Ppt Lecture 6

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MECH3300 : Fracture Mechanics - lecture 6 Dr Rowan Truss (Bldg 45-rm 215, [email protected])

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Transcript of Ppt Lecture 6

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MECH3300 : Fracture Mechanics - lecture 6

Dr Rowan Truss(Bldg 45-rm 215, [email protected])

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ObjectivesStudents should understand:

Design and Materials Selection issues:Use of basic fracture mechanics equationYield before fractureLeak before break

Statistical nature of brittle fracture Wiebull modulus

Case study – Comet aircraft crashes

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Basic fracture mechanics equationK1c = σ Y √πa

combines three quantities, namely;a material property, K1c

the applied tensile stress or design stress, σan allowable flaw size, a

( Note: Y may also be a function of a).

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Yield before brittle fractureK1c = σ Y √πa

The stress required for a crack of size ac to propagate is σ = K1c / (Y √πac)

We want brittle failure stress < yield stress, σy , so in the limit set σ = σy

Rearranging π ac = (1/Y2) (K1c /σy)2

Safest vessel is when allowable flaw size is largest somaximise (K1c /σy)2

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Leak before breakK1c = σ Y √πa

For leak before break the critical flaw size needs to be ≥ t, the thickness of the vessel

t = (1/ π Y2) (K1c /σy)2

Thickness is also set so that vessel will not yield for spherical vessel, radius, r, σ = pr/2t

p = (2/ πr Y2) (K1c /σy)2

Maximise K1c2/σy for highest failure pressure

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M. F. Ashby, Materials Selection in Mechanical Design, Butterworth Hinemann, Oxford, 1999

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Statistics of brittle failureK1c = σ Y √πa

K1c is a material parameter ie constantBrittle failure stress thus depends on flaws sizeReal materials have a distribution of flaw sizesBrittle failure stress also has distribution Measure of breadth of distribution given by Wiebull modulus

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Wiebull Modulusfraction of samples of volume V0

that do not fracture under a tensile load σ

Ps(V0) = exp[-(σ/σ0)m]

σ0 is stress at which survival probability is 1/e

m is Wiebull Modulus

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Comet aircraft failuresRef: D. R. H. Jones, Engineering Materials 3 Materials Failure Analysis Case Studies and Design Implications, Pergamon Press Oxford, 1993 ch13

One of first pressurised cabin commercial aircraftBuilt by de Havillands, UK for BOAC in 19524x turbo-jet enginesCruising altitude of 35,000 ftAll-up weight of 49 tonnes

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Comet aircraft failures2nd May 1953 Plane crashed in tropical thunderstorm in Calcutta – structural failure of the aircraft10 January, 1954 Rome- London flight crashed in good weather – killed 29 passengers and 6 crew8 April, 1954 Rome-Cairo flight crashed again in reasonable weather

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Material dataAluminium alloy DTD546Obsolete – modern equivalent 2000 series alloys

3.5-4.8 wt% Cu< 1.0 wt% Fe<1.5 wt% Si<0.6 wt% Mg< 1.2 wt% Mn< 0.3 wt% TiBalance Al

min σy 325 MPaσuts 418 MPa, actual for failed material 450MPa

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dimensionsFuselage

3.7m diameter33m longThickness of Al sheet 0.91mmPressurised to 0.057MPa

What size crack would cause failure?

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Estimate K1c

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Critical flaw sizeFor pressure, p, in cylindrical pressure vesselHoop stress σ = pr/t

= 0.057*1.85/(0.91x10-3)= 116MPa

For plane strain, assume K1c = 30 MPam1/2

ac = 1/π (K1c/σy)2 = 21mm

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Plane strain?Require t ≥ 2.5 (K1c/σy)2

= 2.5 (30/350)2

= 18mm

Not plane strain, need plane stress analysis

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Plane stress Kc depends on thicknessassume same relationship as known Al alloy 7075-T6

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Critical flaw size – plane stressKc = 2.6 x plane strain value

= ~x80 MPam1/2

For plane stressac = 1/π (K1c/σy)2

= ~150mm

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Validity of using LEFM in plane stressNeed crack size , a ≥ 50 rp , plastic zone size

Plastic zone size in plane stressrp = 1/2p (K1c/σy)2 = 8.3 mm

So probably not valid But error low for crack in infinite sheet

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