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<strong>atw</strong> Vol. 62 (<strong>2017</strong>) | Issue 6 ı June<br />

RESEARCH AND INNOVATION 410<br />

| | Fig. 2.<br />

Nodalization for the primary system of AP1000.<br />

compared with the results of<br />

LOFTRAN, such as pressure, flow rate<br />

etc. The comparison results show that<br />

RELAP5 has the capability to predict<br />

the system parameters [11] correctly.<br />

Among above these parameters, the<br />

reactor coolant temperature is the<br />

most important parameter for the<br />

PRHRS loop, as shown in Figure 3.<br />

As depicted in Fig. 3, the results of<br />

RELAP5 and LOFTRAN exhibit the<br />

same trend. A similar value of maximum<br />

temperature has been observed<br />

in the two results. During the accident,<br />

however, a difference in the sequence<br />

of events and response of the reactor<br />

control system can lead to a slight<br />

difference in the temperature trend.<br />

This has no significant influence on<br />

the analysis.<br />

3 Calculation methods<br />

3.1 Latin hypercube sampling<br />

Latin Hypercube Sampling (LHS) [16,<br />

17] is an improvement over the traditional<br />

Monte Carlo sampling method.<br />

It can overcome its drawbacks, in that<br />

most of sampled results lie near the<br />

average value. In order to improve the<br />

accuracy of the parameters, therefore,<br />

the method covers the upper and<br />

lower limits of the distributions.<br />

Hence, this method has the ability to<br />

determine any value, as long as the<br />

parameters are known. The steps are<br />

as follows.<br />

(1) For each variable, the probability<br />

distribution is divided into N nonoverlapping<br />

equal probability<br />

interval [0, 1/N], [1/N, 2/N],…,<br />

[(N-1)/N, 1]. This ensures that<br />

the degree of the correlation of<br />

LHS is small.<br />

(2) The random standard normal<br />

sample matrix Z N×n is used to<br />

represent the order of sample<br />

points, and the integer matrix<br />

R N×n is used to record information<br />

regarding the ordering of the<br />

above sample points. Hence,<br />

R ij = k shows that the sequence<br />

of the j th variable in the i th sampling<br />

is k.<br />

(3) According to in each interval, the<br />

cumulative probability function<br />

of each sample point in the Latin<br />

hypercube can be obtained randomly,<br />

as shown in Eq. (1).<br />

(1)<br />

Here, i = 1,..., N and j = 1,..., n.<br />

The function r a n d (0,1) represents<br />

a random number, which is<br />

uniformly distributed in the [0,1]<br />

interval.<br />

(4) In the Latin hypercube, the sampling<br />

points are obtained by the<br />

method of equal probability<br />

change, as shown in Eq. (2).<br />

(2)<br />

Here, φ –1 (.) is the inverse normal<br />

distribution function.<br />

3.2 Grey Relation Method<br />

The Grey Relational Method [8] is a<br />

quantitative technique for comparative<br />

analysis. The basic idea is to determine<br />

the exponent of each factor in<br />

the correlation, according to their<br />

degree of similarity with the geometry<br />

of sequence curve. If the curve is close<br />

for a particular factor, it would have a<br />

high exponent in the correlation. X 0 is<br />

defined as the target parameter, with<br />

k referring to the sequence of the<br />

parameter, denoted as {X 0 (k)}. It is<br />

assumed that there are a total of m<br />

control parameters, and a parameter j<br />

in the same sequence k is called the<br />

comparison sequence, denoted as<br />

{X j (k)} (k = 1,…, N)(j = 1,…, m). In<br />

this correlation, the exponent of each<br />

factor can be obtained by comparing<br />

the tendency of development between<br />

the target and influence parameters.<br />

These steps are shown as follows [18].<br />

(1) The reference and comparison sequences<br />

are normalized, as shown<br />

in Eq. (3).<br />

(3)<br />

(2) The absolute value of difference<br />

between the reference and the<br />

comparison sequences is calculated<br />

as Eq. (4) based on above normalization<br />

results.<br />

(4)<br />

a) Results of RELAP5. b) Results of LOFTRAN.<br />

| | Fig. 3.<br />

Reactor coolant temperature.<br />

(3) Maximum and minimum absolute<br />

values are calculated shown as<br />

Eq. (5)-(6).<br />

(5)<br />

(6)<br />

Research and Innovation<br />

Reliability Analysis on Passive Residual Heat Removal of AP1000 Based on Grey Model ı Qi Shi, Zhou Tao, Muhammad Ali Shahzad, Li Yu and Jiang Guangming

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