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  • 8/12/2019 Chapter 4 Sp 2014 Economic Uncertainties Part 2

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    PE 3003/6413

    PE 3003/6413 Spring 2014

    Chapter 4

    Part 2

    Econom ic Uncertaint ies

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    Outline

    1. Range Analysis

    2. Probability

    3. Cumulative Probability and Density Functions

    4. Expected Value

    5. Decision Three Analysis6. Distribution Functions

    7. Monte Carlo Simulation

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    Distribution Functions

    Density functions are commonly used in engineering

    to describe physical systems

    Density distribution of a loading in a beam

    For any point x along the beam , the density c an bedescr ibed b y a funct ion (in grams /cm )

    The total loading between points a and b is

    determ ined as the integral of the density fu nc t ion

    f rom a to b

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    Distribution Functions

    Common Density Functions

    Uniform

    Triangular Distribution

    Normal Distribution

    Log-Normal Distribution

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    Uniform Distribution

    A continuous random variable X with p robabi li ty densi ty

    funct ion

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    Uniform Distribution

    Let the continuous random variable X denote the porosity

    measured in core samples. Assume that the range of X is [0,

    20 %], and assume that the probability density function of Xis

    f(X)=0.05, 0X20

    1. What is the probability that a measurement of porosity isbetween 5 and 10 %?

    2. What is the mean and variance of the core samples?

    E(X)= 10% and Var(X)=33.33 %

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    Uniform Distribution

    Random Number

    A set of numbers that have nothing to do with the other

    numbers in the sequence

    Random numbers have no defined sequence or formulation.

    Thus, for any n random numbers, each appears with equalprobability

    All computer languages and spread sheet has a random

    function that return a random number uniformly distributed

    between 0 and 1

    a b

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    Uniform Distribution

    VBA Random number initialization

    Const Seed As Double = 1000

    ' Random numbers Seed set

    Dim RndVal As Double

    Randomize (Seed)RndVal = Rnd(-Seed)

    ' After this command random numbers can be generated as

    follows

    RndVal = Rnd()

    We will use this in Monte Carlo section

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    Uniform Distribution

    Random number Generation between aand b

    VBA

    Function RandAB(a As Double, b As Double) As Double

    RandAB = (b - a) * Rnd() + a

    End Function

    Excel

    =rand()*(b-a)+a

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    Uniform Distribution

    Strengths

    Easy to create

    Easy to understand

    Simple implementation and calculation

    Weakness Almost always inappropriate, except as random number

    generation

    Use cautiously with low iterations (Monte Carlo)

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    Triangular Distribution

    a bc

    f(x)

    x

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    Triangular Distribution

    Cumulative Distribution

    bx

    bxccbab

    xb

    bxaacab

    ax

    xax

    PxF

    1

    1

    0

    )(

    2

    2

    1. a is the minimum outcome of the random

    variable.

    2. cis the mode (most likely) of the random

    variable.3. bis the maximum outcome of the random

    variable.

    4. F(x) is the cumulative probability of all

    possible outcomes of the random variable

    between aandx.

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    Triangular Distribution

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    Triangular Distribution

    Random numbers generation

    generate a random number (P) uniformly distributed between

    0 to 1 (refer to uniform distribution random numbers)

    random number is calculated using the inverse of the

    triangular distribution as follows:

    See VBA template on WebCT

    1

    11

    0

    0

    Pb

    Pab

    accbabPb

    ab

    acP

    aacabP

    Pa

    x

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    Triangular Distribution

    Strengths

    Easy to create

    Easy to understand

    Simple implementation

    Weakness Likeliestoften confuse with mean or P50 and very difficult to

    defend

    End points are sometimes difficult to estimate

    Poor approximation of Log-Normal

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    Normal Distribution

    The most widely used model for the distribution of a

    random variable

    Whenever a random experiment is replicated, the random variable

    that equals the average (or total) result over the replicates tends

    to have a normal distribution as the number of replicates becomes

    large.

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    Normal Distribution

    Probability density function

    Mean and Variance

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    Normal Distribution

    Let the continuous random variable X denote the porosity

    measured in core samples. Assume that X is normally

    distributed with 10% mean and 4% variance

    1. What is the probability that a measurement of porosity

    exceeds 13%?

    Excel => =1-NORM.DIST(13,10,SQRT(4),TRUE) = 0.06681

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    Normal Distribution

    Probabilities associated with a normal distribution

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    Normal Distribution

    Random numbers generation

    generate a random number (P) uniformly distributed between

    0 to 1 (refer to uniform distribution random numbers)

    random number is calculated using the inverse of the normal

    distribution as follows:

    Excel

    =NORM.INV(RAND(), Mean,Sigma) where p=rand()

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    Normal Distribution

    Strengths

    Easy to create

    Easy to understand

    Simple implementation

    Weakness Not really true nature at the ends

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    Log-Normal Distribution

    Variables in a system sometimes follow an exponential

    relationship as x=exp(w)

    If the exponent is a random variable, say W, X=exp(W)is a random

    variable

    An important special case occurs when W has a normal

    distribution. In that case, the distribution of X is called alognormal distribution.

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    Log-Normal Distribution

    Probability density function

    Mean and Variance

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    Log-Normal Distribution

    Random numbers generation

    generate a random number (P) uniformly distributed between

    0 to 1 (refer to uniform distribution random numbers)

    random number is calculated using the inverse of the normal

    distribution as follows:

    Excel

    =LOGNORM.INV(rand(),,)

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    Log-Normal Distribution

    Strengths

    Easy to create

    Easy to understand

    Logical starting points for many inputs

    Extremely common in nature Weakness

    Not really true nature at the ends

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    Binomial Distribution

    Bernoulli Trial or Experiment:

    Flip a coin 10 times. Let X=number of heads obtained.

    A worn machine tool produces 1% defective parts. Let X

    =number of defective parts in the next 25 parts

    produced.

    The random variable in each case is a count of the

    number of trials that meet a specified criterion

    Assumed that the trials that constitute the random

    experiment are independent

    probability of a success in each trial is constant

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    Binomial Distribution

    A random experiment consists of n Bernoulli trialssuch that

    1. The trials are independent

    2. Each trial results in only two possible outcomes,

    labeled as success and failure3. The probability of a success in each trial, denoted as p,

    remains constant

    The random variable Xthat equals the number of

    success has a binomial random variable with

    parameters n(number of trials or experiments) andsuccess probability p

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    Binomial Distribution

    We are drilling 5 wildcats in a new basin where thechance of a discovery (wildcat success ratio) is 0.15

    on each well. Assuming each well is a Bernoulli trial,

    what is the probability of only one discovery in the

    fives wells drilled?

    n=5

    p=0.15

    S=1

    P(S=1)=0.3915

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    Outline

    1. Range Analysis

    2. Probability

    3. Cumulative Probability and Density Functions

    4. Expected Value

    5. Decision Three Analysis

    6. Distribution Functions

    7. Monte Carlo Simulation

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    Gas Metering Problem

    wq Oq

    Gq GP GT

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    Gas Metering Problem

    The gas flow rate is measured a certain pressure andtemperature

    Gas flow rate need to be reported at standard

    conditions (Deterministic Model)

    )67.459(0283.0)(

    G

    GGSCG

    Tz

    Pqq

    qG(SC): gas flow rate at standard conditions [MSCF/D]qG: gas flow rate at in-situ conditions [MCF/D]

    PG: gas pressure [psia]

    TG: gas temperature [F]

    z: gas compressibility factor [-]. For simplicity z=0.9

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    Gas Metering Problem

    For a given time

    ][19.203

    )67.459120(9.00283.0

    30010)( MSCF/D

    SCGq

    qG: 10 [MCF/D]

    PG: 300 [psia]

    TG: 120 [F]z: 0.9 (for simplicity)

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    Gas Metering Problem

    Unfortunately qG, PGand TGhas associateduncertainties

    0

    0.1

    0.2

    0.3

    0.4

    0.5

    0 10 20

    f(qG

    )

    qG[MCFD/D]

    0

    0.02

    0.04

    0.06

    0.080.1

    0.12

    0.14

    280 300 320

    f(PG

    )

    PG[psia]

    0

    0.05

    0.1

    0.150.2

    0.25

    100 120 140

    f(TG

    )

    TG[F]

    qGis normally distributed

    with mean of 10MCFD

    and 1 MCFD of standard

    deviation

    PGis normally

    distributed with mean of

    300 psia and 3 psia of

    standard deviation

    TGis normally

    distributed with

    mean of 120 F and

    2 F of standard

    deviation

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    Gas Metering Problem

    Uncertainties need to be propagated to get theuncertainty in qG,

    )67.459(0283.0)(

    G

    GGSCG

    Tz

    Pqq

    0

    0.1

    0.2

    0.3

    0.4

    0.5

    0 10 20

    f(qG

    )

    qG[MCFD/D]

    0

    0.02

    0.04

    0.06

    0.08

    0.1

    0.12

    0.14

    280 300 320

    f(PG

    )

    PG[psia]

    0

    0.05

    0.1

    0.15

    0.2

    0.25

    100 120 140

    f(TG

    )

    TG[F]

    0

    0.1

    0.2

    0.3

    0.4

    0.5

    0 10 20

    f(qG

    )

    qG[MCFD/D]

    Monte Carlo is used to

    propagates this uncertainties

    Though the Deterministic

    Model

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    Gas Metering Problem

    Assume qG, PGand TGare not correlated

    Assume

    qGis no rmal ly dis tr ibuted w ith mean of 10MCFD and 1

    MCFD of s tandard deviat ion

    PGis normally dis tr ibuted with mean of 300 psia and 3 psia

    of standard deviat ion

    TGis norm all y d is tr ib u ted w ith mean of 120 F and 2 F o f

    standard deviat ion

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    Gas Metering Problem

    Follow the steps below:

    1. Calculate the average qG(SC) using the average values for qG,PGand TG

    2. Generate a random number following qGdistribution

    3. Generate a random number following PGdistribution4. Generate a random number following TGdistribution

    5. Calculate qG(SC)using the deterministic model

    6. Repeat from steps 2 to 5 until maximum number of iterations is

    reached or the average value of all calculated qG(SC)is close

    enough to the qG(SC)

    calculated in step 1

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    Gas Metering Problem

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    Gas Metering Problem

    192

    194

    196

    198

    200

    202

    204

    0 200 400 600 800 1000 1200

    Average

    Iterations

    Convergence Plot

    Simulation Deterministic Model

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    Gas Metering Problem

    Histogram

    Min 141.0443

    Max 271.6897

    N of classes 10

    Step 13.06453288

    Left Right Interval Freq Freq [frac]

    141.04 154.10 [141.04-154.1] 6 0.006006006

    154.10 167.16 (154.1-167.16) 22 0.022022022

    167.16 180.22 (167.16-180.22) 102 0.102102102

    180.22 193.28 (180.22-193.28) 185 0.185185185

    193.28 206.34 (193.28-206.34) 269 0.269269269206.34 219.40 (206.34-219.4) 222 0.222222222

    219.40 232.46 (219.4-232.46) 128 0.128128128

    232.46 245.52 (232.46-245.52) 52 0.052052052

    245.52 258.58 (245.52-258.58) 11 0.011011011

    258.58 271.64 (258.58-271.64) 2 0.002002002

    Total 999 1

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    Gas Metering Problem

    Histogram

    0

    0.05

    0.1

    0.15

    0.2

    0.25

    0.3

    Histogram

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    Gas Metering Problem

    Average and Standard Deviation and Normal

    Approximation

    Average 203.28

    St Deviation 20.38

    Pessimistic Mean Optimistic162.53 203.28 244.03

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    0.00%

    10.00%

    20.00%

    30.00%

    40.00%

    50.00%

    60.00%

    70.00%

    80.00%

    90.00%

    100.00%

    140 160 180 200 220 240 260

    F(qG(SC)

    qG(SC) [MSCFD]

    Gas Metering Problem

    Cumulative Freq DistributionPercentile qG(SC)

    2.50% 161.89

    5.00% 169.61

    10.00% 176.58

    15.00% 182.73

    20.00% 187.41

    25.00% 190.97

    30.00% 193.8035.00% 196.52

    40.00% 200.47

    45.00% 202.97

    50.00% 205.85

    55.00% 208.28

    60.00% 210.93

    65.00% 213.48

    70.00% 216.58

    75.00% 219.57

    80.00% 223.08

    85.00% 227.71

    90.00% 232.09

    95.00% 239.09

    97.50% 247.22

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    Monte Carlo Process

    1. Define all the variables

    Identify all the measure variables of interest (i.e. NPV, oil price,

    etc.) or all variables that affect the evaluation

    2. Define the variables relationships in the deterministic

    projection model Equations or other numerical calculations

    3. Sort the input variables into two groups

    Variables that we known with certain (represented by single

    point value)

    Significant unknowns will be represent by random variables(exact value can not be specified)

    4. Define random variable distributions

    Usually, the best available expert is assigned to judge each

    random variable

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    Monte Carlo Process

    5. Perform the respective simulation trials1. Calculate the deterministic average using the average values all

    random variables into the deterministic equation

    2. Generate a random number following the distribution of each

    random variable

    3. Calculate the outcome using the deterministic model4. Repeat from steps 2 to 5 until maximum number of iterations is

    reached or the average value of all calculated values in step 3 is

    close enough to the calculated in step 1

    6. Calculate

    Plot the histogram Expected and standard deviation value of the outcomes

    Plot the cumulative frequency distribution

    P90

    P50

    P10

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    P90, P50 and P10

    Other disciplines

    Mao-Jones, J. (2012). Decision & Risk Analysis. Merrick & Company Technical Paper.

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    P90, P50 and P10

    Other disciplines

    Holm, S. Suleymanov, V. Vanvik, N.

    (2011). Shtokman flow assurance

    challenges a

    Systematic approach to analyzeuncertaintiesPart 2.15thMultiphase

    Production Technology Conference,

    Canes (2012)

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    P90, P50 and P10

    Other disciplines

    Holm, S. Suleymanov, V. Vanvik, N.

    (2011). Shtokman flow assurance

    challenges a

    Systematic approach to analyzeuncertaintiesPart 2.15thMultiphase

    Production Technology Conference,

    Canes (2012)

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    P90, P50 and P10

    Other disciplines

    P10, P50 and P90 are defined as the percentile of the

    outcome

    This classical definition will apply if you are dealingwith

    1. Facility engineers or any other engineer who is

    designing an equipment

    2. Flow assurance engineers

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    P90, P50 and P10

    Petroleum Resources Management System (PRMS)

    (Society of Petroleum Engineers 2007)

    f

    Reserves [MMBBL or BSCF]

    1P

    10

    th

    2P

    50th

    3P

    90th

    Proved Provable Possible

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    P90, P50 and P10

    Petroleum Resources Management System (PRMS)

    (Society of Petroleum Engineers 2007)

    Low Est imate:

    Conservative estimate of the quantity that will

    actually be recovered from the accumulation bya project

    There should be at least 90% probability (P90)

    that the quantities actually recovered will equal

    or exceed the low estimate

    This is the definition that will be used in this

    course owing to we are working directely with

    the reserves

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    P90, P50 and P10

    Reserves [MMBBL or BSCF]1P

    10th

    Should be at least a 90%

    probability that the quantities

    actually recovered will equal or

    exceed the estimate

    P90

    Low Estimate

    This is the definition that will be used in this course

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    P90, P50 and P10

    Reserves [MMBBL or BSCF]

    2P

    P50

    there should be at least a 50%

    probability that the actual

    quantities recovered will equal or

    exceed the 2P estimate

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    P90, P50 and P10

    Petroleum Resources Management System (PRMS)

    (Society of Petroleum Engineers 2007)

    High Estimate:

    Optimistic estimate of the quantity that will

    actually be recovered from an accumulation by aproject

    There should be at least a 10% probability (P10)

    that the quantities actually recovered will equal

    or exceed the high estimate

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    P90, P50 and P10

    Reserves [MMBBL or BSCF]3P

    90th

    there should be at least

    a 10% probability that

    the actual quantities

    recovered will equal

    or exceed the 3P

    estimate.

    P10This is the definition that will be used in this course

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    P90 P50

    P90, P50 and P10

    Summary: we will use P10= 10% sure that the value (i.e. Reserve or NPV) is

    higher than P10

    P90= 90% sure that the value (i.e. Reserve or NPV) is

    higher than P90

    P10

    NPV[MM$]

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    Example 1

    The production of a new well can be predicted using decline curve analysisand historical data from nearby reservoirs. The hyperbolic decline curve is

    given by:

    bi iDibqq1

    0 1

    Where

    q= Oil flow rate [BPD]

    q0= Initial oil flow rate (time zero) [BPD]Di= Initial Nominal Decline [Fraction / year]

    b= Hyperbolic Exponent factor (some authors use the term n)

    i = integervalue of the time [year].

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    Example 1

    The net revenue of the well in a particular yearican be estimated by:

    DTOATvenueReNet iii 1)(

    1. A(i) is the gross revenue in year igiven by

    Wc

    WcWaterCosticePrGasGORicePrOildaysqA ii

    1365

    Wcis the water cut

    2. O(i)is the operational cost in yearI

    3. D= is the depreciation in year i.

    4

    CapexD

    where Capexis the initial investment and 4 years is the taxable life of the

    well; Tis the income tax rate

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    Example 1

    Finally, the net present value of this well can be calculated as follows:

    Capex

    MROR

    venueReNetesentValuePrNet

    ii

    i

    1

    )(

    1

    where MRORis the minimum rate of return. The well will be closed when the Net

    Revenue becomes negative (NetRevenue(i) < 0). Thus the life of the well corresponds

    to the year before the net revenue becomes less than zero. In other words the

    summation will be carried out until Net Revenue becomes negative

    Using this mathematical formulation, We created a user define function in excel that

    can return the NPV for a well (Deterministic Model)

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    Example 1

    Lets consider the following random variables:1. Initial flow rate q0is normally distributed with mean =500

    and standard deviation of 30 BPD

    2. Oil price is uniform distributed between 85 and 120 $/BPD

    3. Gas price in uniform distributed between 2 and 6 $/Mscf

    The certain variables are:

    GOR 0.3 [Mscf/BBL]

    WaterCost 0.13 [$/BBL]

    Wc 0.5

    O(i) 301,000.00 [$]T 0.29

    MROR 0.13

    Di 0.7 [1/year]

    b 1.5

    Capex 2,000,000 [$]

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    Example 1

    Run a Monte Carlo simulation assuming that the random variablesare independent and not correlated

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    Example 2

    The recoverable oil using the volumetric approach in a givenprospect is given

    rf

    Bo

    ShA,Nr W

    17587

    whereAis the drainage area [acres], his the net pay [ft], is porosity [-], Swis

    the water saturation [-],Bois the formation volume factor [bbl/stb] and rf

    is the recovery factor [-]. Nris in stb

    Example 2 template contains a user define function that calculatesNrand

    can be used to setup a Monte Carlo Simulation.

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    Example 2

    Consider the following random variables1. is porosity [-] is normally distributed with mean 0.14 and

    standard deviation of 0.02

    2. Swis the water saturation [-]. Uniform distributed between 0.2

    and 0.4.

    3. his the net pay [ft]. Normally distributed mean 15 and standarddeviation of 1.5 feet's

    4. Ais the drainage area [acres]. Lognormal distributed with =4.35 and

    =0.246 (mean 80 and std of 20 Acres)

    5. rf is the recovery factor [-]. Normally distributed with mean of

    0.34 and standard deviation of 0.05.6. Bois the formation volume. Uniform distributed between 1.15

    and 1.25