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  • Principles of Tribology , 2nd Edition 摩擦學原理(第2版)
    該商品所屬分類:研究生 -> 工學
    【市場價】
    1854-2688
    【優惠價】
    1159-1680
    【作者】 溫詩鑄、黃平 
    【所屬類別】 圖書  教材  研究生/本科/專科教材  工學 
    【出版社】清華大學出版社 
    【ISBN】9787302485261
    【折扣說明】一次購物滿999元台幣免運費+贈品
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    【本期贈品】①優質無紡布環保袋,做工棒!②品牌簽字筆 ③品牌手帕紙巾
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    內容介紹



    開本:16開
    紙張:膠版紙
    包裝:平裝-膠訂

    是否套裝:否
    國際標準書號ISBN:9787302485261
    作者:溫詩鑄、黃平

    出版社:清華大學出版社
    出版時間:2017年10月 

        
        
    "
    編輯推薦
    本書彙集摩擦學研究進展以及作者和同事們從事該領域研究的成果,繫統地闡述摩擦學的基本原理與應用,全面反映現代摩擦學的研究狀況和發展趨勢。    全書共21章,由潤滑理論與潤滑設計、摩擦磨損機理與控制、應用摩擦學等三部分組成。除摩擦學傳統內容外,還論述了摩擦學與相關學科交叉而形成的研究領域。本書針對工程實際中各種摩擦學現像,著重闡述在摩擦過程中的變化規律和特征,進而介紹基本理論和分析計算方法以及實驗測試技術,並說明它們在工程中的實際應用。    本書可作為機械設計與理論專業的研究生教材和高等院校機械工程各類專業師生的教學參考書,亦可供從事機械設計和研究的工程技術人員參考。 
    內容簡介
    本書彙集摩擦學研究的*進展及作者和其同事從事該領域的研究成果,繫統地闡述摩擦學的基本原理與應用,全面反映現代摩擦學的研究狀況和發展趨勢。
    全書共 21章,由潤滑理論與潤滑設計、摩擦磨損機理與控制、應用摩擦學等 3部分組成。除摩擦學傳統內容外,還論述了摩擦學與相關學科交叉而形成的研究領域。本書針對工程實際中的各種摩擦學現像,著重闡述摩擦過程中的變化規律和特征,進而介紹基本理論、分析計算方法以及實驗測試技術,並說明它們在工程中的實際應用。
    本書可作為機械設計與理論專業的研究生教材以及高等院校機械工程各類專業師生的教學參考書,也可以供從事機械設計和研究的工程技術人員參考。
    作者簡介
    溫詩鑄 清華大學精密儀器與機械學繫教授。1932年生於江西省豐城市。1955年畢業於清華大學機械制造繫後留校任教,歷任機械設計教研室主任、摩擦學研究室主任、摩擦學國家重點實驗室主任。長期從事機械設計與理論專業的教學和研究,出版《摩擦學原理》(第1、2、3版)、《耐磨損設計》、《彈性流體動力潤滑》、《納米摩擦學》、《界面科學與技術》、《Principles of Tribology》等6部著作,發表學術論文500餘篇。獲國家自然科學獎二等獎、國家技術發明獎三等獎、全國優秀科技圖書獎一、二等獎以及省部級科技進步獎等共19項。1999年被選為中國科學院院士。
    目錄
    Contents
    About the Authors xvii
    Second Edition Preface xix
    Preface xxi
    Introduction xxiii
    Part I Lubrication Theory 1
    1 Properties of Lubricants 3
    1.1 Lubrication States 3
    1.2 Density of Lubricant 5
    1.3 Viscosity of Lubricant 7
    1.3.1 Dynamic Viscosity and KinematicViscosity 7
    1.3.1.1 Dynamic Viscosity 7
    1.3.1.2 Kinematic Viscosity 8
    1.3.2 Relationship between Viscosity andTemperature 9

    Contents


    About the Authors xvii


    Second Edition Preface xix


    Preface xxi


    Introduction xxiii


    Part I Lubrication Theory 1


    1 Properties of Lubricants 3


    1.1 Lubrication States 3


    1.2 Density of Lubricant 5


    1.3 Viscosity of Lubricant 7


    1.3.1 Dynamic Viscosity and Kinematic
    Viscosity 7


    1.3.1.1 Dynamic Viscosity 7


    1.3.1.2 Kinematic Viscosity 8


    1.3.2 Relationship between Viscosity and
    Temperature 9


    1.3.2.1 Viscosity–Temperature Equations 9


    1.3.2.2 ASTM Viscosity–Temperature Diagram
    9


    1.3.2.3 Viscosity Index 10


    1.3.3 Relationship between Viscosity and
    Pressure 10


    1.3.3.1 Relationships between Viscosity,
    Temperature and Pressure 11


    1.4 Non-Newtonian Behaviors 12


    1.4.1 Ree–Eyring Constitutive Equation 12


    1.4.2 Visco-Plastic Constitutive Equation
    13


    1.4.3 Circular Constitutive Equation 13


    1.4.4 Temperature-Dependent Constitutive
    Equation 13


    1.4.5 Visco-Elastic Constitutive Equation
    14


    1.4.6 Nonlinear Visco-Elastic Constitutive
    Equation 14


    1.4.7 A Simple Visco-Elastic Constitutive
    Equation 15


    1.4.7.1 Pseudoplasticity 16


    1.4.7.2 Thixotropy 16


    1.5 Wettability of Lubricants 16


    1.5.1 Wetting and Contact Angle 17


    1.5.2 Surface Tension 17


    1.6 Measurement and Conversion of Viscosity
    19


    1.6.1 Rotary Viscometer 19


    1.6.2 Off-Body Viscometer 19


    1.6.3 Capillary Viscometer 19


    References 21


    2 Basic Theories of Hydrodynamic
    Lubrication 22


    2.1 Reynolds Equation 22


    2.1.1 Basic Assumptions 22


    2.1.2 Derivation of the Reynolds Equation
    23


    2.1.2.1 Force Balance 23


    2.1.2.2 General Reynolds Equation 25


    2.2 Hydrodynamic Lubrication 26


    2.2.1 Mechanism of Hydrodynamic Lubrication
    26


    2.2.2 Boundary Conditions and Initial
    Conditions of the Reynolds Equation 27


    2.2.2.1 Boundary Conditions 27


    2.2.2.2 Initial Conditions 28


    2.2.3 Calculation of Hydrodynamic
    Lubrication 28


    2.2.3.1 Load-Carrying CapacityW 28


    2.2.3.2 Friction ForceF 28


    2.2.3.3 Lubricant FlowQ 29


    2.3 Elastic Contact Problems 29


    2.3.1 Line Contact 29


    2.3.1.1 Geometry and Elasticity Simulations
    29


    2.3.1.2 Contact Area and Stress 30


    2.3.2 Point Contact 31


    2.3.2.1 Geometric Relationship 31


    2.3.2.2 Contact Area and Stress 32


    2.4 Entrance Analysis of EHL 34


    2.4.1 Elastic Deformation of Line Contacts
    35


    2.4.2 Reynolds Equation Considering the
    Effect of Pressure-Viscosity 35


    2.4.3 Discussion 36


    2.4.4 Grubin FilmThickness Formula 37


    2.5 Grease Lubrication 38


    References 40


    3 Numerical Methods of Lubrication
    Calculation 41


    3.1 Numerical Methods of Lubrication 42


    3.1.1 Finite Difference Method 42


    3.1.1.1 Hydrostatic Lubrication 44


    3.1.1.2 Hydrodynamic Lubrication 44


    3.1.2 Finite Element Method and Boundary
    Element Method 48


    3.1.2.1 Finite Element Method (FEM) 48


    3.1.2.2 Boundary Element Method 49


    3.1.3 Numerical Techniques 51


    3.1.3.1 Parameter Transformation 51


    3.1.3.2 Numerical Integration 51


    3.1.3.3 Empirical Formula 53


    3.1.3.4 SuddenThickness Change 53


    3.2 Numerical Solution of the Energy
    Equation 54


    3.2.1 Conduction and Convection of Heat 55


    3.2.1.1 Conduction Heat Hd 55


    3.2.1.2 Convection Heat Hv 55


    3.2.2 Energy Equation 56


    3.2.3 Numerical Solution of Energy Equation
    59


    3.3 Numerical Solution of
    Elastohydrodynamic Lubrication 60


    3.3.1 EHL Numerical Solution of Line
    Contacts 60


    3.3.1.1 Basic Equations 60


    3.3.1.2 Solution of the Reynolds Equation
    62


    3.3.1.3 Calculation of Elastic Deformation
    62


    3.3.1.4 Dowson–Higginson FilmThickness
    Formula of Line Contact EHL 64


    3.3.2 EHL Numerical Solution of Point
    Contacts 64


    3.3.2.1 The Reynolds Equation 65


    3.3.2.2 Elastic Deformation Equation 66


    3.3.2.3 Hamrock–Dowson FilmThickness
    Formula of Point Contact EHL 66


    3.4 Multi-Grid Method for Solving EHL
    Problems 68


    3.4.1 Basic Principles of Multi-Grid Method
    68


    3.4.1.1 Grid Structure 68


    3.4.1.2 Discrete Equation 68


    3.4.1.3 Transformation 69


    3.4.2 Nonlinear Full Approximation Scheme
    for the Multi-Grid Method 69


    3.4.3 V andWIterations 71


    3.4.4 Multi-Grid Solution of EHL Problems
    71


    3.4.4.1 Iteration Methods 71


    3.4.4.2 Iterative Division 72


    3.4.4.3 Relaxation Factors 73


    3.4.4.4 Numbers of Iteration Times 73


    3.4.5 Multi-Grid Integration Method 73


    3.4.5.1 Transfer Pressure Downwards 74


    3.4.5.2 Transfer Integral Coefficients
    Downwards 74


    3.4.5.3 Integration on the Coarser Mesh 74


    3.4.5.4 Transfer Back Integration Results
    75


    3.4.5.5 Modification on the Finer Mesh 75


    References 76


    4 Lubrication Design of Typical Mechanical
    Elements 78


    4.1 Slider and Thrust Bearings 78


    4.1.1 Basic Equations 78


    4.1.1.1 Reynolds Equation 78


    4.1.1.2 Boundary Conditions 78


    4.1.1.3 Continuous Conditions 79


    4.1.2 Solutions of Slider Lubrication 79


    4.2 Journal Bearings 81


    4.2.1 Axis Position and Clearance Shape 81


    4.2.2 Infinitely Narrow Bearings 82


    4.2.2.1 Load-Carrying Capacity 83


    4.2.2.2 Deviation Angle and Axis Track 83


    4.2.2.3 Flow 84


    4.2.2.4 Frictional Force and Friction
    Coefficient 84


    4.2.3 InfinitelyWide Bearings 85


    4.3 Hydrostatic Bearings 88


    4.3.1 Hydrostatic Thrust Plate 89


    4.3.2 Hydrostatic Journal Bearings 90


    4.3.3 Bearing Stiffness andThrottle 90


    4.3.3.1 Constant Flow Pump 91


    4.3.3.2 Capillary Throttle 91


    4.3.3.3 Thin-Walled OrificeThrottle 92


    4.4 Squeeze Bearings 92


    4.4.1 Rectangular Plate Squeeze 93


    4.4.2 Disc Squeeze 94


    4.4.3 Journal Bearing Squeeze 94


    4.5 Dynamic Bearings 96


    4.5.1 Reynolds Equation of Dynamic Journal
    Bearings 96


    4.5.2 Simple Dynamic Bearing Calculation 98


    4.5.2.1 A Sudden Load 98


    4.5.2.2 Rotating Load 99


    4.5.3 General Dynamic Bearings 100


    4.5.3.1 Infinitely Narrow Bearings 100


    4.5.3.2 Superimposition Method of Pressures
    101


    4.5.3.3 Superimposition Method of Carrying
    Loads 101


    4.6 Gas Lubrication Bearings 102


    4.6.1 Basic Equations of Gas Lubrication
    102


    4.6.2 Types of Gas Lubrication Bearings 103


    4.7 Rolling Contact Bearings 106


    4.7.1 Equivalent Radius R 107


    4.7.2 Average Velocity U 107


    4.7.3 Carrying Load PerWidthW/b 107


    4.8 Gear Lubrication 108


    4.8.1 Involute Gear Transmission 109


    4.8.1.1 Equivalent Curvature Radius R 110


    4.8.1.2 Average Velocity U 111


    4.8.1.3 Load PerWidthW/b 112


    4.8.2 Arc Gear Transmission EHL 112


    4.9 Cam Lubrication 114


    References 116


    5 Special Fluid Medium Lubrication 118


    5.1 Magnetic Hydrodynamic Lubrication 118


    5.1.1 Composition and Classification of
    Magnetic Fluids 118


    5.1.2 Properties of Magnetic Fluids 119


    5.1.2.1 Density of Magnetic Fluids 119


    5.1.2.2 Viscosity of Magnetic Fluids 119


    5.1.2.3 Magnetization Strength of Magnetic
    Fluids 120


    5.1.2.4 Stability of Magnetic Fluids 120


    5.1.3 Basic Equations of Magnetic
    Hydrodynamic Lubrication 121


    5.1.4 Influence Factors on Magnetic EHL 123


    5.2 Micro-Polar Hydrodynamic Lubrication
    124


    5.2.1 Basic Equations of Micro-Polar Fluid
    Lubrication 124


    5.2.1.1 Basic Equations of Micro-Polar Fluid
    Mechanics 124


    5.2.1.2 Reynolds Equation of Micro-Polar
    Fluid 125


    5.2.2 Influence Factors on Micro-Polar
    Fluid Lubrication 128


    5.2.2.1 Influence of Load 128


    5.2.2.2 Main Influence Parameters of
    Micro-Polar Fluid 129


    5.3 Liquid Crystal Lubrication 130


    5.3.1 Types of Liquid Crystal 130


    5.3.1.1 Tribological Properties of
    Lyotropic Liquid Crystal 131


    5.3.1.2 Tribological Properties
    ofThermotropic Liquid Crystal 131


    5.3.2 Deformation Analysis of Liquid
    Crystal Lubrication 132


    5.3.3 Friction Mechanism of Liquid Crystal
    as a Lubricant Additive 136


    5.3.3.1 Tribological Mechanism of
    4-pentyl-4′-cyanobiphenyl 136


    5.3.3.2 Tribological Mechanism of
    Cholesteryl Oleyl Carbonate 136


    5.4 Electric Double Layer Effect inWater
    Lubrication 137


    5.4.1 Electric Double Layer Hydrodynamic
    Lubrication Theory 138


    5.4.1.1 Electric Double Layer Structure 138


    5.4.1.2 Hydrodynamic Lubrication Theory of
    Electric Double Layer 138


    5.4.2 Influence of Electric Double Layer on
    Lubrication Properties 142


    5.4.2.1 Pressure Distribution 142


    5.4.2.2 Load-Carrying Capacity 143


    5.4.2.3 Friction Coefficient 144


    5.4.2.4 An Example 144


    References 145


    6 Lubrication Transformation and Nanoscale
    Thin Film Lubrication 147


    6.1 Transformations of Lubrication States
    147


    6.1.1 Thickness-Roughness Ratio ? 147


    6.1.2 Transformation from Hydrodynamic
    Lubrication to EHL 148


    6.1.3 Transformation from EHL to Thin Film
    Lubrication 149


    6.2 Thin Film Lubrication 152


    6.2.1 Phenomenon ofThin Film Lubrication
    153


    6.2.2 Time Effect of Thin Film Lubrication
    154


    6.2.3 Shear Strain Rate Effect onThin Film
    Lubrication 157


    6.3 Analysis ofThin Film Lubrication 158


    6.3.1 Difficulties in Numerical Analysis of
    Thin Film Lubrication 158


    6.3.2 Tichy’s Thin Film Lubrication Models
    160


    6.3.2.1 Direction Factor Model 160


    6.3.2.2 Surface Layer Model 161


    6.3.2.3 Porous Surface Layer Model 161


    6.4 Nano-Gas Film Lubrication 161


    6.4.1 Rarefied Gas Effect 162


    6.4.2 Boundary Slip 163


    6.4.2.1 Slip Flow 163


    6.4.2.2 Slip Models 163


    6.4.2.3 Boltzmann Equation for Rarefied Gas
    Lubrication 165


    6.4.3 Reynolds Equation Considering the
    Rarefied Gas Effect 165


    6.4.4 Calculation of Magnetic Head/Disk of
    UltraThin Gas Lubrication 166


    6.4.4.1 Large Bearing Number Problem 167


    6.4.4.2 Sudden Step Change Problem 167


    6.4.4.3 Solution of Ultra-Thin Gas
    Lubrication of Multi-Track Magnetic Heads 167


    References 169

    前言
    Second Edition Preface
    This edition of Principles of Tribology,based on the first edition, is formed by revising the inadequacies
    of the original edition and its beingimproved in response to the hotspots of recent
    tribology research. Since the book wasfirst published, the readers have offered various suggestions
    and opinions, and given the developments intribology research, we thought it necessary
    to make this revision of the book.
    Although one important task for thisedition was to make some error corrections, it retains
    the basic framework of the first edition,with 21 chapters in three parts.
    Also, in response to the rapid developmentof high-speed railways and the implementation

    Second Edition Preface


    This edition of Principles of Tribology,
    based on the first edition, is formed by revising the inadequacies


    of the original edition and its being
    improved in response to the hotspots of recent


    tribology research. Since the book was
    first published, the readers have offered various suggestions


    and opinions, and given the developments in
    tribology research, we thought it necessary


    to make this revision of the book.


    Although one important task for this
    edition was to make some error corrections, it retains


    the basic framework of the first edition,
    with 21 chapters in three parts.


    Also, in response to the rapid development
    of high-speed railways and the implementation


    of the lunar exploration project in China,
    rolling friction has become more important, so it is


    brought into a separate chapter (11).
    Although in the previous version, rolling frictionwas mentioned


    as a typical phenomenon of friction, we
    only gave some basic definitions. In Chapter 11,


    we give more detail on rolling friction
    definitions, rolling friction theories and stick-slip phenomena


    in rolling friction, as well as contact and
    heat generation of rolling friction between


    wheel and rail. In fact, rolling friction
    exists widely in transportation, automobile, machinery


    manufacturing, production and daily life,
    and it has functions which cannot be substituted by


    sliding friction.


    Another new area of content in this edition
    is tribology research in MEMS


    (micro-electromechanical system) covered in
    Chapter 20. This includes the application


    of atomic force microscopy in tribology of
    MEMS, micro motor tribology research and micro


    analysis of wear mechanisms. This content
    is focused on recent tribology research and the


    rapid development of MEMS.


    Also, ecological tribology, a hot topic in
    tribology research, has been introduced in


    Chapter 21. This chapter includes zero
    friction and superlubrication, green lubricating oil,


    friction-induced noise and its control,
    plus remanufacturing technologies and self-repairing


    technology. Ecological tribology research
    will become an important research direction for the


    future.


    Of course, the new content is far more than
    just rolling friction, MEMS tribology and green


    tribology, but limited space here precludes
    more detailed coverage of the additions. We hope


    that the contents of the book will be more
    systematic and accurate in this edition.


    We present our most sincere thanks to our
    colleagues and graduate students for their enthusiastic


    support, and to all the others who have
    provided help and made a contribution to the


    development of tribology research in
    general and this edition in particular.


    March 2016 Wen Shizhu


    Huang Ping

    在線試讀
    Part I Lubrication Theory 命命命命1 
    PropertiesofLubricants Many.uidsserveaslubricantsinindustry.Amongthem,oilandgreasearethemostcommonlyused.Air,waterandliquidmetalsarealsousedasspeciallubricants;forexample,liquidsodiumis often used as a lubricant in nuclear reactors. In some situations, solid lubricants, such as graphite,molybdenumdisul.deorpolytetra.uoroethylene(PTFE)canalsobeused.Inthis.rstchapter we will discuss the viscosity and density of lubricants, as they are the two importantphysicalpropertiesassociatedwithlubrication.Inlubricationtheory,themostimportantphysicalpropertyofalubricantisitsviscosity,themostimportantfactorindeterminingthelubrication.lmthickness.Inhydrodynamiclubrica-tion, the lubricant .lm thickness is proportional to the viscosity, while in elastohydrodynamiclubricationitisproportionaltotheviscositytothepowers0.7.Althoughinboundarylubrica-tiontheviscositydoesnotdirectlyin.uencethe.lmthickness,theoilpackagesformedbetweenpeaksandvalleysofroughnesswillcarrypartoftheload.Thereforelubricantviscosityisclosely命relatedtoitsload-carryingcapacity.命Furthermore, viscosity is also an important factor in.uencing the frictional force.A high-viscosity lubricant not only causes a lot of friction loss, but also produces a lotof heat, which make cooling control di.cult. Because temperature rise caused by frictioncan lead to failure of the lubricant .lm, the surface will be worn increasingly. Therefore, areasonableviscosityisrequiredforpracticallubrication.The performance of elastohydrodynamic lubrication (EHL) also depends on the rheologi-cal characteristics of a lubricant. In point or line contacts, an EHL .lm is very thin, less thanonemicro-meter,butthepressure is veryhigh,upto1GPa. And,becausethecontactareaisoftenverysmall,theshearratemaybehigherthan107s–1 suchthatthepassingtimeis very short, less than 10–3s. Therefore, a friction process is always accompanied by high tem-perature. For such conditions, the properties of a lubricant are quite di.erent from those ofa Newtonian .uid. In such cases, therefore, it is necessary to study the rheological proper-tiesoflubricants.Experimentsshowthatalthoughthe.lmthicknessformuladerivedfromtheNewtonian.uidmodelisusuallyappliedtotheelastohydrodynamiclubrication,thefrictionalforce and temperature calculated by a Newtonian .uid model will cause a large error. There-fore, in thermo-elastohydrodynamic lubrication (TEHL), more realistic non-Newtonian .uidmodelsshouldbeused.Thesebelongtoalubricantrheologystudywhichwillnotonlyhelpusunderstand the lubrication mechanism more deeply but also has major signi.cance in energyconservationandimprovementinthelifeofmechanicalelements. 
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