Recirculation Line — 28 inch

Stresses and dimensions are given in the corresponding sections for the 12 inch line. IGSCC crack initiation and growth are the dominant degradation mechanisms. Table F.24 summarizes the results for this weld.

Table F.24 Cumulative PRAISE Results for the Weld
in the 28 inch Recirculation Line

Подпись:odw=2.0 ksi

ote=1.75 ksi P = 1,125 psi Type 304 full residual stress 3 HU-CD/yr

F.3.7 Feedwater Elbow

The feedwater elbow is one of the base case systems. This system is subject to flow accelerated corrosion (FAC), which can be a serious degradation mechanism if left unchecked. PRAISE can not model FAC, but some analyses are provided for fatigue crack initiation and growth.

F.3.7.1 Dimensions and Welds — The layout of the feedwater system is given in the piping isometrics made available to the panel members. There are some 123 welds in the two loops of the feedwater systems, all but 6 of them in 12 and 20 inch piping. The 12 inch lines are schedule 100 (17.4 mm [0.687 inches] thick) and the 20 inch lines are schedule 80 (32.5 mm [1.281 inches] thick). The material is A — 333 Grade 6 (which is a carbon steel).

F.3.7.2 Stresses and Cycles — The feedwater line elbow is considered in Reference F.5, so this is evidently the high stress point in the system. Note that there are at least 6 such elbows in a feedwater system. (There are many more elbows, but they are likely to not be so highly stressed). The degradation mechanism is fatigue and flow accelerated corrosion (FAC). Stresses do not contribute to FAC, so are not needed for this mechanism. For fatigue, there are a considerable number of cycles of high stress amplitude. They are available from Reference F.5. Table F.25, which (except for the column of temperatures) is page A.25 of Reference F.5, summarizes the stresses. These stresses are “decomposed” according to the procedure discussed above for the surge line. The analysis reported in Reference F.5
used a temperature of 590°F (310°C), as indicated in the text at the top of Table F.25. However, Table 5­123 of Reference F.18 provides the temperatures for these transients, and it is suggested that these temperatures be used, because their use is more realistic and less conservative. They are included as the right-hand column of Table F.25. The temperature influences the strain-life curve, and has a noticeable effect on the computed failure probabilities because of its influence on the initiation probabilities.

The values of the deadweight and restraint of thermal expansion under normal operation that Reference F.5 uses for this location are

Cdw = 0

Cte = 115 MPa (16.68 ksi).

The stress history in Table F.25 most likely contains seismic events. It is not possible to eliminate them from the list using information currently available, but their influence on the calculated failure probabilities is expected to be minimal.

Table F.25 Summary of Stress Cycles for Feedwater Line Elbow
(from Page A.25 of NUREG/CR-6674 [F.5])

NAME OF PLANT

=

GE-NEW

NAME OF COMPONENT

=

FEEDWATER

LINE ELBOW

NUM OF LOAD PAIRS

=

28

MATERIAL

=

LAS

WALL THICK (INCH)

=

1.000

INNER DIAMETER

=

12.000

AIR/WATER

=

WATER

TEMPERATURE(F)

=

590.000

SULFUR(WHT%)

=

. 015

DISOL O2 (PPM)

=

.100

STR RATE (%/SEC)

=

0.00100

USEAGE(DETERM.)

=

3.68800

P-INITIATION@40

=

1.59E-01

P-INITIATION@60

=

3.65E-01

P-TWC @40

=

1.01E-03

p-twc @60

=

1.46E-02

LOAD PAIR

AMP(KSI)

NUM/4 0 YR

EDOT(%/S)

USEAGE

TEMP, °C

HIGH 18/LOW 21

106.040

5.0

.117000

.025000

200

HIGH 18/LOW 21

103.960

5.0

.114000

. 024000

200

HIGH 18/LOW 21

102.610

5.0

.113000

. 024000

200

HIGH 14/LOW 17

91.590

8.0

.001000

.123000

200

HIGH 8/LOW 17

89.400

10.0

.095000

. 037000

200

HIGH 3/LOW 16

88.270

5.0

.094000

.018000

200

HIGH 8/HIGH 7

83.760

126.0

. 041000

.519000

200

HIGH 7/HIGH 7

81.430

10.0

.086000

. 033000

215

HIGH 7/LOW 13

67.930

97.0

.001000

.740000

200

HIGH 7/LOW 13

66.710

14.0

.001000

.101000

200

HIGH 7/LOW 15

61.290

6.0

.001000

.035000

200

HIGH 7/LOW 15

61.160

64.0

.001000

.451000

212

HIGH 8/LOW 12

55.500

92.0

.001000

.391000

200

HIGH 3/LOW 12

46.630

88.0

.001000

.254000

215

HIGH 7/LOW 22

42.880

15.0

.001000

. 029000

212

HIGH 3/HIGH 7

39.440

212.0

.001000

.315000

215

HIGH 3/HIGH 7

38.130

69.0

.001000

.104000

224

HIGH 3/LOW 20

36.800

11.0

.001000

. 014000

224

HIGH 4/LOW 20

34.320

60.0

.001000

. 053000

215

LOW 11/LOW 20

32.950

203.0

.001000

.122000

200

HIGH 7/LOW 11

32.530

360.0

.001000

.203000

200

HIGH 6/LOW 11

29.770

222.0

. 025000

. 035000

200

HIGH 2/HIGH 19

26.090

30.0

. 028000

.003000

212

HIGH 5/HIGH 19

26.040

81.0

. 028000

.007000

200

HIGH 5/HIGH 9

21.640

96.0

.001000

.012000

212

HIGH 1/HIGH 11

20.560

40.0

.001000

.003000

200

LOW 10/LOW 11

14.180

30.0

.001000

.001000

200

HIGH 5/LOW 11

11.220

11515.0

.001000

.008000

200

F.3.7.3 Results — PRAISE runs for this component were made using the version that can treat fatigue crack initiation with details of the circumferential variation of the stresses. The feedwater system is

relatively more likely to experience water hammer, so the influence of an overload event with a stress of 0.42cflo = 128 MPa (18.5 ksi) above that normally present was considered. This stress is denoted as cDL, and results were generated for one cycle of this stress at 24, 39, or 59 years. The results are summarized in Table F.26, which includes the effects of cDL (columns D & F).

Table F.26 Cumulative PRAISE Results for Feedwater Line Elbow

A

B

C

D

E

F

G

Stresses

Ref.

F.5

Table F.25

Table F.25

Table F.25

Table F.25

Table F.25

80% of Table F.25

Failure

Criterion

^flow

^flow

^flow

^flow

^flow & J-T

^flow & J-T

^flow

Odl

no

no

no

ODL@(t-1)

no

ODL@(t-1)

no

о

A

25

<10-8

2.5×10-8

1.0×10-7

3.10×10-6

<10-7

40

0.001

2×10-6

5.69×10-6

7.19×10-6

1.54×10-5

1.43×10-4

<10-7

60

0.0146

1.8×10-4

2.57×10-4

2.59×10-4

~5×10-4

2.9×10-3

4.6×10-7

Ref F.6 Table 4-8

108 trials

GEN6TWA4

>100

25

<10-8

1.5×10-6 *

<10-7

1.70×10-6*

40

<10-8

1.5×10-6 *

<10-7

1.70×10-6*

60

<10-8

1.50×10-6*

2.1×10-6 *

GENC6TW4

>1500

25

<10-7

40

<10-7

60

<10-7

axi-

symmetric actual T

reduced

stresses

* also a break

Case A is directly from Reference F.5, and Case B is directly from Table 4-8 of Reference F.6. Case C is Case B rerun with 108 trials. Cases D-G are variations of C with different failure criteria, overloads and reduction of stresses. The results for various failure criteria (critical net section stress only or critical net section stress and tearing instability) show that consideration of tearing instability noticeably increases the computed failure probability (compare, for instance, cases C&E). Consideration of an overload event also has a noticeable effect (E&F). The use of lower stresses markedly reduces the computed failure probabilities (G & C). In the case of an overload event, the probability of a 100 gpm failure is the same as a complete pipe break.

F.3.7.4 Alternate Procedure — The results of Table F.26 show that the probability of a large leak was obtainable from the Monte Carlo procedure only when a large overload occurred. When this did not occur, there were no leaks of even 380 lpm (100 gpm) in 107 or 108 trials. In order to obtain estimates for the larger leak probabilities, the alternate procedure discussed for the surge line was also applied to Case C of Table F.26 for the feedwater elbow.

As before, the crack length for a given leak rate, b( q), was obtained from a pcPRAISE run, along with the half-crack length of any cracks that become through-wall. Figure F.11 provides a plot of the leak rate as a function of b for the feedwater elbow.

12000

image143

half crack length, b, inches

Figure F.11 Leak Rate as a Function of Half Crack Length for Feedwater Elbow Base Case C

The results in Table F.27 are obtained from this figure and the corresponding pcPRAISE results. This table also includes the portion of the circumference that is cracked and the proportion of the crack opening area to the flow area of the pipe. It is seen that the opening area of the crack is nearly equal to the flow area of the pipe when the leak rate is 19,000 lpm (5,000 gpm). The value of b for a complete pipe break, as obtained from Equation E.7 is also included. Table F.29 defines b( q).

Table F.27 Half Crack Lengths and Areas for a Given Leak Rate
(Feedwater Elbow Base Case C)

q, gpm

b,

inches

b

nRI

A,

in2

A

Apipe

100

5.737

0.32

1.837

0.02

1500

9.743

0.55

27.554

0.27

5000

11.095

0.62

90.877

0.91

DEGB

15.925

0.89

As before, the next step is to estimate the probability of having a through-wall crack exceeding a given length as a function of time. The modified version of pcPRAISE was used to generate a table of values of b and the time at which the leak first occurred. A run was made with 107 trials, with 2,607 cracks becoming through-wall within 60 years. This corresponds to a leak probability of 2.607×10-4 at 60 years, which agrees closely with the leak probability obtained earlier. Of these 2,607 cracks, none appeared before 25 years, and 64 occurred between 25 and 40 years. The statistical distribution of these 64 cracks at 40 years provides the probability of having a through-wall crack greater than a given length within 40 years. Extrapolation is required to obtain results for the crack lengths included in Table F.27. Figure F.12 shows the complementary cumulative distribution of b at 40 years, along with the curve fit of Equation F.10.

P(> b) = e“534(b-1) (40 years) [F.10]

Note that the plot starts at a half-crack length of 25 mm (1 inch), and that the data are closely approximated by a straight line on log-linear scales.

image144

Figure F.12 Complementary Cumulative Distribution of Half-Crack Length of Through-Wall
Cracks in Feedwater Elbow within 40 Years, Along with Fit

Figure F.13 provides a similar plot for the 2,607 through-wall cracks that occurred within 60 years. Equation F.11 is the fit of the distribution at 60 years within the range of interest.

P(> b) = 0.0274e“2’25(b_1) (60 years) [F.11]

Note that in this case the data appear bilinear and are not well approximated by a straight line on log — linear scales. To represent the data at the longer crack lengths of interest, a straight line was assumed beyond a crack length of 50 mm (2 inches). This corresponds to a probability below about 0.003.

rO

Подпись: 10Подпись: 10Подпись: 10Подпись: -4Подпись: 1.0 1.5 2.0 2.5 3.0 3.5Подпись:image150Подпись: 10

ь

яз

Ы>

Й

‘>

яЗ

Л

<4-1

0

1

-D

О

1-І

Й4

Figure F.13 Complementary Cumulative Distribution of Half-Crack Length of Through-Wall
Cracks in Feedwater Elbow within 60 Years, Along with Fit

The probability of a leak exceeding a given size within 40 and 60 years is then obtained by taking using the value of b for a given leak rate from Table F.27 in conjunction with Equations F.10 and F.11, respectively. Table F.28 summarizes the results.

Table F.28 Cumulative Results for Feedwater Elbow Case C

time

years

P(> q)

25

Л

p

ос

40

5.69×10-6

О

A

60

2.57×10-4

25

О

О

Л

40

1.03×10-11

60

6.44×10-7 *

25

О

О

LO

Л

40

5.29×10-21

60

7.84×10-11

25

LO

л

40

3.88×10-24

60

3.74×10-12

со

25

CL

Ш

40

2.44×10-35

О

60

7.14×10-17

* direct Monte Carlo gave <10’8

The leak (>0) results in Table F.28 came directly from the Monte Carlo simulation. With 108 trials, no leaks exceeding 380 lpm (100 gpm) were obtained. Hence, the Monte Carlo simulation predicts <10-8 probability of a leak exceeding 380 lpm (100 gpm) within 60 years. The alternative procedure gave a corresponding value of 6.44×10-7. This suggests that the alternative procedure overestimates the probability of a given leak, as was also the case for the surge line elbow.