TOTT( TMTK
Storens Ins-ttu±e of Techr.ology
Bloljoken, Iie
Jersey
PEPO?T rTo.
JBOAT InV1STIGATION
for
E. S. VMTD:RBILT, ESQ.
relating to the design of
fl A T G E R
by
W. STÀRLIG BURGESS, ESQ.
and
SP.RKiAN STEFTIETJS, IITC.
Deift University of Technology
Ship HydromechaniCs laboratory
Library
Mekelweg 2
26282 CD DeIft
Phone: +31 (0)15 2786873 E-mail: p.w.deheer@tudelft.fll
-
i-Index
PART I
Basic InIoimatjon und Test Results
PAGE
ScriDtiofl
of Hodels3
General Order of Procedure
5
Vertical Fesistances, All Boats
6
Final Close-Hauled Comparison, All Boats
9
Hull Characteristics at Fixed Lateral Forces, All Boats - 15
Final ReaohinT Comparison
17
PART II
Detailed Tests an SDecial InvestiGations
Preliminary Close-Hauled Comparison (vrith JEETANOE)
21 Effective fetted Area
23
Preliminary Study of Function of Centerboard, EfDEAVOIJR I
. 25
Reliability of Calculated Best Values of V5, PAINBOVI and
YA!TIE 27
Kinetic Stability
29
Further Study of Function of Centerboard, 77-C 31
Detailed Comoarisons of Hulls
36 77-C iith 77-D at 30° heel
77-02 and D2 vith 77-C and D
. Encountered 'iaves 40 Balance of RAIiTflOT 47 Preliminary Balance of 77-C 52 PART III RANGER
Final Balance of 77-C, Effect of Centerboards
55
18, Selection of 77-C for RMTGER
63
APP DIC ES
A Test Points of Close-Hauled SDeeds, RAINB
64 B Correlation of Stevens an-I
7ashinton Vertical Pesistances, 77-C 66
C Estimates of Centerboard Pressures, 77-C
74
NOTE: - A Dreliminary consideration of pick-up, made on the
six-meter boats TOOD and IIDIAH SCOUT durint' the
course of this
in-vestigation, is discussed in Technical
emoranchnn No. 20.
ç
2--PAJ' I
*
An inaccurate model
of 77-B, designated
77-X, was tested
for vertical
re-sistance only.
It is not considered in this report.
R-34
scrirition of "ocls
This report
considers the tests of
twelve* modele
-TTEETÀMOE, with 1936
keel.
Data from Report No.
12DEAVOUJ I, with
estiriated centerboard
AflTBOVT, with 1936
keel
T7-A,B, C, D, the
first group of
new 87 ft. designs
77-C2, D2, the originAl C and D models with the rudder
extended
profiles
the C model with fortvard sections reduced to avoid
over-displacement, and counter lat7ered.
a new wide model
77-CE, a cmb'tion
of the forebody of C, with the afterbody
of E.
Particulars are given
in Fig. 1.
-5-2. Genere]. Order of Procedure
TACE had been tested previously, and was referred to only for
pur-poses of comparison.
77-A, B, C, and D, were designed while the tests of FEÏDKAVOtTR I and RAITTBOT were in Progress.
77-C
and D were tested before77-A
nd B,
end were altered to 77-C2 andD2 while the tests of
77-A
and B were in progress.On the basis of the test results through and including those of 77-C2 and D2, it was concluded
-- that the 87 ft. L.W.L. was desirable.
- that the extension of the rudder profile, as in 77-C2
and. 2, was undesirable.
- that 77-C was the most promising of the new models, and that attention miht vieil be concentrated on the possibility of improving her.
- that the widest model, 77-A, was undesirable, but that another model of comparable width ought to be tried.
77-E and CE were then designed in an attempt to improve 77-C without departing materially from her lines, and 77-F in an attempt to provide a better wide model.
On test, 77-F was not found superior to 77-A, nor were 77-E or CE found
superior to
77-C.
77-C was finally selected for RANGER.
6
3. Vertical Resistances, All
Boats
Tabulation
Fig. 2 Curves for PAIfl3C)TT, EUDEAVOUR I and RANGER Fig. 3
For all of the tests considered in this paragraoh, the centerboards
were removed from the models1 and the slots filled in with wax. The
cal-cula-tod wetted area of each boat was used in expanding its measured model resistances. The sand corrections, sho'm in Fi. 2, were determined (in most cases) from two runs, with strip widths of 1/2" and 1" respectively.
The fact that ENDEAVOUR I has the lowest sand coefficient of all the
models may mean that her calculated resistances are a little on the high side. There is evex-,r reason to
suppose, hovrever, that the resistances of 77-C are in general less than those of either RAIHBO{ or ENDEAVOUR I.
It will be noted that the resistances of 77-C compare very favorably
with those of all the other boats at all speeds up to about 9 3/4 knots,
and that they are lower than those of any other boat for the range 8-9 3/4 knots. They are appreciably higher than those of several other boats at
high speeds, and this fact led to the low counter profiles adopted for
77-E and CE. The lower counters helped the hi'h-speed resistances to some extent. But these resistances were not considered of sufficient
moor-tance to influence the final selection of 77-C for RANOER. A difference
of 500 pounds in the vertical resistance at speeds of the order of 12 to 13 knots, corresponds to about i/io of a knot difference of speed.
-9-4. Final Close-Hauled Ccnarison, All Boats.
Curwes of best V vs. VT Fig. 4
Tabulated values of (F cos o), )., and C.L.R. Fig. 5
tta.iled Calculations for
vou I Fig. G
Fig. 7
77-C, RA1GER Fig. 8
For all of the tests considered
in
this oaragraph, the centerboardswere dropped 7 ft., and their wetted areas were added to the calculated wetted areas of the boats in exoandinr the heeled model resistances.
The tests were r with (in most cases) a 3/4" sand strip, the sand
cor-rections being consistent with those in Fig. 2.
Referriig to Fig. 4, it will be noted
-- that 77--C is the best boat at all wind steeds less than about 16 Imots and that she is only slightly
Inferior to 77-A at very high wind speeds.
- that the next best boats are 77_CE and 77-E in that
order.
-
that the second wide boat, 77-F,, has much the samedeficiency as the first wide boat, 77-A, at very low wind speeds.
Because it was argued that wind speeds of less than 16 lniots were much more likel'r to be encountered than wind speeds greater than 16 knots, it was concluded from Fig. 4 that the choice for BÌJJGER lay beLween 77-C and
Photographs were taken
of
the weather side of all of the models atSpeed o. Knots Heel Angle
19 9.631 200
21 10.40 30°
with correct lateral forces. These hotograohs (copies of which are
avniJable) show a cicaei- ouarter wave for 77-C than for any of the others.
R 34 - Fig. 5
StaMlfty, Lee-ways and Lon.
C.L.R.
FINAL CLOSE-HATJLED COTPARIS0
(All floats)
Víith Centerboards
100
Heel
Sp. No.
Caic.
No.
(F11 cos e)
13 XDegrees
14 15 15C.L.R.
% L.W.L.
1415
Rep.
12
EETAH0E 3EDAV0UR I
VIII
6410
2.51
2.22
1.97
46.21
46,07
46.00
RAIJflOEY V5764
2.45
2.20
42,57
42,57
77-A
II
7269
3.02
2.70
2.43
48,00
46.60
48.60
77-B
II
f665
2.89
2.62
2.37
47.00
46.64
46.84
77-C (PJdTCER)
III
6495
2.67
2.45
2,24
45.01
4483
44,69
II
6225
2.53
2.26
1.98
46.44
46.44
46.44
77-C2
VII
6367
2.80
2.55
44.21
44.21
V6325
2.74
2.45
45.63
45.63
77-E
II
6565
2.74
2.49
2.27
46.71
46.71
46.71
77-F
II
6975
2.92
2.61
2.31
46.34
46.33
46.33
77-CE
IV
6508
2.61
2.35
45.91
45.47
200
Heel
Sp. No.
19 20 2119
2021
TfEETK0E //r 3
9640
2.47
40.60
EHDEAVOTTR I12180
2.57
2.30
1.98
46.90
48.17
49.79
RkIHB07
11400
2.68
2.41
2.14
44.45
45.71
47.26
77-A
As13811
3.14
2.79
2,47
49.45
50.51
52.16
77-B
12900
2.99
2.73
2.49
48.81
49.73
50.85
77-C (RJ:GER)
12470
2.80
2.49
2.20
46.57
47.52
49.56
77-D
11840
2.61
2.30
2.00
49.29
50.78
52.53
77-C2
12351
3.03
2.74
2.45
44.62
45.43
46.51
77-D2
Above11680
2.78
2.47
2.18
47.49
48.52
49.86
77-E
12620
2.88
2.54
2.21
48.48
49.95
51.75
77-F
13220
2.92
2.57
2.24
47.95
49.09
50.58
12530
2.73
2.35
2.14
47.66
48.78
50.30
30° Heel
Sp. No.
20 21 22 20 21 22 WEETACT J! 313150
3,63
3.08
2.46
45.04
47.65
52.56
EDEAV0TTR I15940
3.54
3.07
2.70
49.93
51.48
53.36
RA1I507T15130
3.81
3.37
2.98
47.55
49,93
52.66
77-A
As18235
4.30
3.88
3.54
50.85
52.44
54.46
77-B
17115
4.42
3.97
3.55
51.05
52.75
54.98
77-C (PACER)
16590
3.05
3.d2
3.00
49.36
52.07
54.73
77-D
15811
3.72
3.37
3.05
51.30
53.22
55.10
77-C2
16633
4.12
3.62
3.15
48.28
50.85
53.95
77-D2
Above15940
3.91
3.44
3.02
51.47
54.39
53.02
77-E
16713
3.99
344
2.94
51.86
54.23
57.23
77-F
17400
3,95
3.49
3.07
50.77
52.80
55.50
77_CE16740
3.73
3.31
2.90
50.14
51.82
55.29
Calculations for Wind and Boat Speeds
E1DEAVOUR I 0Sp. No.
100
With Centerboard
20°
Calo. No
VIII
30°
126.947
1314
7.329
7.711
158,098
199.63].
2010.02
2110.40
2010.02
2110.40
2210,79
R51212
1317
14241565
26852955
3388
3530
3900
4465
(F116410
12180
15940
F116508
12962
18408
COO.1891
.2055
.2222
.244].
.2205
.2427
.2783
.2215
.2447
.2001
S 13.4-014.30
15,19
16.38
13.40
14.55
16.46
11.83
12.91
14.56
KR.877
.952
1,023
1.120
.750
.822
.943
.529
.578
.657
VA13.57
13.58
13,62
13.65
21.85
21.89
21.89
29.83
30.00
0.11
(p + x)
19.95
20,84
21.71
22.9].
20,95
22.20
24.10
21.55
22.61
24.5
Y38.54
42.00
45.65
49.91
35,90
38.94
43.00
31.72
33.70
36.58
VT7.435
7.220
7.030
6.948
13.34
13.15
13.10
20.85
20,80
20.75
V5.438
5.445
5,390
5,214
7.800
7,790
7,600
8,520
8.645
8.663
X2.80
2.51
2,22
1,97
2.57
2.30
1.98
3.54
3.07
2.70
Lon:. C.L.R,
46.43
'16.21
46,07
46.00
46,90
48.17
49.79
49.94
51.48
53,36
Calculations for Wind and Boat Spood
PA IN BOW -0Sp.
o.
100
With Conterl)oflrd
200
Calo. No, V
30°
12 13 14 19 20 21 20 21 22 iT6.947
7.329
7.711
9.631
10.02
10.40
10.02
10.40
10.79
11531241
1355 26702930
33633555
40.234678
coe)
5764
11400
15130
5852
12132
17471
co
0)8
.2000
.2153
.2351
.2342
.2574
.2950
.2350
.2659
.3092
14.00
14.81
15.87
14.09
15.28
17.20
12.48
13.91
15.93
hR.926
.995
1.079
.793
.870
.990
.557
.625
.720
12.60
12.89
12.94
21.19
21.21
21.28
29.17
29.29
29.43
(+ x)
20.53
21.34
22.41
21.71
22.90
24.83
22.16
23.60
25.62
Y41.46
45.06
49.26
37.93
40.94
45.09
32.90
35.48
38.99
V6.815
6.627
6.510
12,75
12.61
12.51
20.26
20.18
20.25
V5.207
5.180
5,035
7.596
7.565
7.340
8.412
0.470
8.386
X2.72
2,45
2.20
2,60
2.41
2.14
3.81
3.37
2.93
Lon. C.L.R.
42.64
42.57
42.57
44.45
45.71
47.26
47.55
49.93
52,56
o
Sp. ITo.
Ca1ou1tion
for Wind and goat Speeds
77.-C (RANGER)WiIh Centerboard
100
20°
Calo, No. III
30°
12 13 14 15 J.9 20 21 20 21 22
6.947
7.329
7.711
8.098
9.631
10.02
10,40
10.02
10.40
10.79
R81097
1178
1282
1409
2535
2787
3158
35233914
4529
(FE cas
6495
12470
16690
FE6594
13270
19273
co
o)
.1690
.1814
.1975
.2171
2033
2235
.2532
.2110
.2346
.2713
12.29
12.97
13.86
14,90
12,47
13,53
15.04
11.33
12.46
14,18
.785
.841
.913
1.000
.691
.758
.855
.502
.554
.639
VA13.65
13.56
13.68
13.70
22.11
22.14
22.19
30.59
30.69
30.74
+ x)
18.81
19.50
20.39
21,43
20.08
21.13
22.66
21.03
22.13
23.88
Y36.41
39.44
42.98
47,04
34.27
36.85
40.28
30.60
32.68
35.69
VT7.419
7,178
6,988
6.838
13.48
13.32
13.22
21.53
21.40
21.36
5,591
5.660
5.641
5.519
7,960
8.015
7.935
0.615
8.750
8.765
X2,96
2.67
2.45
2.24
2,80
2.49
2.20
3.85
3.42
3.00
LonG. C.L.R. %
45.43
45.01
44.83
44.59
46,57
47,52
49.56
49.36
52.07
54.78
15
-5. Comparison of Hull C}iaracteristics
at Fixed Lateral Forces, All Boats
Tabulation (EETMOE omitted) Fig. 9
This table shows the heeled resistances and leevtays which
would occur,
at given speeda and heel angles, if all of the boats had the stability of
77-C. It, therefore,
comoares the hydrodynn.io characteristics of the
hulls, quite apart from their stabilities.
It is interesting to note that this comparison indicates higher
Wj_
herentN resistances for 77-A, as cornoared with 77-C,
in every case, and0
that these are reflected in the lower values of best V
for 77-A at 10
and 200, in Fig. 17. In other uoids, the greater stabiity of 77-A does
not offset her greater inherent resistances until hih heel angles
are reached. An additional calculation for the values of best Vm
for 77-C, in which she was arbitrarily assimied
to have the stability of 77A (see
Fig. 17), indicated an improvement in 77-C at every heel angle. Thus it
my be concluded that the higher inherent resistance, and not the greater
stability, is responsible for the relatively poorer performance of 77-A at moderate heel angles.
It appears, then, that within reason, for boats of this class,
- inherent resistance is more important than stability* at lavi and moderate heel angles.
- stability* is more important than
inherent resistance at high heel angles.
* This refers to stability
obtained by altering the hull form. The 77-C
calculation on 77-A stability,
as well.as numerous similar calculations for boats in other classes, sho;rs
the desirability of the lowest possible center
of gravity, whatever the hull form.
Heeled Reietance
and Leeway Angloo at Stability
of 77-C, RANGER
With Centerboard
BedAn1lc
Speed ro3.
cCalo.
12 100 13 146495
15 13 200 19 2012470
21 19300
20 2116690
22Fes s±anco
DA7C'UR IVIII
1232 13231436
1558
2493
272].2978
3429
3359
3593
3981
4544
V 1209 1278 13892532
2558
3018
3435
35263776
4296
4925
77-A
II
1161
1243
1347
1482
2480
2637
2821
3287
3425
3730
4015
4680
77-II
1137
1249
1392
1472
2463
2631
2853
3213
3523
37G84163
4759
77-C ÇRAJGDR)III
1097 1178 12821409
23582535
27873158
3257
3523
3014
4529
77-D
II
1177
12671382
1504
2466
2689
2920
3296
3415
5014
4166
4699
-VII
1205
1267
1385
2816
3092
3459
3959
4379
4359
7 7-D2 V1082
1247
1365
2625
2007
3206
3751
4141
4090
77-j
II
10681220
12971524
2544
2632
2929
3407
3362
3639
4018
4597
77-F
II
1134
12721371
1469
2495 2618 29663209
33063616
3981
4560
77-Iv
1117
1197
1295
1493
2446
2560
2858
3204
3493
3645
4±:)7Leeivay Anle
EiDEAVOUR IVIII
2,80
2.55
2.26
1.99
2.88
2.59
2.28
2.02
4.15
3q62
3.17
2.32
RA I ECW V3.00
2.69
2.53
3.21
2,96
2.57
2.37
4.69
4.20
3.76
3.37
77-A
II
3.02
2.71
2.45
2.14
3.09
2.69
2.35
2.06
4.46
3.93
3,52
3.17
77-13II
3.11
2.88
2.61
2.26
3.29
2.96
2.69
2.41
4.79
4.34
3.85
3.48
77-C (rxcER)
III
2.96
2.67
2.45
2.24
3.13
2.00
2.49
2.20
4.28
3,35
3.42
3.00
77-D
II
2.96
2.67
2.39
2.08
3.06
2.78
2.39
2.14
4.40
3.95
3.50
3.23
77.-02
VII
3.10
2.82
2.61
3.06
2.76
2.49
4.24
3.64
3.11
7 7-D2 V3.11
2.82
2.53
2.92
2.59
2.32
4.15
3.60
3.25
77-E
II
2.92
2.65
2.43
2.26
3.15
2.00
2.43
2.26
4.36
3,93
3.52
3.06
77-F
II
3.04
2.74
2.54
2.14
3.13
2.74
2,9
2,04
4.15
3.97
3.41
2.02
IV2.94
2.6].
2.35
2.26
3.11
2.72
2.34
2.14
3.73
3.29
2.88
. 17
-6,
Fil Reachin Corison
Curves of' V5 vs. VT fors 90° FIg. lO
fl1DEAVOUR I
RAINB7
77-C (WIGER)
Based on
- special heeled
tests without
centerboards,- o o
at 10 and 20 heel, and at high
speeds.
-
an extension of the GTMCRACK sailcoeffi-cients
to the higher S anc-les whichcorre-spond to reaching with VT abean.
Because the tests did. not
cover heel angles
of less than 100, thecurves in Fig. 10 cover
reaching at high speeds only. The shapes of these curves aro consistent with the fullrange curve for 77-C shown in Fig. 11.
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PART II
- 21
7. Preliminary Close-au1ed Comparisons.
Curves of best Vmcj. vs. VT for TAHOE, RAINDO7,
ENDEAVOUR I, ad 77-C Fig. 12
The calculations on which these preliminary curves were based,
fol-lowed the Drecedent set in the WEETAOE work (Ret,ort
12) by iorin the
wetted area of the centerboard in the calculation of the heeled resis-tances. Subsequent investi-ation indicated the oropriety of inc1udin
this area (see par. a), and it wa included in all later work. By
orit-tin it, the curves for the other boats are strictly comparable vrith those
for YEETAIOE.
As the addition of the board area tends to reduce the calculated
heeled resistances, the values of Vng are in general lower in Fig. 12 than in Fig. 4.
23
-8. Effective Yletted
pj-Chart of vertical resistance differences Fig. 13
This chart shows
the effects on the vertical resistances of threedifferent types of alteration, each of which increased the wetted area.
Bo&t Alteration % Increase of
Wetted Area
RAflBOW loading from 84 to 87 ft. L.I.L. 4.4
77-C rerrular centerboard dropped 7 ft. 4.6
77-C small centerboard dropped 4 ft. 1.2
77-D extendin rudder profile 5.0
It will be noted that, except for the addition of the small board to
77-C, the percentae increases of wetted area were almost identical. The
effects on the resistances, as shown in Fig. 13, were, however, very
dif-ferent. In all cases the increase of wetted area was included in
calcu-lating the resistances for the altered condition.
It was concluded fron Fig. 13,
- that the wetted area added to 77-D by extending the
pro-file aft did not increase the skin friction, and may
pos-sibly have reduced the eddy-n-ing. (The model
resis-teneco of 77-D2, comoared with those of 77-D, were about the sane at low speeds and slightly lower at high speeds.)
-
that
nothing definite could be deduced from the RITB07testo because of the enera1ly different form which
re-sulted from loadin her dovm. (The orders of magnitude
of the resistance changes are consistent with those found
for SEVE. SRAS (Report Ho. lo), and for WEETANOE (Report
No. 12).
- that the calculated resistances of 77-C with the regular
board were largo enouh, even with the board area
in-cluded, and would have been unreasonably large with the
board area omitted.
The last conclusion is the justification for including the centerboard area
in all subsequent calculations of heeled resistances with centerboard.
MIIIIm.tr.. Oth IIaI henri. N U I,
.
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25
-9.
Preliminarv Studî öf the Function of the Centerboard,
EîDEAVOR I.
Curves of V
vs. VT, at particular values of V8
Fig. 14.
In Report !o. 12, it was concluded that the centerboard damaged the
close-hauled ahilit' of WEETAMOE.
It was, therefore, desirable t.
et
further data on the fimction of the centerboard as early as nossible in
the present investiation.
EIDEAVOTJR I offered the first opportunity.
Instead of best
1Tmg' Fig. 14 shows actual V
vs. VT, for definite
values of V, with and vrithout the centerboard. TIe tvo curves 1yin
farthest to the rirht represent values
of V5 which correspond closely to
the best
values (see Fì. 4); the other
curves represent values of
V8 tiTo speed rnmibers (about 3/4 imot)
loner,
ThIs chart indicates that the centerboard
does little good when V8
corresponds to the best Vm,., as sho
by the calculations,* but that it
becomes important wheneverV3 is
reduced (that is, whenever the boat is
pinched).
The question then arises cf the
accuracy with which the
cal-culations reflect the best values of V5 at n±iich to sail.
*
thereby confìrmin
the TEETACE conclusion.
27
-10.
Reliability of' Calu1ated
Rest Values of , JIi3c, YJHtEE.Curves of
and V
vs. 9
Fig. 15
Fig. 15 shows Professor Fay's curve
of V5 for best Vm, vs. 9, based
on sailin data from YiEE in
1935.
Aainst this arc shown the
calcu-lated values of V
for best 7
for RAINBOW (see Fig. 4), and test points
from RJJfl13T in
1936.*
There is little doubt that Professor
Fay'scurve shoots off too much
to the right at hih heel angles.
e1ow about 22
heel, hovrever, his
curve is in very ood agreement vrith the calculated values for
JNBO'J.
Further,
the RAINBOWtest. noints, a1thouh sewhat scattered, do not
sug-gest any systemrna.tic error in the calculated
values.*
Detailod notes
recarding the individual testpoints
aregiven in
jj.iiJii
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Il
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f .424_-" J .. 1I:;: :it:i
il'
i' t ,'No
sin O coz O
= 1002.803
X 101
EA20°
5.270
10_330°
7.098 x 10
WEETALOE 310°
Lbs.
Ft0
338.3
Lbs.
Lbs.
'J o Lbs.
.4-) Cri OC) E- O E-c 4) 20 9640 9875.9762
30°
13150
13190
.9970
E1ÎDEAVOUR Iloo
328.2
6410
6835
.9378
200
1218G12820
.9501
300
15940
16760.9511
-Jr
RAINBT
100331.0
5764
6205
.9289
20°
-11400
11710
.9735
30°
15130
77-A
100
366.1
7.66
7860
7269
.9274
200
14777
13811
.9346
30°
19903
18235
.9162
77-?
100
368.6
7.17
7408
6665
.8997
20°
13929
12900
.9261
30°
18760
17115
.123
77-C
10°
373.0
6.72
70266495
.9244
70901.009
.9161
20°
13210
12470
.9440
13627
1.031
.9151
3017792
16690
.381
18264
1.027
.9138
ir
77-D
10°
369.1
6.60
6625 6225.9117
20°
12838
11840.9223
300
17291
15811.9144
Stati.c Stáb.,
XGT sin O cos O
- Fri co
O EA54.67 + 6.33 = 61.00
r.
r-IO.
-p_4
r-.D 4) O o C)o o
r) C) o p .cZ 4) p -o r-1 C 4) t) r-( C) 4) ç C)) ci L) ci C/D O E-) C)ci E-40
-? C)) L-' C)ci 4) 30Analysis of' StabiiiUes
R 34
Fie.
0 C) O 16 4 o -D 4.) o (D 4.) O r (D (D d (D (1) t'- 4-) O C)Q) 100
o o00
o00
o o
o00
o (D Q) rD31
-12. Further tudy of Nunction of
Centerboard, 77-C RAITGER
Curves of best V, vs. VT for 77-C
Fig. 17 Curves of' RS/(FH
cos e).,, ENDEAVOUR I and 77-C Fig. 18
Curves of 1ee'ay angles, X, ENDEAVOUR I arid 77-C Fig. 19
FIg. 14 indicates that the centerboard
does little good to ENDEAVC%TJR
I
when she Is sailed at the best values of V3 as shown by the
calculations. Fig. 15 indicates that the calculated
best values of V3 are consistent with
the observed values for RATiT30T. Par. li
raises the auestion of' whether or not the considerably
greater reduction of stability caused br the larce
centerboard of 77-C may not have an undesirable effect on the close-hauled
ability of' this boat.
Fig. 17 answers the
last nuostion in the negative. It shows that the
centerboard increases the best V of 77-C over nearly the
entire rne of
WInd speeds. An examination of tìe
values of 1T, corresponding to lower values of V5,
as show-n by this crt, indicates tat the centerboard is even
more irnrortant to 77-C than to ENDEAVOUR I
(see Fig. 14) when the boats are
1.4
Fig. 18 throws some li"ht on the
reason for the difference in the
ef-fect of' the centerboard
on these two boats. It shows that, particularly at 10 , and to some extent at 200, the
unfavorable effect of the centerboard on
the ratio RS/(FH
cos e)
is delayed to a higher soeed in the case of 77-C
than in the case of ENDEAVOUR I. At 10°, with V5 enual
ITo. 14
(corresDond-Ing aprroimate1y to best V1 in FIgs. 4 and 17),
the ratio for 77-C is better with the hoard,
whilethat for ENDEAVOUR I is dist5nctly inferior.
At 30 , with V equal No. 22, the
ratios are better for both boats with the board.
Fig. 19 throws additional
light on the behavior of the ratio
cos e) just referred to.
It brinr'-s ou-b the very considerably
greater leeways of 77-C when both boats
are sailed without centerhoards, and the fact that the leewavs are made
very nearly equal when the boats are
sailed with the boards.
Reasonin froi Figs. 18 and 19
together, it may be concluded that the centerboard reduces the
heeled resistance at rolativel low sDecds,vrhere
without it the leewa'r is abnormally hih,
but that it increases the
resis-tance at relatively
high speeds where the leei'ray is moderate
in any case.
* The points for 77-C on the
stabilities of 77-A, shown in Fig. 17,
are dis-cussed in rar. 5.
32
-In other z'ords, at 1071
peods the resistance of the
board itself is less
important than the extra
ros5stance caused by hiih loerray, while
at
rela-tively hih soeeis the resistance
of the hull cannot be appreciably
af-fected by rioderate reductions
of loe'.'rav and the resistances of the board
- 36
13.
Detailed Comparisons of Hulls
77-C with 77-D at
330
heel.
Tabule.tion of resistances
Fig. 20
Fig. 4 shows 77-D distinctly inferior -to 77-C in close-hauled ability.
This is partially e
lamed by the lower stability of 77-D but principally
by the higher heeled resistances.
To isolate the cause of the hih heeled resistances, special tests
of
77-C and 77-D were made at 30
heel with no lateral forces.
The results of'
these tests ccmbned rith the basic resistances (oars. 3 and 4) oeruut
sea-arate evaluations of the added resistances due to heel alone, and of the
so-called induced drags.
These are given in Fig
20.
Fig. 20 shows Lwu sets of induced drag values for 77-D,
one
correspond-ing to the actual stabiliti of this boat
andthe other to the stability of
77-C.
The higher heeled resistances of 77-D
are brouht about both by
higher induced drags and by higher resistances due to heel alone.
77-C
and
vrith 77-C and D.
Tabulation of
characteristics Fig. 21This table gives detailed figures showing the effects
on the various
hull characteristics of extendia.g the rudder profiles
of 77-C and D to mce
77-C2 and D2.
It will be noted that the alteration
-- caused an increase of leevray in every case.
- moved the CL.R. forward in every case except for the D
model at 30
- had minor effects on the stabilities.
- imroved the resistances of the C model slightly at 100
but injured them at higher heel angles.
- improved the resistances of the D model at all heel
angles.
37
-The vreather side photographs at 300 heel, speed number 21, Indicate that the alteration caused some increase in the quarter-wave disturbance in both eases.
38
Coarison of Searate Effects on Resistance
of
Heel and Leeway
77-C and 77-D at 300 Heel R 34 - Fig, 20 o) 77-C Speed ITo. 19 20 21 22 30°, 30°, 00, (FE o) 16690 (FE = 0
(Fif cos o) = O (Vertical) Induced Drag 3257 2238 1979 1019 3523 2511 2248 1012 3914 2951 2608 963 4529 3646 3160 883 (III) (y (I
Resistance due to Eec]. 259 263 343 486
Total Added Resistance 1278 1275 1306
1369 77-D 300, 300, 00, (FE cos e) 15811 (F11 0)3 0
(FE cos = O (Vertical) Induced Drag 3350 2358 2050 992 3665 2658 2289 1007 4018 3088 2633 930 4742 3740 3167 1002 (II) (iii) (I)
Resistance due to Heel 308 369 455
573
Total Added Resistance 1292 1376
1385 1575 77-D 30°, 30°, 0°, (FE cos e) 16690 (F11 cos o) - 0 (F11
003 e)
= O (Vertical) Induced Drag 3415 2358 2050 1057 3814 2658 2289 1156 4166 3088 2633 1073 4899 3740 3167 1159 (Fig. (III) (I) on 77-C stab.Resistance due to heel 308 369 455 573
Total Added 2esistance 1365 1525
Comparison of Hull Charactori8tic
77-C2 and D2 with 77-C and D.
Heel An1e
Speed No.
10°
20°
12 13 14 19 20 21 20 30 21 22X - DoroeB
C2,96
2,67
2.45
2.80
2.49
2.20
3.85
3.42
3.00
III
C23.07
2.60
2.55
3.03
2.74
2.45
4.12
3.62
3.15
VII
D2.34
2.53
2,26
2.61
2.30
2.00
3.72
3.37
3.05
(ii)
23,04
2,74
2.45
2.78
2.47
2.18
3.91
3.44
3.02
(V)C.L.R. - % L.'T.L.
C45.43
45.01
44.83
46.57
47.52
49.56
49.36
52.07
54.78
(iii)
C244.21
44.21
44.21
44,62
45.43
46.51
40.28
50.35
53.95
(viI)
CA to D46.44
46.44
46.44
49.29
50.78
52.53
51.38
53.22
55.10
(Ii)
245.63
45.63
45.63
47.49
48.52
49.86
51.47
54.39
58.02
(y)
(F008 o),
C C2(Iii
(vii
649512470
16690
6365
12350
166û0 D(Ii)
622511840
151310 D2 (V) 632511880
15940Roostanoo .. Lbs.
C 1097 11781288
25352702
3158
3523
3914
4529
(III
C2 1083 1166 12582595
2862 3216 36764077
4631
(vii
D1152
12521361
2622
2861
32663665
4081
4142
(ii)
CA D21111
12251363
25562798
3148
3595
3985
4552
(y)
I-J.40
14. Encountered V'avos
Estimates of pitching period of RAINBT Fig. 22
Table of excess resistances due to encountered
waves Fig. 23
Curve8 of vs. VT Fig. 24
RAI BC
77-A
77-C
Observation during the strnmier of 1936 led to the conclusion that the
pitchin of J-boats which is accompanied by en occasional heavy pound and
a noticeable reduction of speed, is caused by the comarative1y large seas
which are likely to sveep across the iewport race area. These seas
apar-ently ori'inate off shore; they are in general distinguishable from the shorter, steeper seas built up b.- the local winds, and they seem to have a much more pronounced effect on the boats.
As a background for an attempt to evaluate their effect by means of model tests, the followin" data were obtained, during August, 1936, on
several occasions when important pitching
occurred.
Average Averac-e Average
wave length, X
wave height, crest to trough, h
pitching period, RAIB07 (84')
!A1uE
EETA"0E (84') WEETAMOE (87') 80-90 ft. 2.5-4 ft. 3.8 sec. 3.9 sec. 4.0 seca 3.6 seo.The pitching amplitude was observed
to
beirregular, building up
pro-gresslvoly until killed by a heavy pound.
Assuming, for these average data,
V5 9.5 knots
l)i:iig:ii 7.5 knots
41
-the period of encoimter, T0, 18
'I - 9.5 x 1.669 - 16.05 VTa!
-
20.90 36.95 85--
- 2.30 secs. 36.95 if the raves were being taken head-on, and- 7.5 i 1.689 12,67
as before 20.90 33.57 85
Te 2.53 secs.
if the raves were coming from the direction of the wind. In either case
(or with any reasonable values of V3 or Vm) it is evident that the
encoun-ter period, Te, is considerably less than he observed pitchin eriods, T.
Fig. 22 shows preliminary and revised estimates of the natural
pitch-ing period, T, of RIITBC'T. The preliminary estimate was rade before the
observed data viere available, the revised estimate afterwards, and with the
object of determining whether or not the assumption that T = observed T,
would lead to absurd values for the individual radii of gyration, k, of the
several divisions of the total weight. fly far the most imorant item in
the estimates is the value of k for the hull weight. That necessary in the
revised estimate looks high, but perhaps not unreasonably so.
From the foregoing data and calculations, the most obvious conclusions are
-- that the pitching is initiated by the encountered waves.
-
that the encountered waves are not regular enough toper-mit a steady-state pitching in the encounter period to become
established.
42
-- that the nitching ceriod is about ocual to the natural -
per-od, and that both of these are greater than the encounter
period.
- that the natural period is not so much greater than the
en-counter period as to nrevent a succession of enen-counters from
building up the amplitude of natural pitching. with the
gradual change in the phase which this imlies, successive
encounters evidently build up the artlitude until an an-proach to phase onposition causes a heavy pound dth a defi-nite tendency to stop the pitching.
10 means of avoidiñg this situation suggests itself. The oitching
would probably be reduced òy a substantial increase in the natural
erod.
But there is no obvious means by which this period could be increased by
enough to cause a noticeable change, even if the stability of the boat were sorously impaired by shifting weichts to the ends.
The increase of length from 64 ft. to 87 ft. L.W.L. appears to he in the right direction, but its effect on the natural period is too small to be important.
With eQuivalent construction weights T o
)'TT
Fig. 23 shows the excess resistances due to waves encountered
head-on, as determined by model tests of RAITB0W, 77-A, and 77-C. The tests
were nade at 20 heel, with the proer lateral force
for each model (par. 4), and in waves of the following sizes.
A h
Long Vaves 98 ft. 2.5 ft.
Short llaves 68 ft. 2.5 ft.
The natural pitching
periods of the models wore adjusted,before
test, to0.8 sec.
If (Tn)m = 0.8
then (Ta) = 0.8
xf
3.9 secs.Tests of 77-A were included in an effort to discover whether or not her
wider ben '«oul.:l have a noticeable effect on the
excess rocisaucs. The
-
43--Fig. 24 shorTs best V vs. VT calculated from the unfaired total re-sistances in the iOfl encotntcred wavec. It ill be noted thr.L, for all
three boats, the hiher resistances do not materially alter the calculated
values of V5 for bec-L V, from those calculated for still water (see Fia. 4). The best value of V are, however, anoreciably lower, which means that the calculations iniicate the decirabilit'T of 1:eeoin the boat
movinr well, throu-h encountered waves. The principal reason for this
in-dication is the fact that the excess resistances in
ri'.
23 decrease, ingeneral, as V5 increases.
The losses of V indicated by
Firs. 24
areRAIflBO1T .96 knots
77-A .80 "
77-C .84
44
-Natural Pjtchn Period
RAINBOW
Restor.n Torcue rer Radian, Q.
Taken from the lines, for small displacements
from equilibriwn, in still wate r
Q - 25 z ft.-lbs.
Natural Pitching Period, (ConDlete cycle).
T=21TJí.
21JL
-
3.39 secs.R 34 - Fig. 22
= 3.80 secs. Radius of Grration, k.
Pro]. 1rni nary
Es t iniat e Second Est iriate (tons) x (ft.)2 (tons-ft.2) ee1 so x io2 8000 84 x 112 = 10200 RIg 4 x 602 ioaoo = hull 70 x 352 85700 GO Ï 41.8 = 1049002 154 104530 148 132000 2 k - 104500 679 k2 132000 - 892 154 148 k - 26.05 ft. k = 29.87 ft.
X h
Loxg Waves 98' 2.5'
Short Waves 68' 2.5'
R 34
- Fjr. 23
45
-Eicess Pesis-tarices due to Encountered Waves
20° Heel
- 3,9 sec.
Speed Tb. 16 17 18 19 20
R&IÎt30VT Lonr! Waves 3549 3603 3677
3769 4110 (viii) No ïavcs 2234 2440 2670 2q36 (V) Wave Resistance 1369 1237 1099 1174 Short Waves 2545 2620 2721 3023 3372 (vili) ITo Waves 2234 2440 2670
236
(y) Wave Resistance 386 281 353 43677A
Lon: 1Taves 361B 35773702 3992 4145 (III)
No ïaves 2500 2633 2732 3010 (II)
Wave Resistance 1077 1064 1210 1135
Short ;7aves 3150 3189 3132 3370 3606 (iii)
No Waves 2500 2633 2702 3010 (II) Wave Resistance 639 494 8 96
77C
Long waves 3356 3459 351]. 3570 3769 (VI) To Javes 2097 2220 2358 2535 2787 (iii) Wave Resistance 1259 1239 1153 1035 982Short .raves 2580 2699 2933 3092 3308 (vi)
No waves 2097 2220 2353 2535 2737 (iii)
47
-.
Balance of RAIfl3OT
Tabulated balance data
Fig. 25
Balance layouts
Fig. 26
In the balance diagrams, the C.E. i
taken 32.60 ft. aft of the
for-ward end of the 84 ft. L.T.L.
This firuro results from vTei-hting 85
of
the fore triangle at tvrice the mainsail weicht.
Vïarnei-'s PAPOOSE tests
are the basis for this wei-htin, (see Tech.
emo.o. 16).
The following
ratios are interesting in this connection.
85
Fore Triangle
Total Sal Arca
PAPOOSE
0.17
JILL
o 27
lUDIAN SCOUT0.31
SEVEN SEAS0.27
RA III BO 35
PAUGERO 36
Recause the unbalance arms detei-raìned with the
rudder contre.l
an-peared to im1y hi'her rudder post torques than
were Iovm to exist, a
rudder post drncmoneter was built, and tests
were made to cletenrinc the
torques reouired -to hold the heLn at the angles
required to effect
Der-fect 'balance.
These, and a f eiv measurements of the torques reuired to
hold the heLm central, are
iven in Fig. 25.
Th
original estimate of the torque requIred to effect balance
at,
say, 20
heel end speed To. 16 vías
Rudder
Orce =
2.40 x 11400
40 x 3.94
= 730 lbs.
730 ft.-lbs. torque at 1 ft. radius
where
2.4-0 = unbalance arm with board, Fig. 25
114-00
F11 cas O from Fi. 5
40 = asswned arm for rudder couple
0.94 = cos 20°
48
-The measured torque for th
same case (helm angle = L 2.700) is 374 ft.-lbs.
(Fig. 25), or about 1/2
f the original estinate.
This result suests
that a lare part of the force
set up by the rudder is exerted
on the
dead-wood ahead of lte
Considering the gear ratio of
the steering gear,
, and the size of
the wheel, about 4 ft. diari.,
it may be concluded that
none of the measured
torques shown in FI. 25 involve
excessive holdin
forces on the nart of
the helmmnan.
'fhis conclusion removed
ono Question regarding the validity
to the balances deduced from the
tests.
Concerning these balances
as a whole, It Is interesting to comoare the
follovring excerpts from
corresDondence carried on while the tests were in
progress, with the data in Fig. 25.
From
r. Olin Stephens, October 9, 1936.
-WWe
are anxious to hear anything further in regard to
your
balance figures.
Rod, Like and Starling all
aTree that RAflTfl0T
carried some weather helm without
the centerboard but that the
ten-dency is to have slightly too much lee helm when the board ìs
low-ered."
From Mr. Olin Stephens, October 12,
1936.
-"In the first place,
RAI1BOW without her board carries
a
fairly stronr' weather helm under
windward conditions which is
re-cluced as her soeed increases under
reaching conditions, so that she
is considered very well balanced
for reaching except that
on a
close roach at really high speed
I believe she carried a slight lee
helm.
T1VIith the board down
the tendency is to
cariy slightly too
much lee helm but this is not
as strong for windward conditions as
the weather helm which she
carnee under the same conditions with
the board up.
"VIith working hoadsails
and the board dovm I believe that
she is almost oerfct1'r balanced but with the quadrilateral
iihs
ordinarily used the lee helm is
picked up.
I think you must bear
in mind this fact, that
a change in size of the headsail used
vri11
n 49 n
-alway-s alter the balance.
Lare quadrilateral or
enoa jibs willi
always move the C.2. forward thus increasing
ay tendency toward
leo helm.
Rod rnows PÄPBOT'S balance
venT well and if you have
any particular nuostions you could Drobably get an answer by
call-Ing him on the 'uhone.
'I think that :'ou are probably riTht in ju'iring that the
C.E. for RPJIIOT has been taken too far ionrard.
PerhaDs the
weighting of the fore trianle at 1.7 tines
its actual area maY
very well bring this about and if this is the case in general it
will show up more in these boats which
carry a relatively largo
fore triangle.
"I think we should also remember
that in comnaring the
imbalance arms in thesc bir boats
we are necessarily dealins in
large nunhers.
A comnarison vrith any of the smaller boats such
as
the
sixesTT or 40 ft. waterline
cruising boats mibt be easier if'
the imbalance arms were divided in all casos by the waterline
length.
FreIn
Tre W. Starling Burgess, October 14, 1936.
Your letter of the 13th interests
me very much indeed.
The large lateral force that
appears to be exerted with a
comoara-tively small rudder torniie is undoubtedly owing to thc building up
of pressure on the deadwood well ahead of
the rudder itself.
Thethree dimensional models of forces of
this nature as most
care-fully measured on dirigible rudders and skags
show an enormous
peal: ahead of the rudder and forces rapidly
falling aray on the
rudder itself.
agree entirely that your balance diagrams are
consis-tent with observations aboard ship."
.. 52
-16. Preliinar 3alariee of 77-C
Tabulated balance
data Fis. 25(80e
par. is)3a1nee layouts Fig. 27
The data and charts considered in this pararaph cover the sarre cases
as those for RAITBOW, with rudder central, in par. 15. The model of 77-C
'as not fitted 'b'rith adjustable rudder.
With the C.E. 36.92 ft. aft of Sta. O, 'the
unbalance
arms- with
the
centerboard are lee-acting, as for RAflTBOW, andhave appreciably smaller marnitudes.
- without centerboard all of thn are veather-acting, arid have eneraliy larger magnitude5 than those of RAIllBG'T.
Nol1CsN0ER) 2Ot1ti Nolkt FEACMlt.1G ALAN(.I LA',out
3U2.l
5pMo Wor. A,.. 21 12.11 1.15 CAcl'1n Xfl(a): ws
L[ ,, ', tJjt.92 - i-i...._._.__ -Lor,a,C.L.ft5l.7LWL No.ÎÎC ÇJ'1GEt) O-it. NooRoREACtING I3ALAPCE LAQ.,1
&.c O.2I SeNo. tÇNOr Ut0AHM5 8 9.249 W 840' 25 11.16 W508 C*a ('Io fl (a) 549LWt. r' lt 4)Af)%L.W.L. (ie W840'-I25) W,50Ô'
C.t.Ar.o;A05t9a
-2I-z :JO'1EcLWTH OAItL) Ho.1 IC FrEi)
3At,Nc.1. LA'UU F &Al.t 0?' S,N0. t(r.oîs Ut.l,t,_APMb l 24q Ll.54 21 (019 L460 LCLR41267.LWL, LONG.C.L.R. 4.SO7.UtLL.
i-.'
h
:2O'tEELWIm oftw BALANCE LANOUT -5t..t 02-'l' :5rNo. Kwors UNe.AL.AR.-n ) Ç)41 L 2.82' -ô 4ô0 L 0.66' 20 0.02 L I. G.-'-c.I'lo. No.77C çg'(O'H Et L WITH X)Att D
eLANcL LAYOUT 02')' SeNo NNOT Un.ARM II 8560 LIôO 14 11)) L020' G'a,.t'Io. C.E.Art or STA. "0" (viz) L2.ö2 ('16) L0.86' (20) L ISO' C EAr! o 5g.., 'D S(92' CE Art or SA'O" 36.92' (n) L 1.60, (4) 1.2. 1 G.C.LU. 456.SZL.W.L Io,.0 CLR. 47.WX L.W.L. Lc.C.?.41.60ZL.W.L. --Lo,.O.C.L.R 44.SO/.LW,L. Lo. C.L.i. 45.607. L)N.L.
54
-r
PART III
_ 56
-17. F'1 Palarices of 77-C.
Effect of Cerx.terboards. Tabulated balance dataClose-hauled speeds
Reaching speeds
B1ence layouts
Fig. 23 Fig. 29
Close-hauled speeds FIg. 30
Reaching speeds Fig. 31
To si!rnlify the fine.]. analyses of the balance of this boat, the follow-Ing ccrabinations of speed and heel angle were selected as typical,
and it 'as asstrnied that balance
should be
effected, as far as possible, without he1n angles.The follovrinz excerpt is fron a letter fron Mr. Olin Stephenz, dated October 12, 1936.
In reard
to the C Desin, the C.L.R.
moves over alonger fore en-! aft ran:e than inthe case of RAIIIBO7T. VTe must not for-et reaching conditions and I think that a cood wa:,r of
lccatin' the board
7ould
be to first put the rig at the bestpossible point for
balance
under reachingconditions
withoutthe board ani then to nut the board where it
Trill
properlycor-rect the balance
for windward work. I think our next desim ith a lower stern than 77-fl mar have a still longer range ofn
C.L.P, positions.
Fron the point of ew of reachin, without centerboards, the most
outstanding differences between the balances of PÄIN2O and. 77-C, in
R-3
O So. Ho. Knots
Close-hauled 100 14 7.711 200 18 9.249 300 10.02 Reaching 100 18 9.249 200 23 11.16 30 25 11.94