UNIVERSITAS PERTAHANAN Mekanika Kekuatan Material (Material Failure) PERTEMUAN Ke- 1 PROGRAM STUDI S1 TEKNIK MESIN 31 AGUSTUS 2021 FAKTOR PENYEBAB KEGAGALAN MATERIAL Faktor Cacat Product Faktor Lingkungan/Proses Kimia Faktor Mekanik/Fisik Patahan Sel Satuan • Atom-atom pada logam membentuk sel satuan • Masing-masing sel satuan memiliki bidang geser/slip • Bidang geser, adalah bidang yang memiliki kerapatan atom yang tinggi Analisa Kegagalan 2011 Kristal Face Center Cubic (FCC) Konsep Pembebanan Model Patahan Intergranulasi Retak/Cleavage Patah Geser Retak Semu Patahan Fatik Fracture mechanisms • Ductile fracture – Terdeformasi plastis • Brittle fracture – Tidak atau sedikit terdeformasi plastis – Catastrophic Ductile vs Brittle Failure Fracture behavior: Very Ductile Moderately Ductile Brittle Large Moderate Small • Classification: %AR or %EL • Ductile fracture is usually desirable! Ductile: warning before fracture Brittle: No warning Example: Failure of a Pipe • Ductile failure: --one piece --large deformation • Brittle failure: --many pieces --small deformation Moderately Ductile Failure • Evolution to failure: Small cavity formation Initial necking Coalescence of cavities to form a crack Crack propagation Final shear fracture Moderately Ductile Failure • Resulting fracture surfaces (steel) 50 50mm mm 100 mm Fracture surface of tire cord wire loaded in tension. Particles serve as void nucleation sites. Ductile vs. Brittle Failure brittle fracture cup-and-cone fracture Brittle Failure Arrows indicate pt at which failure originated Brittle Fracture Surfaces • Intragranular or Transgranular (within grains); most brittle materials Brittle Fracture Surfaces • Intergranular (between grains) Flaws are Stress Concentrators! Results from crack propagation • Griffith Crack a s m 2so t t 1/ 2 K t so where t = radius of curvature so = applied stress sm = stress at crack tip Kt = Stress concentration factor Concentration of Stress at Crack Tip Engineering Fracture Design • Avoid sharp corners! s so max Stress Conc. Factor, K t = s w smax r, fillet radius o 2.5 h 2.0 increasing w/h 1.5 1.0 0 0.5 1.0 sharper fillet radius r/h Crack Propagation Cracks propagate due to sharpness of crack tip • A plastic material deforms at the tip, “blunting” the crack. deformed region brittle plastic Energy balance on the crack • Elastic strain energy• energy stored in material as it is elastically deformed • this energy is released when the crack propagates • creation of new surfaces requires energy When Does a Crack Propagate? Crack propagates if above critical stress, σc 2 E s sc a 1/ 2 i.e., sm > sc or where – – – – – Kt > Kc K cs 0 K c Ys c a Y 2 E s E = modulus of elasticity s = specific surface energy a = one half length of internal crack Y = Dimensionless parameter Kc = Fracture Toughness = sc/s0 For ductile => replace s by s + p where p is plastic deformation energy Three Mode of Crack Displacement Mode I Opening or Tensile mode Mode II Sliding mode Mode III Tearing mode Plain Strain Fracture Toughness Metals/ Alloys Graphite/ Ceramics/ Semicond Polymers Composites/ fibers 100 C-C (|| fibers) K Ic (MPa · m0.5 ) 70 60 50 40 30 Steels Ti alloys Al alloys Mg alloys 20 2 Al/Al oxide(sf) Y 2 O 3 /ZrO 2 (p) 4 C/C ( fibers) 1 3 Al oxid/SiC(w) 5 Si nitr/SiC(w) Al oxid/ZrO 2 (p) 4 Glass/SiC(w) 6 10 7 6 5 4 Diamond Si carbide Al oxide Si nitride PET PP 3 PVC 2 1 0.7 0.6 0.5 1 PC <100> Si crystal <111> Glass -soda Concrete PS Polyester Glass 6 Plane Strain Fracture Toughness data Design Against Crack Growth • Crack growth condition: K ≥ Kc = Ys a • Largest, most stressed cracks grow first! --Result 1: Max. flaw size dictates design stress. sdesign Kc Y amax --Result 2: Design stress dictates max. flaw size. amax 1 K c Ysdesign amax s fracture no fracture fracture amax no fracture s 2 Loading Rate • Increased loading rate... -- increases sy and TS -- decreases %EL s sy TS • Why? An increased rate gives less time for dislocations to move past obstacles. e Larger loading rate TS e Smaller loading rate sy e Impact Testing (Charpy) (Izod) final height initial height Temperature • Increasing temperature... --increases %EL and Kc • Ductile-to-Brittle Transition Temperature (DBTT)... Impact Energy FCC metals (e.g., Cu, Ni) BCC metals (e.g., iron at T < 914°C) polymers Brittle More Ductile High strength materials ( s y > E/150) Temperature Ductile-to-brittle transition temperature Fracture Surface of Steel Influence of C in Iron Fatigue • Fatigue = failure under cyclic stress. specimen compression on top bearing motor bearing counter flex coupling tension on bottom • key parameters -- S, σm, σmax and frequency smax s sm smin • Key points: --can cause part failure, even though smax < sc. --causes ~ 90% of mechanical engineering failures. S time Fatigue Design Parameters • Fatigue limit: --no fatigue if S < fatigue limit S = stress amplitude case for steel (typ.) unsafe Fatigue limit safe 10 • Sometimes, the fatigue limit is zero! 3 5 7 10 10 10 N = Cycles to failure 9 S = stress amplitude case for Al (typ.) unsafe safe 10 3 5 7 10 10 10 N = Cycles to failure 9 Fatigue Mechanism • Crack grows incrementally da m K dN typ. 1 to 6 ~ s a crack origin increase in crack length per loading cycle • Failed rotating shaft --crack grew even though Kmax < Kc --crack grows faster as • s increases • crack gets longer • loading freq. increases. Final rupture Beachmarks and Striations Beachmarks • Macroscopic dimension • Found in component that interrupted during crack propagation stage Single beachmark may contain thousands of striations Striations • Microscopic dimension • Represent advance distance of crack front during single load cycle Improving Fatigue Life 1. Mean stress S = stress amplitude Increasing near zero or compressive s m moderate tensile s m Larger tensile s m sm N = Cycles to failure 2. Remove stress concentrators. bad better bad better Improving Fatigue Life • Surface Treatment (imposing residual compressive stress within thin film outer surface layer) --Method 1: shot peening shot Improving Fatigue Life • Surface Treatment (imposing residual compressive stress within thin film outer surface layer) --Method 2: carburizing or nitriding C-rich gas Other Fatigue due to Environment • Thermal fatigue σ = αEΔT Normally induced at elevated temperature • Corrosion fatigue deleterious influence and produce shorter fatigue life Creep Sample deformation at a constant stress (s) vs. time s,e s 0 t Primary Creep: slope (creep rate) decreases with time. (Strain Hardening) Secondary Creep: steadystate i.e., constant slope. (Recovery) Tertiary Creep: slope (creep rate) increases with time, i.e. acceleration of rate. Creep • Occurs at elevated temperature, T > 0.4 Tm tertiary primary secondary elastic Secondary Creep • Strain rate is constant at a given T, s -- strain hardening is balanced by recovery stress exponent (material parameter) Qc e s K 2s exp RT n • Strain rate increases for higher T, s applied stress Stress (MPa) strain rate material const. activation energy for creep (material parameter) 200 100 427°C 538 °C 40 20 10 10 -2 10 -1 Steady state creep rate 649 °C 1 es (%/1000hr) Creep Failure • Failure: • Estimate rupture time along grain boundaries. S-590 Iron, T = 800°C, s = 20 ksi g.b. cavities applied stress 20 10 Stress, ksi 100 data for S-590 Iron • Time to rupture, tr T ( 20 logtr ) L function of applied stress time to failure (rupture) temperature 1 12 16 20 24 28 L(10 3 K-log hr) 24x103 K-log hr T ( 20 logtr ) L 1073K Ans: tr = 233 hr Examples of Material Failure Tugas Mandiri 1. 2. 3. 4. Apa yang dimaksut dengan kegagalan material? Klasifikasikan dan uraikan penyebab kegagalan material? Uraikan dan jelaskan jenis-jenis patahan? Jelaskan zona kurva deformasi plastis dan elastis pada grafik uji tarik? 5. Jelaskan apa yang di maksud dengan necking? 6. Jelaskan perbedaan patahan ductile dan brittle? 7. Jelaskan dan uraikan patahan Transgranular dan Intergranular? 8. Sebutkan dan jelaskan pengaruh kegagalan material baja? 9. Sebutkan tahapan menganalisa kegagalan material? 10. Jelaskan yang dimaksud dengan tegangan Yield Strength? Terima Kasih