Materials Selection- Fatigue Intro Flashcards
What can fluctuating or cyclic stresses lead to?
Failure at a stress level lower than the yield or ultimate tensile strength
Stress range, amplitude, ratio and mean stress
Stress range = σmax-σmin=Δ σ
Stress amplitude =Δ σ/2=σa
Stress ratio = σmin/σmax =R
Mean stress = 1/2(σmax+σmin)
3 factors to cause fatigue failure
Maximum tensile stress of sufficiently high value
Large enough fluctuation (range/ amplitude) of applied stress
Sufficiently large number of cycles N of the applied stress
Diagram for how fatigue testing works
See page 6 lecture 4
Fatigue testing in lab
Material subjected to relatively large stress amplitude (about 2/3 UTS). Number of cycles at this fluctuating stress required to cause failure is measured. Process repeated at progressively smaller stress amplitudes.
Describe S-N curve
Stress amplitude on y axis and number of cycles to failure on log scale x axis. Generally curves down and sometimes reaches minimum. If know stress amplitude, read off number of cycles to failure from line.
Fatigue endurance limit σe or Se
Stress below which the lifetime of the part is infinite
High cycle fatigue
Nf >10^3-10^4
Deformation largely elastic with some localised (or microscopic) plasticity.
Low cycle fatigue
Higher levels of stress amplitude means fatigue life decreases such that Nf<10^3-10^4
More plastic deformation occurs
Stages of high cycle fatigue failure
Occurs by initiation and growth of a crack in a component. Stable crack growth occurs with successive cyclic tensile stresses until it reaches a critical crack length. Then fast fracture takes place.
What does high cycle fatigue fracture look like?
See slide 11 and 12 lecture 4
Graph of crack length against number of cycles for HCF
Crack length on log y axis. N/Nf on normal x axis. Region 1 is crack initiation and early crack growth, line steep and gets shallower. Region 2 is stable crack growth with very shallow gradient over about 0.17 to 0.7 on x axis. Region 3 is final fast fracture and line curves up like exponential. See slide 13
Crack initiation and early crack growth
Depend on microstructure and plastic flow properties of the material. Small fatigue crack initially grows along shear planes which are 45° to tensile stress axis. Finer grains mean closer spacing between grain boundaries which crack has to break through so increased yield strength. Then tension driven crack propagation perpendicular to tensile stress axis for stable crack growth.
Stable crack growth
Fatigue crack growth normal to tensile load. Growth rate fairly insensitive to microstructure (grain size has only small effect). Crack growth rate can be modelled using Paris law equation
Paris law equation
da/dN=C(ΔK)^m=C(YΔ σrt(πa))^m C and m constants different for each material K is stress intensity parameter a is crack length N is number of cycles Y is geometry factor