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Lab 6B -Fracture Toughness and Fracture Toughness-limited Design

Lab 6B -Fracture Toughness and Fracture Toughness-limited Design. Big bang for the buck!. What is Fracture Toughness??. Toughness is the resistance of a material to the propagation of crack.

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Lab 6B -Fracture Toughness and Fracture Toughness-limited Design

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  1. Lab 6B -Fracture Toughness and Fracture Toughness-limited Design Big bang for the buck!

  2. What is Fracture Toughness?? • Toughness is the resistance of a material to the propagation of crack. • Assumes that a sample of material contains a small sharp crack (i.e. so small it doesn’t really reduce the cross sectional area, s = P/A). • FRACTURE TOUGHNESS, K1c, is the key material property!! • Fracture toughness, K1c, is measured in the lab using compact fracture specimens – see samples.

  3. Fracture Toughness versus Strength: • Strength is resistance to plastic flow and thus is related to the stress required to move dislocations through the solid. The initial strength is called the yield strength. Strength generally increases with plastic strain because of work hardening, reaching a maximum at the tensile strength. The tensile strength is related to the strength of atomic bonds. • Toughness is the resistance of a material to the propagation of a crack. A material with low fracture toughness, if it contains a crack, may fail before it yields. A tough material will yield, work harden even when cracked – the crack makes no significant difference.

  4. What happens to a material with a small crack? Get high stress around crack, crack propogates and get sudden failure. Stress around crack is high due to Kt , but nominal stress is much lower than material yield strength! Yields then work hardens, absorb energy and redistribute stress. In other words, crack makes no significant difference! What happens when you nick a brittle material??

  5. Ductile Fracture: A plastic zone forms at the crack tip where the stress would otherwise exceed the yield strength σy. Stages of ductile fracture: b. Plastic def’m when stress exceeds yield. c. Weaken and fail locally due to inclusions which act as stress concentrations – this creates tiny voids. Voids continue to grow and coalesce to form larger voids. d. Remaining area gets smaller increasing stress until tensile strength is exceeded then fracture.

  6. Motivation for Fracture Mechanics • Very hard (if not impossible) to build a structure that is defect free (completely without cracks). • Cracks already in material (inclusions or voids). • Cracks caused by shrinkage in castings and welding. • Cracks caused by machining. • Cracks caused by cyclic loading (fatigue). • Cracks caused by corrosion. • Are we all doomed to mega disasters??? • KEY – DAMAGE TOLERANT DESIGN – THE MATERIAL MUST HAVE SUFFICIENT FRACTURE TOUGHNESS SO A NOTICEABLE CRACK CAN BE DETECTED BEFORE FAILURE. THIS IS THE BASES OF DAMAGE TOLERANT DESIGN – EXTREMELY IMPORTANT FOR AERSOPACE INDUSTRY.

  7. Brittle Behavior Causes: • Boilers to burst • Bridges to collapse • Aircraft to crash • Pipes to split • CATASTROPHIC FAILURES

  8. Tests for Toughness: (a) The tear test. (b) The impact test. Both are used as acceptance tests and for quality control, but neither measures a true material property (one that is independent of size and shape). To get at the real, underlying material properties we need the ideas of stress intensity and fracture toughness!!

  9. The Mechanics of Fracture Far from the crack where r >> c, the local stress falls to the value of s. Near the crack r << c, the local stress rises sharply as: Lines of force in a cracked body under load; the local stress is proportional to the number of lines per unit length, increasing steeply as the crack tip is approached.

  10. The Mechanics of Fracture So, for a given value of r, the local stress scales as Which there fore is a measure of the intensity of the local stress. This quantity is called the mode 1 stress intensity factor (the ‘mode 1’ means tensile fracture and is given the symbol K1.

  11. The Mechanics of Fracture = mode 1 stress intensity factor Constant depending on geometry/loading Average stress (i.e. away from crack) Crack size Failure when K1 = K1c where K1c is a material property called fracture toughness.

  12. The Mechanics of Fracture = mode 1 stress intensity factor Constant depending on geometry/loading Average stress (i.e. away from crack) Crack size Failure when K1 = K1c where K1c is a material property called fracture toughness.

  13. Mode 1 Stress intensities K1 associated with short cracks. In all cases, c << w. Internal penny shaped crack

  14. Again, Failure when: Failure stress at which fracture will occur. For small cracks, failure will be yield not fracture – check both!!!! Transition fro failure due to fracture vs failure due to yield will occur at ccrit. Cracks < ccrit will yield Cracks > ccrit will fracture Think!

  15. Failure by yield Failure by fracture

  16. Summary:

  17. How to measure fracture toughness, K1c Measuring fracture toughness, K1c. Two test configurations are shown here. Again, fracture toughness is a material property not to be confused with impact.

  18. A chart of fracture toughness Klc and modulus E. The contours show the toughness, Gc.

  19. A chart of fracture toughness K1c and yield strength σy. The contours show the transition crack size, ccrit.

  20. Damage-tolerant Design • KIC = fracture toughness; E = Young's modulus; σf = failure strength (the yield strength for metals and ductile polymers, the tensile strength for ceramics, glasses and brittle polymers loaded in tension; the flexural strength or modulus of rupture for materials loaded in bending).

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