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东南大学:《建筑力学 Architectural Mechanics》课程教学课件(英文讲稿)A09 Axial Loading Concept of Stress & Strain

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东南大学:《建筑力学 Architectural Mechanics》课程教学课件(英文讲稿)A09 Axial Loading Concept of Stress & Strain
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Axial LoadingConcept of Stress & Strainmi@se.edl.cn

Axial Loading Concept of Stress & Strain mi@seu.edu.cn

Contents·Introduction(拉压变形简介)·DiagramofAxialForces(轴力图)·ConceptofStresses(应力的概念)·GeneralStressStateofaPoint(点的一般应力状态)·StressesActingonCrossSections(拉压杆横截面上的应力)·Saint-VenantsPrinciple(圣维南原理)·StressesActingonObliqueSections(拉压杆斜截面上的应力)·DeformationofAxiallyLoadedBars(拉压杆的变形)·ElasticConstantsofEngineeringMaterials(常见工程材料的弹性常数)·NonuniformTension/compression(非均匀拉压)·StrainEnergy(应变能)·StrainEnergyDensity(应变能密度)·MechanicalBehaviorofMaterials(材料的力学性能)·NominalStress-strainCurve(名义应力应变曲线)·StressandDeformationIndicesofLow-carbonSteel(低碳钢的应力和变形指标)2

• Introduction(拉压变形简介) • Diagram of Axial Forces(轴力图) • Concept of Stresses(应力的概念) • General Stress State of a Point(点的一般应力状态) • Stresses Acting on Cross Sections(拉压杆横截面上的应力) • Saint-Venant’s Principle(圣维南原理) • Stresses Acting on Oblique Sections(拉压杆斜截面上的应力) • Deformation of Axially Loaded Bars(拉压杆的变形) • Elastic Constants of Engineering Materials(常见工程材料的弹性常数) • Nonuniform Tension/compression(非均匀拉压) • Strain Energy(应变能) • Strain Energy Density(应变能密度) • Mechanical Behavior of Materials(材料的力学性能) • Nominal Stress-strain Curve(名义应力应变曲线) • Stress and Deformation Indices of Low-carbon Steel(低碳钢的应力和变形指标) Contents 2

Contents:Yield Stress,Ultimate Stress andPercentElongation ofEngineering Materials(常见工程材料的屈服应力、强度极限和断后伸长率)·Strain(Work)Hardening(冷作硬化)·Mechanical Behavior ofGeneral DuctileMaterials under Tension(塑性材料的拉伸力学性能)·MechanicalBehaviorofBrittleMaterialsunderTension(脆性材料的拉伸)·MechanicalBehaviorofLow-carbonSteelunderCompression(低碳钢的压缩)·MechanicalBehaviorofCastIronunderCompression(铸铁的压缩力学性能)·MechanicalBehaviorofCreet(混凝土的力学性能)·MechanicalBehaviorofWood(木材的力学性能)·MechanicalBehaviorofCompositeMaterials(复合材料的力学性能)·MechanicalBehaviorofViscoelasticMaterials(粘弹性材料的力学性能)·StrengthCondition(强度条件)·FailureofBrittlevs.DuctileBarsunderTension(脆性和塑性杆件的拉伸失效)·StressConcentration(拉压杆中的应力集中现象)3

• Yield Stress, Ultimate Stress and Percent Elongation of Engineering Materials (常见工程材料的屈服应力、强度极限和断后伸长率) • Strain (Work) Hardening(冷作硬化) • Mechanical Behavior of General Ductile Materials under Tension(塑性材料的 拉伸力学性能) • Mechanical Behavior of Brittle Materials under Tension(脆性材料的拉伸) • Mechanical Behavior of Low-carbon Steel under Compression(低碳钢的压缩) • Mechanical Behavior of Cast Iron under Compression(铸铁的压缩力学性能) • Mechanical Behavior of Creet(混凝土的力学性能) • Mechanical Behavior of Wood(木材的力学性能) • Mechanical Behavior of Composite Materials(复合材料的力学性能) • Mechanical Behavior of Viscoelastic Materials(粘弹性材料的力学性能) • Strength Condition(强度条件) • Failure of Brittle vs. Ductile Bars under Tension(脆性和塑性杆件的拉伸失效) • Stress Concentration(拉压杆中的应力集中现象) Contents 3

IntroductionBrake cable,L=460mmHand brakepivotAh=660mmh.=490mmW37.5mmP(Resultantofdistributedpressure)4550mm-Uniformhand-100mm-brakepressure4

Introduction 4

IntroductionERH: Load: equal and opposite forces along bar axis: Deformation: extension (contraction) along bar axis andcontraction (extension) transversely5

F F F F • Load: equal and opposite forces along bar axis • Deformation: extension (contraction) along bar axis and contraction (extension) transversely Introduction 5

Internal Forces Illustrated by Method of SectionsInternal Force. The change of interaction force among various parts of asolid body, introduced by external loadingThe Method of SectionFFnVnmII6

Internal Force • The change of interaction force among various parts of a solid body, introduced by external loading. The Method of Section F1 F2 m I F1 F2 m I R M o F1 Fn F2 m I II m Internal Forces Illustrated by Method of Sections 6

Sign Convention of Axial Forces: Coordinate: a right-handed systemMO: Centroid of the cross-sectionAx: Cross-section normal (Bar axis)F. Forces: Fn, Fsy, Fs?: Moments: T, My, M,: Axial Force (Fn)Fo Along bar axis+o Extends or contracts the bar along bar axis一F Positive for tension; Negative for compression(-)o Assuming positive for all unknown axial forces7

F1 F2 m I o x y z FN T M FSy y FSz Mz • Coordinate: a right-handed system O: Centroid of the cross-section x: Cross-section normal (Bar axis) • Forces: FN , FSy , FSz • Moments: T, My , Mz • Axial Force (FN ) o Along bar axis o Extends or contracts the bar along bar axis o Positive for tension; Negative for compression o Assuming positive for all unknown axial forces FN (+) FN (-) Sign Convention of Axial Forces 7

Procedure of Method of Sections: Sectioning the member: Taking either portion: Substituting the other portion with internal forces·EquilibratingmmFFmmFFFFNFn = FFn = -F8

• Sectioning the member • Taking either portion • Substituting the other portion with internal forces • Equilibrating Procedure of Method of Sections F F m m F FN FN = -F F F m m F FN FN = F 8

Diagram of Axial Forces: Abscissa: position of cross sections: Ordinate: axial force: Positive for tension; negative for compressionmm+X9

• Abscissa: position of cross sections • Ordinate: axial force • Positive for tension; negative for compression. F F m m FN x Diagram of Axial Forces 9

Sample Problem. Plot the diagram of axial forceB 2 kN/m CD 1 kN3kN A. Solution2 m—/-2 m—/2 m—1. Internal force in AB、CD3 kNFnFNAB = 3 kNxFNcD = -1 kN2m- x2. Internal force in BCFn(x)=3-2x(0<x<2)33. Diagram of axial forceF (kN)C4. Maximum internal force[FN,max | = 3 kN110

• Plot the diagram of axial force 3 kN A B 2 kN/m C D 1 kN 2 m 2 m 2 m 1. Internal force in AB、CD N N 3 kN 1 kN AB CD F F    2. Internal force in BC 3 kN 2 m x FN x FN,max  3 kN 3. Diagram of axial force FN kN 3 1 4. Maximum internal force Sample Problem F x x x N       3 2 0 2   • Solution 10

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