Effect of L/D Ratio on the Performance of a Four-Lobe Pressure Dam Bearing
|
|
- Lesley Evangeline Lewis
- 6 years ago
- Views:
Transcription
1 Vol:, No:8, 007 Effect of L/D Ratio on te Performance of a Four-Lobe Pressure Dam Bearin G Busan, S S Rattan, and N P Meta International Science Index, Mecanical and Mecatronics Enineerin Vol:, No:8, 007 wasetor/publication/6 Abstract A four-lobe pressure dam bearin wic is produced by cuttin two pressure dams on te upper two lobes and two relief-tracks on te lower two lobes of an ordinary four-lobe bearin is found to be more stable tan a conventional four-lobe bearin In tis paper a four-lobe pressure dam bearin supportin riid and flexible rotors is analytically investiated to determine its performance wen L/D ratio is varied in te rane 075 to 5 Te static and dynamic caracteristics are studied at various L/D ratios Te results sow tat te stability of a four-lobe pressure dam bearin increases wit decrease in L/D ratios bot for riid as well as flexible rotors Keywords Four-lobe pressure dam bearin, finite-element metod, L/D ratio I INTRODUTION HE present trend in te industry is to run te T turbomacines at i speeds Te ordinary circular bearins, wic are te most common type of te bearins, are found to be unstable at i speeds It is found tat te stability of tese bearins can be increased by te use of multilobes and te incorporation of pressure dams in te lobes Te analysis of multi-lobe bearins was first publised by Pinkus [] It was followed by Lund and Tomson [] and Malik [] et al, wo ave some desin data wic included bot static and dynamic caracteristics for laminar, as well as turbulent flow reimes Te experimental stability analysis of suc types of bearin []-[5] sowed tat te analytical stability analysis reflects te eneral trends in experimental data Te analytical dynamic analysis as sown tat noncylindrical pressure dam bearinsare found to be very stable L/D ratio is one of te important [6]-[9] parameters tat affects te stability of a bearin Te effect of L/D ratio on te stability of circular bearins was discussed by Lund [0], Badley [] et al and Hori[] Te effect of L/D ratio on te performance of two-lobe and tree-lobe pressure dam bearins was studied by Meta [] and Rattan [] respectively Te present study is undertaken to investiate Manuscript received October 5, 007 G Busan is wit te National Institute of Tecnoloy, Kuruksetra- 69, Haryana, India (pone: 9-7-6; fax: ; e- mail: aroraian@ yaoocom) SS Rattan is wit te National Institute of Tecnoloy, Kuruksetra- 69, Haryana, India ( ss_rattan@otmailcom) NP Meta is Director, MME, Mullana, Ambala, Haryana, India ( npmeta@yaoocoin) te effect of L/D ratio on te performance of a four-lobe pressure dam bearin supportin riid and flexible rotors II NOMENLATURE c : radial clearance c m : minimum film tickness for a centered saft,,, : oil-film dampin coefficients xy yx yy xy, yx, yy, : dimensionless oil-film dampin coefficients, ( ω c / W ) 0,,,, : coefficients of te caracteristic equation D : diameter e : eccentricity F : dimensionless saft flexibility, W / ck : oil-film tickness, c ( cosθ ) : dimensionless oil-film tickness, / c k : saft stiffness K, K, K, K : oil-film stiffness coefficients xy yx yy K K xy, K yx, K yy, : dimensionless oil-film stiffness coefficients, K K ( c / W ) L : bearin lent N : journal rotational speed O i : lobe center of lobe i (i,,,) p : oil-film pressure R : journal radius μnld R S : Sommerfeld no, W c V : periperal speed of journal W : bearin external load x, z : coordinates for bearin surface (xperiperal, z-alon saft axis) φ : attitude anle α : wirl rate ratio, α φ / ω International Scolarly and Scientific Researc & Innovation (8) scolarwasetor/07-689/6
2 Vol:, No:8, 007 International Science Index, Mecanical and Mecatronics Enineerin Vol:, No:8, 007 wasetor/publication/6 β : squeeze rate ratio, β / ω : eccentricity ratio, e / c δ : ellipticity ratio, ( c m / c) θ : anle measured from te line of centers in te direction of rotation θ : oil-roove anle ρ μ ω v : fluid density : averae fluid viscosity : rotational speed : dimensionless tresold speed, / ω ( c / ) : ravitational acceleration const III ANALYSIS Te Reynolds Equation for te laminar flow is: x μ x z μ z x Te above equation is non-dimensionalized by makin te followin substitutions: Te non-dimensionalized equation tus obtained is: p x x p π α sin x Te various assumptions made in te derivation of te Reynolds Equation are tat te fluid is Newtonian, no slip occurs at te bearin surface, inertia terms are nelected, oil viscosity is constant and curvature is neliible Te Reynolds equation is analysed for a pressure profile usin te finite element metod[5] Te eometry of a four-lobe pressure dam bearin is sown in Fi A four-lobe pressure dam bearin is produced by cuttin two pressure dams on te upper two lobes and two relieftracks on te lower two lobes of an ordinary four-lobe bearin Te various eccentricity ratios and attitude anles of te lobes of te four-lobe pressure dam bearin are iven by: π β cos x D L x z πp c x, z,, p, D x x L ce,, μω φ R θ x α and β R D c ω ω p 6Rω φ sinθ e cosθ () δ δ cos( π / φ) δ δ sin( π / φ) p z z δ δ sin( π / φ) δ δ cos( π / φ) π x () () φ 5π / γ sin φ 7π / γ sin φ π / γ sin φ π / γ sin ( (sinπ / φ) ( (cosπ / φ) ( (cosπ / φ) ( (sin π / φ) Fi A four-lobe pressure dam bearin Eac lobe of te bearin is analysed separately Since te pressure profile as to be symmetrical about te bearin centre line, only alf of te lobe is taken for analysis Fluid pressures at nodal points are taken by applyin te Reynolds boundary conditions Te mes size used is x 5 for eac lobe Te resultin matrix is stored in a banded form Ten it is solved by te Gauss-elimination metod Stiffness and dampin coefficients are determined separately for eac lobe and ten added Te values of tese stiffness and dampin coefficients, saft flexibility, and dimensionless speed are ten used to evaluate te coefficients of te caracteristic equation, wic is a polynomial of te 6t order for flexible rotors Tis caracteristic equation as been taken from Han [6] and is obtained from te eneral case of an eccentrically mounted rotor on a flexible saft s s 6 Te caracteristic equation is: F v were 5 v 0 s v ( F F ) ( v F F0 v v F ) ( F ) s ( Fv v ) s v Step Relief track s 0 Lobe Oil supply R o φ o θ o o Step o o Lobe Lobe W 0 Lobe Relief track () International Scolarly and Scientific Researc & Innovation (8) scolarwasetor/07-689/6
3 Vol:, No:8, 007 o yy xy yx 0 K yy K K yy K yy K yy K yy K xy K yx K xy yx K yx xy (5) EENTRIITY RATIO L/D 075 L/D 0 L/D 5 International Science Index, Mecanical and Mecatronics Enineerin Vol:, No:8, 007 wasetor/publication/6 For a riid rotor, te value of F (dimensionless flexibility) is taken as zero Te value of F for most of te practical rotors vary from 05 to 0 and te same as been considered for te case of flexible rotors Te system is considered as stable if te real part of all roots is neative For a particular bearin eometry and eccentricity ratio, te values of dimensionless speed are increased until te system becomes unstable Te maximum value of speed for wic te bearin is stable is ten adopted as te dimensionless tresold speed Te present analysis as been done for te bearin wit te followin parameters wic ave been optimized for te best stability[7] S d 0, L d 08, L t 05, θ s 55, θ 0 Te ellipticity ratio ( δ ) 05 is selected for te present study Te value of L/D ratio is varied from 075 to 5 and te bearin is investiated for its static and dynamic caracteristics IV RESULTS AND DISUSSION Te effect of L/D ratio on te static caracteristics of a four-lobe pressure dam bearin is sown in Fis to 6 Te values of L/D ratios considered for tis purpose are 075, 0 and 5 It is observed from te Fis and tat wit te increase in L/D ratio, eccentricity ratio decreases wereas, te attitude anle increases for a particular value of Sommerfeld number Te minimum film tickness is observed to increase wit an increase in L/D ratio, wen considered for a particular value of Sommerfeld number (Fi ) Fis 5 and 6 sow te effect of L/D ratio on oil-flow and friction coefficients Tere is a considerable fall in te oil-flow, wereas tere is no sinificant cane in te friction coefficient wit te increase in L/D ratio wen considered for a particular value of Sommerfeld number Te effect of L/D ratio on te stability of a four-lobe bearin supportin a riid rotor is sown in Fiure 7 Te plots sow tat bot te zone of infinite stability and te minimum tresold speed increase wit decrease in L/D ratio Te zone of infinite stability increases from 06 to 0 and te minimum tresold speed from 9 to 865 wen L/D ratio decreases from 5 to 075 Tese effects are due to reduction in load carryin capacity of te bearin ATTITUDE ANGLE MINIMUM FILM THIKNESS Fi Effect of L/D ratio on eccentricity ratio L/D 075 L/D 05 L/D Fi Effect of L/D ratio on attitude anle L/D 075 L/D 0 L/D Fi Effect of L/D ratio on minimum film tickness International Scolarly and Scientific Researc & Innovation (8) scolarwasetor/07-689/6
4 Vol:, No:8, 007 FLOW OEFFIIENT L/D 075 L/D 0 L/D reduced wit te increase in flexibility of te rotor wile tere is no cane in te zone of infinite stability 00 0 Stable Unstable L / D 075 L / D 0 L / D 5 International Science Index, Mecanical and Mecatronics Enineerin Vol:, No:8, 007 wasetor/publication/6 FRITION OEFFIIENT Fi 5 Effect of L/D ratio on flow coefficient L/D 075 L/D 0 L/D Fi 6 Effect of L/D ratio on friction coefficient FOUR-LOBE PRESSURE DAM BEARING 0 0 Fi 7 Effect of L/D ratio on te stability of a four-lobe dam bearin supportin a riid rotor (F0) L/D 075 L/D 0 L/D 5 pressure Fis 8 and 9 sow te effect of L/D ratio on te stability of a four-lobe bearin supportin flexible rotors Te results are found to be similar to tat of te bearin supportin a riid rotor It is also observed from tese plots of te stability tat for a particular L/D ratio te minimum tresold speed is 0 0 Fi 8 Effect of L/D ratio on te stability of a four-lobe dam bearin supportin a flexible rotor (F05) 00 0 Stable Unstable L / D 075 L / D 0 L / D 5 pressure 0 0 Fi 9 Effect of L/D ratio on te stability of a four-lobe pressure dam bearin supportin a flexible rotor (F0) V ONLUSION Te eccentricity ratio decreases wile attitude increases wit an increase in L/D ratio Te minimum oil-film tickness increases wit an increase in L/D ratio Te oil flow coefficient decreases wit an increase in L/D ratio Te friction coefficient remains almost uncaned wit an increase in L/D ratio 5 Bot te minimum tresold speed and te zone of infinite stability increase wit decrease in L/D ratio for a four-lobe bearin supportin riid rotor as well as flexible rotor Terefore te stability of a four-lobe pressure dam bearin increases wit decrease in L/D ratio International Scolarly and Scientific Researc & Innovation (8) scolarwasetor/07-689/6
5 Vol:, No:8, For a particular L/D ratio te minimum tresold speed reduces wit increase in te rotor flexibility wile te zone of infinite stability remains uncaned International Science Index, Mecanical and Mecatronics Enineerin Vol:, No:8, 007 wasetor/publication/6 REFERENES [] O Pinkus, Analysis and aracteristics of Tree-Lobe Bearins, ASME Journal of Basic Enineerin, vol 8, pp 9, 959 [] J W Lund, and K K Tomson, A alculation Metod and Data for te Dynamic oefficients of Oil Lubricated Journal Bearins, Proceedins of te ASME Desin and Enineerin onference, Minneapolis, pp, 978 [] M Malik, Maes andra and R Sinasan, Desin Data for Offset- Halves Journal Bearins in Laminar and Turbulent Flow Reimes, ASLE Trans, pp -0, 98 [] J Nicolas, L E Barrett, and M E Leader, Experimental Teoretical omparison of Instability Onset Speeds for a Tree Mass Rotor Supported by Step Journal Bearin, Trans ASME, Journal of Mecanical Desin, pp -5, 980 [5] R D Flack, M E Leader, and E J Gunter, An Experimental Investiation on te Response of a Flexible Rotor Mounted in Pressure Dam Bearins, Trans ASME, Journal of Mecanical Desin, pp 8-850, 980 [6] N P Meta, A Sin, and B K Gupta, Dynamic Analysis of Finite Half-Elliptical Pressure Dam Bearins wit Rotor Flexibility Effects, ASLE Trans, vol 9, no, pp 6-66, 986 [7] N P Meta, and A Sin Stability of Finite Ortoonally-Displaced Pressure Dam Bearins, ASME Journal of Triboloy, vol 09, no, pp 78-70, 987 [8] N P Meta, and S S Rattan, Performance of Tree-Lobe Pressure Dam Bearins, Wear, pp 8-85, 99 [9] N P Meta, S S Rattan, and G Busan, Static and Dynamic aracteristics of Four-Lobe Pressure Dam Bearins, Triboloy Letters, vol 5, no, pp 5-0, 00 [0] J W Lund, Self-excited stationary wirl orbits of a journal in sleeve bearins, PD Tesis, Rensselaer Polytecnic Institute, NY, 966 [] R H Badley, and J F Booker, Turborotor Instability: Effect of Initial Transients on Plane Motion, Trans ASME, Journal of Lubrication Tecnoloy, pp 65-6, 969 [] Y Hori, A Teory of Oil Wip, Trans ASME, Series E, pp89, 959 [] N P Meta, A Sin, and B K Gupta, Stability of Finite Elliptical Pressure Dam Bearins wit Rotor Flexibility Effects, ASLE Trans, vol9, no, pp , 986 [] S S Rattan, Stability analysis of pressure dam bearins usin finite element metod, PD Tesis, Kuruksetra University, 995 [5] G Busan, S S Rattan, and N P Meta, Hydrodynamic Lubrication Analysis of Four-Lobe Pressure Dam Bearins by Finite-Element Metod, Proceedins nd International and 9 t National onference on Fluid Mecanics and Fluid Power, IIT Roorkee, pp 8, 00 [6] E J Han, Te Excitability of Flexibility Rotors in Sort Sleeve Bearins, Trans ASME, Journal of Lubrication Tecnoloy, pp 05, 975 [7] G Busan, S S Rattan, and N P Meta, Stability Analysis of Four-Lobe Pressure Dam bearins, Triboloy Letters, vol, no, pp -7, 00 International Scolarly and Scientific Researc & Innovation (8) scolarwasetor/07-689/6
STATIC AND DYNAMIC CHARACTERISTICS OF HYDRODYNAMIC FOUR- LOBE JOURNAL BEARING WITH COUPLE STRESS LUBRICANTS
STATIC AND DYNAMIC CHARACTERISTICS OF HYDRODYNAMIC FOUR- LOBE JOURNAL BEARING WITH COUPLE STRESS LUBRICANTS B. Chetti, b.chetti@gmail.com, Institute of sciences and Technology, Center University of Khemis
More informationSTABILITY ANALYSIS OF CIRCULAR PRESSURE DAM HYDRODYNAMIC JOURNAL BEARING WITH COUPLE STRESS LUBRICANT
VO. 5, NO. 10, OCTOBER 010 ISSN 1819-6608 006-010 Asian Research Publishing Network (ARPN). All rights reserved. STABIITY ANAYSIS OF CIRCUAR PRESSURE DAM HYDRODYNAMIC JOURNA BEARING WITH COUPE STRESS UBRICANT
More informationAnalysis of Static and Dynamic Load on Hydrostatic Bearing with Variable Viscosity and Pressure
Indian Journal of Science and Tecnology Supplementary Article Analysis of Static and Dynamic Load on Hydrostatic Bearing wit Variable Viscosity and Pressure V. Srinivasan* Professor, Scool of Mecanical
More informationThe Measurement of the Gravitational Constant g with Kater s Pendulum
e Measurement of te Gravitational Constant wit Kater s Pendulum Abstract A Kater s pendulum is set up to measure te period of oscillation usin a lamppotocell module and a ektronix oscilloscope. Usin repeated
More informationTheoretical Analysis of Flow Characteristics and Bearing Load for Mass-produced External Gear Pump
TECHNICAL PAPE Teoretical Analysis of Flow Caracteristics and Bearing Load for Mass-produced External Gear Pump N. YOSHIDA Tis paper presents teoretical equations for calculating pump flow rate and bearing
More informationA simplified thermohydrodynamic stability analysis of the plain cylindrical hydrodynamic journal bearings
Louisiana State University LSU Digital Commons LSU Master's Teses Graduate Scool 4 A simplified termoydrodynamic stability analysis of te plain cylindrical ydrodynamic journal bearings Sumit Singal Louisiana
More informationQuasi-geostrophic motion
Capter 8 Quasi-eostropic motion Scale analysis for synoptic-scale motions Simplification of te basic equations can be obtained for synoptic scale motions. Consider te Boussinesq system ρ is assumed to
More informationCircular Bearing Performance Parameters with Isothermal and Thermo-Hydrodynamic Approach Using Computational Fluid Dynamics
Circular Bearing Performance Parameters with Isothermal and Thermo-Hydrodynamic Approach Using Computational Fluid Dynamics Amit Chauhan 1 Department of Mechanical Engineering, University Institute of
More informationAN ANALYSIS OF AMPLITUDE AND PERIOD OF ALTERNATING ICE LOADS ON CONICAL STRUCTURES
Ice in te Environment: Proceedings of te 1t IAHR International Symposium on Ice Dunedin, New Zealand, nd t December International Association of Hydraulic Engineering and Researc AN ANALYSIS OF AMPLITUDE
More informationSolutions to the Multivariable Calculus and Linear Algebra problems on the Comprehensive Examination of January 31, 2014
Solutions to te Multivariable Calculus and Linear Algebra problems on te Compreensive Examination of January 3, 24 Tere are 9 problems ( points eac, totaling 9 points) on tis portion of te examination.
More informationINTRODUCTION DEFINITION OF FLUID. U p F FLUID IS A SUBSTANCE THAT CAN NOT SUPPORT SHEAR FORCES OF ANY MAGNITUDE WITHOUT CONTINUOUS DEFORMATION
INTRODUCTION DEFINITION OF FLUID plate solid F at t = 0 t > 0 = F/A plate U p F fluid t 0 t 1 t 2 t 3 FLUID IS A SUBSTANCE THAT CAN NOT SUPPORT SHEAR FORCES OF ANY MAGNITUDE WITHOUT CONTINUOUS DEFORMATION
More informationContinuity and Differentiability of the Trigonometric Functions
[Te basis for te following work will be te definition of te trigonometric functions as ratios of te sides of a triangle inscribed in a circle; in particular, te sine of an angle will be defined to be te
More informationAnalysis of Hydrodynamic Journal Bearing Using CFD and FSI Technique
Analysis of Hydrodynamic Journal Bearing Using CFD and FSI Technique Priyanka Tiwari M.E. Student of Government Engineering College Jabalpur, M.P.-India Veerendra Kumar Principal of Government Engineering
More informationNonlinear Dynamic Analysis of a Hydrodynamic Journal Bearing Considering the Effect of a Rotating or Stationary Herringbone Groove
G. H. Jang e-mail: ghjang@hanyang.ac.kr J. W. Yoon PREM, Department of Mechanical Engineering, Hanyang University, Seoul, 133-791, Korea Nonlinear Dynamic Analysis of a Hydrodynamic Journal Bearing Considering
More informationSqueeze film effect at elastohydrodynamic lubrication of plain journal bearings
Science, Juliana Engineering Javorova, & Education, Anelia Mazdrakova 1, (1), 16, 11- Squeeze film effect at elastoydrodynamic lubrication of plain journal bearings Juliana Javorova *, Anelia Mazdrakova
More informationSection 15.6 Directional Derivatives and the Gradient Vector
Section 15.6 Directional Derivatives and te Gradient Vector Finding rates of cange in different directions Recall tat wen we first started considering derivatives of functions of more tan one variable,
More informationCHAPTER 1 INTRODUCTION Hydrodynamic journal bearings are considered to be a vital component of all the rotating machinery. These are used to support
CHAPTER 1 INTRODUCTION Hydrodynamic journal bearings are considered to be a vital component of all the rotating machinery. These are used to support radial loads under high speed operating conditions.
More information(a) At what number x = a does f have a removable discontinuity? What value f(a) should be assigned to f at x = a in order to make f continuous at a?
Solutions to Test 1 Fall 016 1pt 1. Te grap of a function f(x) is sown at rigt below. Part I. State te value of eac limit. If a limit is infinite, state weter it is or. If a limit does not exist (but is
More informationThe Verlet Algorithm for Molecular Dynamics Simulations
Cemistry 380.37 Fall 2015 Dr. Jean M. Standard November 9, 2015 Te Verlet Algoritm for Molecular Dynamics Simulations Equations of motion For a many-body system consisting of N particles, Newton's classical
More informationPolynomial Interpolation
Capter 4 Polynomial Interpolation In tis capter, we consider te important problem of approximatinga function fx, wose values at a set of distinct points x, x, x,, x n are known, by a polynomial P x suc
More informationStability Analysis of a Hydrodynamic Journal Bearing With Rotating Herringbone Grooves
G. H. Jang e-mail: ghjang@hanyang.ac.kr J. W. Yoon PREM, Department of Mechanical Engineering, Hanyang University, Seoul, 33-79, Korea Stability Analysis of a Hydrodynamic Journal Bearing With Rotating
More informationInvestigation of pressure distributions for a finite elastohydrodynamic journal bearing lubricated by Ferro fluids with couple stresses
Aerican Journal of Applied Mateatics 14; (4): 135-14 Publised online Auust 3, 14 (ttp://www.sciencepublisinroup.co/j/aja) doi: 1.11648/j.aja.144.14 ISSN: 33-43 (Print); ISSN: 33-6X (Online) Investiation
More informationMANY scientific and engineering problems can be
A Domain Decomposition Metod using Elliptical Arc Artificial Boundary for Exterior Problems Yajun Cen, and Qikui Du Abstract In tis paper, a Diriclet-Neumann alternating metod using elliptical arc artificial
More informationThe modeling of hydraulic fractures applies three fundamental equations:
Te modelin of ydraulic fractures applies tree fundamental equations: 1. Continuity. Momentum (Fracture Fluid Flow) 3. LEFM (Linear Elastic Fracture Mecanics) Solution Tecnique Te tree sets of equations
More informationNumerical Differentiation
Numerical Differentiation Finite Difference Formulas for te first derivative (Using Taylor Expansion tecnique) (section 8.3.) Suppose tat f() = g() is a function of te variable, and tat as 0 te function
More informationAnalysis of Fluid Film Stiffness and Damping coefficient for A Circular Journal Bearing with Micropolar Fluid
et International Journal on Emerging Technologies 5(1): 206-211(2014) ISSN No. (Print) : 0975-8364 ISSN No. (Online) : 2249-3255 Analysis of Fluid Film Stiffness Damping coefficient for A Circular Journal
More information2.3 Algebraic approach to limits
CHAPTER 2. LIMITS 32 2.3 Algebraic approac to its Now we start to learn ow to find its algebraically. Tis starts wit te simplest possible its, and ten builds tese up to more complicated examples. Fact.
More informationA = h w (1) Error Analysis Physics 141
Introduction In all brances of pysical science and engineering one deals constantly wit numbers wic results more or less directly from experimental observations. Experimental observations always ave inaccuracies.
More informationFerrofluid Lubrication equation for non-isotropic porous squeeze film bearing with slip velocity. Rajesh C. Shah * M.M.Parsania
Matematics Today Vol.28(June-Dec-212)43-49 ISSN 976-3228 Ferrofluid Lubrication equation for non-isotropic porous squeeze film bearing wit slip velocity Rajes C. Sa * Department of Applied Matematics,
More informationMath Spring 2013 Solutions to Assignment # 3 Completion Date: Wednesday May 15, (1/z) 2 (1/z 1) 2 = lim
Mat 311 - Spring 013 Solutions to Assignment # 3 Completion Date: Wednesday May 15, 013 Question 1. [p 56, #10 (a)] 4z Use te teorem of Sec. 17 to sow tat z (z 1) = 4. We ave z 4z (z 1) = z 0 4 (1/z) (1/z
More informationVibration in a Cracked Machine Tool Spindle with Magnetic Bearings
Te Open Mecanical Engineering Journal, 8,, 3-39 3 Open Access Vibration in a Cracked Macine Tool Spindle wit Magnetic Bearings Huang-Kuang Kung and Bo-Wun Huang Department of Mecanical Engineering, Ceng
More informationPhysics Courseware Physics I
Definition of pressure: Force Area ysics Courseware ysics I Bernoulli Hydrostatics equation: B A Bernoulli s equation: roblem.- In a carburetor (scematically sown in te fiure) calculate te minimum speed
More informationNumerical analysis of three-lobe journal bearing with CFD and FSI
Numerical analysis of three-lobe journal bearing with CFD and FSI Pankaj Khachane 1, Dinesh Dhande 2 1PG Student at Department of Mechanical Engineering, AISSMSCOE Pune, Maharashtra, India 2Assistant Professor
More informationPolynomial Interpolation
Capter 4 Polynomial Interpolation In tis capter, we consider te important problem of approximating a function f(x, wose values at a set of distinct points x, x, x 2,,x n are known, by a polynomial P (x
More informationSimulation and verification of a plate heat exchanger with a built-in tap water accumulator
Simulation and verification of a plate eat excanger wit a built-in tap water accumulator Anders Eriksson Abstract In order to test and verify a compact brazed eat excanger (CBE wit a built-in accumulation
More informationGrade: 11 International Physics Olympiad Qualifier Set: 2
Grade: 11 International Pysics Olympiad Qualifier Set: 2 --------------------------------------------------------------------------------------------------------------- Max Marks: 60 Test ID: 12111 Time
More information(4.2) -Richardson Extrapolation
(.) -Ricardson Extrapolation. Small-O Notation: Recall tat te big-o notation used to define te rate of convergence in Section.: Suppose tat lim G 0 and lim F L. Te function F is said to converge to L as
More information1 The concept of limits (p.217 p.229, p.242 p.249, p.255 p.256) 1.1 Limits Consider the function determined by the formula 3. x since at this point
MA00 Capter 6 Calculus and Basic Linear Algebra I Limits, Continuity and Differentiability Te concept of its (p.7 p.9, p.4 p.49, p.55 p.56). Limits Consider te function determined by te formula f Note
More informationQuasiperiodic phenomena in the Van der Pol - Mathieu equation
Quasiperiodic penomena in te Van der Pol - Matieu equation F. Veerman and F. Verulst Department of Matematics, Utrect University P.O. Box 80.010, 3508 TA Utrect Te Neterlands April 8, 009 Abstract Te Van
More information6. Non-uniform bending
. Non-uniform bending Introduction Definition A non-uniform bending is te case were te cross-section is not only bent but also seared. It is known from te statics tat in suc a case, te bending moment in
More information4. The slope of the line 2x 7y = 8 is (a) 2/7 (b) 7/2 (c) 2 (d) 2/7 (e) None of these.
Mat 11. Test Form N Fall 016 Name. Instructions. Te first eleven problems are wort points eac. Te last six problems are wort 5 points eac. For te last six problems, you must use relevant metods of algebra
More information232 Calculus and Structures
3 Calculus and Structures CHAPTER 17 JUSTIFICATION OF THE AREA AND SLOPE METHODS FOR EVALUATING BEAMS Calculus and Structures 33 Copyrigt Capter 17 JUSTIFICATION OF THE AREA AND SLOPE METHODS 17.1 THE
More informationComparison of Efflux Time between Cylindrical and Conical Tanks Through an Exit Pipe
International Journal of Applie Science an Enineerin 0. 9, : - Comparison of Efflux Time between Cylinrical an Conical Tanks Trou an Exit Pipe C. V. Subbarao * epartment of Cemical Enineerin,MVGR Collee
More informationChapter 8. Numerical Solution of Ordinary Differential Equations. Module No. 2. Predictor-Corrector Methods
Numerical Analysis by Dr. Anita Pal Assistant Professor Department of Matematics National Institute of Tecnology Durgapur Durgapur-7109 email: anita.buie@gmail.com 1 . Capter 8 Numerical Solution of Ordinary
More informationWYSE Academic Challenge 2004 Sectional Mathematics Solution Set
WYSE Academic Callenge 00 Sectional Matematics Solution Set. Answer: B. Since te equation can be written in te form x + y, we ave a major 5 semi-axis of lengt 5 and minor semi-axis of lengt. Tis means
More informationVibro-Acoustics of a Brake Rotor with Focus on Squeal Noise. Abstract
Te International Congress and Exposition on Noise Control Engineering Dearbor MI, USA. August 9-, Vibro-Acoustics of a Brake Rotor wit Focus on Sueal Noise H. Lee and R. Sing Acoustics and Dynamics Laboratory,
More informationRecall from our discussion of continuity in lecture a function is continuous at a point x = a if and only if
Computational Aspects of its. Keeping te simple simple. Recall by elementary functions we mean :Polynomials (including linear and quadratic equations) Eponentials Logaritms Trig Functions Rational Functions
More informationNumerical analysis of a free piston problem
MATHEMATICAL COMMUNICATIONS 573 Mat. Commun., Vol. 15, No. 2, pp. 573-585 (2010) Numerical analysis of a free piston problem Boris Mua 1 and Zvonimir Tutek 1, 1 Department of Matematics, University of
More informationNumerical Analysis MTH603. dy dt = = (0) , y n+1. We obtain yn. Therefore. and. Copyright Virtual University of Pakistan 1
Numerical Analysis MTH60 PREDICTOR CORRECTOR METHOD Te metods presented so far are called single-step metods, were we ave seen tat te computation of y at t n+ tat is y n+ requires te knowledge of y n only.
More informationImplementation of a Thermo- Hydrodynamic Model to Predict Morton Effect
Implementation of a Thermo- Hydrodynamic Model to Predict Morton Effect Antonini *, Fausti and Mor Polibrixia srl, Via A. Tadini 49, 25125 Brescia. *orresponding author: Via Branze 45, 25123 Brescia, massimo.antonini@polibrixia.it
More informationCLOSED CONVEX SHELLS Meunargia T. Mixed forms of stress-strain relations are given in the form. λ + 2µ θ + 1
Seminar of I. Vekua Institute of Applied Matematics REPORTS, Vol. 43, 207 CLOSED CONVEX SHELLS Meunargia T. Abstract. If Ω is a closed convex sell, ten S : x 3 = 0 is an ovaloid. It is proved tat in tis
More informationShear Thinning and Hydrodynamic Friction of Viscosity Modifier- Containing Oils. Part II: Impact of Shear Thinning on Journal Bearing Friction
Tribology Letters 208 66:9 ttps://doi.org/0.007/s249-08-040-z ORIGINAL PAPER Sear Tinning and Hydrodynamic Friction of Viscosity Modifier- Containing Oils. Part II: Impact of Sear Tinning on Journal Bearing
More informationMath 1241 Calculus Test 1
February 4, 2004 Name Te first nine problems count 6 points eac and te final seven count as marked. Tere are 120 points available on tis test. Multiple coice section. Circle te correct coice(s). You do
More informationQuantum Numbers and Rules
OpenStax-CNX module: m42614 1 Quantum Numbers and Rules OpenStax College Tis work is produced by OpenStax-CNX and licensed under te Creative Commons Attribution License 3.0 Abstract Dene quantum number.
More informationExperimental Investigations of Whirl Speeds of a Rotor on Hydrodynamic Spiral Journal Bearings Under Flooded Lubrication
International Conference on Fluid Dynamics and Thermodynamics Technologies (FDTT ) IPCSIT vol.33() () IACSIT Press, Singapore Experimental Investigations of Whirl Speeds of a Rotor on Hydrodynamic Spiral
More informationTest 2 Review. 1. Find the determinant of the matrix below using (a) cofactor expansion and (b) row reduction. A = 3 2 =
Test Review Find te determinant of te matrix below using (a cofactor expansion and (b row reduction Answer: (a det + = (b Observe R R R R R R R R R Ten det B = (((det Hence det Use Cramer s rule to solve:
More informationMath 31A Discussion Notes Week 4 October 20 and October 22, 2015
Mat 3A Discussion Notes Week 4 October 20 and October 22, 205 To prepare for te first midterm, we ll spend tis week working eamples resembling te various problems you ve seen so far tis term. In tese notes
More informationFlow of a Rarefied Gas between Parallel and Almost Parallel Plates
Flow of a Rarefied Gas between Parallel and Almost Parallel Plates Carlo Cercignani, Maria Lampis and Silvia Lorenzani Dipartimento di Matematica, Politecnico di Milano, Milano, Italy 033 Abstract. Rarefied
More informationDevelopment and experimental verification of a numerical model for optimizing the cleaning performance of the doctor blade press roll tribosystem
Development and experimental verification of a numerical model for optimizing te cleaning performance of te doctor blade press roll tribosystem M. Rodríguez Ripoll, B. Sceicl,, D. Bianci, B. Jakab, F.
More informationComment on Experimental observations of saltwater up-coning
1 Comment on Experimental observations of saltwater up-coning H. Zang 1,, D.A. Barry 2 and G.C. Hocking 3 1 Griffit Scool of Engineering, Griffit University, Gold Coast Campus, QLD 4222, Australia. Tel.:
More informationModel development for the beveling of quartz crystal blanks
9t International Congress on Modelling and Simulation, Pert, Australia, 6 December 0 ttp://mssanz.org.au/modsim0 Model development for te beveling of quartz crystal blanks C. Dong a a Department of Mecanical
More informationHYDROMAGNETIC BOUNDARY LAYER MICROPOLAR FLUID FLOW OVER A STRETCHING SURFACE EMBEDDED IN A NON-DARCIAN POROUS MEDIUM WITH RADIATION
HYDROMAGNETIC BOUNDARY LAYER MICROPOLAR FLUID FLOW OVER A STRETCHING SURFACE EMBEDDED IN A NON-DARCIAN POROUS MEDIUM WITH RADIATION MOSTAFA A. A. MAHMOUD, MAHMOUD ABD-ELATY MAHMOUD, AND SHIMAA E. WAHEED
More information4.2 - Richardson Extrapolation
. - Ricardson Extrapolation. Small-O Notation: Recall tat te big-o notation used to define te rate of convergence in Section.: Definition Let x n n converge to a number x. Suppose tat n n is a sequence
More informationChapter 5 FINITE DIFFERENCE METHOD (FDM)
MEE7 Computer Modeling Tecniques in Engineering Capter 5 FINITE DIFFERENCE METHOD (FDM) 5. Introduction to FDM Te finite difference tecniques are based upon approximations wic permit replacing differential
More informationPrediction of Coating Thickness
Prediction of Coating Tickness Jon D. Wind Surface Penomena CE 385M 4 May 1 Introduction Tis project involves te modeling of te coating of metal plates wit a viscous liquid by pulling te plate vertically
More informationCombining functions: algebraic methods
Combining functions: algebraic metods Functions can be added, subtracted, multiplied, divided, and raised to a power, just like numbers or algebra expressions. If f(x) = x 2 and g(x) = x + 2, clearly f(x)
More informationExam 1 Review Solutions
Exam Review Solutions Please also review te old quizzes, and be sure tat you understand te omework problems. General notes: () Always give an algebraic reason for your answer (graps are not sufficient),
More informationDistribution of reynolds shear stress in steady and unsteady flows
University of Wollongong Researc Online Faculty of Engineering and Information Sciences - Papers: Part A Faculty of Engineering and Information Sciences 13 Distribution of reynolds sear stress in steady
More informationResearch Article Stability Analysis of Journal Bearing: Dynamic Characteristics
Research Journal of Applied Sciences, Engineering and Technology 9(1): 47-52, 2015 DOI:10.19026/rjaset.9.1375 ISSN: 2040-7459; e-issn: 2040-7467 2015 Maxwell Scientific Publication Corp. Submitted: July
More informationSensitivity analysis of size effect on the performance of hydrostatic bearing
Sensitivity analysis of size effect on te erformance of ydrostatic bearing Cen Dongju 1a, Dong Liua 1, Zou Suai 1 and Fan Jinwei 1 1 College of Mecanical Engineering and Alied Electrics Teclogy, Beijing
More informationClick here to see an animation of the derivative
Differentiation Massoud Malek Derivative Te concept of derivative is at te core of Calculus; It is a very powerful tool for understanding te beavior of matematical functions. It allows us to optimize functions,
More informationAvailable online at ScienceDirect. Procedia Technology 23 (2016 ) 42 50
Available online at www.sciencedirect.com ScienceDirect Procedia Technology 23 (216 ) 42 5 3rd International Conference on Innovations in Automation and Mechatronics Engineering, ICIAME 216 On the stiffness
More informationContinuity and Differentiability Worksheet
Continuity and Differentiability Workseet (Be sure tat you can also do te grapical eercises from te tet- Tese were not included below! Typical problems are like problems -3, p. 6; -3, p. 7; 33-34, p. 7;
More informationUNIVERSITY OF MANITOBA DEPARTMENT OF MATHEMATICS MATH 1510 Applied Calculus I FIRST TERM EXAMINATION - Version A October 12, :30 am
DEPARTMENT OF MATHEMATICS MATH 1510 Applied Calculus I October 12, 2016 8:30 am LAST NAME: FIRST NAME: STUDENT NUMBER: SIGNATURE: (I understand tat ceating is a serious offense DO NOT WRITE IN THIS TABLE
More informationWe name Functions f (x) or g(x) etc.
Section 2 1B: Function Notation Bot of te equations y 2x +1 and y 3x 2 are functions. It is common to ave two or more functions in terms of x in te same problem. If I ask you wat is te value for y if x
More informationFINITE ELEMENT STOCHASTIC ANALYSIS
FINITE ELEMENT STOCHASTIC ANALYSIS Murray Fredlund, P.D., P.Eng., SoilVision Systems Ltd., Saskatoon, SK ABSTRACT Numerical models can be valuable tools in te prediction of seepage. Te results can often
More informationSecurity Constrained Optimal Power Flow
Security Constrained Optimal Power Flow 1. Introduction and notation Fiure 1 below compares te optimal power flow (OPF wit te security-constrained optimal power flow (SCOPF. Fi. 1 Some comments about tese
More informationLinear and Nonlinear Analysis of Plain Journal Bearings Lubricated With Couple Stress Fluid
ISSN 2395-1621 Linear and Nonlinear Analysis of Plain Journal Bearings Lubricated With Couple Stress Fluid #1 Deepali Kangude 1 deepalikangude94@gmail.com 1 P.G. student Mechanical Department, DYPIET Pimpri,
More information3.1 Extreme Values of a Function
.1 Etreme Values of a Function Section.1 Notes Page 1 One application of te derivative is finding minimum and maimum values off a grap. In precalculus we were only able to do tis wit quadratics by find
More informationACCESS TO SCIENCE, ENGINEERING AND AGRICULTURE: MATHEMATICS 1 MATH00030 SEMESTER /2019
ACCESS TO SCIENCE, ENGINEERING AND AGRICULTURE: MATHEMATICS MATH00030 SEMESTER 208/209 DR. ANTHONY BROWN 6. Differential Calculus 6.. Differentiation from First Principles. In tis capter, we will introduce
More informationADCP MEASUREMENTS OF VERTICAL FLOW STRUCTURE AND COEFFICIENTS OF FLOAT IN FLOOD FLOWS
ADCP MEASUREMENTS OF VERTICAL FLOW STRUCTURE AND COEFFICIENTS OF FLOAT IN FLOOD FLOWS Yasuo NIHEI (1) and Takeiro SAKAI (2) (1) Department of Civil Engineering, Tokyo University of Science, 2641 Yamazaki,
More information1 Calculus. 1.1 Gradients and the Derivative. Q f(x+h) f(x)
Calculus. Gradients and te Derivative Q f(x+) δy P T δx R f(x) 0 x x+ Let P (x, f(x)) and Q(x+, f(x+)) denote two points on te curve of te function y = f(x) and let R denote te point of intersection of
More informationSTUDIES ON THE MAXIMUM HARVESTABLE HYDROPOWER IN OPEN CHANNELS - APPLICATION TO A WATER WHEEL AND A TURBINE
SUDIES ON HE MAXIMUM HARVESABLE HYDROOWER IN OEN CHANNELS - ALICAION O A WAER WHEEL AND A URBINE. F. elz;. Bedarff Introduction Abstract: is work is about te upper limit for te ydropower ained in an open
More informationMATH 155A FALL 13 PRACTICE MIDTERM 1 SOLUTIONS. needs to be non-zero, thus x 1. Also 1 +
MATH 55A FALL 3 PRACTICE MIDTERM SOLUTIONS Question Find te domain of te following functions (a) f(x) = x3 5 x +x 6 (b) g(x) = x+ + x+ (c) f(x) = 5 x + x 0 (a) We need x + x 6 = (x + 3)(x ) 0 Hence Dom(f)
More informationThermohydrodynamic analysis of a worn plain journal bearing
Tribology International 37 (2004) 129 136 www.elsevier.com/locate/triboint Thermohydrodynamic analysis of a worn plain journal bearing M. Fillon, J. Bouyer Université de Poitiers, Laboratoire de Mécanique
More informationModelling lubricated revolute joints in multibody mechanical systems
183 Modelling lubricated revolute oints in multibody mechanical systems P Flores 1, H M Lankarani 2, J Ambrósio 3 and J C P Claro 1 1 Departamento de Engenharia Mecânica, Universidade do Minho, Guimarães,
More informationInertia Effects in Rheodynamic Lubrication of an Externally Pressurized Converging Thrust Bearing using Bingham Fluids
Journal of Applied Fluid Mecanics, Vol. 1, No., pp. 587-594, 19. Available online at www.jafmonline.net, ISSN 175-645, EISSN 175-645. DOI: 1.18869/acadpub.jafm.75.54.8914 Inertia Effects in Reodynamic
More informationFriction Coefficient s Numerical Determination for Hot Flat Steel Rolling at Low Strain Rate
American ournal of Applied Matematics 05; 3(5: -8 Publised online September 6, 05 (ttp://www.sciencepublisinggroup.com/j/ajam doi: 0.648/j.ajam.050305.3 ISS: 330-0043 (Print; ISS: 330-006X (Online riction
More informationLarge eddy simulation of turbulent flow downstream of a backward-facing step
Available online at www.sciencedirect.com Procedia Engineering 31 (01) 16 International Conference on Advances in Computational Modeling and Simulation Large eddy simulation of turbulent flow downstream
More informationVelocity distribution in non-uniform/unsteady flows and the validity of log law
University of Wollongong Researc Online Faculty of Engineering and Information Sciences - Papers: Part A Faculty of Engineering and Information Sciences 3 Velocity distribution in non-uniform/unsteady
More informationDerivation Of The Schwarzschild Radius Without General Relativity
Derivation Of Te Scwarzscild Radius Witout General Relativity In tis paper I present an alternative metod of deriving te Scwarzscild radius of a black ole. Te metod uses tree of te Planck units formulas:
More information158 Calculus and Structures
58 Calculus and Structures CHAPTER PROPERTIES OF DERIVATIVES AND DIFFERENTIATION BY THE EASY WAY. Calculus and Structures 59 Copyrigt Capter PROPERTIES OF DERIVATIVES. INTRODUCTION In te last capter you
More informationOptimal Shape Design of a Two-dimensional Asymmetric Diffsuer in Turbulent Flow
THE 5 TH ASIAN COMPUTAITIONAL FLUID DYNAMICS BUSAN, KOREA, OCTOBER 7 ~ OCTOBER 30, 003 Optimal Sape Design of a Two-dimensional Asymmetric Diffsuer in Turbulent Flow Seokyun Lim and Haeceon Coi. Center
More informationInfluence of radial clearance on the static performance of hydrodynamic journal bearing system
Volume, Issue (26) 658-563 ISSN 237-3258 Influence of radial clearance on the static performance of hydrodynamic journal bearing system RK Awasthi, Harpreet Singh Bitta Department of Mechanical Engineering,
More informationEvaluation and Accurate Estimation from Petrophysical Parameters of a Reservoir
American Journal of Environmental Engineering and Science 2016; 3(2): 68-74 ttp://www.aascit.org/journal/ajees ISSN: 2381-1153 (Print); ISSN: 2381-1161 (Online) Evaluation and Accurate Estimation from
More informationSAMCEF For ROTORS. Chapter 1 : Physical Aspects of rotor dynamics. This document is the property of SAMTECH S.A. MEF A, Page 1
SAMCEF For ROTORS Chapter 1 : Physical Aspects of rotor dynamics This document is the property of SAMTECH S.A. MEF 101-01-A, Page 1 Table of Contents rotor dynamics Introduction Rotating parts Gyroscopic
More informationUniversity Mathematics 2
University Matematics 2 1 Differentiability In tis section, we discuss te differentiability of functions. Definition 1.1 Differentiable function). Let f) be a function. We say tat f is differentiable at
More informationPeriodic Orbits in the Photogravitational Restricted Problem When the Primaries Are Triaxial Rigid Bodies
International Journal of Astronomy and Astropysics 06 6 - Publised Online Marc 06 in SciRes. ttp://www.scirp.org/journal/ijaa ttp://dx.doi.org/0.46/ijaa.06.6009 Periodic Orbits in te Potogravitational
More informationThe Derivative as a Function
Section 2.2 Te Derivative as a Function 200 Kiryl Tsiscanka Te Derivative as a Function DEFINITION: Te derivative of a function f at a number a, denoted by f (a), is if tis limit exists. f (a) f(a + )
More informationJournal-Bearing Databook
Tsuneo Someya (Editor) Journal-Bearing Databook With Contributions by T. Someya, J. Mitsui, J. Esaki, S. Saito, Y Kanemitsu, T. Iwatsubo, M.Tanaka, S. Hisa, T. Fujikawa, H. Kanki With 60 Figures and 5
More information