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Mechanical Properties of Structural Steels in Hydrogen B.P. Somerday, K.A. Nibur, C. San Marchi, and M. Yip Sandia National Laboratories Livermore, CA DOE Hydrogen Pipeline Working Group Meeting Aiken, SC September 25-26, 2007

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  • Mechanical Properties of

    Structural Steels in Hydrogen

    B.P. Somerday, K.A. Nibur, C. San Marchi, and M. Yip Sandia National Laboratories

    Livermore, CA

    DOE Hydrogen Pipeline Working Group Meeting Aiken, SC

    September 25-26, 2007

  • HHH

    d/dt 0

    H2H2

    Methods for measuring mechanical properties

    of structural steels in hydrogen

    d/dt > 0 d/dt > 0 strength of materials: UTS, YS, f, RA

    H2HH H H2H H2H H2H HH2H H2

    fracture mechanics: KIH, KTH

    HH H

    H H

    H H

    H

    H H

    d/dt 0

    H

    H H

    H

    H

    H HH

    H

    H

    HH H

    H

    H2H2 H2 H2 H2

    H2

  • Tensile Testing Carbon Steel in H2

    Extrusion Direction/ L-C Orientation

    T

    T

    Base HA

    Z

    Weld

    Wel

    d

    Alloys: 106 Grade B Multi-pass SMAW w/out stress

    relief Specimens machined in 3

    conditions: Base metal, Weldand HAZ

    Orientation: L-C Atmosphere: 10.3 MPa H2,

    ambient pressure Air Strain Rate: 10-4 /sec # of samples per matrix point:

    6 Argon purge followed by H2

    pressurization Soak (30 min.) at pressure Test to failure

  • Tensile Properties

    Mechanical Properties Average Properties

    0.2%Yield (MPa)

    Dev. UTS (MPa)

    Dev. Elong. at

    failure

    Dev. Reduction of

    Area (%) Dev.

    Air 355.3 15.8 484.6 8.6 0.29 0.04 68.6 1.5

    Bas

    e

    H2 357.1 32.9 486.4 17.8 0.19 0.04 30.8 5.0

    Air 343.0 20.0 490.4 9.0 0.28 0.01 74.9 2.2

    Wel

    d

    H2 350.0 16.1 480.9 12.0 0.21 0.02 30.5 6.4

    Air 349.3 20.8 482.3 7.6 0.27 0.04 71.0 1.7

    HA

    Z

    H2 338.2 18.5 475.5 9.6 0.19 0.04 30.4 6.8

  • Fractography

    Fracture Surface

    Area

    Air Hydrogen HAZ Samples

    Reduction of Area reduced when tested in hydrogen

  • Crack propagation resistance of X100 steel

    Alloy composition C Mn Si P S Ti V Ni Cu Mo Cr

    0.073 1.86 0.11 0.009

  • Measurement of sustained-load cracking thresholds

    wedge opening load (WOL) cracking threshold specimen

    Loading bolt

    Load cell

    13 mm

    strain gage leads (Excitation and DAQ)

    Load

    (P)

    Po Ko

    PTH KTH

    incubation time= f(environment, Ko)

    Time in H2

    Specimen loaded to Ko>KTH using bolt while contained in glove box (Ar with ~1 ppm O2)

    Loaded specimen exposed to H2, crack extends after incubation time

    Crack arrests at K=KTH

  • High-pressure H2 gas severely degrades crack

    propagation resistance of X100 steel

    Stre

    ss in

    tens

    ity fa

    ctor

    , K (

    ksii

    n1/2)

    X100 in air H2 gas pressure (MPa)

    0 25 50 75 100 125 150 400

    150

    KJIc Ko KTH

    X100 Steel C-L orientation 25 oC

    no crack extension after >1000 hrs

    150

    100 100

    50 50

    0 0

    1/2 )

    Stre

    ss in

    tens

    ity fa

    ctor

    , K (

    MP

    am400 350

    350 300

    300 250

    250 200

    200

    X100 in 15 kpsi H2 gas

    0 5 10 15 20 25 H2 gas pressure (kpsi)

  • Images of fracture surfaces from X100 tested in

    H2 show long crack lengths and delaminations

    H2-assisted crack extension from precrack

    a/W=0.94

    http:a/W=0.94

  • FEM calculations verify K solution and demonstrate

    K dominance for long cracks in WOL specimen

    a / W = 0.941 KI

    VmE / W1/ 2

    0.18

    0.16

    0.14

    0.12

    0.1

    0.08

    0.06

    0.04

    0.02

    0 0.5 0.6 0.7 0.8 0.9 1

    a / W ASTM E1681: KI = 57.5 MPa m FEM elastic: KI = 63.8 MPa m FEM plastic: J = 16.0 kJ/m2

    Calculations by M. Dadfarnia and P. Sofronis JEKIJ = 2 KIJ = 62.2 MPa m1

    ASTM E1681

    FEM

  • Incubation time for crack extension depends on Ko

    Initial stress intensity factor, Ko (MPam1/2)

    0 30 60 90 120 150 2700

    0 30 60 90 120 150

    cracking in H2 no cracking in H2

    X100 Steel WOL specimens 15 kpsi H2 gas 25 oC

    no crack extension after >2500 hr

    KTH In

    cuba

    tion

    time

    (hr)

    2400

    2100

    1800

    1500

    1200

    900

    600

    Load

    (P)

    Po Ko

    PTH KTH

    incubation time

    Time in H2 300 0

    Initial stress intensity factor, Ko (ksi in1/2)

    Measurement of sustained-load cracking threshold in H2 cannot be assured unless crack propagates

  • Crack branching may account for no crack extension

    in specimens with Ko>KTH

    Incu

    batio

    n tim

    e (h

    r)

    SA 372 Gr. J in 15 kpsi H2

    Initial stress intensity factor, Ko (MPam1/2)

    0 30 60 90 120 150 2700

    2400

    2100

    1800

    1500

    1200

    900 X100 in 15 kpsi H2 600

    300

    0 0 30 60 90 120 150

    Initial stress intensity factor, Ko (ksi in1/2)

    precrack

    cracks propagated in H2

    cracking in H2 no cracking in H2

    X100 Steel WOL specimens 15 kpsi H2 gas 25 oC

    no crack extension after >2500 hr

    KTH

  • Low-alloy steels for pressure vessels:

    sustained-load cracking thresholds in H2 gas

    Yield strength, Sy (ksi) 87 92 97 102 107 112 117 122 127 132 137

    160

    600 650 700 750 800 850 900 950

    Cr-Mo Steels WOL specimens

    4130 steel

    100 MPa H2 gas

    25 oC DOT 3AAX

    Loginow and Phelps, Corrosion, 1975

    4145 steel 4147 steel

    SA 372 Grade J

    DOT 3T

    80 80

    60

    60

    140

    140 120

    120

    1/2 )

    (M

    Pa

    mK

    TH

    100 100

    (ksi

    in1/

    2 )K

    TH

    4040

    2020

    0 0

    Yield strength, Sy (MPa)

    Thresholds in modern Cr-Mo steels are higher than thresholds in older steels

  • Stainless steels for piping: tensile fracture results

    for specimens precharged in hydrogen gas

    316 stainless steels with ~140 wppm hydrogen

    Tensile fracture resistance of H-precharged specimens is sensitive to nickel content but not strain hardening

  • Stainless steels tested in hydrogen gas vs precharged show different tensile fracture behavior

    H2 H2

    H2

    H2 H2

    H2

    H

    H H H

    HH

    H H

    0

    20

    40

    60

    80

    100R

    educ

    tion

    of A

    rea,

    RA

    (%)

    1 1 2

    2 3

    4

    3

    4

    3

    4

    Internal Hydrogen 3 - air 4 - H-precharged

    External Hydrogen 1 - 69 MPa He 2 - 69 MPa H 2

    A-286 San Marchi et al., SAE World Congress, 2007

    S (MPa) = 720 850 790 810 810 y

    Stable stainless steels may not exhibit loss in RA when strained in H2 due to limited H uptake

  • System for measuring fatigue crack growth

    in high-pressure H2 nearly complete

    vessel on mechanical test frame

    gas manifold

    Pressure vessel can contain H2 gas up to 20 kpsi (138 MPa)

  • What is metric for qualifying steels for H2 pipelines?

    Tech. Ref. Hydrogen Compatibility of Materials, www.ca.sandia.gov/matlsTechRef

    10-1

    10-2

    10-3 X70 (6.9 MPa H2) X42 (6.9 MPa H2) X60 (6.9 MPa H2) A516 (6.9 MPa H2)

    10-4 1020 (7.0 MPa H2) SA 105 (6.9 MPa H2) X70 (6.9 MPa N2)

    10-5 X42 (6.9 MPa N2) X60 (air) A516 (air) 1020 (air)

    10-6 SA 105 (34.5 MPa He)

    10-7

    Stress intensity factor range, K (MPam1/2) 1 10 100

    Fatig

    ue c

    rack

    gro

    wth

    rate

    , da/

    dN (

    mm

    /cyc

    le)

    Carbon Steels frequency = 0.1 to 1 Hz load ratio = 0.1 to 0.15 Fatigue crack growth rates in

    H2 greater than growth rates in air or inert gas

    Fatigue crack growth rates in H2 vary by factor of 10

    What is acceptable fatigue crack growth rate?

  • Assess fatigue crack growth data by conducting

    fracture mechanics analysis of pipeline

    Assume pipeline subjected to pressure cycling

    p

    Ri Ro

    aot

    p pR=pmin/pmax~0.1 R=pmin/pmax~0.8 pmax pmax

    pmin

    pmin time time

    Calculate number of pressure cycles for crack to reach critical depth

    calculated from threshold for sustained-load cracking, KTH, or fracture toughness, KIH ac

    a

    ao number of pressure cycles, N Nc

    X

    calculated from da/dN vs K relationship

  • Assume steel, dimensions, and maximum

    pressure are similar to current H2 pipelines

    p

    Ri Ro

    aot

    Data for Air Products H2 pipelines (ASME, Hydrogen Standardization Interim Report, 2005)

    API 5L X42 steel, manufactured with ERW Inner radius, Ri = 6.0 in Wall thickness, t, from 0.219 to 0.500 in

    Maximum operating pressure, p = 1500 psi

    Assume existing defect with depth ao and length parallel to pipeline axis Simulates defect along manufacturing

    (seam) weld

  • Select appropriate material property data Fa

    tigue

    cra

    ck g

    row

    th ra

    te, d

    a/dN

    (in

    /cyc

    le)

    10-2

    Cialone et al., Met Trans A, 1985

    10-3

    10-4

    10-6

    10-5 1000 psi H2, R=0.1 1000 psi N2, R=0.1 1000 psi H2, R=0.8 1000 psi N2, R=0.8

    10-7

    Stress intensity factor range, K (ksiin1/2)

    10-8

    1 10 100

    API 5L X42 Steel frequency = 1 Hz

    da/dN=(3.55x10-11)K3.83

    da/dN=(2.51x10-12)K6.56

    Need da/dN vs K for X42 ERW in 1500 psi H2 gas assume data for 1000 psi H2

    gas representative assume data for weld and base

    metal are similar Need da/dN vs K at relevant

    R ratio and frequency pressure cycling parameters

    for pipeline unknown use data at R=0.1 and

    frequency=1 Hz Need fracture toughness for

    X42 ERW in 1500 psi H2 gas KIH=44 ksiin1/2 for weld HAZ in

    1000 psi H2 (Cialone et al., ASTM STP 962, 1988)

  • Fatigue crack growth rates similar in base

    metal, fusion zone, and HAZ for X60 steel

    Fatig

    ue c

    rack

    gro

    wth

    rate

    , da/

    dN (

    mm

    /cyc

    le)

    Wachob, NASA-CR-166334, 1981

    10-2

    10-3 base metal (6.9 MPa H2) SA weld FZ (6.9 MPa H2) SA weld HAZ (6.9 MPa H2) base metal (air) SA weld FZ (air) SA weld HAZ (air)

    10-4

    10-5

    1/2)Stress intensity factor range, K (MPam

    X60 Steel frequency = 1 Hz load ratio = 0.15

    1 10 100

  • Calculate number of pressure cycles to reach

    critical crack depth for three cases

    cycle 1 cycle 2

    p

    Ri Ro

    aot

    K1=f(ao,p,Ro,Ri,t) K2=f(a1,p,Ro,Ri,t) p

    1500 psi

    150 psi cycles

    a=(2.51x10-12)K1 6.56 a1=ao+a

    a=(2.51x10-12)K2 6.56 a2=a1+a

    ao a1 a2

    Case 1: t=0.330 in (h=65% SMYS) and ao/t=0.10

    Case 2: t=0.500 in (h=43% SMYS) and ao/t=0.10

    Case 3: t=0.500 in (h=43% SMYS) and ao/t=0.05

    http:ao/t=0.05http:ao/t=0.10http:ao/t=0.10

  • 0.3

    0.7

    0.8

    Number of pressure cycles vs crack depth

    relationships: H2 compared to inert gas

    crac

    k de

    pth

    / wal

    l thi

    ckne

    ss, a

    /t

    0.6

    0.5

    0.4

    0.2

    0.1

    0.0 0 50000 100000 150000 200000 250000

    hydrogen t=0.50 in h=43% SMYS

    nitrogen t=0.50 in h=43% SMYS

    X42 Pipeline hydrogen or nitrogen gas pressure cycle = 150 - 1500 psi inner diameter = 12 in

    X

    X critical crack depth calculated from KIc

    critical crack depth calculated from KIH

    10-2

    Fatig

    ue c

    rack

    gro

    wth

    rate

    , da/

    dN (

    in/c

    ycle

    )

    10-3

    10-4

    10-5

    10-6

    10-7

    1 10 100

    API 5L X42 Steel frequency = 1 Hz

    da/dN=(3.55x10-11)K3.83

    da/dN=(2.51x10-12)K6.56

    1000 psi H2, R=0.1 1000 psi N2, R=0.1

    10-8

    number of pressure cycles Stress intensity factor range, K (ksiin1/2)

    Number of cycles to critical crack depth reduced

    by about factor of 40 in H2 compared to inert gas

  • 0.3

    0.7

    0.8

    Number of pressure cycles vs crack depth

    relationships in H2 for varying dimensions

    crac

    k de

    pth

    / wal

    l thi

    ckne

    ss, a

    /t

    0.6

    0.5

    0.4

    0.2

    0.1

    0.0 0 5000 10000 15000 20000 25000 30000 35000 40000 45000

    case 1 t=0.33 in h=65% SMYS

    case 2 t=0.50 in h=43% SMYS

    case 3 t=0.50 in h=43% SMYS

    X42 Pipeline hydrogen gas pressure cycle = 150 - 1500 psi inner diameter = 12 in

    X

    X X

    critical crack depths calculated from KIH

    10-2 API 5L X42 Steel frequency = 1 Hz

    1000 psi H2, R=0.1

    case 1 initial K

    case 2 initial K

    case 3 initial K

    da/dN=(2.51x10-12)K6.56

    10-8

    1 10 100 Stress intensity factor range, K (ksiin1/2)number of pressure cycles

    Fatig

    ue c

    rack

    gro

    wth

    rate

    , da/

    dN (

    in/c

    ycle

    )

    10-3

    10-4

    10-5

    10-6

    10-7

    Number of cycles to critical crack depth is sensitive to applied stress and initial crack depth

    http:da/dN=(2.51x10-12)K6.56

  • ASME applies safety factors on critical crack depth

    and number of cycles to critical crack depth

    a/ac

    1.0

    0.25

    critical crack depth critical crack depth

    M.D. Rana et al., ASME PVP, 2007 cycles to

    Safety factors: a/ac = 0.25 N/Nc = 0.5

    0.5 1.0 N/Nc

    0.500

    0.500

    0.500

    0.330

    t (in)

    43% SMYS

    43% SMYS

    43% SMYS

    65% SMYS

    h

    112,545125,2600.10inert

    20,69038,7900.05H2

    2,6602,7350.10H2

    5351700.10H2

    0.5 x Nccycles to 0.25 x ac

    ao/tEnvironment

  • Lifetime of steel hydrogen pipeline depends on

    both material properties and structural design

    Fatigue crack growth law da/dN=CKn in stage II

    Fracture toughness or threshold for sustained-load cracking does not significantly affect cycles to critical crack depth

    Wall thickness affects stress (K)

    Initial crack depth depends on detection limit of NDE

    Operating pressure affects stress (K) and material properties

  • Fatigue crack growth rates depend on

    load cycle profile

    da/d

    N (

    mm

    /cyc

    le)

    Walter and Chandler, Effect of Hydrogen on Behavior of Materials, 1976

    0.04 SA 105 Steel H2 pressure = 100 MPa K = 44 MPam

    0.03 load ratio = 0.1

    0.02

    0.00 0 200 400 600 800 1000 1200 1400

    Seconds Per Cycle

    0.01

    0.5 sec ramp 100 sec ramp

    Mechanical Properties ofStructural Steels in HydrogenMethods for measuring mechanical propertiesof structural steels in hydrogenTensile Testing Carbon Steel in H2Tensile PropertiesFractographyCrack propagation resistance of X100 steelMeasurement of sustained-load cracking thresholdsHigh-pressure H2 gas severely degrades crackpropagation resistance of X100 steelImages of fracture surfaces from X100 tested inH2 show long crack lengths and delaminationsFEM calculations verify K solution and demonstrateK dominance for long cracks in WOL specimenIncubation time for crack extension depends on KoCrack branching may account for no crack extensionin specimens with Ko>KTHLow-alloy steels for pressure vessels:sustained-load cracking thresholds in H2 gasStainless steels for piping: tensile fracture resultsfor specimens precharged in hydrogen gasStainless steels tested in hydrogen gas vs prechargedshow different tensile fracture behaviorSystem for measuring fatigue crack growthin high-pressure H2 nearly completeWhat is metric for qualifying steels for H2 pipelines?Assess fatigue crack growth data by conductingfracture mechanics analysis of pipelineAssume steel, dimensions, and maximumpressure are similar to current H2 pipelSelect appropriate material property dataFatigue crack growth rates similar in basemetal, fusion zone, and HAZ for X60 steelCalculate number of pressure cycles to reachcritical crack depth for three casesNumber of pressure cycles vs crack depthrelationships: H2 compared to inert gasNumber of pressure cycles vs crack depthrelationships in H2 for varying dimensionsASME applies safety factors on critical crack depthand number of cycles to critical crack depthLifetime of steel hydrogen pipeline depends onboth material properties and structural designFatigue crack growth rates depend onload cycle profileFatigue crack growth rates depend onload cycle profile

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