resistance vs. load reliability analysisresistance vs. load reliability analysis 2. assume r and l...

28
Resistance vs. Load Reliability Analysis Let L be the load acting on a system (e.g. footing) and let R be the resistance (e.g. soil) Then we are interested in controlling R such that the probability that R > L (i.e. the reliability) is acceptably high or, equivalently, that R < L (i.e. the failure probability) is acceptably low, where [ ] P (,) RL rl R L f r l drdl −∞ < < = ∫∫ and where is the joint (bivariate) distribution of R and L. (,) RL f rl [ ] (,) P RL f r l dr dl r R r dr l L l dl = < + < +

Upload: others

Post on 19-Jan-2021

4 views

Category:

Documents


0 download

TRANSCRIPT

Page 1: Resistance vs. Load Reliability AnalysisResistance vs. Load Reliability Analysis 2. Assume R and L are either normally or lognormally distributed. The event {R < L} is the same as

Resistance vs. Load Reliability Analysis

Let L be the load acting on a system (e.g. footing) andlet R be the resistance (e.g. soil)

Then we are interested in controlling R such that the probabilitythat R > L (i.e. the reliability) is acceptably high or, equivalently,that R < L (i.e. the failure probability) is acceptably low, where

[ ]P ( , )RLr l

R L f r l drdl∞ ∞

−∞ <

< = ∫ ∫and where is the joint (bivariate) distribution of R and L.( , )RLf r l

[ ]( , ) PRLf r l dr dl r R r dr l L l dl= < ≤ + < ≤ +∩

Page 2: Resistance vs. Load Reliability AnalysisResistance vs. Load Reliability Analysis 2. Assume R and L are either normally or lognormally distributed. The event {R < L} is the same as

Bivariate Distributions

[ ]2 2

1 1

1 2 1 2P ( , )l r

RLl r

l L l r R r f r l drdl< ≤ < ≤ = ∫ ∫∩

Page 3: Resistance vs. Load Reliability AnalysisResistance vs. Load Reliability Analysis 2. Assume R and L are either normally or lognormally distributed. The event {R < L} is the same as

Resistance vs. Load Reliability Analysis

The estimation of typically requires vast amountsof data, which is generally impractical.

Simplifications:1. assume R and L are independent so that

and

( , )RLf r l

( , ) ( ) ( )RL R Lf r l f r f l=

[ ]P ( ) ( ) ( ) ( )R L L Rr l r l

R L f r f l drdl f l f r drdl∞ ∞ ∞ ∞

−∞ < −∞ <

< = =∫ ∫ ∫ ∫

Page 4: Resistance vs. Load Reliability AnalysisResistance vs. Load Reliability Analysis 2. Assume R and L are either normally or lognormally distributed. The event {R < L} is the same as

Resistance vs. Load Reliability Analysis

2. Assume R and L are either normally or lognormallydistributed.The event {R < L} is the same as the events

i) {R – L < 0}ii) {R/L < 1}

If both R and L are normally distributed, thenX R L= −

is also normally distributed with parameters

(assuming R and L are independent).

2 2 2X R L

X R L

μ μ μ

σ σ σ

= −

= +

Page 5: Resistance vs. Load Reliability AnalysisResistance vs. Load Reliability Analysis 2. Assume R and L are either normally or lognormally distributed. The event {R < L} is the same as

Reliability Index

• the reliability index, β, is the number of standard deviations the mean is from failure.

• superior to the Factor-of-Safety approach because it depends on both the mean and the standard deviation.

• failure occurs if X < 0 (normal) or ln X < 0 (lognormal).Defining

ln

ln

, (normal)

, (lognormal)

X

X

X

X

μβσμβσ

=

=

[ ] [ ] ( )

[ ] [ ] ( )ln

ln

P failure P 0 , (normal)

P failure P ln 0 , (lognormal)

X

X

X

X

X

X

μ βσ

μ βσ

⎛ ⎞= < = Φ − = Φ −⎜ ⎟

⎝ ⎠⎛ ⎞

= < = Φ − = Φ −⎜ ⎟⎝ ⎠

Page 6: Resistance vs. Load Reliability AnalysisResistance vs. Load Reliability Analysis 2. Assume R and L are either normally or lognormally distributed. The event {R < L} is the same as

Resistance vs. Load Reliability Analysis

• Suppose load is normally distributed with mean 10 and standard deviation 3

• Suppose resistance is normally distributed with mean 20 and standard deviation 4.

• Then X = R – L has mean and variance

• Mean FS = μR /μL = 20/10 = 2• Reliability index = β = μX /σX = 10/5 = 2• Probability of failure =

2 2 2 2 2

20 10 10

4 3 25X R L

X R L

μ μ μ

σ σ σ

= − = − =

= + = + =

[ ] [ ] 0 10P P 05

( 2) 0.023

R L X −⎛ ⎞< = < = Φ⎜ ⎟⎝ ⎠

= Φ − =

Page 7: Resistance vs. Load Reliability AnalysisResistance vs. Load Reliability Analysis 2. Assume R and L are either normally or lognormally distributed. The event {R < L} is the same as

Resistance vs. Load Reliability Analysis

Now [ ] [ ] [ ]P P 0 = P 0 X

X

R L R L X μσ

⎛ ⎞< = − < < = Φ −⎜ ⎟

⎝ ⎠where is the standard normal cumulative distributionfunction.

( )xΦ

Page 8: Resistance vs. Load Reliability AnalysisResistance vs. Load Reliability Analysis 2. Assume R and L are either normally or lognormally distributed. The event {R < L} is the same as

Resistance vs. Load Reliability Analysis

Alternatively, if R and L are lognormally distributed, thenRXL

=

is also lognormally distributed with parameters

ln ln ln2 2 2ln ln ln

X R L

X R L

μ μ μ

σ σ σ

= −

= + (assuming independence)

so that [ ] [ ] [ ] [ ]ln

ln

P P / 1 P 1 P ln 0

X

X

R L R L X X

μσ

< = < = < = <

⎛ ⎞= Φ −⎜ ⎟

⎝ ⎠

Page 9: Resistance vs. Load Reliability AnalysisResistance vs. Load Reliability Analysis 2. Assume R and L are either normally or lognormally distributed. The event {R < L} is the same as

Resistance vs. Load Reliability Analysis

• Suppose load is lognormally distributed with mean 10 and standard deviation 3

• Suppose resistance is lognormally distributed with mean 20 and standard deviation 4.

• Then X = R/L is lognormally distributed

20, 4R Rμ σ= = →( )

22ln 2

2ln ln

ln 1 0.0392

ln 0.5 2.976

RR

R

R R R

σσμ

μ μ σ

⎛ ⎞= + =⎜ ⎟

⎝ ⎠= − =

10, 3L Lμ σ= = →( )

22ln 2

2ln ln

ln 1 0.0862

ln 0.5 2.259

LL

L

L L L

σσμ

μ μ σ

⎛ ⎞= + =⎜ ⎟

⎝ ⎠= − =

Page 10: Resistance vs. Load Reliability AnalysisResistance vs. Load Reliability Analysis 2. Assume R and L are either normally or lognormally distributed. The event {R < L} is the same as

Resistance vs. Load Reliability Analysis/ ln ln lnX R L X R L= → = −

ln ln ln2 2 2ln ln ln ln

0.717

0.125 0.354X R L

X R L X

μ μ μ

σ σ σ σ

= − =

= + = → =

[ ]ln

ln

0.717 2.02 P / 1 ( 2.02) 0.0220.354

X

X

R Lμβσ

= = = → < = Φ − =

Page 11: Resistance vs. Load Reliability AnalysisResistance vs. Load Reliability Analysis 2. Assume R and L are either normally or lognormally distributed. The event {R < L} is the same as

Reliability Index

Page 12: Resistance vs. Load Reliability AnalysisResistance vs. Load Reliability Analysis 2. Assume R and L are either normally or lognormally distributed. The event {R < L} is the same as

Reliability Index

More generally, system failure can be defined in terms ofa failure or limit state function. Also called the safety margin

1 2( , , )M g Z Z= …

Failure occurs when M = g(Z1, Z2, …) < 0. In this case, thereliability index is defined as

M

M

μβσ

=

Problem: different choices of the function M lead to differentreliability indices (e.g. M = R – L or M = ln(R/L) both implyfailure when M < 0, but lead to different values of β in firstorder approximations).

Page 13: Resistance vs. Load Reliability AnalysisResistance vs. Load Reliability Analysis 2. Assume R and L are either normally or lognormally distributed. The event {R < L} is the same as

Reliability IndexExample 1: suppose that M = R – Land R and L are normally distributed. Then

2 2 (assuming independence)M R L

M R L

μ μ μ

σ σ σ

= −

= +and

so that2 2

R L

R L

μ μβσ σ

−=

+

and [ ] [ ] ( )P failure P 0M β= < = Φ −

This is exact, so long as R and L are normally distributedand independent (if not independent then must involvecovariances in computation of σM).

Page 14: Resistance vs. Load Reliability AnalysisResistance vs. Load Reliability Analysis 2. Assume R and L are either normally or lognormally distributed. The event {R < L} is the same as

Reliability IndexExample 2: suppose that M = ln( R / L ) = lnR – lnLand R and L are lognormally distributed. Then

ln ln

2 2ln ln (assuming independence)

M R L

M R L

μ μ μ

σ σ σ

= −

= +and

so that ln ln2 2ln ln

R L

R L

μ μβσ σ

−=

+

and [ ] [ ] ( )P failure P 0M β= < = Φ −

This is exact, so long as R and L are lognormally distributedand independent (if not independent then must involvecovariances in computation of σM).

Page 15: Resistance vs. Load Reliability AnalysisResistance vs. Load Reliability Analysis 2. Assume R and L are either normally or lognormally distributed. The event {R < L} is the same as

Reliability IndexExample 3: suppose that M = ln( R / L ) = lnR – lnLand R and L are normally distributed. Then the distributionof M is complex and we must approximate its moments;

2 22 2ln ln

2 22 2

2 2

ln ln (to first order)

=

R L

M R L

M R L

R LR L

R L

M MR L

V V

μ μ

μ μ μ

σ σ σ

σ σμ μ

∂ ∂⎛ ⎞ ⎛ ⎞+⎜ ⎟ ⎜ ⎟∂ ∂⎝ ⎠ ⎝ ⎠

+ = +

2 2R L

R L

μ μβσ σ

−=

+now

2 2

ln lnR L

R LV Vμ μβ −

=+

It was

These are clearly different.

in Example 1

Page 16: Resistance vs. Load Reliability AnalysisResistance vs. Load Reliability Analysis 2. Assume R and L are either normally or lognormally distributed. The event {R < L} is the same as

Hasover-Lind Reliability Index

Hasover and Lind (1974) solved this ambiguity by mappingthe set of system variables, Z, onto a set of standardized (meanzero, unit variance) and uncorrelated variables, X

[ ]( )E= −X A Z Z

where the transformation matrix A is the solution ofT =ZAC A I

where CZ is the matrix of covariances between the systemvariables, Z, and I is the identity matrix. In terms of Z,

[ ]( ) [ ]( )1min E EZ

T

Lβ −

∈= − −Zz

z Z C z Z

where LZ is the failure surface. The value of z which minimizesthis is called the design point, z*.

Page 17: Resistance vs. Load Reliability AnalysisResistance vs. Load Reliability Analysis 2. Assume R and L are either normally or lognormally distributed. The event {R < L} is the same as

Hasover-Lind Reliability Index

Hasover-Lind’s reliability index is the minimum distance fromthe mean to the failure surface in standardized space(figure from Madsen, Krenk, and Lind, 1986)

Page 18: Resistance vs. Load Reliability AnalysisResistance vs. Load Reliability Analysis 2. Assume R and L are either normally or lognormally distributed. The event {R < L} is the same as

Going Beyond Calibration• Must move beyond calibration for real benefits of LRFD• Simple probability-based methods take load and

resistance distributions into account- nominal or characteristic resistance: Rn = kRμR- nominal or characteristic load: Ln = kLμL

• Design: ϕ Rn = γ Ln

P[failure] P[ ] P[ / 1]R L R L= < = <

Page 19: Resistance vs. Load Reliability AnalysisResistance vs. Load Reliability Analysis 2. Assume R and L are either normally or lognormally distributed. The event {R < L} is the same as

• let M = ln(R/L)• then P[failure] P[ 0]M= <

• β is the reliability index• typically β ranges from 2.0 to 3.0

Going Beyond Calibration

Page 20: Resistance vs. Load Reliability AnalysisResistance vs. Load Reliability Analysis 2. Assume R and L are either normally or lognormally distributed. The event {R < L} is the same as

We want to produce a design such that the mean and standard deviation ofresistance satisfies

[ ]P 1 P ln ln 0 ( )R R LL

β⎡ ⎤< = − < = Φ −⎢ ⎥⎣ ⎦

In detailln ln

2 2ln ln

0 E[ln ln ]P[ln ln 0] P ( )SD[ln ln ]

R L

R L

R LR L ZR L

μ μ βσ σ

⎛ ⎞⎡ ⎤ −− − ⎜ ⎟− < = < = Φ − = Φ −⎢ ⎥ ⎜ ⎟−⎣ ⎦ +⎝ ⎠so that2ln ln

ln ln ln ln2 2ln ln

R LR L R L

R L

μ μ β μ μ β σ σσ σ

−= ⇒ = + +

+ln ln ln0.75 ( )L R Lμ β σ σ+ +

Now, since 2ln lnln( ) 0.5L L Lμ μ σ= − and ( )2

ln lnexp 0.5R Rμ μ σ= + Rwe get

To determine both load and resistance factors:

{ } { }2 2ln ln ln lnexp 0.5 0.75 exp 0.5 0.75R L R R L Rμ μ σ βσ σ βσ⎡ ⎤= + − +⎣ ⎦

or

{ } { }2 2ln ln ln lnexp 0.5 0.75 exp 0.5 0.75R R R L R Lσ βσ μ σ βσ μ+ = − +

Page 21: Resistance vs. Load Reliability AnalysisResistance vs. Load Reliability Analysis 2. Assume R and L are either normally or lognormally distributed. The event {R < L} is the same as

Writing this in terms of the nominal load and resistance ( 1) ( 1)

n R R R

n L L L

R k kL k k

μμ

= <

= >

gives us{ } { }2 2

ln ln ln lnexp 0.5 0.75 exp 0.5 0.75R R L Ln n

R L

R Lk k

σ βσ σ βσ⎡ ⎤ ⎡ ⎤− − − +⎢ ⎥ ⎢ ⎥=⎢ ⎥ ⎢ ⎥⎣ ⎦ ⎣ ⎦

Recalling that our LRFD has the form n nR Lϕ γ= implies

Resistance factor:{ }

{ }

2ln ln

2ln ln

exp 0.5 0.75

exp 0.5 0.75

R R

R

L L

L

k

k

σ βσϕ

σ βσγ

− −=

− +=Load factor:

Page 22: Resistance vs. Load Reliability AnalysisResistance vs. Load Reliability Analysis 2. Assume R and L are either normally or lognormally distributed. The event {R < L} is the same as

If load factors are known (e.g. from structural codes) then the resistancefactor becomes dependent on both the resistance variability and theload variability. In this case, our LRFD can be written

i i

i

i n i ni i

n i ni n R R

L LR L

R k

γ γϕ γ ϕ

μ= ⇒ = =

∑ ∑∑

{ }2

2 2ln ln2

1exp

1

ii nLi

R LR L R

Q Vk V

γβ σ σ

μ

⎛ ⎞+⎜ ⎟= − +⎜ ⎟+⎝ ⎠

wherei i in L LL k μ=

i

i

i

nL L

i i L

Lk

μ μ= =∑ ∑2 2i iL LiL

LL L

VV

μσμ μ

= =∑ (assuming loads are independent)

Page 23: Resistance vs. Load Reliability AnalysisResistance vs. Load Reliability Analysis 2. Assume R and L are either normally or lognormally distributed. The event {R < L} is the same as

Going Beyond Calibration

• thus, for given target reliability index and variances, the resistance factor can be computed as

which depends on- coefficient of variation of load ( )- coefficient of variation of resistance ( )- load factors γι- characteristic coefficients,

LV

RV

and iR Lk k

{ }2

2 2ln ln2

1exp

1

ii nLi

R LR L R

L Vk V

γϕ β σ σ

μ

⎛ ⎞+⎜ ⎟= − +⎜ ⎟+⎝ ⎠

Page 24: Resistance vs. Load Reliability AnalysisResistance vs. Load Reliability Analysis 2. Assume R and L are either normally or lognormally distributed. The event {R < L} is the same as

Problems Implementing LRFD

• the coefficient of variation of resistance depends on;- variability in material properties- error in design models- measurement and correlation errors- construction variability

• with steel and concrete, the material property variability does not change significantly with location (quality controlled materials)

• with soils, the material property mean and variability change within a site and from site to site

Page 25: Resistance vs. Load Reliability AnalysisResistance vs. Load Reliability Analysis 2. Assume R and L are either normally or lognormally distributed. The event {R < L} is the same as

Problems Implementing LRFD

• there is a dependence between resistance and load which is generally absent (or small) in structural engineering, e.g. shear strength is dependent on stress;

tanf cτ σ φ= +

Page 26: Resistance vs. Load Reliability AnalysisResistance vs. Load Reliability Analysis 2. Assume R and L are either normally or lognormally distributed. The event {R < L} is the same as

Problems Implementing LRFD

• No common definition of “characteristic value”- often defined as a “cautious estimate of the

mean”, but sometimes as a low percentile- we badly need a standard definition (median?)

• VR changes with intensity of site investigation- resistance factor should approach 1.0 as the

site is more thoroughly investigated- this would lead to a complex table of resistance

factors (however, see, e.g., AS 5100, AS 2159,AS4678, Eurocode 7, NCHRP507)

Page 27: Resistance vs. Load Reliability AnalysisResistance vs. Load Reliability Analysis 2. Assume R and L are either normally or lognormally distributed. The event {R < L} is the same as

Future Directions

• probabilistic methods generally limited to “single random variable” models (e.g. R vs. L)

• to consider the effect of spatial variability, random field simulation combined with finite element analysis is necessary (RFEM)

• the random field simulation allows the representation of a soil’s spatial variability

• the finite element analysis allows the soil to fail along “weakest paths” (decreased model error)

Page 28: Resistance vs. Load Reliability AnalysisResistance vs. Load Reliability Analysis 2. Assume R and L are either normally or lognormally distributed. The event {R < L} is the same as

Conclusions

• geotechnical engineers led the way with Limit States concepts (1940’s) but have been slow to migrate to reliability-based design methods.

• the most advanced LRFD codes currently are AS 5100 and Eurocode 7.

• all current LRFD geotechnical codes have load and resistance factors calibrated from older WSD codes, with some adjustments based on engineering judgement and simple probability methods.