ML20236A929

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Assessment of Boraflex Gap Distributions in Quad Cities Spent Fuel Storage Racks
ML20236A929
Person / Time
Site: Quad Cities  Constellation icon.png
Issue date: 05/28/1987
From:
NORTHEAST TECHNOLOGY CORP.
To:
Shared Package
ML20236A865 List:
References
NET-044-1, NET-44-1, NUDOCS 8707280273
Download: ML20236A929 (27)
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TCO NORTHEASTTECHNOLOGYCORP Report No.: NET-044-1 AN ASSESSMENT GF BORAFLEX GAP DISTRIBUTIONS IN THE QUAD CITIES SPENT FUEL STORAGE RACKS 5-28-87 Prepared for SOUTHERN SCIENCES DIVISION OF BLACK AND VEATCH by NORTHEAST TECHNOLOGY CORP P

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TABLE OF CONTENTS a

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1

1.0 INTRODUCTION

2 2.0 ASSUMPTIONS......................................

4 3.0.-ANALYTICAL METHOD................................

4 3.1- Gap Size Distribution....................,..

3.2 Axial Distribution of Gaps.................. 6 3.3 Gap Density per Axial Interval.............. 8 10 4.0 DISCUSSION.......................................

11 References............................................

Appendix A: Gap Sequences for a Cumulative Gap Size of 10' i

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l 1.0 INTROrdUTION The occurrence of gaps in the Boraflex absorber in the Quad Cities spent fuel storage ra::ks . can result in an increase in the reactivity state of the fuel / rack system.

The magnitude of reactivity increase will depend on the rize of the ;sps and their axial elevation relative to gaps in neighboring panels. - '. Isolated gaps will have a relatively small reactivity effect whereas the effect - will be . larger when gaps in neighboring panels occur at the same axial elevation.

This report . describes a methodology developed to quantify the probability of gap occurrence and gap elevation as a function of gap size. The method provides a means to compute the gap density (number of inches of gap per axial interval) .as well as the probability of gaps occurring at the same axial elevation in adjacent panels. The results of the analysis provide the basis for' establishing conservative bounding cases for subsequent reactivity calculation.

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' 2. 0. ASSUMPTIONS Neutron radioassay measurements III conducted at the Quad Cities spent fuel pool have confirmed the occurrence of gaps in the Boraflex neutron absorber panels. The formation of gaps and subsequent growth has been attributed to shrinkage of the restrained panels of Boraflex.(

Crosslinking in the Boraflex polymer causes the panels to shrink when exposed to gamma radiation .from the spent fuel.

Data from the BISCO qualification programI3I indicate that crosslinking and hence shrinkage saturates at about 1 to 2 x l 10 10 rads. At this exposure the measured l

volumetric shrinkage is approximately 20% based on test reactor irradiations. If it is assumed that shrinkage is isotropic, this would result- in an upper bound cumulative gap of 10 inches in a 152 inch Boraflex panel.

The neutron radioassay measurements which utilize the special test method III provide some insight as to the gap

site ' distribution and the axial distribution of gaps.

However, it is noted that these tests involved a relatively small sample (31 detectable gaps in 28 panels).

Furthermore, the measurements only reflect the condition of the gaps after two refueling outages ( gamma dose estimated L

to be about 10 8 rads) while further gap growth may occur.

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Accordingly, the following conservative assumptions have 'been developed to provide a bounding estimate ' of gap as size distribution and axial elevation of gaps:

=

1. Every panel will eventually develop at least one gap and the total cumulative gap size is 10" per panel.
2. The gap size distribution is uniform (ies gaps of any, size have equal probability of occurring).
3. No gaps occur in the lower 40" of Boraflex as confirmed by the special test measurements.
4. In the range of 40" to 150" the axial distribution of gaps.is uniform.

Figure 4-2 of Reference 2 may indicate a non-uniform axial distribution although the sample size is too small to be conclusive. The analysis described subsequently has examined the effect of a non-uniform axial distribution in order to provide a worst-case bounding condition.

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3.0 ANALYTJCAL METHOD E

The occurrence of. gaps, their size and axial elevation a

in a. panel of Botaflex depends on three probabilities:

1. the probability'that a particular panel will have a certain' number of gaps,
2. the probability that a particular gap will have a certain size,
3. the probability that a particular gap will have a certain axial elevation.

the lack of sufficient As discussed previously, measurement data and the potential ' for further gap growth.

precludes'the development of discrete distributions based on the data. Instead, simple uniform distributions based on the global characteristics of the data are used to develop an anslytical' solution.

3.1; pagg size distribution the present derivation, it is For the purpose of assumed that all of the gaps occur to a resolution of 1".

Therefore, none of the gaps is less than 1" in length and ,

all have integer lengths with a cumulative length of 10" in any given panel. There are only 512 combinations of integer length gaps that sum to 10". A Fortran program was j

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4 developed to generate these 512 combinations which are tabulated in Appendix A. Since the probability that any gap will be of a certain integer length is assumed unifort , it is equally likely that a gap will be of length l', 2", 3"...

np to 10" (ie, the probability is (1/10) that the gap will be of a given length).

The probability of a particular sequence of gaps occurring can be computed explicitly from the table in Appendix A. Suppose the sequence (4 2 4} (nurtter 489 in Appendix A) _ occurs in some panel. This imp).ies that there are three gaps: the first is 4" long, the second 2", and the third 4". To generate this sequence, a 4" gap must be' chosen. This has a probability of (1/10) of occurring. In this sequence, the second gap chosen in a 2" gap. Since the  ;

total gap length can not exceed 10", the choices for the second gap are limited to gaps between 1" and 6". Thus, the probability of this choice occurring is (1/6). Finally, another 4" gap is chosen with probability (1/4) . While the range of choice is dependent on the previous gaps chosen in the sequence, the choice of each gap is independent so that the probability of the sequence is the product of the probabilities of each gap in the sequence. For the sequence

{4 2 4}, the probability of the sequence occurring is (1/10)x(1/6)x(1/4). Summing the probabilities of those 5

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sequences having the same number of gaps gives a distribution for the number of gaps in any panel. This is tabulated in Table 3.1.

Table 3.1 shows that the most probable number of gaps per panel is three. To determine the probability of a given 4

gap-size in any panel, the probability of each sequence is weighted by the number of gaps of a given size produced by the sequence and summed for all 512 scquences. For example, for the sequence {4 2 4} (sequence number 484 in Appendix A), the probability of producing a 2' gap is equal to the .

i sequence probability of 0.004167. For the same sequence, the probability of producing a 4" gap is twice the sequence probability, or 0.008334. The probability of this sequence

}

producing a gap size other than 4" or 2" is zero.

A second Fortran program was developed to compute the individual sequence probabilities and to perform the probability weighting and summing. The results are tabulated in Tnble 3.2 3.2 Axial Distribution gi gang The NNC special measurements indicate no detectable gaps in the lower 40" of the 28 panels tested. It is therefore assumed that gaps can occur only between 40 and 150" and the probability of occurrence is uniform in this 6

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region. This' assumption ~ is conservative' since it maximizes- j the gap density 'in the central portion of the panel 'which r

would have the greatest reactivity:effect.

As a matter of convention,'the axial elevation of a gap- o is measured 'from the bottom of the panel' to the bottom of

the.' gap. If we consider an axial interval of length L in the panel' , the probability of a gap of size S occurring in any axial interval of length L ist L / [(150 - 40) - (S - 1))

Tnis is accus11y. only valid for any interval at least a gap length away from the- top of . the - panel since gaps cannot physically extend beyond the top. of the panel. For. every

(-

10" axial interval in the panel, the probability that a gap of size's will have bottom edge within that interval is  !

tabulated-in. Table 3.3.

l- .P(axial) is the probability the gap reference elevation For (bottom of the gap) falls within a 10" axial interval.

gaps large: than 1", there is a finite probability that the gap will not fall entirely within the 10" interval but will overlap into the adjacent intervals. That probability depends on the size of the gap and the assumption that the h- gaps occur with a 1" resolution and is compiled in Table 3.4.

In . theory it may be possible for more than one gap to 7

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r occur in a given 10" interval, but physically this is

.unlikely. For a. gap to form between two gaps or between a gap: and an end .of the panel there must exist a sufficient length of panel-for axial shrinkage and stresses sufficient to produce yielding. Thus it is assumed that each interval will contain at most one gap.

3.3 ftag- Density gar AKlal interval I

For a given gap-size, the probability that some portion of the gap will occur in ' a 10" axial interval is given by the product of tne probability that a gap of size S occurs (Table 3.2), the probability the bottom of the gap occurs in a 10" axial interval (Table 3-3), and the probability that the given portion of the gap is in (or out of) the interval (Table 3.4). These products are tabulated in Table 3.5.

Certain entries in Table 3.5 can be summed to give the overall probability of a given length of gap occurring in a i

given axial interval. For example, there are three ways a 9" gap can occur in a given intervals by a 9" gap being wholly within the interval; by a 10" gap having only 9 of its 10" in the interval; or by a 10" ge.p in the adjacent t

interval with 9" overlapping into the interval of interest.

The probability of 9" of gap occurring in a given interval is then the sum of the probabilities of the three ways that 8

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nine inches of gap can occur. The total probabilities are tabulated in Table 3.6.

For a given number of panels, Table 3.6 can be used to axial compute the total length of gap occuring in a 10 interval. For a 4 by 4 array of cells with 32 effective full panels, the total gap length per 10" axial interval is 30.4 inches.

If the distribution shown in Figure 4-2 of Reference 2 is used, there is a 6 out of 31 chance that a gap will occur in axial interval 8 (midplane). For the same 4 by 4. array of cells, this gives a total gap length of 61.9 inches.

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1 4.0 DISCUSSION The probabilities summarized in Table 3.5 can be used to compute the. probability of gaps occuring at the same axial elevation in adjacent panels in a fuel storage cell.

E For. an arbitrary panel, Table 3.1 indicates that the probability of having a 10" gap somewhere in the panel is i 10

~1 If we consider a second panel in the storage cell,  ;

Table 3.5 indicates that the probability of a 10" gap occurring at a particular axial elevation is 0.00099, or 10

-3 Thus, the probability of two adjacent panels having 10" gaps at the same axial elevation is 10 x 10-3, or

-1 10

~4 A third panel will have a 10" gap at the same axial

~1 -3 x 10-3, or 10-7; a elevation with probability 10 x 10 fourth panel with probability 10-10, and so on.

The procedure described above can be repeated for gaps of various sizes and ca9 be used to determine worst case distributions based on their probability of occurrence.

This is expected to provide limiting configurations of gaps for' reactivity calculations.

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REFERENCES:

le .Special Neutron Attenuation Test for.High Density Spent Fuel ~ Storage Racks (Wet), National Nuclear Corporation for CECO Quad Cities, CECO P.O. No.

309763, December, 1986.

2. Preliminary Assessment of Boraflex Performance in

.the Quad Cities Spent Fuel Storage Racks, NETCO Report No. NET-042-1, April 10, 1987.

> 3. Irradiation Study of Boraflex Neutron Shielding Material, BISCO Report 748-10-1, Rev. 1, August 12, 1981.

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t APPENDIX A GAP SEQUENCES FOR A CUMULATIVE GAP SIZE OF 10"

i Secuence Fecuence NC8 h ber _ropabilitv D

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g 1 1~ 1 1 1 1 1 '1 1 1 1 0.275573E-06 2 2 3

1 1 1 1 1 1 1 1 0 0.248016E-05 1 2 1 1 1 1 1 1 1 0 0.220459E-05 4 1 1 2 5

1 1 1 1 1 1 0 0.192901E-05 1 1 1 2 1 1 1 1 1 0 0.165344E-05 6 1 1 2 7

1 1 1 1 1 1 0 0.137787E-05 j 1 1 1 1 1 2 1 1 1 0 0.110229E-05 8 1 1 9 1 1 1 1 1 2 1 1 0 0.826720E-06 10 1 1 1 1 1 1 1 2 1 0 0.551146E-06 1 1 0.275573E-06 1 1 1 1 1 2 0 11 3 1 1 1 1 1 1 1 0 0 0.198413E-04  !

12 2 2 1 13 1 1 1 1 1 0 0 0.173611E-04 1 3 0 14 1 1 1 1 1 1 0- 0.154321E-04 2 1 2 f 1 1 1 1 0 0 0.148810E-04  ;

15 1 2 2 16 1 1 1 1 1 0 0 0.132275E-04 i 1 1 3 1 1 1 1 1 0 -0 0.115741E-04 17 2 2 18 1 1 1 1 1 1 0 0 0.124008E-04 1 2 1 2 1 1 1 1 0 0 0.110229E-04 19 1 2 2 20 1 1 1 1 1 0 0 0.964506E-05 1 1 1 3 1 1 1 1 0 0 0.826720E-05 21 2 2 0 22 1 1 1 1 1 1 0 0.992063E-05 1 2 1 1 2 1 1 1 0 0 0.881834E-05 23 1 2 2 24 1 1 1 1 1 0 0 0.771605E-05 {

1 1 1 2 2 1 1 1 0 0 0.661376E-05 25 1 3 26 1 1 1 1 1 1 0 0 0.551146E-05 2 2 27 1 1 1 1 1 1 0 0 0.744048E-05 1 2 1 1 1 2 1 1 0 0 0.661376c-05 21 1 1 2 1 1 2 1 1 0 0 0.578704E-05 29~ 2 30 1 1 1 1 2 1 1 0 0 0.496032E-05 1 1 1 1 2 2 1 1 0 0. 0.413360E-05 31 1 t 1 1 1 3 1 1 0 0 0.330688E-05 32 2 33 1 1 1 1 1 2 1 0 0 0.496032E-05 1 2 1_ 1 1 1 2 1 0 0 0.440917E-05 34 2  !

35 1 1 1 1 1 2 1 0 0 0.385802E-05 1 1 1 2 t 1 2 1 0 0 0.330688E-05  ;

36 2 2 37 1 1 1 1 1 1 0 0 0.275573E-05 )

1 1 1 1 1 2 2 1 0 0 0.220459E-05 '

38 39 1 1 1 1 1 1 3 1 0 C 0.165344E-05 2

40 1 1 1 1 1 1 2 0 0 0.248016E-05 1 2 1 1 1 1 -1 2 0 0 0.220459E-05 41 2 2 0 42 1 1 1 1 1 1 0 0.192901E-05 ,

1 1 1 2 1 1 1 2 0 0 0.165344E-05 43 1 1 1 1 2 1 1 2 0 0 0.137787E-05 44 2 45 1 1 1 1 1 1 2 0 0 0.110229E-05 46 1 1 1 1 1 1 2 2 0 0 0.826720E-06 1

47 1 1 1 1 1 1 3 0 0 0.551146E-06

'4 1 1 1 1 1 1 0 0 0 0.138889E-03 4B 3 2 49 1 1 1 1 1 0 0 0 0.119048E-03 2 3 ,

50 1 1 1 1 1 0 0 0 0.104167E-03 1 4 1 1 1 1 1 0 0 0 0.925926E-04 51 3 2 52 1 1 1 1 1 0 0 0 0.992063E-04 2 2 2 1 1 1 1 0 0 0 0.868056E-04 53 3 2 54 1 1 1 1 1 0 0 0 0.771605E-04 2 3 55 1 1 1 1 1 0 0 0 0.744048E-04 1 2 3 0 56 1 1 1 1 0 0 0.6613765-04 1 1 4 1 1 1 1 0 0 0 0.578704E-04 57 3 2 58 1 1 1 1 1 0 0 0 0.793651E-04 2 2 1 2 1 1 1 0 0 0 0.694444E-04 A-1

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59 1 3. 1 2 1 1 1 0- 0 0- 0.617264E-04 60 2 1. ~2 2 1 1- 1- 0 0 0 0.595238E-04 i 61 1 2 2 2 1 1 1 0 0 0 0.529101E-04 62 1 1- 3 2 1 1 1 0 0 0 0.462963E-04.

63 2 -1 1 3 1 1 1 0 0. 0 0.496032E-04

<, 64 1 2 1 3 1 1 1 0 0 0 0.440917E ! 65 1 3 2 3 1 1 1 0 0 0 0.385802E-04 66 1 1 1 4 1 1 1 0 0 0 0.330688E-04 67 3 1 1 1 2 1- 1 0 0 0 0.595238E-04 68 2 -2 1 1 2 1 1 0 0 0 0.520833E-04 69 1 3 1 1 2 1 1 0 0 0 0.462963E-04 70 2 1 2 1 2 1 1 0 0 :D- 0.4464295-04 71 1 2. 2 1 2 1 1 0 0 0 0.396825E-04 72 1 1 3 1 2 1 1 0 0- 0 0.347222E-04 73 2 1 1 2 2 1 1 .0 0 0 0.372024E-04 74 'l 2 1 2 2 1 1 0 0 0 0.330688E-04 h 75 1 1 2 2 2 1 1 0 0 0 0.289352E-04, 76 1 1 1 3 2 1 1 0 0 0 0.248016E 77 2 -1 1 1 3 1 1 0 0 0 0.297619E-04

78 1 2 1 1 3 1 1 0 0 0 0.264550E-04 79 1 1 2 1 3 1 1 0 0 0 0.231481E-04 80 1 1 1 2 3 1 1 0 0 D 0.198413E-04 81 1' 1 1 1 4 1 1 0 0 0 0.165344E-04 82 3 .1 I 1 1 2 1 0 0 0 0.396825E-04 83- 2 2 1 1 1- 2 1 0 0 0 0.347222E-04 84- 1 3 1 1- 1 2 1 0 0 0 0.308642E-04 85 2 1 2 1 1 2 1 0 0 0 0.297619E-04 86 1 2 2 1 1 2 1 0 0 0 0.2645SOE-04 87 1 .1 3 1 1 2 1 0' O O 0.231481E-04 88 2 1. 1 2 1
2 1 0 0 0 0.248016E-04 ,

80 1 2 1 2 1 2 1 0- 0 0 0.220459E 90 1  ? 2 2 1 2 1 0 0 0 0.192901E-04 91 1 1 1 3 1 2 1 0 0 0 0.165344E-04' 92 2 1 1 1 2 2. 1 0 0 0 0.198413E-04 93 1 2 1 1 2 2 1 0 0 0 0.176367E-04 94 1 1 2 1 2 2 1 0 0 0 0.154321E-04 95 1 1 1 2 2 2 1 0 0 0 0.132275E-04 96- 1 1 1 1 3 2 1 C 0 0 0.110229E-04 97 2 1 -1 1 1 3 1 0 0 0 0.148810E-04 98 1 2 1 1 1 3 1 0 0 0 0.132275E-04 99 1 1 2 1 1 3 1 0 0 0 0.115741E-04 100 1 1 1 2 1 3 1 0 0 0 0.992063E-05 101 1 1 1 1 2 3- 1 0 0 0 0.826720E-05 102 1 1 3 1 1 4 1 0 0 0 0.661376E-05 103 3 1 1 1 1 1 2- 0 0 0 0.198413E-04 104 2 2 1 1 1 1 2 0 0 0 0.173611E-04  :

105 1 3 1 1 1 1 2 0 0 0 0.154321E-04  !

106 2 1 2 1 1 1 2 0 0 0 0.148810E-04 107 1 2 2 1 1 1 2 0 0 0 0.132275E-04 108 1 1 3 1 1 1 2 0 0 'O 0.115741E-04 iO9 2 1 1 2 1 1 2 0 0 0 0.124008E-04

,310 1 2 1 2 1 1 2 0 0 0 0.110229E-04 111 I 1 2 2 1 1 2- 0 0 0 0.964506E-05

, 112 1 1 1 3 1 1 2 0 0 0 0.826720E-05 113 2 1 1 1 2 1 2 0 0 0 0,992063E-05 114 1 2 1 1 2 1 2 0 0 0 0.881834E-D5 115 1 1 2 1 2 1 2 0 0 0 0.771605E-05 116 1 1 1 2 2 1 2 0 0 0 0.661376E-05 A-2

Sectuence Secuence C8P

  • Drofabilitv Drber 117 1 1 1 1 3 1 2 0 0 0 0.551146E-05 118 2 1 1 1 1 2 2 0 0 0 0.744048E-05 119 1 2 1 1 1 2 2 0 0 0 0.661376E-05 120 1 1 2 1 1 2 2 0 0 0 0.578704E-05 121 1 1 1 2 1 2 2 0 0 0 0.496032E-05 122 1 1 1 1 2 2 2 0 0 0 0.413360E-05 123 1 1 1 1 1 3 2 0 0 0 0.330688E-05 124 2 1 1 1 1 1 3 0 0 0 0.496032E-05 125 1 2 1 1 1 1 3 0 0 0 0.440917E-05 126 1 1 2 1 1 1 3 0 0 0 0.385802E-05 127 1 1 1 2 1 1 3 0 0 0 0.33068BE-05 128 1 1 1 1 2 1 3 0 0 0 0.275573E-05 129 1 1 1 1 1 2 3 0 0 0 0.220459E-05 130 1 1 1 1 1 1 4 0 0 0 0.165344E-05 4 131 5 1 1 1 1 1 0 0 0 0 0.833333E-03 132 4 2 1 1 1 1 0 0 0 0 0.694444E-03 133 3 3 1 1 1 1 0 0 0 0 0.59523BE-03 J 134 2 4 1 1 1 1 0 0 0 0 0.520833E-03  !

135 1 5 1 1 1 1 0 0 0 0 0.462963E-03 l 136 4 1 2 1 1 1 0 0 0 0 0.555556E-03 l 137 3 2 2 1 1 1 0 0 0 0 0.476190E-03  !

138 2 3 2 1 1 1 0 0 0 0 0.416667E-03 I 139 1 4 2 1 1 1 0 0 0 0 0.370370E-03 1 140 3 1 3 1 1 1 0 0 0 0 0.396625E-03 l 141 2 2 3 1 1 1 0 0 0 0 0.347222E-03 q 142 1 3 3 1 1 1 0 0 0 0 0.308642E-03 l 143 2 1 4 1 1 1 0 0 0 0 0.297619E-03 144 1 2 4 1 1 1 0 0 0 0 0.264550E-03 1 145 1 1 5 1 1 1 0 0 0 0 0.231481E-03 l 146 4 1 1 2 1 1 0 0 0 0 0.416667E-03 l 147 3 2 1 2 1 1 0 0 0 0 0.357143E-03 1 148 2 3 1 2 1 1 0 0 0 0 0.312500E-03 l 149 1 4 1 2 1 1 0 0 0 0 0.277778E-03 1 150 3 1 2 2 1 1 0 0 0 0 0.297619E-03 l 151 2 2 2 2 1 1 0 0 0 0 0.260417E-03  !

152 1 3 2 2 1 1 0 0 0 0 0.231481E-03  !

153 2 1 3 2 1 1 0 0 0 0 0.223214E-03 )

154 1 2 3 2 1 1 0 0 0 0 0.198413E-03 155 1 1 4 2 1 1 0 0 0 0 0.173611E-03  !

156 3 1 1 3 1 1 0 0 0 0 0.238095E-03 l 157 2 2 1 3 1 1 0 0 0 0 0.208333E-03 l 158 1 3 1 3 1 1 0 0 0 0 0.185185E-03 l 159 2 1 2 3 1 1 0 0 0 0 0.178571E-03 l 160 1 2 2 3 1 1 0 0 0 0 0.158730E-03 J 161 1 1 3 3 1 1 0 0 0 0 0.13E889E-03 l 162 2 1 1 4 1 1 0 0 0 0 0.148810E-03 ,

163 1 2 1 4 1 1 0 0 0 0 0.132275E-03 I 164 1 1 2 4 1 1 0 0 0 0 0.115741E-03 l 165 1 1 1 5 1 1 0 0 0 0 0.992063E-04 l 166 4 1 1 1 2 1 0 0 0 0 0.277778E-03 167 3 2 1 1 2 1 0 0 0 0 0.238095E-03 168 2 3 1 1 2 1 0 0 0 0 0.208333E-03 169 1 4 1 1 2 i 0 0 0 0 0.J 8 518 5E-03 170 3 1 2 1 2 1 0 0 0 0 0.198413E-03 l 171 2 2 2 1 2 1 0 0 0 0 0.173611E-03 172 1 3 2 1 2 1 0 0 0 0 0.154321E-03 1 173 2 1 3 1 2 1 0 0 0 0 0.148810E-03 174 1 2 3 1 2 1 0 0 0 0 0.132275E-03 A-3 i

- a Secuence Secuence Mer C#I F' "'"#' "rdabilitv 175 1 1 4 1 2 1 0 0 0 0 0.115741E-03 176 3 1 1 2 2 1 0 0 0 0 0.158730E-03

-177 2 2 1 2 2 1 0 0 0 0 0.138889E-03 178 1 3 1 2 2 1. 0 0 0 0 0.123457E-03 179 2 1 2 2 2 .1 0 0 0 0 0.119048E-03 180 1 2 2 2 2 1 0 0 0 0 0.105820E-03 181 1 1 3 2 2 1 0 0 0 0 0.925926t-04 182 2 1 1 3 2 1 0 0 0 0 0.992063E-04 183 1 2 1 3 2 1 0 0 0 0 0.881834E-04 184 1 1 2 3 2 1 0 0 0 0 0.771605E-04 185 1 1 1 4 2 1 0 0 0 0 0.661376E-04 186 3 1 1 1 3 1 0 0 0 0 0.119048E-03 187 2 2 1 1 3 1 0 0 0 0 0.104167E-03 J 188 1 3 1 1 3 1 0 0 0 0 0.925926E-04 l 189 2 1 2 1 3 1 0 0 0 0 0.892E67E-04 190 1 2 2 1 3 1 0 0 0 0 0.793651E-04 191 1 1 3 1 3 1 0 0 0 0 0.694444E-04 192 2 1 1 2 3 1 0 0 0 0 0.744048E-04 193 1 2 1 2 3 1 0 0 0 0 0.661376E-04 194 1 1 2 2 3 1 0 0 0 0 0.578704E-04 195 1 1 1 3 3 1 0 0 0 0 0.496032E-04 196 2 1 1 1 4 1 0 0 0 0 0.595238E-04 197 1 2 1 1 4 1 0 0 0 0 0.529101E-04 198 1 1 2 1 4 1 0 0 0 0 0.462963E-04 199 1 1 1 2 4 1 0 0 0 0 0.396825E-04 200 1 1 1 1 5 1 0 0 0 0 0.330688E-04 201 4 1 1 1 1 2 0 0 0 0 0.138889E-03 202 3 2 1 1 1 2 0 0 0 0 0.119048E-03 203 2 3 1 1 1 2 0 0 0 0 0.104167E-03 204 1 4 1 1 1 2 0 0 0 0 0.925926E-04 205 3 1 2 1 1 2 0 0 0 0 0.992063E-04 206 2 2 2 1 1 2 0 0 0 0 0.868056E-04 207 1 3 2 1 1 2 0 0 0 0 0.771605E-04 208 2 1 3 1 1 2 0 0 0 0 0.744048E-04 209 1 2 3 1 1 2 0 0 0 0 0.661376E-04 210 1 1 4 1 1 2 0 0 0 0 0.576704E-04 211 3 1 1 2 1 2 0 0 0 0 0.793651E-04 212 2 2 1 2 1 2 0 0 0 0 0.694444E-04 213 1 3 1 2 1 2 0 0 0 0 0.617284E-04 214 2 1 2 2 1 2 0 0 0 0 0.595238E-04 215 1 2 2 2 1 2 0 0 0 0 0.529101E-04 216 1 1 3 2 1 2 0 0 0 0 0.462963E-04 217 2 1 1 3 1 2 0 0 0 0 0.496032E-04 218 1 2 1 3 1 2 0 0 0 0 0.440917E-04 219 1 1 2 3 1 2 0 0 0 0 0.385802E-04 220 1 1 1 4 1 2 0 0 0 0 0.330688E-04 221 3 1 1 1 2 2 0 0 0 0 0.595238E-04 222 2 2 1 1 2 2 0 0 0 0 0.520833E-04 223 1 3 1 1 2 2 0 0 0 0 0.462963E-04 224 2 1 2 1 2 2 0 0 0 0 0.446429E-04 225 1 2 2 1 2 2 0 0 0 0 0.396825E-04 226 1 1 3 1 2 2 0 0 0 0 0.347222E-04 227 2 1 1 2 2 2 0 0 0 0 0.372024E-04

.228 1 2 1 2 2 2 0 0 0 0 0.330685E-04 229 1 1 2 2 2 2 0 0 0 0 0.289352E-04 230 1 1 1 3 2 2 0 0 0 0 0.248016E-04 231 2 1 1 1 3 2 0 0 0 0 0.297619E-04 232 1 2 1 1 3 2 0 0 0 0 0.264550E-04 A-4

s

  • . 4 ~.

Sequence Fecuence Cap Feouence Drofability-Ntsrber 2

233. I 1 2 1' 3 2 0 0 0 0 0.231481E-04  !

234- 1- 1 1 2 3 2 0 0 0 0 0.198413E 235 1 1- 1 1 4 2 0 0- 0 0 0.165344E-04 236- 3 1 1 1- 1 3 0 0 0 0 0.396825E-04

,237 2 2 1 1 1 3 0 0 0 0 0.347222E-04:

238 :1 3 1 1 1 3 0 0 O' O 0.308642E-04 239 2 1 2 1 1 3 -0 0 0 0 -0.297619E-04 240 '1 1 2 1 1 3 0 0 0 0 0.264550E-Qu ,I 241 1 1 3 1. 1 3 0 0 0' O 0.231481E-04 242 2 1 1 2 1 3 0 0 0 0 0.248016E-04 243 1' 2 1 2 1 3 0 0 0 0 0.220459E-04 '

244 1 1 2 2 1 3 0 0 0 0 0.192901E-04 245 1 1 1 3 1~ 3 0 0 0 0 0.165344E-04 'i 246 2 1 1 1 2 3 0 0 0 0 0.196413E-04 4 247' 1 2 1 1 2 3 0 0 0. 0- 0.176367E-04 248 1 1 2 1 2 3 0 0 0 0 0.154321E-04 240 1 1 1 2 2 3 0 0 'O O 0.132275E-04 250 1 1 1 1 3 3 0 0 0 0 'O.110229E l 251 2 1 1 1 1 4 0 0 0 0 0.148810E-04 }

252 1 2 1 1 1 4 0 0. 0 0 0.132275E-04 253 1 '1 2 1 1 4 0 0 0 0 0.115741E-04 {

254. 1 1 1 2 1 4 0 0 0 0 '0.992063E-05 l 255 1 1 1 1 2 4 0 0 0 0 0.826720E-05 1 256 1 1 .1 1 1- 5 0 0 0 0 0.661376E-05 257 6 1 1 1 1 0 0 0 0 0 0.416667E-02 2FB 5 2 1 1 1 0 0 0 0. 0 0.333333E-02 259 4 3- 1 1 1 0 0 0 0- 0 0.277778E-02 260 '3 4' 1 1- 1 0 0 0 0 0 0.238095E-02 261 2 5 1 1 1 0 0 0 0 0 0.208333E-02 262- 1 6 1 1 1 0 0 0 0 0 0.185185E-02  ;

263- 5- 1 2 1 1 0 0 0 0 0 0.250000E-02

~264- 4 2 2 1 1 0 0 0 0 0 -0.208333E-02 265 3 3 2 1 1 0 0 'O O -0 0.178571E-02 266 2 4 2 1 1 0 0 0 0 0 0.156250E-02 267 1 5 2 1 1 0 0 0 0 0 0.138889E-02 268 4 1 3 1 1 0 0 0 0 0 0.166667E-02 269 3 2 3 1 1 0 0 0 0 0- 0.142857E-02 270 2 3 3 1 1 0 0 0 0 0 0.125000E-02 $

271 1 4 3 1 1 0 0- 0 0 0. 0.111111E-02 j 272 3 1 4 1 1 0 0 0 0 0 0.119048E-02 ,

273 2 2 4 1 1 0 0 0 0 0 0.104167E-02 274~ 1 3 4 1 1 0 0 0 0 0 0.925926E-03 275 2 1 5 1 1 0 0 0 0 0 0.892857E-03 276 1 2 5 1 1 0 0 0 0 0 0.793651E-03 277 1 1 6 1 1 0 0 0 0 0 0.694444E-03 l 278 5 1 1 2 1 0 0 0 0 .0 . 0.166667E-02 279 4 2 1 2 1 0 0 0 0 0 0.138889E-02  !

280 3 3 1 2 1 0 0 0 0 0 0.119048E-02 1

)

281 2 4 1 2 1 0 0 0 0 0 0.104167E-02 282 1 5 1 2 1 0 0 0 0 0 0.925926E-03 283 4 1 2 2 1 0 0 0 0 0 0.111111E-02 284 3 2 2 2 1 0 0 0 0 0 0.952381E-03 285 2 3 2 2 1 0 0 0 0 0 0.833333E-03 286 1 4 2 2 1 0 0 0 0 0 0.740741E-03 287 ~3 ~1 3 2 1 0 0 0 0 0 0.793651E-03 288- 2 2' 3 2 1 0 0 0 0 0 0.694444E-03 289 1 3 3 2 1 0 0 0 0 0 0.617284E-03 290 2 1 4 2 1 0 0 0 0 0 0.595238E-03 l A-5

__ I

o 8 8 Cep Fecuence Sih 291 1 2 4 2 1 0 0 0 0 0 0.529101E-03 292 1 1 5 2 1 0 0 0 0 0 0.462963E-03 293 4 1 1 3 1 0 0 0 0 0 0.833333E-03 294 3 2 1 3 1 0 0 0 0 0 0.714286E-03 295 2 3 1 3 1 0 0 0 0 0 0.625000E-03 296 1 4 1 3 1 0 0 0 0 0 0.555556E-03 l 297 3 1 2 3 1 0 0 0 0 0 0.595238E-03 '

298. 2 2 2 3 1 0 0 0 0 0 0.520833E-03 299 1 3 2 3 1 0 0 0 0 0 0.462963E-03 300 2 1 3 3 1 0 0 0 0 0 0.446429E-03 301 1 2 3 3 1 0 0 0 0 0 0.396825E-03 302 1 1 4 3 1 0 0 0 0 0 0.347222E-03 303 3 1 1 4 1 0 0 0 0 0 0.476190E-03 1 304 2 2 1 4 1 0 0 0 0 0 0.416667E-03 305 1 3 1 4 1 0 0 0 0 0 0.370370E-03 306 2 1 2 4 1 0 0 0 0 0 0.357143E-03 307 1 2 2 4 1 0 0 0 0 0 0.317460E-03 308 1 1 3 4 1 0 0 0 0 0 0.277778E-03 309 2 1 1 5 1 0 0 0 0 0 0.297619E-03 310 1 2 1 5 1 0 0 0 0 0 0.264550E-03 311 1 1 2 5 1 0 0 0 0 0 0.231481E-03 312 1 1 1 6 1 0 0 0 0 0 0.198413E-03 1 313 5 1 1 1 2 0 0 0 0 0 0.833333E-03 314 4 2 1 1 2 0 0 0- 0 0 0.694444E-03 315 3 3 1 1 2 0 0 0 'O 0 0.59523BE-03 4 316 2 4 1 1 2 0 0 0 0 0 0.520833E-03 317 1 5 1 1 2 0 0 0 0 0 0.462963E-03 318 4 1 2 1 2 0 0 0 0 0 0.555556E-03 319 3 2 2 1 2 0 0 0 0 0 0.476190E-03 320 2 3 2 1 2 0 0 0 0 0 0.416667E-03 .

321 1 4 2 1 2 0 0 0 0 0 0.370370E-03

~322 3 1 3 1 2 0 0 0 0 0 0.396825E-03 323 2 2 3 1 2 0 0 0 0 0 0.347222E-03 324 1 3 3 1 2 0 0 0 0 0 0.308642E-03 325 2 1 4 1 2 0 0 0 0 0 0.297619E-03 326 1 2 4 1 2 0 0 0 0 0 0.264550E-03 327 1 1 5 1 2 0 0 0 0 0 0.231481E-03 328 4 1 1 2 2 0 0 0 0 0 0.416667E-03 329 3 2 1 2 2 0 0 0 0 0 0.357143E-03 330 2 3 1 2 2 0 0 0 0 0 0.312500E-03 331 1 4 1 2 2 0 0 0 0 0 0.277778E-03 332 3 1 2 2 2 0 0 0 0 0 0.297619E-03 333 2 2 2 2 2 0 0 0 0 0 0.260417E-03 334 1 3 2 2 2 0 0 0 0 0 0.231481E-03 335 2 1 3 2 2 0 0 0 0 0 0.223214E-03 336 1 2 3 2 2 0 0 0 0 0 0.198413E-03 337 1 1 4 2 2 0 0 0 0 0 0.173611E-03 338 3 1 1 3 2 0 0 0 0 0 0.238095E-03 339 2 2 1 3 2 0 0 0 0 0 0.208333E-03 340 1 3 1 3 2 0 0 0 0 0 0.185185E-03 341 2 1 2 3 2 0 0 0 0 0 0.178571E-03 342 1 2 2 3 2 0 0 0 0 0 0.158730E-03 343 1 1 3 3 2 0 0 0 0 0 0.138889E-03 344 2 1 1 4 1. 0 0 0 0 0 0.148810E-03 345 1 2 1 4 2 0 0 0 0 0 0.132275E-03 346 1 1 2 4 2 0 0 0 0 0 0.115741E-03 347 1 1 1 5 2 0 0 0 0 0 0.992063E-04 348 4 1 1 1 3 0 0 0 0 0 0.277778E-03 A-6

_ - - . - - - _ - - _ _ - - - - - . _ _ _ i

- o Secuence Secuence Ntsrber I "* Drofabilitv 349 3 2 1 1 3 0 0 0 0 0 0.238095E-03 350 2 3 1 1 3 0 0 0 0 0 0.208333E-03 351 1 4 1 1 3 0 0 0 0 0 0.185185E-03 352 3 1 2 1 3- 0 0 0 0 0 0.198413E-03 353 2 2 2 1 3 0 0 0 0 0 0.173611E-03' 354 1 3 2 1 3 0 0 0 0 0 0.154321E-03 355 2 1 3 1 3 0 0 0 0 0 0.148810E-03 356 1 2 3 1 3 0 0 0 0 0 0.132275E-03 357 1 1 4 1 3 0 0 0 0 0 0.115741E-03 H' 358 3 1 1 2 3 0 0 0 0 0 0.158730E 359 2 2 1 2 3 0 0 0 0 0 0.138889E-03 360 1 3 1 2 3 0 0 0 0 0 0.123457E 33 361 2 1 2 2 3 0 0 0 0 0 0.11904BE-03 362 1 2 2 2 3 0 0 0 0 0 0.105820E-03 363 1 1 3 2 3 0 0 0 0 0 0.925926E-04 364 2 1 1 7 3 0 0 0 0 0 0.992063E-04 365 1 2 1 3 3 0 0 0 0 0 0.881834E-04 366 1 1 2 3 3 0 0 0 0 0 0.771605E-04 367 1 1 1 4 3 0 0 0 0 0 0.661376E-04 368 3 1 1 1 4 0 0 0 0 0 0.119048E-03 369 2 2 1 1 4- 0 0 0 0 0 0.104167E-03 370 1 3 1 1 4 0 0 0 0 0 0.925926E-04 371 2 1 2 1 4 0 0 0 0 0 0.892857E-04 372 1 2 2 1 4 0 0 0 0 0 0.793651E-04 373 1 1 3 1 4 0 0 0 0 0 0.694444E-04

.374 2 1 1 2 4 0 0 0 0 0 0.744048E-04 375 1 2 1 2 4 0 0 0 0 0 0.661376E-04 =

376 1 1 2 2 4 0 0 0 0 0 0.578704E-04 377 1 1 1 3 4 0 0 0 0 0 0.496032E-04 378 2 1 1 1 5 0 0 0 0 0 0.595230E-04 379 1 2 1 1 5 0 0 0 0 0 0.529101E-04 380 1 1 2 1 5 0 0 0 0 0 0.462963E-04 381 1 1 1 2 5 0 0 0 0 0 -0.396825E-04 I 382 1 1 1 1 6 0 0 0 0 0 0.330688E-04 383 7 1 1 1 0 0 0 0 0 0 0.166667E-01 384 5 2 1 1 0 0 0 0 0 0 0.125000E-01 385 5 3 1 1 0 0 0 0 0 0 0.100000E-01 386 4 4 1 1 0 0 0 0 0 0 0.833333E-02 387 3 5 1 1 0 0 0 0 0 0 0.714286E-02 l 388 2 6 1 1 0 0 0 0 0 0 0.625000E-02 389 1 7 1 1 0 0 0 0 0 0 0.555556E-02 390 6 1 2 1 0 0 0 0 0 0 0.S33333E-02 391 5 2 2 1 0 0 0 0 0 0 0.666667E-02 392 4 3 2 1 0 0 0 0 0 0 0.555556E-02 393 3 4 2 1 0 0 0 0 0 0 0.476190E-02 l 394 2 5 2 1 0 0 0 0 0 0 0.416667E-02 '

395 1 6 2 1 0 0 0 0 0 0 0.370370E-02 396 5 1 3 1 0 0 0 0 0 0 0.500000E-02 397 4 2 3 1 0 0 0 0 0 0 0.416667E-02 398 3 3 3 1 0 0 0 0 0 0 0.357143E-02 399 2 4 3 1 0 0 0 0 0 0 0.312500E-02  ;

400 1 5 3 1 0 0 0 0 0 0 0.277778E-02 1 401 4 1 4 1 0 0 0 0 0 0 0.333333E-02 ,

402 3 2 4 1 0 0 0 0 0 0 0.285714E-02 403 2 3 4 1 0 0 0 0 0 0 0.250000E-02 404 1 4 4 1 0 0 0 0 0 0 0.222222E-02 i 405 3 1 5 1 0 0 0 0 0 0 0.238095E-02 406 2 2 5 1 0 0 0 0 0 0 0.208333E-02 A-7 I i

i

. - _ _ _ _ _ . i

. , l 2

S uence Cep Fecuence kh.

407 1 3 5 1 0 0 0 0 0 0 0.195185E-02 408 2 1 6 1 0 0 0 0 0 0 0.178571E-02 409 1 2 6 1 0 0 0 0 0 0 0.158730E-02 410 1 1 7 1 0 0 0 0 0 0 0.138889E-02 411 6 1 1 2 0 0 0 0 0 0 0.416667E-02 412 5 2 1 2 0 0 0 0 0 0 0.333333E-02 413 4 3 1 2 0 0 0 0 0 0 0.277778E-02 414 3 4 1 2 0 0 0 0 0 0 0.238095E-02 415 2 5 1 2 0 0 0 0 0 0 0.208333E-02 416 1 6 1 2 0 0 0 0 0 0 0.185185E-02 417 5 1 2 2 0 0 0 0- 0 0 0.250000E-02 l t

418 4 2 2 2 0 0 0 0 0 0 0.208333E-02 419 3 3 2 2 0 0 0 0 0 0 0.178571E-02 420 2 4 2 2 0 0 0 0 0 0 0.156250E-02 421 1 5 2 2 0 0 0 0 0 0 0.138889E-02 422 4 1 3 2 0 0 0 0 0 0 0.166667E-02 423 3 2 3 2 0 0 0 0 0 0 0.142857E-02 424 2 3 3 2 0 0 0 0 0 0 0.125000E-02 425 1 4 3 2 0 0 0 0 0 0 0.111111E-02 426 3 1 4 2 0 0 0 0 0 0 0.119048E-02 427 2 2 4 2 0 0 0 0 0 0 0.104167E-02 428 1 3 4 2 0 0 0 0 0 0 0.925926E-03 429 2 1 5 2 0 0 0 0 0 0 0.892857E-03 430 1 2 5 2 0 0 0 0 0 0 0.793651E-03 431 1 1 6 2 0 0 0 0 0 0 0.694444E-03 432 5 1 1 3 0 0 0 0 0 0 0.166667E-02 433 4 2 1 3 0 0 0 0 0 0 0.138889E-02 434 3 3 1 3 0 0 0 0 0 0 0.119048E-02 435 2 4 1 3 0 0 0 0 0 0 0.104167E-02 436 1 5 1 3 0 0 0 0 0 0 0.925926E-03 437 4 1 2 3 0 0 0 0 0 0 0.111111E-02 438 3 2 2 3 0 0 0 0 0 0 0.952381E-03 439 2 3 2 3 0 0 0 0 0 0 0.833333E-03 )

440 1 4 2 3 0 0 0 0 0 0 0.740741E-03 441 3 1 3 3 0 0 0 0 0 0 0.793651E-03 442 2 2 3 3 0 0 0 0 0 0 0.694444E-03 443 1 3 3 3 0 0 0 0 0 0 0.617284E-03 444 2 1 4 3 0 0 0 0 0 0 0.595238E-03 445 1 2 4 3 0 0 0 0 0 0 0.529101E-03 446 1 1 5 3 0 0 0 0 0 0 0.462963E-03 447 4 1 1 4 0 0 0 0 0 0 0.833333E-03 448 3 2 1 4 0 0 0 0 0 0 0.714286E-03 449 2 3 1 4 0 0 0 0 0 0 0.625000E-03 450 1 4 1 4 0 0 0 0 0 0 0.555556E-03

- 451 3 1 2 4 0 0 0 0 0 0 0.595238E-03 452 2 2 2 4 0 0 0 0 0 0 0.520833E-03 453 1 3 2 1 0 0 0 0 0 0 0.462963E-03 454 2 1 3 4 0 0 0 0 0 0 0.446429E-03 455 1 2 3 4 0 0 0 0 0 0 0.396825E-03 4t6 1 1 4 4 0 0 0 0 0 0 0.347222E-03 457 3 1 1 5 0 0 0 0 0 0 0.476190E-03 458 2 2 1 5 0 0 0 0 0 0 0.416667E-03 459 1 3 1 5 0 0 0 0 0 0 0.3703700-03 460 2 1 2 5 0 0 0 0 0 0 0.357143E-03 461 1 2 2 5 0 0 0 0 0 0 0.317460E-03 462 1 1 3 5 0 0 0 0 0 0 0.277778E-03 463 2 1 1 6 0 0 0 0 0 0 0.297619E-03 464 1 2 1 6 0 0 0 0 0 0 0.264550E-03 A-8

7 t

.,i O ., 7 Secuence Secuence Nster #P 'e"' Drofabilitv L 465~ 1 1- 2' 6 0 0 0 0- 0 0 0.231481E 466 1 1 1 7 0 0 0 0 0 0 0.198413E-03 467 8. 1 1 0 0 0 0 0 0 0 0.500000E-01 i 468 7 2 .1 0 0 0 0 0 O' O 0.333333E-01 469- 6 3 1 0 0 0 0 0- ~0 0 0.250000E-01 470 5 4 1 0 0 0 0 0 0 0 0.200000E-01 471- 4 5 1 0 0 0 0 0 0 0 0.166667E-01 472 3 6 1 0- 0 0 0 0 0 0 0.142857E-01

( 473 2 7 1 0 0 0 0 0 0 0- 0.125000E-01 L

474 1 '8 1 0- 0 0 0 0 0 0 0.111111E-01 475 7- 1 2 0 0 0 0 0 0 0 0.166667E-01 476 6 2 2 0 0 0 0 0 0 0 0.125000E-01 477 5 3 2 0 0 0 0 0 0 0 0.100000E-01 478. 4 4 2 0 0 0 0. 0 0 0 0.833333E-02 479 3 5 2- 0 0 0 0 'O O' O 0.714286E-02

'480 2 '6 2 0. 0 0 0 0 0 0 0.625000E-02 j 481 1 7 2 0- 0 0 0 0 'O O' O.555556E-02 '

482 6 1 3 0 0 0 0 0 0 0 0.833333E-02 1 483 5 2 3 0 0 0 0 0 0 0 0.666667E-02 1 484 4 3 3 0 0 0 0 0 0 'O 0.555556E-02 485 3 4 3 0 0 0 0 0- 0 0 0.476190E-02 486 '2 5 3 0 0 0 0 0 0 0 0.416667E-02 487- 1 6 3 0 0 0 0 0 0 0 0.370370E 488 5 1 4 0 0 0 0 0 0 0 0.500000E-02 489 4 .2 4- 0' O O O O 'O O 0.416667E-02 490 3 3 4 0 0 0 0 0 0' O 0.357143E-02 491 2. 4 4 0 0 0 'O O O O 0.312500E-02 492 1 5 4 0 0 0 0 0 'O O 0.277778E-02 493 4 1 5 -0 0 0 0 0 0 0 0.333333E 494 3 2 5 0 0 0 0 0 0 0- 0.285714E-02 495 2- 3 5 0 0 0 0 0 0 0 0.250000E-02 496 1 4 5 0 0 0 0 0 0 0 0.222222E-02 497 3 1 6 0 0 0 0 .0 0- 0 0.238095E-02 498 2 2 6 0 0 0 0 0 0 0 0.208333E-02:

499 1 3 6 0 0 0 0 0 0 0 0.185185E-02 500 2 1 7 0 0 0 0 0 0 0 0.178571E-02 501 1 2 7 0 0 0 0 0 0 0 0.158730E-02 502 1 1 8 0 0 0 0 0 0 0 0.138889E-02 503 9 1 0 0 =0 0 0 0 0 0 0.100000E+00 504 8 2 0 0 0 0 0 0 0 0 0.500000E-01 505- 7 3 0 0 0 0 0 0 0 0 0.333333E-01 506 '6 4 0 0 0 0 0 0 0 0 0.250000E-01

(

507' 5 5 0 0 0 0 0 0 0 0 0.200000E-01 508 4 6 0 0 0 0 0 0 0 0 0.166667E-01 L 509 3 7 0 0 0 0 0 0 0 0 0.142857E-01 510 2 8 0 0 0 0 0 0 0 0 0.125000E-01 511 1 9 0 0 0 0 0 0 0 0 0.111111E-01 512 10 0 0 0 0 0 0 0 0 0 0.100000E+00 l

A-9 l t - - _ - - - - _ _ - - _ - -

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