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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

(2)

-

i-Index

PART I

Basic InIoimatjon und Test Results

PAGE

ScriDtiofl

of Hodels

3

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.

(3)

ç

2--PAJ' I

(4)

*

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.

12

DEAVOUJ 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)

-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 before

77-A

nd B,

end were altered to 77-C2 and

D2 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)

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.

(7)

-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 centerboards

were 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 same

deficiency 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 at

Speed 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.

(8)

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 X

Degrees

14 15 15

C.L.R.

% L.W.L.

14

15

Rep.

12

EETAH0E 3

EDAV0UR I

VIII

6410

2.51

2.22

1.97

46.21

46,07

46.00

RAIJflOEY V

5764

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

V

6325

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 21

19

20

21

TfEETK0E //r 3

9640

2.47

40.60

EHDEAVOTTR I

12180

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

As

13811

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

Above

11680

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! 3

13150

3,63

3.08

2.46

45.04

47.65

52.56

EDEAV0TTR I

15940

3.54

3.07

2.70

49.93

51.48

53.36

RA1I507T

15130

3.81

3.37

2.98

47.55

49,93

52.66

77-A

As

18235

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

Above

15940

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_CE

16740

3.73

3.31

2.90

50.14

51.82

55.29

(9)

Calculations for Wind and Boat Speeds

E1DEAVOUR I 0

Sp. No.

100

With Centerboard

20°

Calo. No

VIII

30°

12

6.947

13

14

7.329

7.711

15

8,098

19

9.63].

20

10.02

21

10.40

20

10.02

21

10.40

22

10,79

R5

1212

1317

1424

1565

2685

2955

3388

3530

3900

4465

(F11

6410

12180

15940

F11

6508

12962

18408

COO

.1891

.2055

.2222

.244].

.2205

.2427

.2783

.2215

.2447

.2001

S 13.4-0

14.30

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

VA

13.57

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

Y

38.54

42.00

45.65

49.91

35,90

38.94

43.00

31.72

33.70

36.58

VT

7.435

7.220

7.030

6.948

13.34

13.15

13.10

20.85

20,80

20.75

V

5.438

5.445

5,390

5,214

7.800

7,790

7,600

8,520

8.645

8.663

X

2.80

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

(10)

Calculations for Wind and Boat Spood

PA IN BOW -0

Sp.

o.

100

With Conterl)oflrd

200

Calo. No, V

30°

12 13 14 19 20 21 20 21 22 iT

6.947

7.329

7.711

9.631

10.02

10.40

10.02

10.40

10.79

1153

1241

1355 2670

2930

3363

3555

40.23

4678

co

e)

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

Y

41.46

45.06

49.26

37.93

40.94

45.09

32.90

35.48

38.99

V

6.815

6.627

6.510

12,75

12.61

12.51

20.26

20.18

20.25

V

5.207

5.180

5,035

7.596

7.565

7.340

8.412

0.470

8.386

X

2.72

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

(11)

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

R8

1097

1178

1282

1409

2535

2787

3158

3523

3914

4529

(FE cas

6495

12470

16690

FE

6594

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

VA

13.65

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

Y

36.41

39.44

42.98

47,04

34.27

36.85

40.28

30.60

32.68

35.69

VT

7.419

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

X

2,96

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

(12)

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.

(13)

Heeled Reietance

and Leeway Angloo at Stability

of 77-C, RANGER

With Centerboard

Bed

An1lc

Speed ro3.

c

Calo.

12 100 13 14

6495

15 13 200 19 20

12470

21 19

300

20 21

16690

22

Fes s±anco

DA7C'UR I

VIII

1232 1323

1436

1558

2493

272].

2978

3429

3359

3593

3981

4544

V 1209 1278 1389

2532

2558

3018

3435

3526

3776

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

37G8

4163

4759

77-C ÇRAJGDR)

III

1097 1178 1282

1409

2358

2535

2787

3158

3257

3523

3014

4529

77-D

II

1177

1267

1382

1504

2466

2689

2920

3296

3415

5014

4166

4699

-VII

1205

1267

1385

2816

3092

3459

3959

4379

4359

7 7-D2 V

1082

1247

1365

2625

2007

3206

3751

4141

4090

77-j

II

1068

1220

1297

1524

2544

2632

2929

3407

3362

3639

4018

4597

77-F

II

1134

1272

1371

1469

2495 2618 2966

3209

3306

3616

3981

4560

77-Iv

1117

1197

1295

1493

2446

2560

2858

3204

3493

3645

4±:)7

Leeivay Anle

EiDEAVOUR I

VIII

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 V

3.00

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

77-13

II

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 V

3.11

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

IV

2.94

2.6].

2.35

2.26

3.11

2.72

2.34

2.14

3.73

3.29

2.88

(14)

. 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 sail

coeffi-cients

to the higher S anc-les which

corre-spond to reaching with VT abean.

Because the tests did. not

cover heel angles

of less than 100, the

curves in Fig. 10 cover

reaching at high speeds only. The shapes of these curves aro consistent with the full

range curve for 77-C shown in Fig. 11.

(15)

AD( N U I. N. , : r r j E4

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PART II

(17)

- 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.

(18)

23

-8. Effective Yletted

pj-Chart of vertical resistance differences Fig. 13

This chart shows

the effects on the vertical resistances of three

different 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 RITB07

testo 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.

(19)

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(20)

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.

(21)

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's

curve 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 RAINBOW

test. noints, a1thouh sewhat scattered, do not

sug-gest any systemrna.tic error in the calculated

values.

*

Detailod notes

recarding the individual test

points

are

given in

(22)

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(23)

No

sin O coz O

= 100

2.803

X 101

EA

20°

5.270

10_3

30°

7.098 x 10

WEETALOE 3

10°

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 I

loo

328.2

6410

6835

.9378

200

1218G

12820

.9501

300

15940

16760

.9511

-Jr

RAINBT

100

331.0

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

7026

6495

.9244

7090

1.009

.9161

20°

13210

12470

.9440

13627

1.031

.9151

30

17792

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.,

X

GT sin O cos O

- Fri co

O EA

54.67 + 6.33 = 61.00

r.

r-I

O.

-p

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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-4

0

-? C)) L-' C)ci 4) 30

Analysis 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) 1

00

o o

00

o

00

o o

o

00

o (D Q) rD

(24)

31

-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.

(25)

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

(26)

- 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

and

the 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. 21

This 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.

(27)

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.

(28)

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

(29)

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 22

X - DoroeB

C

2,96

2,67

2.45

2.80

2.49

2.20

3.85

3.42

3.00

III

C2

3.07

2.60

2.55

3.03

2.74

2.45

4.12

3.62

3.15

VII

D

2.34

2.53

2,26

2.61

2.30

2.00

3.72

3.37

3.05

(ii)

2

3,04

2,74

2.45

2.78

2.47

2.18

3.91

3.44

3.02

(V)

C.L.R. - % L.'T.L.

C

45.43

45.01

44.83

46.57

47.52

49.56

49.36

52.07

54.78

(iii)

C2

44.21

44.21

44.21

44,62

45.43

46.51

40.28

50.35

53.95

(viI)

CA to D

46.44

46.44

46.44

49.29

50.78

52.53

51.38

53.22

55.10

(Ii)

2

45.63

45.63

45.63

47.49

48.52

49.86

51.47

54.39

58.02

(y)

(F

008 o),

C C2

(Iii

(vii

6495

12470

16690

6365

12350

166û0 D

(Ii)

6225

11840

151310 D2 (V) 6325

11880

15940

Roostanoo .. Lbs.

C 1097 1178

1288

2535

2702

3158

3523

3914

4529

(III

C2 1083 1166 1258

2595

2862 3216 3676

4077

4631

(vii

D

1152

1252

1361

2622

2861

3266

3665

4081

4142

(ii)

CA D2

1111

1225

1363

2556

2798

3148

3595

3985

4552

(y)

I-J.

(30)

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

be

irregular, 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

(31)

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 to

per-mit a steady-state pitching in the encounter period to become

established.

(32)

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, to

0.8 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

(33)

-

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, in

general, as V5 increases.

The losses of V indicated by

Firs. 24

are

RAIflBO1T .96 knots

77-A .80 "

77-C .84

(34)

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.

(35)

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 386 281 353 436

77A

Lon: 1Taves 361B 3577

3702 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 982

Short .raves 2580 2699 2933 3092 3308 (vi)

No waves 2097 2220 2353 2535 2737 (iii)

(36)
(37)

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 SCOUT

0.31

SEVEN SEAS

0.27

RA III B

O 35

PAUGER

O 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°

(38)

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

(39)

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.

The

three 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."

(40)

.. 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, and

have appreciably smaller marnitudes.

- without centerboard all of thn are veather-acting, arid have eneraliy larger magnitude5 than those of RAIllBG'T.

(41)

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. NooRo

REACtING 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

-2

I-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.

(42)

54

-r

PART III

(43)

_ 56

-17. F'1 Palarices of 77-C.

Effect of Cerx.terboards. Tabulated balance data

Close-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 a

longer 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 best

possible point for

balance

under reaching

conditions

without

the board ani then to nut the board where it

Trill

properly

cor-rect the balance

for windward work. I think our next desim ith a lower stern than 77-fl mar have a still longer range of

n

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

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