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MULTI-ELEMENT GENERALIZED POLYNOMIAL CHAOS FOR ...

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912 XIAOLIANG WAN AND GEORGE EM KARNIADAKIS<br />

π 1<br />

π 3<br />

π 1<br />

π 3<br />

4<br />

2<br />

0<br />

−2<br />

x 10−4<br />

6<br />

π 2<br />

0 0.5 1<br />

x 10 −3<br />

−4<br />

−6<br />

0 0.5 1<br />

x<br />

x 10 −3<br />

p=1<br />

−0.5<br />

p=2<br />

−1<br />

x<br />

x 10−11<br />

6<br />

x 10−14<br />

1.5<br />

4<br />

2<br />

0<br />

−2<br />

π 4<br />

1.5<br />

1<br />

0.5<br />

x 10−7<br />

2<br />

0 0.5 1<br />

x 10 −3<br />

−4<br />

−6<br />

0 0.5 1<br />

x<br />

x 10 −3<br />

−0.5<br />

p=3 p=4<br />

−1<br />

x<br />

Fig. 3.1. Orthogonal polynomials for random variable X, π1 to π4.<br />

1<br />

0.5<br />

0<br />

−0.5<br />

π 2<br />

p=1 p=2<br />

−1<br />

−1 −0.5 0 0.5 1<br />

−0.5<br />

−1 −0.5 0 0.5 1<br />

y<br />

y<br />

0.4<br />

0.2<br />

0<br />

−0.2<br />

−0.4<br />

p=3<br />

−0.6<br />

−1 −0.5 0<br />

y<br />

0.5 1<br />

π 4<br />

0<br />

1<br />

0.5<br />

0<br />

1<br />

0.5<br />

0<br />

0.2<br />

0.1<br />

0<br />

−0.1<br />

p=4<br />

−1 −0.5 0<br />

y<br />

0.5 1<br />

Fig. 3.2. Orthogonal polynomials for random variable Y , π1 to π4.<br />

3.1.2. Orthogonal polynomials for Beta distribution. From the ME-gPC<br />

scheme, we know that the orthogonal basis in each random element depends on a<br />

particular part of the PDF of the random inputs. We now demonstrate such a dependence<br />

using a Beta-type random variable X with α = 1 and β = 4. For simplicity, we<br />

consider only two random elements: [−1, 0] and [0, 1]. We define a random variable

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