Materials, Failure and LSFs
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Transcript of Materials, Failure and LSFs
7/29/2019 Materials, Failure and LSFs
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Material PropertiesFailure Modes
Limit State FunctionsReferences
Structural Integrity
Day 1-3: Materials, Failure, and LSFs
Dr N.C. RentonPhD CEng MIChemE
School of Engineering, University of Aberdeen, U.K.
UCAN, Bogota, 12th-15th July, 2011 Structural Integrity Day 1-3: Materials, Failure, and LSFs
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Material PropertiesFailure Modes
Limit State FunctionsReferences
‘Safety is a state of mind ’
UCAN, Bogota, 12th-15th July, 2011 Structural Integrity Day 1-3: Materials, Failure, and LSFs
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Material PropertiesFailure Modes
Limit State FunctionsReferences
Outline
1 Material Properties
2 Failure Modes
3 Limit State Functions
UCAN, Bogota, 12th-15th July, 2011 Structural Integrity Day 1-3: Materials, Failure, and LSFs
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Material PropertiesFailure Modes
Limit State FunctionsReferences
Constitutive Relation
Figure: The stress-strain relation for Carbon Steels
UCAN, Bogota, 12th-15th July, 2011 Structural Integrity Day 1-3: Materials, Failure, and LSFs
M i l P i
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Material PropertiesFailure Modes
Limit State FunctionsReferences
Crack Resistance
There are two ways of representing the crack resistance of a material:
1 Energy based interpretation e.g. Toughness G , J -Integral
2 Stress field e.g. Stress Intensity Factor K :
The stress intensity factor is common for most carbon steels, and the
mode I opening equation is given by:
K I = Y σ (πa)1/2 (1)
where Y is a dimensionless function related to the crack geometry(a, 2c ), a is the crack depth, 2c is the crack length. When K I reachessome critical value, and provided the level of plastic strain around thecrack is small (small scale yielding), the crack propagates in a brittlefashion at the speed of sound. The critical value is known as K IC , oftenreferred to as the fracture toughness.
UCAN, Bogota, 12th-15th July, 2011 Structural Integrity Day 1-3: Materials, Failure, and LSFs
Material Properties
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Material PropertiesFailure Modes
Limit State FunctionsReferences
Corrosion Resistance
Figure: Corrosion damage to duplex SS
UCAN, Bogota, 12th-15th July, 2011 Structural Integrity Day 1-3: Materials, Failure, and LSFs
Material Properties
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Material PropertiesFailure Modes
Limit State FunctionsReferences
Corrosion Resistance
Figure: Tafel Plot (Current v/s Potential) of a Stainless Steel
UCAN, Bogota, 12th-15th July, 2011 Structural Integrity Day 1-3: Materials, Failure, and LSFs
Material Properties
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Material PropertiesFailure Modes
Limit State FunctionsReferences
Corrosion Resistance
The corrosion resistance of a material depends on a number of things:
Chemical Composition: Cr, Mo, W, Ni, Cu, N.
Presence of protective oxide film.
Plastic deformation i.e. number of dislocations per unit volume.
Crystallographic structure i.e. Ferrite (bcc), Austenite (FCC),Martensite, etc
Diffusion coefficients
All are important in determining the materials ability to avoid particularcorrosion mechanisms, and hence failure.
UCAN, Bogota, 12th-15th July, 2011 Structural Integrity Day 1-3: Materials, Failure, and LSFs
Material Properties
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Material PropertiesFailure Modes
Limit State FunctionsReferences
Failure Mode: Burst
The engineering system we are going to concentrate on is a steel pressurecontaining vessel. The failure mode we are going to examine iscatastrophic burst by overpressure which will provide the framework forthe course. The problem is simplified by considering only the hoop stress
σh caused by the internal pressure, and the assumption of a thin-walledcylinder. The hoop stress is then:
σh =P .D
2.t × g (D , t ,wall loss defect) (2)
where P is the internal pressure (Pa); D is the vessel diameter(m); t isthe wall thickness of the vessel where t = r 2 − r 1(m); andg (D , t ,wall loss defect) is a dimensionless function that represents anarea of wall loss through corrosion.
UCAN, Bogota, 12th-15th July, 2011 Structural Integrity Day 1-3: Materials, Failure, and LSFs
Material Properties
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pFailure Modes
Limit State FunctionsReferences
Limit State Functions
Freudenthal[1, 2] and Shinozuka[3] introduced a modelling approach of the event ’failure’ in structural reliability problems. The failure event, orlimit state, is modelled by defining a safety margin M , a scalar, where:
M ≤ 0 corresponds to failureM > 0 corresponds to safe operation
In the simplest case M is defined in terms of the capacity of the system(R ) and the demand placed on it (S ) in which case failure can be
described by: M = R − S (3)
The techniques are described in detail in [4, 5].
UCAN, Bogota, 12th-15th July, 2011 Structural Integrity Day 1-3: Materials, Failure, and LSFs
Material Properties
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Failure ModesLimit State Functions
References
Limit State Functions
In our example, failure occurs when the hoop stress exceeds the ultimatestress σu of the steel the vessel is constructed from. The capacity R isthe ultimate stress σu and the demand S is the applied stress σh. The
safety margin or limit state function can then be written as:
M = σu − σh (4)
and hence:
M = σu −
P .D
2.t g (D , t ,wall loss defect) (5)
UCAN, Bogota, 12th-15th July, 2011 Structural Integrity Day 1-3: Materials, Failure, and LSFs
Material Properties
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Failure ModesLimit State Functions
References
References
[1] A. M. Freudenthal. “Safety, Reliability, and Structural Design”. In:Transactions of ASCE 127.Paper No 3372 (1962), pages 304–319.
[2] A. M. Freudenthal, J. M. Garrelts, and M. Shinozuka. “The Analysisof Structural Safety”. In: Journal of the Structural Division ASCE
92.ST1 (1966), pages 267–325.
[3] M. Shinozuka. “Probability of Structural Failure under RandomLoading”. In: Journal of the Engineering Mechanics Division, ASCE
90.EM5 (1964), pages 147–170.
[4] P. Thoft-Christensen and M. J. Baker.Structural Reliability Theory
and its Applications . Springer Verlaag, 1982. isbn: 0387117318.
[5] R.E. Melchers. Structural Reliability Analysis and Prediction. 2nd.1999. isbn: 978-0-471-98771-0.
UCAN, Bogota, 12th-15th July, 2011 Structural Integrity Day 1-3: Materials, Failure, and LSFs