETE MATERIAL MODEL Overview This tehnial note desribes the Modified Darwin-Peknold reinfored onrete
More informationConfidence Intervals for the Squared Multiple Semipartial Correlation Coefficient. James Algina. University of Florida. H. J.
Eet Size Conidene Inteval 1 Conidene Intevals o the Squaed Multiple Semipatial Coelation Coeiient by James Algina Univesity o Floida H. J. Keselman Univesity o Manitoba all D. Penield Univesity o Miami
More informationMass Transfer (Stoffaustausch)
Mass Tansfe (Stoffaustaush) Examination 3. August 3 Name: Legi-N.: Edition Diffusion by E. L. Cussle: none nd 3 d Test Duation: minutes The following mateials ae not pemitted at you table and have to be
More informationAPPENDIX D COMPRESSIBILITY FACTOR EQUATIONS D.1 THE REDLICH KWONG EQUATION
AENDIX D COMRESSIBILIY FACOR EQUAIONS D.1 HE REDLICH KWONG EQUAION he Redlih-Kwong equation is atually an equation of state. It was fomulated by Otto Redlih and Joseph N. S. Kwong in 1949 [Chemial Review
More informationATM Rate Based Traffic Control with Bode Principle
4 Intenational Yuanwei Jounal Jing, of Hui Contol, Zeng, Automation, Qingshen Jing, and Systems, and Ping Yuan vol. 6, no., pp. 4-, Apil 8 AM Rate Based affi Contol with Bode Piniple Yuanwei Jing, Hui
More informationDiscrete-Time Immersion and Invariance Adaptive Control of a Slider-crank Mechanism
Pepints of the 9th Wold Congess he Intenational Fedeation of Automati Contol Cape own South Afia August -9 0 Disete-ime Immesion and Invaiane Adaptive Contol of a Slide-an Mehanism Yapa Yalçın Dept of
More informationA Theory of the Podkletnov Effect based on General Relativity: Anti-Gravity Force due to the Perturbed Non-Holonomic Background of Space
July, 007 PROGRESS IN PHYSICS Volume 3 SPECIAL REPORT A Theoy of the Podkletnov Effet based on Geneal Relativity: Anti-Gavity Foe due to the Petubed Non-Holonomi Bakgound of Spae Dmiti Rabounski and Laissa
More informationA Comment on Increasing Returns and Spatial. Unemployment Disparities
The Society fo conomic Studies The nivesity of Kitakyushu Woking Pape Seies No.06-5 (accepted in Mach, 07) A Comment on Inceasing Retuns and Spatial nemployment Dispaities Jumpei Tanaka ** The nivesity
More informationClassical Approach to the Theory of Elementary Particles
Classial Appoah to the Theoy of Elementay Patiles By Yui N. Keilman Abstat: Pesented hee is an attempt to modify /extend lassial eletodynamis (CED) in ode to enable the lassial appoah (the appoah based
More informationFARADAY'S LAW dt
FAADAY'S LAW 31.1 Faaday's Law of Induction In the peious chapte we leaned that electic cuent poduces agnetic field. Afte this ipotant discoey, scientists wondeed: if electic cuent poduces agnetic field,
More informationChapter 9 Dynamic stability analysis III Lateral motion (Lectures 33 and 34)
Pof. E.G. Tulapukaa Stability and contol Chapte 9 Dynamic stability analysis Lateal motion (Lectues 33 and 34) Keywods : Lateal dynamic stability - state vaiable fom of equations, chaacteistic equation
More informationIn electrostatics, the electric field E and its sources (charges) are related by Gauss s law: Surface
Ampee s law n eletostatis, the eleti field E and its soues (hages) ae elated by Gauss s law: EdA i 4πQenl Sufae Why useful? When symmety applies, E an be easily omputed Similaly, in magnetism the magneti
More information3D Modelling of Temperature Dependent Power Distribution During Microwave Annealing of Doped c-si
IOSR Jounal of Eletial and Eletonis Engineeing (IOSR-JEEE) e-issn: 2278-1676,p-ISSN: 2320-3331, Volume 9, Issue 1 Ve. V (Feb. 2014), PP 46-51 3D Modelling of Tempeatue Dependent Powe Distibution Duing
More information8.022 (E&M) Lecture 13. What we learned about magnetism so far
8.0 (E&M) Letue 13 Topis: B s ole in Mawell s equations Veto potential Biot-Savat law and its appliations What we leaned about magnetism so fa Magneti Field B Epeiments: uents in s geneate foes on hages
More informationTransmission Line Analysis of Beam Deflection in a BPM Stripline Kicker
UCR-JC-126073 PREPRINT Tansmission ine Analysis of Beam Defletion in a BPM Stipline Kike Geoge J. Capoaso Yu Ju Chen Bian Poole This pape was pepaed fo submittal to the 1997 Patile Aeleato Confeene Vanouve,
More informationr ˆr F = Section 2: Newton s Law of Gravitation m 2 m 1 Consider two masses and, separated by distance Gravitational force on due to is
Section : Newton s Law of Gavitation In 1686 Isaac Newton published his Univesal Law of Gavitation. This explained avity as a foce of attaction between all atte in the Univese, causin e.. apples to fall
More informationCircular Motion Problem Solving
iula Motion Poblem Soling Aeleation o a hange in eloity i aued by a net foe: Newton nd Law An objet aeleate when eithe the magnitude o the dietion of the eloity hange We aw in the lat unit that an objet
More informationTHE A-TEMPORAL COSMIC SPACE AND A GENERALIZATION OF THE DIRAC EQUATION
THE -TEMPORL COMC PCE N GENERLZTON OF THE RC EQUTON avide Fisaletti aelife nstitute an Loenzo in Camo PU taly fisalettidavide@libeo.it bstat model desibing an a-temoal sae-gavity endowed with a quantum
More informationSome design questions of vertical screw conveyors
Soe design questions of vetical scew conveyos Soe design questions of vetical scew conveyos DR. J. EKŐ Suay Vetical scew conveyos ae hadly entioned in the hoe technical liteatue They ae vey aely applied
More informationE(r,t) = e 3. r 3. (b) Show that the transverse current, J t,is 3n(n e 3 ) e 3
Polem Set 3 (Jakson 6.20).. An example of the pesevation of ausality and finite speed of popagation in spite of the use of the Coulomg gauge is affoded y a unit stength dipole soue that is flashed on and
More informationCorrespondence Analysis & Related Methods
Coespondene Analysis & Related Methods Oveview of CA and basi geometi onepts espondents, all eades of a etain newspape, osstabulated aoding to thei eduation goup and level of eading of the newspape Mihael
More informationOn the Revolving Ferrofluid Flow Due to Rotating Disk
ISSN 1749-3889 (pint), 1749-3897 (online) Intenational Jounal of Nonlinea Siene Vol.13(212) No.3,pp.317-324 On the Revolving Feofluid Flow Due to Rotating Disk Paas Ram, Kushal Shama Depatment of Mathematis,
More informationCenter for Advanced Studies in Measurement and Assessment. CASMA Research Report. Using G Theory to Examine Confounded Effects: The Problem of One
Cente fo Advaned Studies in Measuement and Assessment CASMA Reseah Repot Numbe 51 Using G Theoy to Examine Confounded Effets: The Poblem of One Robet L. Bennan 1 Januay 017 1 Robet L. Bennan is E. F. Lindquist
More informationAddendum to Nonperturbative QED: Muon Structure and Decay
Applied Physis Reseah; Vol. 6, No. 6; 04 ISSN 96-9639 E-ISSN 96-9647 Published by Canadian Cente of Siene and Eduation Addendu to Nonpetubative QED: Muon Stutue and Deay Buke Rithie Lawene Liveoe National
More informationApplication of Poisson Integral Formula on Solving Some Definite Integrals
Jounal of Copute and Electonic Sciences Available online at jcesblue-apog 015 JCES Jounal Vol 1(), pp 4-47, 30 Apil, 015 Application of Poisson Integal Foula on Solving Soe Definite Integals Chii-Huei
More informationIon-sound waves (electrostatic low frequency waves)
OTHER TYPES of WAVES Ion-sound waves (eletostati low fequeny waves) ae longitudinal waves simila lassial sound in gas s kt k M B plasma sound is slow fo eletons, but fast fo ions Eleton density is in eah
More informationEddy Currents and Magnetic Calibrations in LDX using a Copper Plasma. D.P. Boyle, PPPL M.E. Mauel, D.T. Garnier, Columbia J.
Eddy Cuents and Magneti Calibations in LDX using a Coppe Plasma D.P. Boyle PPPL M.E. Mauel D.T. Ganie Columbia J. Kesne MIT PSFC Coppe Plasma Oveview LDX Magnetis Goals Calibate magneti diagnostis positions
More informationVibrational Modes and Instabilities of a Dust Particle Pair in a Complex Plasma
> REPLACE THIS LINE WITH YOUR PAPER IDENTIFICATION NUMBER (DOUBLE-CLICK HERE TO EDIT) < Vibational Modes and Instabilities of a Dust Patile Pai in a Comple Plasma K. Qiao, L. S. Matthews, and T. W. Hyde,
More informationPhysics 218, Spring March 2004
Today in Physis 8: eleti dipole adiation II The fa field Veto potential fo an osillating eleti dipole Radiated fields and intensity fo an osillating eleti dipole Total satteing oss setion of a dieleti
More informationSWIRLING FLOW DOWNSTREAM A FRANCIS TURBINE RUNNER. Gabriel Dan CIOCAN, PhD. Department of Hydraulic Machinery
Sientifi Bulletin of the Politehnia Univesity of Timisoaa Tansations on Mehanis Speial issue The 6 th Intenational Confeene on Hydauli Mahiney and Hydodynamis Timisoaa, Romania, Otobe -, 4 SWIRLING FLOW
More informationPROPAGATION OF PHOTON IN RESTING AND MOVING MEDIUM. J. Zaleśny. Institute of Physics, Technical University of Szczecin, A b s t r a c t
PROPGTION OF PHOTON IN RESTING ND MOVING MEDIUM J Zaleśny Institute of Physis, Tehnial Univesity of Szzein, l 30 70 Piastów 48, Szzein, Poland b s t a t The popagation of photon in a dieleti may be desibed
More informationStress, Cauchy s equation and the Navier-Stokes equations
Chapte 3 Stess, Cauchy s equation and the Navie-Stokes equations 3. The concept of taction/stess Conside the volume of fluid shown in the left half of Fig. 3.. The volume of fluid is subjected to distibuted
More informationInvestigation of the Centrifugal Force Effect to a Revolving Vane (RV) Machine
Pudue Univesity Pudue e-pubs Intenational Compesso Engineeing Confeene Shool of Mehanial Engineeing 01 Investigation of the Centifugal oe Effet to a Revolving Vane (RV) Mahine Alison Subiantoo alis0004@ntu.edu.sg
More informationSpecial Relativity in Acoustic and Electromagnetic Waves Without Phase Invariance and Lorentz Transformations 1. Introduction n k.
Speial Relativit in Aousti and Eletomagneti Waves Without Phase Invaiane and Loentz Tansfomations Benhad Rothenstein bothenstein@gmail.om Abstat. Tansfomation equations fo the phsial quantities intodued
More informationFARADAY'S LAW. dates : No. of lectures allocated. Actual No. of lectures 3 9/5/09-14 /5/09
FARADAY'S LAW No. of lectues allocated Actual No. of lectues dates : 3 9/5/09-14 /5/09 31.1 Faaday's Law of Induction In the pevious chapte we leaned that electic cuent poduces agnetic field. Afte this
More informationLongitudinal Static Stability
ongitudinal Stati Stability Some definitions C m M V S pithing moment without dimensions (so without influene of ρ, V and S) it is a shape parameter whih varies with the angle of attak. Note the hord in
More information