I N T E R N A L D O C U M E N T I Z
I
SELECTED DIRECTIONAL WAVE SPECTRA
FOR USE IN THE ASSESSMENT OF
WAVE ENERGY CONVERTOR PERFORMANCE
Internal Document 131
J A CRABB
[This document should not be cited in a published bibliography, and is
supplied for the use of the recipient only].
INSTITUTE OF OCEANOGRAPHIC SCIENCES
Wormley, Godalming,
Surrey GU8 5UB
(042-879-4141)
(Director: Dr. A. S. Laughton)
Bidston Observatory,
Birkenhead,
Merseyside L43 7RA
(051-653-8633)
(Assistant Director: Dr. D. E. Cartwright)
Crossway,
Taunton,
Somerset TA1 2DW
(0823-86211)
SELECTED DIRECTIONAL WAVE SPECTRA
FOR USE IN THE ASSESSMENT OF
WAVE ENERGY CONVERTOR PERFORMANCE
Internal Document 131
J A CRABB
May 1981
This document should not be cited in
any other paper or report except as
'personal communication' and it is for
the use of the recipient only.
Institute of Oceanographic Sciences
Crossway
INTRODUCTION
In response to requests for a small number of directional wave spectra
to be offered for use in device tank test programmes, an attempt has
been made to select a smaller subset from the 399 South Uist synthesized
directional spectra. (WESC (79) DA90, WESC (80)
DA 111).
To this end, five parameters summarizing the main properties of each of
the 399 were calculated. It was found that the individual parameters
covered a wide range of values and combined in individual spectra to
produce a wide diversity of spectral types. It has consequently proved
impossible to derive a significantly smaller set which adequately covers
the range of each of the five parameters in realistics combination with
each of the other four.
Since this direct attempt to reproduce the statistics of the set of 399
in a more manageable form was not successful two further approaches,
which represent compromises on the original intention, were pursued.
These have resulted in two overlapping subsets of approximately 40
spectra each.
THE DESCRIPTIVE PARAMETERS
The parameters by which each spectrum is described were chosen for
their simplicity and ease of interpretation, they are described below;
Energy Period
(TE)
Defined as the ratio
/Mo, where
is
the nth moment of the one dimensional variance
spectrum E(f)
Mn =
^2 r
:2 r
f". E(f). df
f \
•1 J
f^ = 0.0444 Hz, fg = 0
.6401 Hz
Power (P)
total intergrated power between f^ and
calculated according to the full (depth
Frequency Width (FW)
the frequency interval within which 80%
of the power is found; ie excludes the
two 10% portions of the power at the highest
and lowest frequencies
Direction Width (DW)
the angular interval within which 80%
of the power in the 80% frequency interval
is found; ie excludes the two 10% portions
of the power found in the angular intervals
immediately North and South of due East (90°)
Peak Direction (DP)
the direction associated with the most
powerful spectral component.
CLASSIFICATION OF SPECTRA-GENERAL
Values of each of the five parameters were calculated for each spectrum
and the spectra were sorted into classes according to the values of the
three parameters DW, TE and FW. Within each of these classes the spectra
were subdivided into classes of power. The spectra were not further
subdivided by DP.
At this point it was apparent that the range of spectral types was too
great to be adequately represented in a subset of some 40 spectra. Even
by effectively excluding one of the parameters (DP) and using moderately
broad class widths for the remainder, some 165 occupied classes resulted
requiring a minimum of one spectrum to represent each.
The only practical way round this difficulty appeared to lie in setting
a number of limited objectives and attempting to select spectra to
satisfy these separately. The objectives defined were:
1. To produce a set of approximately 40 spectra covering as wide a
range as possible of the three parameters DW, TE and FW,whilst deliberately
restricting the ranges of P and DP as described later.
2. To produce a set of approximately 40 spectra covering as wide a
range as possible of the four parameters DW, TE, FW and P associated
with those spectra which contribute the bulk of the energy arriving
The process whereby these spectra were selected is detailed in the
following section and further amplified in the appendix.
It is hoped that the first set will allow device performance figures
already established as functions of the non—directional parameters
Hs and TE to be extended to encompass a realistic range of spectral
'shapes' in both frequency and direction, and that the second set will
allow a direct estimate of the annual productivity of each device
to be made.
It has proved possible, by making the necessary compromises, to arrange
a substantial overlap between the two sets, enabling both objectives
to be realized with a total of 63 spectra.
CLASSIFICATION OF SPECTRA-DETAILED
SET 1
The 399 spectra were sorted according to the values of the three chosen
parameters into the following classes:
DW - four classes
CLASS NO
1
2
3
4
DEGREES
30
60
90
>120
FIV - four classes
CLASS NO
1
2
3
4
Hz
<0.0294
0.0295 -
0.0588 -
>0.0882
0.0587
0.0881
TE - five classes
CLASS NO
1
2
3
4
5
For each range of DW all those spectra jointly occupying a given class
of FW and TE were listed along with the values of P and DP associated
with each. The spectra so listed are the occupants of one cell of a
frequency histogram in the three dimensions DW, FW and TE. The average
power of all the spectra in each occupied cell was calculated. One
spectrum was then selected to represent each cell, subject to the
additional constraints that
1. it should have a DP values of either 240° or 270° (75% of all
the spectra fall in this range)
2. it should have a power close to the mean power for the cell.
A total of 38 spectra resulted from this procedure. The weight to be
attached to each is determined by the population of the cell which it
represents.
The three dimensional histogram is set out in Table 1. This presentation
is expanded in Table 2, where the occupants of each of the 38 classes
are listed by serial number with the values of each of the five parameters.
The classes are numbered in the order in which they are encountered,
reading left to right and down the page, in Table 1. The spectra selected
for both Set 1 and Set 2 are underlined.
The spectra of Set 1 are listed separately by serial number in Table 3 along
with their relative
weights.
SET 2
Each cell of the DW, TE, FW histogram was further subdivided into classes
of power 10 kW/m wide; as previously mentioned this resulted in a total
of 165 occupied classes. This number was reduced to 107 by regrouping
the classes as follows:
Power - nine classes
CLASS NO
1
2
3
4
5
6
7
8
9
A further reduction was effected by restricting consideration to those
conditions under which the majority of the total annual energy is
transported to the site. The distribution of total energy with Hs and
TE, Figure 1, marked with approximate power contours, was inspected
and those sea states which contribute relatively little to the total
energy were identified and excluded.
The following categories of sea state are consequently not represented
in Set 2 (the percentage of the total annual energy thereby excluded
is marked against each category).
Excluded classes are those with:
Power
<
10 kW/m
(excludes 2.4% of total energy)
Power
>
300 kW/m
(
"
8.5% "
"
" )
TE
<
7 seconds
(
"
0.7% "
"
" )
TE
>
12.5 seconds
(
"
0.8% "
"
" )
as well as spectra with unusual combinations of P, FW, DW and TE
(ie classes in the four dimensional histogram occupied by one spectrum
only). A further 11.1% of the total energy was associated with such
spectra.
By this means it was possible to reduce the number of occupied classes
to 46. The spectrum selected to represent each had a power as close as
possible to the mean power of the class and a DP value of either
240° or 270°. The 46 spectra selected represent 267 of the original
399 synthesized spectra and, as shown above, these spectra account
for 76.5% of the total energy in the set and thus, by projection,
of the total energy arriving at the site. When each of the 46 spectra
is weighed according to the number in the class which it represents,
the set has an average power of 55.2 kW/m.
It is envisaged that the use of this set will allow the annual
productivity of a device to be estimated. The weighted average power
output of a device run against this set expressed as a fraction of
the 55.2 kW/m available, is a direct estimate of the device efficiency
of the total annual energy represented may be retrieved. The ability
of the device to capture power in those conditions excluded from the set
and which account for the remaining 23.5% of the annual energy must
be estimated separately. This may be effected by considering the device
performance as established against Sets 1 and 2 in conjunction with the
statistics of the excluded sea states presented in Table 4.
The spectra of Set 2 are listed by serial number and relative weight in
Table 5.
CONCLUSION
The starting point for the present work was the set of 399 directional
wave spectra which are themselves estimates of the probable directional
wave conditions at South Uist. It was originally intended that these
spectra would serve in the early stages of the Wave Energy Programme
in view of the lack of any other more reliable data. It had been
expected that they would, sooner rather than later, be superseded
by measured directional data. There is still no immediate prospect of
this occurring and it appears probable that a crucial evaluation of
individual devices will be undertaken on the basis of the spectra
described here. There must be reservations about proceding on this
basis.
Given, however, that there is no other reasonable way forward it is
encouraging to note that in those respects where it has been possible to
test the representative nature of the 399, no serious shortcoming has
come to light (WESC (80) DA101)(WESC (80) DA105). Furthermore, although
the 399 were seen as a temporary expedient, no concious compromise
on precision was made in the method of their synthesis.
Definite compromises have however been made in the attempts, described
here, to further condense the information which they contain. The results
presented here have been produced in response to strong pressures arising
solely out of practical considerations, and their presentation does not
imply that the estimated range of wave conditions at South Uist is sufficiently
Whilst the spectra listed here have been selected by reasonable and
well-defined criteria, and as such cover a fairly wide range of
conditions against which it is reasonable to check device performance
-particularly for comparative purposes - no attempt has been made to
cover those conditions which might result in extreme responses from
particular devices. The systematic investigation of device performance
in 'extreme' conditions must be outside this test set, and it should be
borne in mind that the 399 themselves cannot cover the whole range
APPENDIX
The 399 spectra of the selected set are taken to be representative
of the 2920 spectra which might be recorded in an average year.
Each spectrum of the selected set therefore represents approximately 7
spectra in the hypothetical whole year set or, alternatively, each
spectrum is representative of conditions which would be experienced
for V 3 9 9 of the year, ie 21.95 hours.
The distribution of the selected set properties is thus a coarser
representation of the supposed annual distribution.
If the ith spectrum has a power Pi, then the average power of the
selected set is.
R
= L: I
a
311
314
(1)
The result of this calculation is 47.8 kW/m and this is taken to be
the mean power which would be measured over the average year.
The total energy arriving at the site per metre of wavefront is
therefore estimated as
E^ = 47.8 X 365 X 24
= 418,728 kWh/m
(2)
Now consider the selection of a smaller number of spectra (Set 2)
for the purpose of estimating device productivity. As explained
in the text a number of spectra were excluded at the outset leaving
267 which then represent the range of conditions supposed to occur
for ^^^/399
of the year. The average power of this set
267
P - 1 , - 1
I z
i
R
Zb7
2 6 7
was 54.5 kW/m. The total energy in one year associated with such
conditions is then
Ep = 54.5 X 267 ^ 365 * 24
399
= 319,476 kWh/m
(4)
= 0.763 X
(5)
As previously described the
267 spectra were divided into classes
according to the values of DW, TE, FW and P associated with each.
One spectrum was chosen to represent the
spectra in the jth class
The mean power of the spectra in the jth class is
2 . ^
0
I T
where
P t , j
is the power of the Lth spectrum in the jth c l a s s .
The chosen spectrum has a power, Pj, as close as possible to
A total of 46 classes were represented in this way.
The weighted average power of the set of 46 (Set 2) is
P - ^ Pj ^ "J ^ j^.
(7)
using (6) and (3)
R
—
J^i
z
=
S'4-S"kW/m
J-'
It is envisaged that the output power of a device in all 46 selected
spectra will be determined. If the output power for the jth spectrum
is Poj, the weighted average output power for the set is
4-6
a
£ R
J='
oj ^ ry
44
Hi
'J
J " '
and the overall efficiency of the device in this range of conditions is
Po
P„
The productivity of the device during the ^^^/399 of the year in
which these conditions prevail is thus estimated to be
Eo = ^
X 0.763 X
kWh/m
This is one element of the final productivity figure. The productivity
of a device under conditions excluded from the set needs to be determined
separately and the resulting energy added to Eo. Approximately half
of the excluded power has, however, been excluded on the grounds of
being associated with very high or very low power sea states, and the rest
of the excluded power is associated with a wide range of spectral
types. It may thus, as a first approximation, be permissible to assume
that the device efficiency under these conditions is substantially
the same as that established for Set 2, and that the annual productivity
is simply
CO
JZ
15
14
13 H
12
1 1 —
1 0
-9 —
8 —
1
6
5
4 —
3
-2 —
1 —
0
3 9 9 U A L I D O B S E R U A T I O N S
T O T A L ENERGY (KUH/M) = 5 0 6 6 6 .
20 19
12 12
12 19 21 11 12 12 10
18 16 n 11 15 12 15
300fth//,T|
10 kw/m
0
I 1 I 1 I
1
2
3
M
' 1 I 1
I 1 ' I ' I I I 1 I ' 1 I I ' I 1
6
1
8
9
10
11
12
13
14
15
16
11
18
19
20
' I ' I ' I
T E
( S )
DISTRIBUTION OF TOTAL MEASURED WAVE ENERGY
WITH
Hs
AND T
E (PPT)
FW
CLASS NUMBER
TE
1
2
3
4
pi
w
1
3
1
g
2
3
15
4
8
7
4
O]
CO
§
4
5
9
FW
CLASS NUMBER
TE
1
2
3
4
ptS
w
1
2
28
2
41
2
5
a
3
56
12
1
w
i
4
5
30
18
2
FW
CLASS NUMBER
TE
FW
1
2
3
4
n
1
2
12
2
15
2
2
:z: 3
20
6
w
(C
a
4
5
18
2
FW
CLASS NUMBER
TE
1
2
3
4
1
1
1
1
2
1
2
5
26
4
%
3
20
4
CO
i
4
8
CO
i
5
1
DW CLASS 1
DW CLASS 2
DW CLASS 3
DW CLASS 4
Distribution of the 399 synthesized directional spectra with
the three parameters DW, FW and TE.
Numbers tabulated are total number of spectra in each class.
CLASS N O .
FW TE DW D M A X P O W E R SPEC
( H z ) (s lecs) ( d e g s ) ( d e g s ) ( k W / m ) N O .
0. 0 5 8 6 5 8 7 0 0 30. 270. 0. 1 8 4 8 0 E 01 28.
0, 0 4 8 8 5. 1 6 0 0 30. 270. 0. 2 0 0 2 0 E 01 29.
0. 0 4 8 8 6, 0 2 0 0 30. 240. 0. 9 9 8 9 0 E 01 143.
0. 0 6 8 4 5. 5 0 0 0 30. 240.. 0. 3 3 0 2 0 E 01 82.
0 0 2 9 3 7. 9 5 0 0 30. 270. 0. 1 1 9 2 0 E 0 2 100.
0. 0 2 9 3 7. 1 6 0 0 30. 240, 0. 1 2 4 5 0 E 0 2 122.
0. 0 2 9 3 7. 3 0 0 0 30. 330. 0. 2 2 0 5 0 E 0 2 205.
0. 0 2 9 3 8. 0 0 0 0 30. 2 4 a 0. 2 7 2 lOE 0 2 258.
0. 0 4 8 8 7. 7 6 0 0 30. 270. 0. 1 1 1 9 0 E 01 10.
0 0391 6. 6 3 0 0 30. 270. 0. 1 8 2 7 0 E 01 13.
0. 0391 7. 2 8 0 0 30. 270. 0. 5 0 6 0 0 E 01 55.
0. 0391 7 6 1 0 0 30. 270. 0. 8 1 8 9 0 E 01 63.
0. 0 5 8 6 6. 7 0 0 0 30. 2 4 0 0. l b 9 8 0 E 0 2 138
0. 0391 6 5 6 0 0 30. 240. 0. 1 1 6 7 0 E 0 2 139.
0. 0 4 8 8 6. 1400 30. 240. 0. 1 0 5 7 0 E 0 2 142.
0. 0 6 8 4 7. 8 7 0 0 30. 240. 0. 1 3 8 4 0 E 01 6.
0. 0 6 8 4 7. 0 1 0 0 30. 240. 0. 3 5 2 4 0 E 01 14.
0, 0 6 8 4 6. 8 7 0 0 30. 240. 0. 2 1 4 3 0 E 01 16.
0. 0781 6 0 5 0 0 30. 240. 0. 5 9 9 6 0 E 01 66.
0. 0 2 9 3 9. 6 0 0 0 30. 270. 0. 5 9 7 lOE 01 57.
0. 0 1 9 5 9. 7 8 0 0 30. 270. 0. 1 6 8 7 0 E 0 2 91
0. 0 2 9 3 9. 0 6 0 0 30. 270. 0. 1 2 6 0 0 E 0 2 99.
0. 0 1 9 5 8. 2 5 0 0 30. 270. 0. 1 9 1 6 0 E 0 2 177.
0. 0 2 9 3 8, 5 0 0 0 30. 330. 0. 2 5 7 l O E 0 2 175
0. 0 2 9 3 8. 3 9 0 0 30. 240. 0. 2.3630E 0 2 184.
0. 0 2 9 3 9. 4 1 0 0 30. 240. 0. 2 1 4 1 0 E 0 2 195.
0, 0 2 9 3 8. 3 5 0 0 30. 270. 0. 3 6 6 4 0 E 0 2 228.
0. 0 1 9 5 9. 2 2 0 0 30. 270. 0. 3 6 1 6 0 E 0 2 229.
0. 0 2 9 3 8. 8 7 0 0 30. 240. 0. 4 8 9 2 0 E 0 2 304.
0. 0 1 9 5 9. 6 4 0 0 30. 240. 0 6 5 0 4 0 E 0 2 297.
0. 0 1 9 5 8. 6 7 0 0 30. 270. 0. 3 5 1 5 0 E 0 2 353,
0. 0 2 9 3 9. 3 0 0 0 30. 330. 0. 1 0 9 8 0 E 0 3 365.
0. 0 1 9 5 9. 7 1 0 0 30. 240. 0. 1 1 3 4 0 E 0 3 366.
0. 0 2 9 3 9. 8 3 0 0 30. 240. 0. 1 3 4 0 0 E 0 3 368.
0 0 3 9 1 9. 5 9 0 0 30. 240. 0. 1 7 0 4 0 E 0 2 109.
0. 0 4 8 8 8. 3 0 0 0 30. 330. 0. 1 7 4 6 0 E 0 2 115.
0. 0 3 9 1 8. 5 9 0 0 30. 270. 0. 2 5 9 2 0 E 0 2 161.
0. 0 3 9 1 8. 6 3 0 0 30. 240. 0. 2 3 3 9 0 E 0 2 163.
0. 0 3 9 1 8. 0 5 0 0 30. 270. 0. 2 6 3 3 0 E 0 2 183.
0. 0 3 9 1 8. 9 5 0 0 30. 330. 0. 2 1 0 2 0 E 0 2 186.
0. 0 3 9 1 8. 1 6 0 0 30. 270. 0 . 2 0 6 4 0 E 0 2 192.
0. 0391 9. 1 7 0 0 30. 330. 0. 6 5 6 5 0 E 0 2 328.
CLASS A V G E P O W E R
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0. 3 3 0 2 0 E 01
0. 1 8 4 0 S E 0 2
0, 7 0 5 9 3 E 01
0. 3 2 6 1 7 E 01
0. 5 0 2 9 7 E 0 2
0. 2 7 1 8 1 E 0 2
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CLASS N O .
12
1 3
FW IE DW D H A X P O W E R SPEC
(Hz) ( s e e s ) ( d e g s ) ( d e g s ) ( k W / m ) N O .
0, 0 5 8 6 7. 7 6 0 0 60. 270. 0. 2 7 2 0 0 E 01 15,
0. 0 3 9 1 8. 0 3 0 0 60. 300. 0, 6 6 1 4 0 E 01 35.
0. 0 3 9 1 7. 6 4 0 0 60. 240. 0, 6 1 9 3 0 E 01 40.
0. 0 4 8 8 6. 8 8 0 0 60. 210. 0, 4 2 8 5 0 E 01 46.
0. 0 3 9 1 7. 2 1 0 0 60. 210. 0, 6 7 4 7 0 E 01 48.
0. 0 3 9 1 6. 9 0 0 0 60. 270. 0, 5 8 7 l O E 01 54.
0. 0 4 8 8 7. 7 5 0 0 60. 240. 0, 841 lOE 01 56.
0. 0 3 9 1 7. 5 5 0 0 60. 270. 0 5 8 0 4 0 E 01 58.
0. 0 4 8 8 6. 7 0 0 0 60. 240. 0, 7 0 5 9 0 E 01 68.
0. 0 3 9 1 7. 9 2 0 0 60. 270. 0. 6 8 8 9 0 E 01 69.
0. 0 4 8 8 6 5 0 0 0 60. 270. 0. 8 6 1 4 0 E 01 145.
0. 0 3 9 1 7. 9 8 0 0 60. 240. 0. 1 6 8 5 0 E 0 2 110.
0. 0391 7. 9 2 0 0 60. 270. 0. 1 5 5 7 0 E 0 2 111.
0. 0 4 8 8 7. 4 0 0 0 60. 240. 0. 1 3 2 1 0 E 0 2 114.
0. 0 5 8 6 7. 2 6 0 0 6 0 270. 0. 1 4 8 0 0 E 0 2 126.
0. 0 5 8 6 6. 3 0 0 0 6 0 270. 0. 1 2 6 7 0 E 0 2 129.
0. 0 3 9 1 7. 0 2 0 0 60. 240. 0. 1 1 7 6 0 E 0 2 136.
0. 0 3 9 1 6. 9 2 0 0 60. 240. 0. 1 3 3 5 0 E 0 2 140.
0. 0 4 8 8 6 7 7 0 0 60. 240. 0. 1 0 8 9 0 E 0 2 144.
0. 0 4 8 8 7. 6 5 0 0 60. 240. 0. 1 7 6 7 0 E 0 2 194.
0 0 4 8 8 7. 4 5 0 0 60. 240. 0. 1 7 9 1 0 E 0 2 199.
0. 0391 6. 6 0 0 0 60. 180. 0. 1 7 7 7 0 E 0 2 209.
0. 0 4 8 8 6. 8 9 0 0 6 0 270. 0. 1 5 6 5 0 E 0 2 213.
0. 0 5 8 6 7. 2 7 0 0 60. 270. 0. 2 0 8 4 0 E 0 2 201
0 0 3 9 1 7. 7 8 0 0 6 0 2 4 0 0. 2 1 0 2 0 E 0 2 206.
0. 0 3 9 1 7, 2 2 0 0 6 0 270. 0. 2 2 8 8 0 E 0 2 208.
0. 0 3 9 1 7. 3 0 0 0 60. 3 3 0 0. 2 5 8 0 0 E 0 2 257.
0. 0 3 9 1 7. 4 8 0 0 60. 270. 0. 2 9 4 6 0 E 0 2 .259.
0. 0 4 8 8 7. 7 2 0 0 60. 270. 0. 2 9 1 2 0 E 0 2 260.
0. 0391 7. 1 0 0 0 6 0 240. 0. 2 4 4 9 0 E 0 2 261.
0. 0 4 8 8 7. 4 0 0 0 60. 270. 0. 2 7 3 8 0 E 0 2 2 7 5
0. 0 3 9 1 7. 1500 60. 270. 0. 2 6 0 lOE 0 2 283.
0. 0 3 9 1 7. 6 2 0 0 60. 240. 0. 3 0 0 6 0 E 0 2 2 6 3
0. 0 3 9 1 7. 6 9 0 0 60. 270. 0. 3 0 9 3 0 E 0 2 265.
0 0 4 8 8 7. 3 0 0 0 60. 300. 0. 3 6 7 3 0 E 0 2 320.
0. 0 3 9 1 7, 8 6 0 0 60. 240. 0. 4 9 5 7 0 E 0 2 311.
0, 0391 7. 6 0 0 0 60, 240. 0, 4 8 7 8 0 E 0 2 312.
0. 0 3 9 1 7. 7 5 0 0 60, 300. 0, 4 8 8 0 0 E 0 2 314.
0. 0 3 9 1 7. 6 4 0 0 60, 330. 0, 4 5 6 0 0 E 0 2 315.
0. 0 5 8 6 7. 1 1 0 0 60, 270. 0, 4 0 2 3 0 E 0 2 319.
0. 0 3 9 1 7. 7 9 0 0 60, 240. 6, 6 1 3 8 0 ^
oi
330.0. 0 6 8 4 6. 4 5 0 0 60. 270. 0, 6 1 3 9 0 E 0 0 4.
0. 0 6 8 4 6. 0 5 0 0 60. 270, 0. 1 1 9 0 0 E 0 2 147.
0. 0 6 8 4 6. 6 1 0 0 60. 300. 0. 1 5 0 0 0 E 0 2 214,
0. 0 6 8 4 6. 9 1 0 0 60. 270, 0, 2 9 4 7 0 E 0 2 277.
0. 0 8 7 9 6. 9 7 0 0 60. 240. 0, 2 2 8 6 0 E 0 2 278.
CLASS A V G E POWER
0. 2 1 1 3 1 E 0 2
0. 1 5 9 6 9 E 02
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p p p p
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w s
m m
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w w w w
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o o o o o o o o o o
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*O^WV)K)K)xlUIN)OC004»
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o o o o o o o o o o o o o
o o p p p p p p p p p p p
W M N N N W N N N N W W K )
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p ^0 p m00
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w SI
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sjo o o o o o o o o o o o o o o o o g o
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W ^ ^ W W H ^ W ^ ^ W ^ W W W ^ ^ W ^ W W W N i ^ O W N * ^ ^
%0 --.O •••0 "O ' O -O ^0 ••0 -O •'O ^0 ^ >0 ^ "O >0 >0 >0 >0 ^0 >0 >0
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o o o o o o o o o o o o o o o o o o o o o o o o o
o o o o o o o o o o o o o o o o o o o o o o o o o
w w
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w w
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o o o o
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o
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o o o o o
w w w w w
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m mm
O O O O O O O O O
H» I-*
CLASS N O .
15
16
17
18
FW TE DW D H A X P O W E R SPEC
( H z ) (B e c s ) ( d e g s ) (degs ) ( k W / m ) N O .
0. 0 3 9 1 9. 4 6 0 0 60. 270. 0. 5 5 5 3 0 E 0 0 2.
0. 0 4 8 8 8. 1 4 0 0 60. 240. 0. 7 2 4 0 0 E 01 33.
0. 0 3 9 1 9. 0 6 0 0 60. 240. 0. 9 6 0 1 0 E 01 42.
0. 0 4 8 8 8. 2 5 0 0 60. 240. 0. 6 0 3 9 0 E 01 72.
0. 0391 9. 9 3 0 0 60. 270. 0. 1 3 4 8 0 E 0 2 93.
0. 0 4 8 8 8. 6 9 0 0 6 0 270. 0. 1 2 9 8 0 E 0 2 103.
0. 0 5 8 6 8. 0 7 0 0 6 0 2 4 0 0. 1 4 8 1 0 E 0 2 108.
0. 0 4 8 8 8 4 3 0 0 6 0 2 4 0 0. 2 9 4 lOE 0 2 240.
0. 0391 8. 4 1 0 0 60. 270. 0, 3 7 3 4 0 E 0 2 249.
0. 0391 8. 4 7 0 0 6 0 2 4 0 0, 3 1 9 1 0 E 0 2 250.
0. 0 3 9 1 8 4 5 0 0 60. 240. 0, 4 1 5 4 0 E 0 2 243.
0. 0 3 9 1 8. 4 6 0 0 60. 2 4 0 0, 6 9 0 0 0 E 0 2 327.
0. 0 6 8 4 S. 0 5 0 0 60, . 240. 0, 3 9 4 2 0 E 01 7.
0. 0 1 9 5 10. 2 8 0 0 60. 270, 0, 1 2 2 7 0 E 0 2 31
0. 0 2 9 3 10. 2 4 0 0 6 0 210. 0, 1 1 4 7 0 E 0 2 45,
0 0 2 9 3 10. 1 5 0 0 60. 210, 0, 2 2 8 2 0 E 0 2 106
0 0 1 9 5 11. 3 1 0 0 60. 270, 0, 2 7 2 4 0 E 0 2 150,
0. 0 1 9 5 to. 2 6 0 0 6 0 240, 0, 2 4 3 9 0 E 0 2 ..JJA-,
0. 0 2 9 3 11. 0 9 0 0 60. 210, 0 2 6 1 3 0 E 0 2 164,
0 0 2 9 3 10. 6 0 0 0 60. 270, 0, 2 6 9 5 0 E 0 2 172,
0. 0 1 9 5 10 7 3 0 0 60. 270. 0, 2 7 3 9 0 E 0 2 197.
0. 0 2 9 3 10. 2 9 0 0 6 0 270, 0, 3 2 1 5 0 E 0 2 165.
0 0 1 9 5 11. 4 6 0 0 60. 270, 0, 3 1 8 6 0 E 0 2 167.
.0. 0 1 9 5 10. 1 7 0 0 6 0 2 7 0 0, 3 9 8 0 0 E 0 2 223,
0 0 1 9 5 10. 1900 60. 210. 0, 3 8 2 7 0 E 0 2 236,
0. 0 0 9 8 10. 8 3 0 0 6 0 270, 0, 4 4 9 7 0 E 0 2 222,
0. 0 1 9 5 11. 2 1 0 0 60. 270, 0. 5 4 4 3 0 E 0 2 220.
0. 0 1 9 5 11. 1200 60. 240, 0. 5 0 4 3 0 E 0 2 232.
0. 0 1 9 5 10. 8 5 0 0 60. 240, 0, 5 7 1 2 0 E 0 2 303,
0. 0 1 9 5 10. 2 6 0 0 60. 270, 0, 5 1 8 7 0 E 0 2 309,
0, 0 1 9 5 11. 0 3 0 0 6 0 270, 0. 7 6 3 9 0 E 0 2 289,
0. 0 2 9 3 11. 8 2 0 0 6 0 270, 0, 8 5 0 2 0 E 0 2 321.
0, 0 2 9 3 10. 3 6 0 0 60. 240, 0. 8 0 6 8 0 E 0 2 324.
0. 0 1 9 5 11, 9 0 0 0 6 0 270. 0. 9 5 2 8 0 E 0 2 322,
0. 0 0 9 8 10. 0 8 0 0 6 0 240. 0. 9 3 5 8 0 E 0 2 341,
0. 0 1 9 5 10. 0 8 0 0 60. 300. 0. 9 6 4 0 0 E 0 2 3 4 i
0. 0 1 9 5 10. 5 4 0 0 60. 240. 0. 1 0 8 6 0 E 0 3 339.
0. 0 1 9 5 11. 1 4 0 0 60. 270. 0, 1 1 9 6 0 E 0 3 338.
0. 0 2 9 3 10. 1 1 0 0 60. 240. 0, 1 1 1 9 0 E 0 3 340.
0. 0 2 9 3 10. 7 4 0 0 60. 300. 0. 1 1 4 9 0 E 0 3 343.
0. 0 2 9 3 11. 7 7 0 0 6 0 270. 0, 1 9 3 0 0 E 0 3 371.
0. 0 2 9 3 10. 3 4 0 0 60. 240. 0. 1 9 6 8 0 E 0 3 386.
0. 0 2 9 3 10. 9 4 0 0 60. 240. 0. 2 8 0 6 0 E 0 3 393,
0. 0 3 9 1 10 8 9 0 0 60. 240. 0. 2 7 5 4 0 E 0 2 152.
0. 0391 10. 8 4 0 0 60. 270. 0. 1 3 5 4 0 E 0 3 364.
CLASS A V G E POWER
0. 2 2 8 2 5 E 0 2
0. 3 9 4 2 0 E 01
0. 7 4 4 lOE 0 2
0. 8 1 4 7 0 E 0 2
CLASS N O .
1 9
2 0
21
22
2 3
FW TE DW D M A X P O W E R SPEC
(Hz) ( s e e s ) ( d e g s ) ( d e g s ) ( k W / m ) N O .
0. 0 0 9 8 12, 4 2 0 0 60. 270. 0. 1 6 6 1 0 E 01 1.
0. 0 1 9 5 12. 9 8 0 0 60. 270. 0. 2 8 4 7 0 E 0 2 87.
0. 0 1 9 5
12.
4 2 0 0 60. 270. 0. 3 4 6 8 0 E 0 2 148.0, 0 1 9 5 12. 1 9 0 0 60. 270. 0. 40.1 O O E 0 2 149.
0. 0 1 9 5 13. 0 0 0 0 60. 270. 0. 4 8 4 3 0 E 0 2 235.
0. 0 1 9 5 12. 4 7 0 0 60. 270. 0. 4 6 2 8 0 E 0 2 242.
0. 0 1 9 5 14. 0 2 0 0 60. 270. 0. 5 § 9 7 b E 0 2
0. 0 1 9 5 13. 3 2 0 0 60. 270. 0. 6 6 6 8 0 E 0 2 219.
0. 0 0 9 8 12 5 4 0 0 60. 270. 0. 7 7 0 6 0 E 0 2 290.
0. 0 1 9 5 12 3 7 0 0 60. 270. 0. 7 0 8 2 0 E 0 2 295.
0. 0 1 9 5 12. 3 1 0 0 60, 270. 0. 8 3 6 9 0 E 0 2 286.
0. 0 1 9 5 13. 7 5 0 0 60. 270. 0. S 6 0 3 0 E 0 2 287.
0. 0 1 9 5
12.
6 4 0 0 60, 270. 0. 8 2 9 5 0 E 0 2 291.0. 0 2 9 3 12. 0 9 0 0 6 0 240. 0. 9 1 0 8 0 E 0 2 323,
0. 0 1 9 5 12. 4 2 0 0 60, 240. 0. 1 1 5 3 0 E 0 3 335,
0. 0 2 9 3
12.
1 2 0 0 6 0 270. 0. 13460E 0 3 336,0. 0 1 9 5
12.
4 3 0 0 60, 300. 0. 1 5 2 8 0 E 0 3 358,0. 0 0 9 3 15. 3 7 0 0 6 0 240. 0. 2 0 3 2 0 E 0 3 356,
0. 0 5 8 6 5. 5 7 0 0 90. 210. 0. 2 7 0 0 0 E 01 2 6
0. 0 4 8 8 5. 9 8 0 0 90. 300. 0 6 5 3 l O E 01 70,
0 0 9 7 7 4. 4 4 0 0 90. 210. 0, 1 6 0 0 0 E 01 30,
0 1 1 7 2 4. 4 2 0 0 9 0 210. 0, 4 2 5 9 0 E 01 85,
0. 0 1 9 5 6. 3 2 0 0 90. 210, 0, 3 0 9 7 0 E 01 27,
0. 0 1 9 5 7. 7 0 0 0 90, 240, 0, 7 0 0 5 0 E 01 37,
0. 0 2 9 3 7. 7 0 0 0 90, 2 4 0 0, 6 5 0 2 0 E 01 • 41,
0. 0 1 9 5 7. 3 8 0 0 9 0 2 4 0 0. 6 6 8 2 0 E 01 44,
0. 0 2 9 3 7. 1 7 0 0 90, 240, 0, 4 7 6 4 0 E 01 60,
0. 0 2 9 3 7. 0 7 0 0 90, 270, 0, 8 7 8 6 0 E 01 121,
0, 0 2 9 3 7. 6 4 0 0 90, 270, 0, 1 3 3 0 0 E 0 2 127,
0. 0 2 9 3 7. 9 8 0 0 90, 240, 0, 1 7 9 0 0 E 0 2 180.
0. 0 2 9 3 6. 9 3 0 0 90, 300, 0, 1 8 6 2 0 E 0 2 211.
0. 0 2 9 3 6. 2 1 0 0 90, 210, 0. 1 6 0 9 0 E 0 2 215.
0. 0 2 9 3 7. 9 6 0 0 90. 330. 0. 2 6 2 9 0 E 0 2 181.
0. 0 1 9 5 8. 0 3 0 0 90. 300. 0. 2 2 1 O O E 0 2 182.
0. 0 4 8 8 7. 0 0 0 0 90. 240. 0. 1 2 8 2 0 E 01 22.
0. 0 3 9 1 6. 6 2 0 0 90. 300. 0. 1 5 6 1 0 E 01 24.
0. 0 4 8 8 7. 1 1 0 0 90. 210. 0. 9 8 1 9 0 E 0 0 25.
0. 0 3 9 1 7. 5 9 0 0 90. 0. 0. 7 4 8 2 0 E 01 50.
0. 0 3 9 1 7. 3 0 0 0 90. 210. 0. 4 1 1 7 0 E 01 59.
0. 0 3 9 1 6. 2 3 0 0 90. 300. 0. 4 8 7 8 0 E 01 76.
0. 0 3 9 1 6. 0 8 0 0 90. 300. 0. 6 1 3 2 0 E 01 77.
0. 0 5 8 6 6. 1 3 0 0 90. 240. 0. 3 9 0 5 0 E 01 84.
0. 0 4 8 8 6. 0 4 0 0 90. 210. 0. 1 5 8 1 0 E 0 2 216.
0. 0 3 9 1 7. 5 3 0 0 90. 330. 0. 2 3 7 4 0 E 0 2 193.
0. 0 5 8 6 7. 3 2 0 0 90. 270. 0. 2 0 8 0 0 E 0 2 204.
0. 0 3 9 1 7. 3 4 0 0 90. 270. 0. 2 6 7 l O E 0 2 255.
0. 0 3 9 1 7. 7 7 0 0 90. 210. 0. 2 6 5 3 0 E 0 2 273.
0. 0 3 9 1 6. 6 7 0 0 90. 210. 0. 2 8 5 3 0 E 0 2 274.
0. 0 5 8 6 6. 2 4 0 0 90. 270. 0. 2 4 3 8 0 E 0 2 280.
CLASS A V G E POWER
0. 7 9 0 4 5 E 0 2
0 4 6 1 5 5 E 01
0, 2 9 2 9 5 E 01
0. 1 2 5 9 5 E 0 2
0 . 1 3 1 2 3 E 0 2
CLASS N O .
2 4
2 5
26
2 7
FW TE DU D M A X P O W E R SPEC
( H z ) ( s e e s ) ( d e g s ) ( d e g s ) (kW/m: ) N O .
0. 0 6 8 4 7. 0 8 0 0 90. 240. 0. 8 5 6 9 0 E 0 0 3.
0. 0 6 8 4 6. 4 3 0 0 90. 270. 0. 2 2 1 5 0 E 0 2 285.
0. 0 1 9 5 8. 9 3 0 0 90. 270. 0. 1 9 t l O E 01 18,
0, 0 2 9 3 9. 0 7 0 0 90. 270. 0. 1 8 1 8 0 E 0 2 95.
0. 0 2 9 3 8. 6 6 0 0 90. 270. 0. 1 6 5 0 0 E 0 2 97.
0. 0 2 9 3 10. 0 1 0 0 90, 210. 0. 1 6 2 9 0 E 0 2 107.
0. 0 2 9 3 8. 7 0 0 0 9 0 3 0 0 0, 2 7 4 4 0 E 0 2 158.
0. 0 1 9 5 9. 7 4 0 0 90. 210. 0, 2 3 1 0 0 E 0 2 166.
0. 0 2 9 3 8. 4 5 0 0 90. 300. 0, 2 7 9 6 0 E 0 2 169.
0. 0 1 9 5 9 6 8 0 0 90. 210. 0, 2 3 7 2 0 E 0 2 170.
0. 0 2 9 3 9 1 0 0 0 90. 270. 0. 2 7 1 4 0 E 0 2 173.
0 0 2 9 3 8. 1 1 0 0 90. 270. 0. 2 0 6 0 0 E 0 2 200.
0. 0 1 9 5 8. 8 0 0 0 90. 300. 0. 3 4 2 lOE 0 2 234.
0. 0 2 9 3 9. 3 3 0 0 90. 270. 0 4 6 1 1 0 E 0 2 233.
0. 0 1 9 5 9. 2 9 0 0 90. 270. 0. 4 3 4 6 0 E 0 2 238.
0. 0 2 9 3 9. 1 6 0 0 90. 270, 0. 4 1 0 8 0 E 0 2 239,
0. 0 2 9 3 8. 9 1 0 0 90. 240, 0, 4 4 5 0 0 E 0 2 299,
0. 0 2 9 3 8. 6 1 0 0 9 0 300, 0 4 9 9 3 0 E 0 2 3 0 5
0, 0 2 9 3 8. 0 4 0 0 90. 0, 0, 5 5 1 2 0 E 0 2 333,
0. 0 2 9 3 9, 0 6 0 0 90. 240. 0, 6 0 7 2 0 E 0 2 294.
0. 0 2 9 3 8. 7 4 0 0 90. 2 7 0 0, 6 3 3 9 0 E 0 2 329,
0 0 1 9 5 9. 9 4 0 0 9 0 300, 0, 1 6 2 6 0 E 0 3 374,
0. 0391 8 1500 90. 240. 0, 2 5 5 4 0 E 01 11,
0. 0391 8. 7 0 0 0 90. 270. 0. 1 9 3 6 0 E 0 2 176
0. 0391 8. 3 5 0 0 90. 270. 0. 4 8 9 0 0 E 0 2 308,
0. 0 3 9 1 9. 8 2 0 0 90. 240. 0. 6 7 7 0 0 E 0 2 326,
0, 0 4 8 8 8. 0 8 0 0 90. 240, 0. 6 9 4 5 0 E 0 2 355,
0. 0 3 9 1 8. 3 2 0 0 90. 270, 0. 1 1 0 2 0 E 0 3 369,
0. 0 2 9 3 11. 0 1 0 0 90. 210, 0. 2 3 8 2 0 E 0 2 92,
0. 0 0 9 8 11. 8 6 0 0 90. 210, 0. 3 7 1 5 0 E 0 2 151,
0. 0 2 9 3 11. 3 7 0 0 9 0 270. 0. 1 2 1 4 0 E 0 3 337,
0. 0 2 9 3 10. 6 9 0 0 90. 300. 0. 1 3 6 4 0 E 0 3 361.
0. 0 2 9 3 10. 4 6 0 0 90. 240. 0, 1 3 4 2 0 E 0 3 363.
0. 0 1 9 5 11. 9 5 0 0 90. 270. 0. 1 4 1 3 0 E 0 3 357.
0. 0 2 9 3
10. 6000
90. 210. 0. 1 4 8 & 0 E 0 3 362.0. 0 1 9 5 10. 9 3 0 0 90. 270. 0. 1 5 2 8 0 E 0 3 359.
0. 0 1 9 5 10. 0 5 0 0 90. 300. 0. 1 6 3 8 0 E 0 3 372.
0. 0 2 9 3 11. 0 4 0 0 90. 240. 0. 1 8 2 6 0 E
03
373.0. 0 2 9 3 10. 9 1 0 0 90. 270. 0. 1 8 7 6 0 E 0 3 383.
0. 0 1 9 5 10. 8 8 0 0 90. 270. 0. 1 9 7 1 0 E 0 3 385.
0. 0 2 9 3 10. 3 3 0 0 90. 270. 0. 1 9 7 8 0 E 0 3 387.
0. 0 1 9 5 11. 0 3 0 0 90. 270. 0. 2 2 6 4 0 E
03
389.0. 0 2 9 3 10. 4 7 0 0 9 0 240. 0. 2 4 5 0 0 E 0 3 391.
0. 0 2 9 3 10. 7 8 0 0 90. 240. 0. 2 8 7 lOE 0 3 394.
0. 0 2 9 3 10. 7 6 0 0 90. 240. 0. 2 9 9 7 0 E 0 3 396.
0. 0 1 9 5 11. 5 6 0 0 90. 210. 0. 4 4 8 6 0 E 0 3 399.
C L A S S A V G E POWER
0. 1 1 5 0 3 E 0 2
0 4 0 1 9 8 E 0 2
0. 5 3 0 2 7 E 0 2
0. 1 8 5 0 8 E 0 3
CLASS N O .
28
29
30
31
32
FW TE OW D H A X P O W E R SPEC CLASS A V G E
( H z ) ( s e e s ) ( d e g s ) ( d e g s ) ( k W / m ) N O . POWER
0. 0 2 9 3 12. 8 7 0 0 90. 270. 0 2 2 3 9 0 E 0 3 381.
0. 0 2 9 3 12. 6 6 0 0 90. 270. 0. 2 4 5 2 0 E 0 3 3 8 l 0. 2 3 4 5 5 E 0 3
0. 0 4 8 8 5. 0 8 0 0 120. 270. 0. 3 5 1 2 0 E 01. 86. 0. 3 5 1 2 0 E 01
0. 0 7 8 1 5. 6 9 0 0 120. 270. 0. 5 3 2 0 0 E 01 75. 0. 5 3 2 0 0 E 01
0. 1 2 7 0 5. 2 3 0 0 150. 270. 0. 3 7 6 3 0 E 01 80.
0. 1 1 7 2 4. 7 0 0 0 210. 210. 0. 3 2 3 5 0 E 01 83. 0. 3 4 9 9 0 E 01
0. 0 2 9 3 7. 1200 120. 270. 0. 6 9 1 9 0 E 01 47.
0. 0 2 9 3 7. 0 2 0 0 120. 0. 0. 7 4 6 9 0 E 01 53.
0. 0 2 9 3 7. 0 8 0 0 120. 300. 0 1 4 8 2 0 E 0 2 196.
0. 0 2 9 3 7. 2 7 0 0 120. 240. 0. 2 9 2 3 0 E 0 2 268.
O 0 2 9 3 7 5 1 0 0 120. 3 3 0 0 4 3 5 3 0 E 0 2 3 1 7 0. 2 0 3 9 4 E 0 2
33
0. 0 3 9 1 7. 7 1 0 0 120. 270. 0. 1 7 6 8 0 E 01 20.
0. 0 3 9 1 7. 4 0 0 0 120. 270. 0. 2 6 6 7 0 E 01 21.
0. 0391 6. 8 4 0 0 120. 2 7 0 0. 5 8 5 8 0 E 01 51.
0. 0 4 8 8 6. 7 6 0 0 120. 270. 0. 6 8 0 7 0 E 01 6 5
0. 0 4 8 8 6. 9 8 0 0 120. 270. 0. 4 9 3 3 0 E 01 67.
0. 0 4 8 8 6. 3 0 0 0 120. 270. 0. 7 3 4 7 0 E 01 74.
0. 0391 6. 2 0 0 0 120. 270. 0. 4 0 3 lOE 01 79.
0, 0 4 8 8 7. 4 0 0 0 120 270, 0. 9 4 4 7 0 E 01 119.
0. 0 4 8 8 7 1700 120. 270. 0 9 3 6 5 0 E 01 132,
0. 0391 6. 3 9 0 0 120 0. 0. 8 0 7 0 0 E 01 134.
0. 0 5 8 6 6. 4 2 0 0 150. 270. 0. 1 0 8 7 0 E 0 2 131.
0 0 4 8 8 6 6 7 0 0 120. 270. 0. 1 0 8 2 0 E 0 2 133.
0. 0 3 9 1 7. 2 1 0 0 120. 2 7 0 0. 2 2 1 6 0 E 0 2 218,
0. 0 4 8 8 7. 1100 120. 270. 0. 2 4 3 7 0 E 0 2 262,
0. 0391 7. 1800 120. 240. 0 2 7 7 6 0 E 0 2 266.
0. 0391 6. 9 5 0 0 120. 270. 0. 2 5 9 3 0 E 0 2 270.
0. 0 4 8 8 7. 2 3 0 0 120. 270. 0. 2 5 0 6 0 E 0 2 271.
0. 0 5 8 6 6. 5 9 0 0 120. 240. 0. 2 6 5 3 0 E 0 2 272.
0. 0 3 9 1 6 4 8 0 0 120. 270. 0. 2 0 9 1 0 E 0 2 284.
0. 0 4 8 8 7. 7 5 0 0 150. 0. 0. 3 2 8 3 0 E 0 2 253.
0. 0 3 9 1 7. 8 2 0 0 180. 330. 0. 3 3 3 9 0 E 0 2 256.
0. 0 3 9 1 7. 0 0 0 0 120. 240. 0. 3 2 6 7 0 E 0 2 279.
0. 0 5 8 6 7. 2 0 0 0 120. 270. 0. 3 6 2 8 0 E 0 2 318.
0. 0 5 8 6 7. 6 4 0 0 120. 210. 0. 4 6 0 7 0 E 0 2 313.
0. 0 4 8 8 7. 5 2 0 0 120. 330. 0. 4 9 7 4 0 E 0 2 334.
0. 0 5 8 6 7. 6 1 0 0 120. 210. 0. 5 8 1 5 0 E 0 2 332. 0. 2 0 9 1 7 E 0 2
CLASS N O .
34
35
36
37
38
FW TE DW D M A X P O W E R SPEC
(Hz) ( s e e s ) ( d e g s ) (degs ) ( k W / m ) N O .
0. 0781 7. 3 4 0 0 120. 270. 0. 1 2 5 0 0 E 0 2 125.
0. 0 7 8 1 6. 2 7 0 0 120. 210. 0, 1 7 1 3 0 E 0 2 217.
0. 0 6 8 4 6. 4 6 0 0 120. 270. 0. 2 0 7 5 0 E 0 2 212.
0. 0 6 8 4 ' 7. 4 9 0 0 180. 300. 0. 3 7 9 7 0 E 0 2 316.
0. 0 2 9 3 8. 7 5 0 0 120. 270. 0. 2 0 2 6 0 E 01 5.
0. 0 1 9 5 8. 6 8 0 0 120. 270. 0. 1 5 5 0 0 E 01 12.
0. 0 2 9 3 9. 3 4 0 0 120. 270. 0. 9 6 3 0 0 E 01 43.
0. 0 2 9 3 9. 6 3 0 0 120 270. 0. 1 3 0 7 0 E 0 2 88.
0. 0 1 9 5 9, 7 5 0 0 120. 270. 0. 1 3 7 4 0 E 0 2 89,
0. 0 1 9 5 9. 2 0 0 0 120. 300. 6. 1 7 3 5 0 E 0 2 " 96.
0. 0 2 9 3 8. 0 9 0 0 120. 300. 0. 2 4 4 4 0 E 0 2 179.
0. 0 2 9 3 8. 8 1 0 0 120. 240. 0. 3 1 1 6 0 E 0 2 230.
0. 0 1 9 5 8. 7 8 0 0 120. 270. 0. 3 4 9 lOE 0 2 241.
0. 0 2 9 3 8. 1 7 0 0 120. 270. 0 3 9 9 2 0 E 0 2 310.
0. 0 2 9 3 8. 6 7 0 0 120. 210. 0. 4 3 1 7 0 E 0 2 296.
0. 0 2 9 3 8. 7 8 0 0 210. 270. 0. 8 5 2 7 0 E 0 2 347.
0. 0 2 9 3 S. 3 6 0 0 120. 210. 0. S 3 8 4 0 E 0 2 351.
0. 0 2 9 3 8. 9 3 0 0 120. 300. 0. 9 6 7 9 0 E 0 2 350.
0. 0 1 9 5 9. 4 9 0 0 120. 270. 0. 9 6 7 3 0 E 0 2 352.
0. 0 2 9 3 8. 3 3 0 0 120 180. 0. 1 2 1 5 0 E 0 3 379.
0. 0 2 9 3 8. 7 8 0 0 120. 210, 0. 1 2 9 0 0 E 0 3 380.
0. 0 1 9 5 9. 5 3 0 0 120. 300. 0. 1 3 4 3 0 E 0 3 376.
0. 0 2 9 3 8. 9 8 0 0 210. 270. 0. 1 3 6 8 0 E 0 3 377.
0. 0 2 9 3 9. 4 9 0 0 120. 300. 0. 1 5 9 0 0 2 0 3 ' —
0. 0 4 8 8 8. 2 9 0 0 120. 270. 0. 1 4 6 5 0 E 01 9.
0, 0391 8. 2 0 0 0 120. 330. 0. 2 1 2 8 0 E 0 2 190.
0. 0391 9. 0 9 0 0 120. 240. 0. 4 8 8 7 0 E 0 2 293.
0. 0391 8. 0 7 0 0 120. 330. 0. 7 0 3 8 0 E 0 2 354.
0. 0 1 9 5 10. 1 2 0 0 120. 270. 0. 2 4 4 9 0 E 01 17.
0. 0 0 9 8 11. 9 2 0 0 120. 240. 0. 8 3 2 0 0 E 01 49.
0. 0 1 9 5 10 7 5 0 0 120. 270. 0. 1 0 4 0 0 E 0 2 32.
0. 0 2 9 3 10. 6 4 0 0 120. 270. 0 2 3 7 2 0 E 0 3 390.
0. 0 1 9 5 11. 2 6 0 0 150. 270. 0. 2 6 3 3 0 E 0 3 388.
0. 0 0 9 3 11. 7 7 0 0 120. 240. 0. 2 8 4 6 0 E 0 3 3 9 2 .
0. 0 2 9 3 10. 9 9 0 0 120. 240. 0. 3 1 7 3 0 E 0 3 395.
0. 0 2 9 3 11. 7 7 0 0 120. 240. 0. 4 5 6 9 0 E 0 3 398.
0. 0 1 9 5 12. 1 1 0 0 120. 270. 0. 4 0 1 8 0 E 0 3 397.
C L A S S A V G E P O W E R
0. 2 2 0 8 8 E 0 2
0. 6 3 7 1 0 E 0 2
0. 3 5 4 9 9 E 0 2
0. 1 9 7 5 6 E 0 3
0. 4 0 1 8 0 E 0 3
