4.7 Comparative Failure-Mode Synthesis & Integrated Flaw and Creep Assessment

Key Takeaways

  • Identifying the governing failure mode before selecting an equation is the single highest-value step in a Part 2 structural question.
  • Critical flaw size scales with the square of the ratio of fracture toughness to applied stress, so halving the applied stress quadruples the tolerable flaw.
  • In fracture mechanics the crack dimension used in the stress-intensity expression is the half-length for an embedded flaw but the full depth for a surface flaw.
  • Fatigue, fracture and creep can act in sequence on the same component: fatigue grows the flaw, fracture mechanics sets the critical size, and creep sets the remaining service life.
Last updated: September 2026

7. Comparative Synthesis of Structural Failure Modes

Table 4.3-1: Mechanical Failure Modes in Welded Construction

Failure MechanismPrimary Driving ForceTypical Crack MorphologyTemperature RegimeMost Vulnerable Weldment RegionPrimary Code Mitigation Strategy
FatigueCyclic stress range ($\Delta\sigma$), stress intensity range ($\Delta K$)Transgranular, flat, fatigue striations, beach marksAmbient to moderate ($T < 0.4 T_m$)Weld toe and root notches, undercut ($K_t$ points)Weld toe grinding/profiling, TIG dressing, HFMI peening, joint geometry optimization
Brittle Cleavage FracturePeak tensile stress exceeding $\sigma_f^*$, $K_I \ge K_{Ic}$Transgranular cleavage along ${100}$ planes, river patterns, bright facetsLow to ambient ($T < T_{\text{DBTT}}$)Coarse-Grained HAZ (CGHAZ), Intercritical HAZ (M-A constituent)Toughness testing (CVN $\ge 27\text{ J}$, CTOD), heat input control, post-weld heat treatment (PWHT)
High-Temp Creep RuptureSustained static stress, vacancy diffusionIntergranular cavitation along transverse grain boundariesElevated ($T > 0.45 T_m$, $T > 370^\circ\text{C}$ for steel)Fine-Grained HAZ (FGHAZ / Type IV zone in CSEF steels)Specify CSEF steels (P91/P92), precise PWHT ($750\text{--}770^\circ\text{C}$), operating temp derating
Lamellar TearingTransverse through-thickness shrinkage strainSub-surface stepped cracks parallel to rolling planeFabrication cooling ($T < 150^\circ\text{C}$)Rolled plate base metal beneath highly restrained T/corner jointsASTM A770 $Z35$ grade plate, low sulfur ($S < 0.005%$), CaSi treatment, weld buttering
Hydrogen Cold CrackingDiffusible hydrogen, high residual stress, susceptible microstructureTransgranular or intergranular microcracks, delayed onsetAmbient ($T < 100^\circ\text{C}$, 24–72 hrs post-weld)CGHAZ hard zones ($> 350\text{ HV}$), root passesLow-hydrogen consumables ($H4$), preheat and interpass control (AWS D1.1 Annex H)

8. Comprehensive Worked Numerical Example: LEFM Flaw Assessment & Larson-Miller Creep Life Prediction

Problem Statement

An engineering critical assessment (ECA) is performed on a welded energy infrastructure facility involving two independent structural failure evaluations:

Part 1: LEFM Critical Flaw Sizing on a Pressure Vessel A cylindrical pressure vessel shell (inner diameter $D_i = 2,000.0\text{ mm}$, wall thickness $t = 40.0\text{ mm}$) fabricated from quenched and tempered steel ($\sigma_y = 480.0\text{ MPa}$, plane strain fracture toughness $K_{Ic} = 55.0\text{ MPa}\sqrt{\text{m}}$ at MDMT of $-20^\circ\text{C}$) operates at internal pressure $p = 8.0\text{ MPa}$. Transverse welding residual stresses in the un-PWHT joint contribute an additional tensile stress $\sigma_{\text{res}} = 60.0\text{ MPa}$ parallel to the hoop direction. Phased array ultrasonic testing (PAUT) reveals an external longitudinal surface crack with geometric factor $Y = 1.12$.

  • Calculate the critical crack depth $a_c$ that would trigger catastrophic brittle fracture at $-20^\circ\text{C}$.
  • Verify whether plate thickness satisfies ASTM E399 plane strain validity.

Part 2: Larson-Miller Creep Life Extrapolation A high-energy Grade 91 steam line ($T_m = 1,510^\circ\text{C} = 1,783\text{ K}$) operates at nominal steam temperature $T_1 = 575^\circ\text{C}$ ($T_{K1} = 848.15\text{ K}$) under an effective hoop stress of $85.0\text{ MPa}$. Experimental creep rupture data for Grade 91 cross-weld joints at $85.0\text{ MPa}$ establishes a Larson-Miller parameter $LMP = 25.40$ (using $C = 20$, with $T$ in Kelvin and $LMP$ scaled by $10^{-3}$).

  • Calculate the projected creep rupture life $t_{r1}$ in operating hours.
  • If a boiler burner tilt malfunction causes a continuous $35^\circ\text{C}$ temperature excursion to $T_2 = 610^\circ\text{C}$ ($T_{K2} = 883.15\text{ K}$), calculate the new rupture life $t_{r2}$ and the percentage loss of operational life.

Step-by-Step Solution

Step 1: Calculate operating hoop stress and total acting stress Internal radius $R_i = D_i / 2 = 1,000.0\text{ mm}$. Thin-wall membrane hoop stress:

σhoop=pRit=8.0 MPa×1,000.0 mm40.0 mm=200.0 MPa\sigma_{\text{hoop}} = \frac{p \cdot R_i}{t} = \frac{8.0\text{ MPa} \times 1,000.0\text{ mm}}{40.0\text{ mm}} = 200.0\text{ MPa}

Total acting tensile stress:

σtotal=σhoop+σres=200.0 MPa+60.0 MPa=260.0 MPa\sigma_{\text{total}} = \sigma_{\text{hoop}} + \sigma_{\text{res}} = 200.0\text{ MPa} + 60.0\text{ MPa} = 260.0\text{ MPa}

Step 2: Calculate critical crack depth $a_c$ Setting applied stress intensity equal to fracture toughness ($K_I = K_{Ic}$):

KIc=Yσtotalπac    πac=KIcYσtotalK_{Ic} = Y \sigma_{\text{total}} \sqrt{\pi a_c} \implies \sqrt{\pi a_c} = \frac{K_{Ic}}{Y \sigma_{\text{total}}} πac=55.0 MPam1.12×260.0 MPa=55.0291.2=0.18887 m1/2\sqrt{\pi a_c} = \frac{55.0\text{ MPa}\sqrt{\text{m}}}{1.12 \times 260.0\text{ MPa}} = \frac{55.0}{291.2} = 0.18887\text{ m}^{1/2}

Squaring both sides:

πac=(0.18887)2=0.035673 m\pi a_c = (0.18887)^2 = 0.035673\text{ m} ac=0.035673π=0.011355 m=11.36 mma_c = \frac{0.035673}{\pi} = 0.011355\text{ m} = 11.36\text{ mm}

Evaluation: Any surface crack exceeding $11.36\text{ mm}$ depth will trigger catastrophic brittle fracture under service pressure at $-20^\circ\text{C}$.

Step 3: Check ASTM E399 plane strain validity

Breq2.5(KIcσy)2=2.5(55.0480.0)2=2.5×(0.11458)2=2.5×0.01313=0.0328 m=32.8 mmB_{\text{req}} \ge 2.5 \left( \frac{K_{Ic}}{\sigma_y} \right)^2 = 2.5 \left( \frac{55.0}{480.0} \right)^2 = 2.5 \times (0.11458)^2 = 2.5 \times 0.01313 = 0.0328\text{ m} = 32.8\text{ mm}

Because actual shell wall thickness $t = 40.0\text{ mm} > 32.8\text{ mm}$, plane strain conditions are fully validated.

Step 4: Calculate creep rupture life at normal design temperature ($575^\circ\text{C}$) LMP=25.40=TK1[20+log10(tr1)]×103LMP = 25.40 = T_{K1} \left[ 20 + \log_{10}(t_{r1}) \right] \times 10^{-3}

25,400=848.15×[20+log10(tr1)]25,400 = 848.15 \times \left[ 20 + \log_{10}(t_{r1}) \right] 20+log10(tr1)=25,400848.15=29.947520 + \log_{10}(t_{r1}) = \frac{25,400}{848.15} = 29.9475 log10(tr1)=29.947520.0=9.9475\log_{10}(t_{r1}) = 29.9475 - 20.0 = 9.9475 tr1=109.9475=8.861×109 hours(Indefinite design life under ideal baseline temperature)t_{r1} = 10^{9.9475} = 8.861 \times 10^9\text{ hours} \quad (\text{Indefinite design life under ideal baseline temperature})

Step 5: Calculate creep rupture life under temperature excursion ($610^\circ\text{C}$) Under the elevated temperature $T_{K2} = 883.15\text{ K}$:

20+log10(tr2)=25,400883.15=28.760720 + \log_{10}(t_{r2}) = \frac{25,400}{883.15} = 28.7607 log10(tr2)=28.760720.0=8.7607\log_{10}(t_{r2}) = 28.7607 - 20.0 = 8.7607 tr2=108.7607=5.764×108 hourst_{r2} = 10^{8.7607} = 5.764 \times 10^8\text{ hours}

Ratio of remaining life:

tr2tr1=5.764×1088.861×109=0.0650=6.50%\frac{t_{r2}}{t_{r1}} = \frac{5.764 \times 10^8}{8.861 \times 10^9} = 0.0650 = 6.50\%

Engineering Insight: A mere $35^\circ\text{C}$ operating temperature excursion accelerates creep damage by a factor of 15.4, destroying $93.5%$ of the component's remaining creep rupture life!


9. Real-World Engineering Scenarios & Exam Pitfalls

Industrial Scenario: Type IV Creep Rupture in a Grade 91 Heat Recovery Steam Generator (HRSG)

An 8-year-old combined-cycle power plant experienced an explosive rupture of a $400\text{ mm}$ diameter Grade 91 main steam pipe elbow weld operating at $565^\circ\text{C}$ and $18\text{ MPa}$. Metallurgical failure analysis revealed that the fracture occurred circumferentially along the fine-grained heat-affected zone (FGHAZ), roughly $2\text{ mm}$ from the fusion boundary, with zero wall thinning or macro-deformation. Microscopic examination identified extensive cavitation void arrays along prior austenite grain boundaries—classic Type IV cracking. The root cause was traced to improper post-weld heat treatment (PWHT): during field erection, local induction heating coils produced an under-temperature band ($710^\circ\text{C}$ instead of the code-mandated $750\text{--}770^\circ\text{C}$ per ASME B31.1), failing to re-precipitate complex carbonitrides. The softened FGHAZ experienced accelerated tertiary creep, leading to premature catastrophe.

Common Exam Traps

Exam Trap 1: Assuming High-Strength Steel Improves Welded Fatigue Strength CWEng examination questions frequently ask how much fatigue design allowable stress increases if ASTM A36 steel ($\sigma_y = 250\text{ MPa}$) is replaced with ASTM A514 quenched-and-tempered steel ($\sigma_y = 690\text{ MPa}$) for an as-welded bridge girder. The correct answer is $0%$! Because geometric notch concentrations at weld toes eliminate initiation life, and high tensile residual stresses enforce $R_{\text{eff}} \approx 1.0$, fatigue design categories (AWS D1.1 / IIW) depend strictly on stress range $\Delta\sigma$, regardless of static yield strength.

Exam Trap 2: Using Celsius Instead of Absolute Temperature in Larson-Miller Calculations The Larson-Miller parameter equation is derived from kinetic Arrhenius rate theory and requires absolute temperature (Kelvin or Rankine). Substituting $T = 575^\circ\text{C}$ instead of $T_K = 575 + 273.15 = 848.15\text{ K}$ will produce completely nonsensical life predictions and is an intentional distractor on Part 1 and Part 2 exams.

Exam Trap 3: Embedded Internal Flaw vs. Surface Crack Dimension in LEFM In the stress intensity formula $K_I = Y \sigma \sqrt{\pi a}$, $a$ represents the half-length of an embedded internal crack ($2a$), but the full depth of an edge or surface crack ($a$). If an exam problem states "an internal embedded planar flaw of length $16\text{ mm}$", you must set $a = 8\text{ mm} = 0.008\text{ m}$. Using $a = 16\text{ mm}$ overestimates $K_I$ by a factor of $\sqrt{2} \approx 1.414$.

Test Your Knowledge

A non-destructive examination of a thick-walled welded vessel identifies an embedded planar crack of depth 2a = 16 mm (crack half-depth a = 8.0 mm = 0.008 m). The vessel is subjected to a nominal tensile stress σ = 220 MPa perpendicular to the crack plane. Assuming an internal crack geometry correction factor Y = 1.0, what is the applied Mode I stress intensity factor K_I, and will unstable fracture occur if the material has a fracture toughness K_Ic = 40.0 MPa√m?

A
B
C
D