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Modeling Uncertainties in Power System by Generalized Lambda Distribution

  • Qing Xiao EMAIL logo
Published/Copyright: March 22, 2014

Abstract

This paper employs the generalized lambda distribution (GLD) to model random variables with various probability distributions in power system. In the context of the probability weighted moment (PWM), an optimization-free method is developed to assess the parameters of GLD. By equating the first four PWMs of GLD with those of the target random variable, a polynomial equation with one unknown is derived to solve for the parameters of GLD. When employing GLD to model correlated multivariate random variables, a method of accommodating the dependency is put forward. Finally, three examples are worked to demonstrate the proposed method.

Appendix A

The parameters ci (c=0,,11) are as follows:

(34)c11=(BC)(3B2BC2AC)(A3B+2C)c10=4A428A3B+12A3C+71A2B290A2BC+47A2C229AB3127AB2C213ABC2+91AC3132B4+311B3C212B2C2+41BC3c9=36A4312A3B+156A3C+921A2B21014A2BC+401A2C2864AB3+1,723AB2C1,974ABC2+831AC3627B4+1,979B3C1589B2C2+333BC3c8=56A4896A3B+612A3C+3634A2B24034A2BC+1,168A2C25,458AB3+9,254AB2C8,112ABC2+3,528AC3+108B4+3,828B3C4,888B2C2+1,200BC3c7=672A4+3,576A3B696A3C4,830A2B2+3,726A2BC3,968A2C27,305AB3+11,952AB2C2,757ABC2+2,958AC3+12,213B418,864B3C+4,535B2C2+132BC3c6=4,236A4+33,276A3B13,284A3C90,969A2B2+91,218A2BC43,565A2C2+65,883AB3101,553AB2C+121,815ABC240,977AC3+48,780B4142,041B3C+92,516B2C216,863BC3c5=10,524A4+100,800A3B44,988A3C337,455A2B2+350,990A2BC155,035A2C2+368,022AB3573,617AB2C+581,208ABC2217,705AC3+78,723B4424,845B3C+360,205B2C275,779BC3c4=13,456A4+151,744A3B70,764A3C606,848A2B2+651,402A2BC290,770A2C2+838,004AB31,341,124AB2C+1,341,342ABC2543,922AC3+30,012B4745,154B3C+776,776B2C2177,242BC3c3=(4)(2,98A429,616A3B+13,962A3C+138,963A2B2154,935A2BC+75,310A2C2234,204AB3+395,191AB2C429,195ABC2+193,482AC3+8,427B4+221,852B3C264,859B2C2+63,324BC3)c2=(16)(194A42,750A3B+1,266A3C+14,614A2B217,420A2BC+10,392A2C227,982AB3+53,159AB2C73,125ABC2+38,442AC32,772B4+50,271B3C58,209B2C2+13,920BC3)c1=(96)(4A458A3B+24A3C+320A2B2480A2BC+460A2C2479AB3+1,551AB2C3,862ABC2+2,460AC31,152B4+4,938B3C4,830B2C2+1,104BC3)c0=1,152(B2C)(BC3B2+2AC)(A6B+6C)

Appendix B

Below are the procedures of evaluating u for a given value of x of GLD:

  1. Determine the search interval u[a,b], set a=0, b=1. Give the precision δ.

  2. Denote u=(a+b)/2, if (ba)<δ, stop and output u=u, otherwise evaluate x: x=λ1+uλ3(1u)λ4λ2.

  3. If u=u, stop and output u=u, otherwise set a=a, b=u for x>x, set a=u, b=b for x<x, and go to Step 2.

Appendix C

Suppose x is a random variable with zero mean and unit variance, it can be represented by Cornish–Fisher expansion as follows:

(35)x=z+16(z21)κ3+124(z3+3z)κ4136(2z35z)κ32+1120(z46z2+3)κ5124(z45z2)κ2κ3+132412z453z2κ33

where z is a standard normal random variable with CDF Φ(z), κi denotes the ith cumulant of x (i=1,,5).

Rewrite the Cornish–Fisher expansion in the form of a fourth polynomial of z:

(36)x=b4z4+b3z3+b2z2+b1z+b0

where bi (i=0,,4) are:

(37)b4=1120κ5+127κ33124κ3κ4b3=124κ3118κ32b2=120κ5+16κ3+524κ3κ453324κ33b1=536κ3218κ4+1b0=140κ516κ3112κ3κ4+17324κ33

Then, for a random variable x with mean μ and standard deviation σ, it can be represented by:

(38)x=μ+σx=μ+σk=04bkzk=k=04akzk

where ak=σbk (k=1,2,3,4), a0=μ+σb0.

For a given percentage, the associated percentile xp can be calculated as follows:

(39)xp=k=04akzpkzp=Φ1(p)

where Φ1() is the inverse CDF of z.

Then, the PDF of x can be constructed with the aid of the PDF of z:

(40)f(xp)=φ(zp)k=14kakzpk1

where φ() is PDF of the standard normal variable.

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Published Online: 2014-3-22
Published in Print: 2014-6-1

©2014 by Walter de Gruyter Berlin / Boston

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