Engineering 45 Mechanical Properties of Metals (2) Bruce Mayer, PE Licensed Electrical & Mechanical Engineer BMayer@ChabotCollege.edu Engineering-45: Materials of Engineering 1 Bruce Mayer, PE BMayer@ChabotCollege.edu • ENGR-45_Lec-15_Metal_MechProp-2.ppt Learning Goals.1 – Mech Props STRESS and STRAIN: • What they are and why they are they used instead of LOAD and DEFORMATION ELASTIC Behavior • How much deformation occurs when Loads are SMALL? • Which materials deform least Engineering-45: Materials of Engineering 2 Bruce Mayer, PE BMayer@ChabotCollege.edu • ENGR-45_Lec-15_Metal_MechProp-2.ppt Learning Goals.2 – Mech Props PLASTIC Behavior • Determine the point at which Dislocations cause PERMANENT deformation • Which materials are most resistant to Permanent Deformation TOUGHNESS and DUCTILITY • What they are • How to Measure them Engineering-45: Materials of Engineering 3 Bruce Mayer, PE BMayer@ChabotCollege.edu • ENGR-45_Lec-15_Metal_MechProp-2.ppt Properties of Solid Materials Mechanical: Characteristics of materials displayed when forces and/or torques are applied to them. Physical: Characteristics of materials that relate to the interaction of materials with various forms of energy. Chemical: Material characteristics that relate to the structure of a material. Dimensional: Size, shape, and finish Engineering-45: Materials of Engineering 4 Bruce Mayer, PE BMayer@ChabotCollege.edu • ENGR-45_Lec-15_Metal_MechProp-2.ppt Material Properties Chemical Physical Mechanical Dimensional Composition Melting Point Tensile properties Standard Shapes Microstructure Thermal Toughness Standard Sizes Phases Magnetic Ductility Surface Texture Grain Size Corrosion Crystallinity Molecular Weight Electrical Optical Acoustic Gravimetric Fatigue Hardness Creep Compression Stability Mfg. Tolerances Flammability Engineering-45: Materials of Engineering 5 Bruce Mayer, PE BMayer@ChabotCollege.edu • ENGR-45_Lec-15_Metal_MechProp-2.ppt Recall ELASTIC Deformation Apply/Remove a SMALL Force-Load to a Specimen 1. Initial 3. Unload 2. SMALL load bonds stretch return to initial d • F Force Load (lb or N) • d Deformation in Response to the Load (in or m) Engineering-45: Materials of Engineering 6 F F Linear- ELASTIC means elastic REVERSIBLE Non-Linearelastic d Bruce Mayer, PE BMayer@ChabotCollege.edu • ENGR-45_Lec-15_Metal_MechProp-2.ppt Recall PLASTIC Deformation Apply/Remove a LARGE Force Load to a Specimen 1. Initial 2. LARGE load bonds stretch & planes shear delastic+plastic PLASTIC means PERMANENT Engineering-45: Materials of Engineering 7 F 3. Unload Planes Still Sheared dplastic F linear elastic linear elastic dplastic d Bruce Mayer, PE BMayer@ChabotCollege.edu • ENGR-45_Lec-15_Metal_MechProp-2.ppt Plastic Deformation - Simple Tension Test (Temperature <Tmelt/3) Elastic+Plastic at larger stress Tensile Stress, Elastic initially P Engineering-45: Materials of Engineering 8 Elastic Recovery permanent (plastic) after load is removed engineering strain, plastic strain Bruce Mayer, PE BMayer@ChabotCollege.edu • ENGR-45_Lec-15_Metal_MechProp-2.ppt YIELD Strength, y Define YIELD Strength as the Stress at Which NOTICEABLE Plastic Deformation Occurs • Define NOTICEABLE as 0.2% → P = 0.002 (0.2%) • For Matl’s WithOUt a well Defined Yield Pt σy = σ(ε = 0.2%) For a 2” gage-length • ΔL = 2”•0.002 = 0.004” (0.1 mm) Engineering-45: Materials of Engineering 9 y tensile stress, σy ≡ Yield Strength engineering strain, P = 0.002 Bruce Mayer, PE BMayer@ChabotCollege.edu • ENGR-45_Lec-15_Metal_MechProp-2.ppt Yield Strength: Comparison y,ceramics >> y,metals >> y,polymers Room T values Based on data in Table B4, Callister 6e. a = annealed hr = hot rolled ag = aged cd = cold drawn cw = cold worked qt = quenched & tempered Engineering-45: Materials of Engineering 10 Bruce Mayer, PE BMayer@ChabotCollege.edu • ENGR-45_Lec-15_Metal_MechProp-2.ppt TENSILE/ULTIMATE Strength Define TENSILE/ULTIMATE Strength (TS/σu) as the MAX-σ Point on the σ-ε Curve • Metals: occurs when noticeable NECKING starts • Ceramics: occurs when CRACK PROPAGATION starts • Polymers: occurs when POLYMER BACKBONES are aligned and about to break engineering stress TS y engineering strain Engineering-45: Materials of Engineering 11 Bruce Mayer, PE BMayer@ChabotCollege.edu • ENGR-45_Lec-15_Metal_MechProp-2.ppt Tensile Strength: Comparison TSceramics TSmetals TScomp >> TSpolymers Room T values Engineering-45: Materials of Engineering 12 Based on data in Table B4, Callister 6e. a = annealed hr = hot rolled ag = aged cd = cold drawn cw = cold worked qt = quenched & tempered AFRE, GFRE, & CFRE = aramid, glass, & carbon fiber-reinforced epoxy composites, with 60 vol% fibers. Bruce Mayer, PE BMayer@ChabotCollege.edu • ENGR-45_Lec-15_Metal_MechProp-2.ppt Ductility → Strain at Fracture At Tensile Fracture Define Ductility in Terms of ELONGATION Engineering tensile stress, smaller %EL (brittle if %EL<5%) Larger %EL (ductile if %EL>5%) Lo Ao Af Engineering tensile strain, Plastic Strain At Tensile Failure Engineering-45: Materials of Engineering 13 % EL L f Lo Lo 100 Bruce Mayer, PE BMayer@ChabotCollege.edu • ENGR-45_Lec-15_Metal_MechProp-2.ppt Lf Ductility → Strain at Fracture Alternative Definition Note: %RA and %EL is Reduction of Area Tend to Be Quite Comparable Lo Ao Af Lf RA Ductility % RA Ao A f Ao Engineering-45: Materials of Engineering 14 100 • Reason: crystal slip does not change material VOLUME. • %RA < %EL possible if internal voids form in neck. • %EL is More Common Than %RA Bruce Mayer, PE BMayer@ChabotCollege.edu • ENGR-45_Lec-15_Metal_MechProp-2.ppt Desirable Mechanical Properties Without Considering Such Factors Cost, Weight, Weldability, etc., The Typically Desired Combination of Strength and Ductility • HIGH σy σy, is the Mechanical DESIGN PARAMETER, not The Ultimate Strength • YIELDING permanently deforms (bends) Structures; typically rendering them NON-functional • HIGH %EL Engineering-45: Materials of Engineering 15 Bruce Mayer, PE BMayer@ChabotCollege.edu • ENGR-45_Lec-15_Metal_MechProp-2.ppt Resilience → Energy Storage Consider the σ·ε Product F dL F dL A L A L Next Consider the σ-ε Curve in the Elastic Range dU Now • F•δL has Units of ENERGY (J) d • A•L has Units of Volume (cu-m) Let U → J/m3 Engineering-45: Materials of Engineering 16 dε Bruce Mayer, PE BMayer@ChabotCollege.edu • ENGR-45_Lec-15_Metal_MechProp-2.ppt Resilience cont. y In The Elastic Range U d r 0.002 the Material Stretches and then In the Elastic Range Returns to the E & y 0.002 so Original Size y y E & d d E Thus Define Resilience, Ur, as the Then the Ur Integral 2 y REVERSIBLE y U r E d E Energy Storage 0 2 0 • U → Area under σ·ε r curve in elastic Rng Engineering-45: Materials of Engineering 17 Ur 2 y 2E Bruce Mayer, PE BMayer@ChabotCollege.edu • ENGR-45_Lec-15_Metal_MechProp-2.ppt E Toughness An Extension of RESILIENCE Beyond the Elastic Range to Plastic-Flow & Fracture A Measure of the TOTAL Energy-per-Vol Absorbance Capability of a Material • to the Total Plastic-Def. Area under the σ-ε curve , Engineering Tensile Stress smaller toughness (ceramics) larger toughness (metals, some composites) smaller toughnessunreinforced polymers Engineering tensile strain, Engineering-45: Materials of Engineering 18 Bruce Mayer, PE BMayer@ChabotCollege.edu • ENGR-45_Lec-15_Metal_MechProp-2.ppt TRUE Stress & Strain Engineering Stress F Ao • F Applied Pull • Ao Original Area But the Specimen NECKS-DOWN, Reducing the Area • So the TRUE Stress T F Ai • Ai Instantaneous Area = f(σ) or f(ε) Engineering-45: Materials of Engineering 19 Bruce Mayer, PE BMayer@ChabotCollege.edu • ENGR-45_Lec-15_Metal_MechProp-2.ppt TRUE Stress & Strain cont Engineering Strain Original (UnLoaded) L0 L Lo In the Instantaneous Case (see Rt) Load at Instant “i” d i dx' x'Pt P ' • Integrating T 0 Li Li d i dx' x' Lo T ln x' Li L0 Engineering-45: Materials of Engineering 20 Thus T ln Li ln Lo T ln Li Lo Bruce Mayer, PE BMayer@ChabotCollege.edu • ENGR-45_Lec-15_Metal_MechProp-2.ppt Engineering/True Stress/Strain For Strain T ln Li Lo Ao Lo F T ; but Ai Ai Li Lo L FLi Li F Li ; T ln Ao Lo Ao Lo Lo Lo and Li Lo L; T ln 1 Now Assume Constant Material VOLUME Ao Lo Ai Li Engineering-45: Materials of Engineering 21 Li Lo L (1 ) Lo Lo T (1 ) Bruce Mayer, PE BMayer@ChabotCollege.edu • ENGR-45_Lec-15_Metal_MechProp-2.ppt Plastic Behavior → - Stress True Stress - Strain Curve Fracture Ultimate Tensile Strength Engineering Stress - Strain Curve Fracture Strain Typical Metal Engineering-45: Materials of Engineering 22 Bruce Mayer, PE BMayer@ChabotCollege.edu • ENGR-45_Lec-15_Metal_MechProp-2.ppt Typ. Work-Hardening Parameters For Most Metals, True Stress Increases in the Plastic Range (not ElastoPlastic) Log(true stress, T) MPa • The Material “Hardens” as it is WORKED K T , plas Note : Log (1) 0 K yintercept K fracture n T , plas n slope necking 0.0010 0.010 0.10 Log (true plastic strain, T) Engineering-45: Materials of Engineering 23 1.0 Bruce Mayer, PE BMayer@ChabotCollege.edu • ENGR-45_Lec-15_Metal_MechProp-2.ppt Strain-Hardening K Work-Hardening Prefactor in MPa or Ksi n Work-Hardening Exponent (unitless) Material 1020 Steel 4340 Steel 2024 Al Alloy 304 Stainless Steel 70/30 Brass Yield Stress (MPa) 300 400 350 210 75 Engineering-45: Materials of Engineering 24 Ultimate Stress (MPa) 420 600 400 550 300 Elastic Modulus (MPa) 207000 207000 72000 185000 110000 K (MPa) n 530 640 690 1275 900 0.26 0.15 0.16 0.45 0.49 Bruce Mayer, PE BMayer@ChabotCollege.edu • ENGR-45_Lec-15_Metal_MechProp-2.ppt Elastic Recovery When a material is released prior to fracture: • Some of the total energy is stored elastically • Some is absorbed by the plastic deformation • The plastic deformation energy represents the lattice strains. Engineering-45: Materials of Engineering 25 The elastic energy will be recovered once the material is released • i.e., the material will unstretch Bruce Mayer, PE BMayer@ChabotCollege.edu • ENGR-45_Lec-15_Metal_MechProp-2.ppt Elastic Recovery cont. To determine the amount that the material recovers: 1. draw a line PARALLEL to the elastic modulus line that goes back to the strain axis 2. The difference in strains provides the recovered length 3. The area under this line is the recovered energy Engineering-45: Materials of Engineering 26 3 1 Elastic Energy, Ur 2 Bruce Mayer, PE BMayer@ChabotCollege.edu • ENGR-45_Lec-15_Metal_MechProp-2.ppt Hardness Short Definition = Resistance to Penetration Metals HandBook "Resistance of metal to plastic deformation, usually by indentation. However, the term may also refer to stiffness or temper, or to resistance to scratching, abrasion, or cutting. It is the property of a metal, which gives it the ability to resist being permanently, deformed (bent, broken, or have its shape changed), when a load is applied. The greater the hardness of the metal, the greater resistance it has to deformation. Engineering-45: Materials of Engineering 27 Bruce Mayer, PE BMayer@ChabotCollege.edu • ENGR-45_Lec-15_Metal_MechProp-2.ppt Hardness, cont. Hardness Resistance to Plastic Indentation LARGE Hardness Indicates Properties: • Resistance to plastic deformation or cracking when loaded in COMPRESSION • Better Wear Resistance e.g., 10mm sphere apply known force (1 to 1000 kg) Smaller indents mean larger hardness d D most plastics measure size of indent after removing load brasses easy to machine Al alloys steels file hard cutting tools nitrided steels diamond increasing hardness Engineering-45: Materials of Engineering 28 Bruce Mayer, PE BMayer@ChabotCollege.edu • ENGR-45_Lec-15_Metal_MechProp-2.ppt WhiteBoard Work Engineering-45: Materials of Engineering 29 Bruce Mayer, PE BMayer@ChabotCollege.edu • ENGR-45_Lec-15_Metal_MechProp-2.ppt Elastic Strain RECOVERY Parallel Lines Ur Engineering-45: Materials of Engineering 30 When a PostYield Load is Removed the Material Recovers along a Line PARALLEL to the initial ELASTIC extension Line Bruce Mayer, PE BMayer@ChabotCollege.edu • ENGR-45_Lec-15_Metal_MechProp-2.ppt