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COMMUNICATION No. 29S

March 1972

(Sgo/ 199)

NEDERLANDS SCHEEPSSTUDIECENTRUM TNO

NETHERLANDS SHIP RESEARCH CENTRE TNO

SHIPBUILDING DEPARTMENT

LEEGHWATERSTRAAT 5, DELFT

*

THE EQUILIBRIUM DRIFT AND RUDDER ANGLES OF A

HOPPER DREDGER WITH A SINGLE SUCTION PIPE

(DE EVENWICHTS DRIFT- EN ROERHOEKEN VAN EEN

HOPPERZUIGER UITGERUST MET EEN ENKELE ZUIGBUIS)

by

IR. C. B. VAN DE VOORDE

RIFLO

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VOORWOORD

Een aanzienhijk dee! van de inspanningen welke tegenwoordig verricht worden in het kader van het onderzoek naar bet stuur-en manoeuvreergedrag van schepstuur-en, heeft veelal betrekking op vaartuigen, die, ook gezien hun eigen afmetingen in relatie met de beperkingen van het vaarwater, moeiiijkheden ondervinden wat betreft hun stuur- en manoeuvreergedrag. Dit rapport vormt

hierop een uitzondering; het heeft betrekking op een

scheeps-type dat moeilijkheden kan ondervinden a!s gevo!g van zijn on-gebruikelijk operationeel doe!.

Veelal vo!doen de gespecialiseerde vaartuigen, in de

bedrijfs-tak van het natte grondverzet, met ccii eigen voortstuwing en

met name de sleephopperzuigers aan hoge eisen te dien aanzien,

vooral bij vrije vaart. Zuigend, hij !age sneiheid, kunnen zieh

echter problemen voordoen, die ernstiger zijn bu het type zuiger uitgerust met één zuigbuis.

In dit kader werd in samenwerking met het ,,Bureau voor Scheepsbouw ir. P. H. de Groot N.y.", optredend namens een tweeta! grote aannemingsmaatschappijen in het natte

grond-verzet, een onderzoek verricht ter beantwoording van de vraag of een sleephopperzuiger met één zuigbuis in de gewenste vaar-richting kan worden gehouden.

Ten behoeve van dit onderzoek werden door bet Nederlands Scheepsbouwkundig Proefstation te Wageningen modelproeven verricht.

De evenwichts roer- en drifthoeken werden grafisch bepaald.

NEDERLANDS SCHEEPSSTtJDIECENTRUM TNO

PREFACE

The greatest efforts performed to-day in the field of research on

steering- and manoeuvring characteristics generally relate to

vessels which may encounter difficulties because of their large size u relation to the depth or width of fairways. This report may be regarded as an exception; it deals with a vessel that may encounter manoeuvring problems because of its unusual mission. As a rule self-propelled specialized dredging ships meet high demands with regard to manoeuvrabiiity in restricted water and this is certainly true for suction hopper dredgers in free running condition. Dredging at low speed however, may cause problems,

which become more serious for the type of suction dredger

fitted Out with one pipe.

The question was ifa suction dredger having one suction pipe could be kept in the prescribed course.

This problem, subject for the investigation described in this

report, was approached in co-operation with "Bureau voor

Scheepsbouw ir. P. H. de Groot N.V.' (Naval architects), as representative of two prominent Dutch dredging contractors.

For this purpose model tests were carried out by the

Nether-lands Ship Model Basin. The equilibrium values of the

drift-and rudder angles were obtained in a graphical way.

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CONTENTS

page

List of symbols

6

Summary

7

i

Introduction

7

2

Particulars of ship and model

7

3

Description of test method

7

4

Test programme

8

5

Results and discussion

8

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LIST OF SYMBOLS

ß

drift angle. positive, when the undisturbed flow comes in at starboard

side.

R

rudder angle; positive to port.

W external force opposite to the direction of advance, representing the

suction pipe loading.

F1

reaction force in the foreward cross-arm: positive to port.

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THE EQUILIBRIUM DRIFT AND RUDDER ANGLES OF A

HOPPER DREDGER WITH A SINGLE SUCTION PIPE

by

Ir. C. B. VAN DE VOORDE

Summary

Series of side-force measurements on a model of a hopper dredger with one suction pipe were conducted for three suction pipe loadings (simulated by a weight over a pulley) and for three ship speeds for various drift angles and various rudder angles. The equilibrium values of the drift and rudder angle were determined graphically from the test results.

Moreover, the propeller thrust and power were measured in the equilibrium configuration for the various conditions investigated.

i

Introduction

During operation of the hopper dredger involved the

loading on the single suction pipe, due to its

asymmet-rical position, causes a yawing moment.

To accomplish a straight course of the vessel this

moment has to be counterbalanced by the effects of

drift and rudder deflection.

The purpose of the tests was to ascertain the

equilib-rium values of the drift and rudder angles for various

loadings on the suction pipe and for various ship

speeds.

Finally, the propeller thrust and power have been

measured under equilibrium conditions.

The tests on a model scale of I to 16 were conducted

in the Shallow Water Laboratory of the Netherlands

Ship Model Basin for a water depth corresponding to

17.5 m.

2

Particulars of ship and model

The principal characteristics of the ship are given in

table 2.

A small scale body plan with the outline of the bow

and the stern is shown in figure 1.

The model was ballasted to have a 2 degrees list to

starboard, which was assumed to be representative

for the working condition. During the tests it appeared

that changes of this heel angle were only negligible.

Propellers

Stock propeller models were used for the tests. The

principal particulars of these propellers are also stated

in table 2 (dimensions scaled up to full

size). The

propeller models are shown in the Appendix.

3

Description of test method

The model is fastened to the carriage by means of two

cross-arms, each containing a force transducer for

measuring the side forces indicated by F1 and F0 (see

fig. 2).

Thus the model is restrained in the adjusted position

defined by the drift angle ß, except that it still has the

CQWE OF SECTIONAL AREAS

7

ORO.O0A.P ORD.20 pp

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8

freedom to move in the longitudinal direction of the

basin i.e. in the direction of advance.

However, in each condition the RPM of the

pro-pellers have been adjusted such, that equilibrium in

the direction of advance was attained. Care was taken

that the equilibrium position of the model relative to

the carriage was such, that the two cross-arms were

perpendicular to the direction of advance.

To simulate the external force on the suction pipe

(ground resistance) a weight W was attached to a wire

over a pulley.

The point of application of this force W is indicated

in figure 2. This force has always been working

oppo-site to the direction of advance irrespective of the drift

angle.

In view of the low speeds investigated, no skin

friction correction force was applied.

4

Test programme

Measurements of the side forces F1 and F0 were carried

out for various rudder defiections to port for each of

the drift angles ß=0; +5; +10 and +15 degrees,

for speeds of 2, 3 and 4 knots and for W-loadings of

lO, 25 and 40 tons. After the test results had been

analysed and the equilibrium values for the rudder and

drift angles were established in the various conditions

specified by the speed and the W-loading, tests were

o 20 10 o lo -20

carried out on the model completely detached from

the carriage, firstly to check the equilibrium and

second-ly to measure the thrust, RPM and torque of the

propellers under equilibrium conditions.

5

Results and discussion

In figure 2 the forces F1 and F0 were plotted versus

the rudder angle for various ß (drift angle) values.

The points of intersection of the F1- and F0-curves

for equal ß-values were determined graphically. The

curve faired through these points represents the

geo-metrical loci of the points, for which F,. = Fa.

The intersection of this curve with the base yields

Table I. The equilibrium values of the rudder and drift angles

________.._k\

iîç

-0lv

rudder angle-j-6.

_..-drigIe +ß

direction of advance

F, F,

-F F,

- o10ts_

00

-R=5°

--

- -

--

-2-100 l00

-

O

/

-150 speed w-equilibrium values in degrees total total

in loading ÒR tI thrust power

knots in tons to port rpm in tons DI-IP

2 IO

+ 7.5

+4.0 95.0 13.22 630 3 10

+ 5.5

+2.5 102.0 14.11 746 4 10

+ 4.0

+ 1.5 111.3 15.66 909 2 25 +10.0 +6.5 140.4 31.24 2124 3 25

+ 8.0

+4.1 149.1 33.67 2447 4 25

+ 6.1

+2.75 156.2 35.35 2724 2 40 +11.0 +6.0 171.6 47.95 3934 3 40

+ 9.0

+5.25 177.3 49.12 4209 4 40

+ 7.6

+3.5 182.7 50.46 4490 is 100 50 00 50 loo 150

starboard RUDDER ANGLE port

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o E o t

5

o

lo

15

20

5 t

5

10

15 20 00 50 10° DRIFT ANGLE 0' 5 100 DRIFT ANGLE 15° i 5 i 00 starboard

Fig. 3. The equilibrium rudder and drift angle for ship speeds of 2, 3 and 4 knots and a W-Ioading of 10 tons.

50

starboard

50 00

RUDDER ANGLE port

50

RUDDER ANGLE

50

100 port Fig. 4. The equilibrium drift and rudder angle for ship speeds of 2, 3 and 4 knots and a W-loading of 25 tons.

loo 15° 9 hit1.:

p,1

-"do

f-4, Il IIrii.. -a"

'7

-\\

1-'.f.

'I'

(9)

o

5 o 10

15

20

diameter of propellers pitch (uniform) pitch ratio

expanded blade area ratio Boss-diameter ratio number of blades

direction of rotation

the equilibrium value of the rudder angle (for which

F = F0 = O). To find the corresponding equilibrium

drift angle, the points for which Ff = F0 have been

Table 2. Particulars of ship and propellers of a twin screw

hopper dredger

plotted on a base, of the drift angle. The intersection

of the curve faired through these points with the base,

yields the equilibrium value of the drift angle. The

results of the measurements are shown in table i and

in the figures 3 through 5.

The equilibrium values as found above were checked

while the model was completely detached from the

carriage. They were found to be correct. It has to be

remarked, however, that the equilibrium is statically

unstable; i.e. at a deviation from the equilibrium drift

angle the occurring static moment to be derived from

the measured static reaction forces on the ship is

such that it will rotate the ship farther away from the

equilibrium position.

The values of RPM, tota! thrust and total DHP as

measured under equilibrium conditions are given in

table i as well.

6 Conclusions

The equilibrium rudder and drift angles decrease

with increasing speed for a constant W-loading

and increase with increasing W-loading for a

constant ship speed.

The equilibrium is statically unstable.

L..

./i/,2

L

\\

0° 5° 10° 15° Q0 50 100 150

DRIFT ANGLE starboard RUDDER ANGLE port

Fig. 5. The equilibrium drift and rudder angle for ship speeds for 2, 3 and 4 knots and a W-loading of 40 tons.

designation symbol unit

length between perpendiculars Lpp m 85 .953

length on waterline LWL m 91.108

breadth moulded B m 16.612

draught moulded (on even keel) T m 7.01

with all appendages

displacement volume moulded V m3 7881

displacement weight moulded metric 8078

(in salt water) tons

without appendages

longitudinal centre of buoyancy

aft of FP FB m 44.34

block coefficient CB 0.788

midship section coefficient CM 0.994

prismatic coefficient Cp 0.793 D min 3200 P mm 2259 P/D 0.706 AE/A0 0.465 dID 0.185

z

4 outward turning

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PI2 DETAIL ANTI-SINGING 80ff 05 - ro Ñ _;,...

--r

';, :'

-TJI

0

____________

TIP

III

II1..

I

1U

-I

No.

_

radius 2350 _ia -particulars xl propeller noses furl size model

i RIGHT HAND PROPELLER I LEFT

HAND PROPELLER 2 RINGS diameter D = 3200 mm pitch at root P = 2259 mro pitch at 0.7 P = 2259 mm

pitch at blade tip

= 2259 mm

disc area

A0 = 8038 mms

exp blade area

A0 = 3 737 m5

proj. blade area

Ar = 3.369 mtm number of blades Z 4 material d1D = 0185 PemJD 0706 A5IA5 = 0.465 AA0 = 0,419 diameter = 200.00 mmmii

material pitch at root

141.18 men,

pitch at 07G

=

141.18 mm

pitch as blade tip

= 141.18 mismo

-propeller mmmodel no 3538 A d= boss diameter

uhrp nudel no. 3791A

drawin9 no. 11 3791-13

scale latro C = i

'

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PUBLICATIONS OF THE NETHERLANDS SHIP RESEARCH CENTRE TNO

PUBLISHED AFTER 1963 (LIST OF EARLIER PUBLICATIONS AVAILABLE ON REQUEST)

PRICE PER COPY DFL. lo.- (POSTAGE NOT INCLUDED)

M = engineering department S = shipbuilding department C = corrosion and antifouling department

Reports

57 M Determination of the dynamic properties and propeller excited vibrations of a special ship stern arrangement. R. Wereldsma,

I 964.

58 S Numerical calculation of vertical hull vibrations of ships by

discretizing the vibration system, J. de Vries, 1964.

59 M Controllable pitch propellers, their suitability and economy for large sea-going ships propelled by conventional, directly coupled engines. C. Kapsenberg. 1964.

60 S Natural frequencies of free vertical ship vibrations. C. B. Vreug-denhil, 1964.

61 S The distribution of the hydrodynamic forces on a heaving and

pitching shipmodel in still water. J. Gerritsma and W. Beukel-man, 1964.

62 C The mode of action of anti-fouling paints : Interaction between anti-fouling paints and sea water. A. M. van Londen, 1964.

63 M Corrosion in exhaust driven turbochargers on marine diesel

engines using heavy fuels. R. W. Stuart Mitchell and V. A. Ogale, 1965.

64 C Barnacle foul ing on aged anti-fouling paints ; a survey of pertinent literature and some recent observations. P. dc Wolf. 1964. 65 S The lateral damping and added mass of a horizontally oscillating

shipmodeL G. van Leeuwen, 1964.

66 S Investigations into the strength of ships' derricks. Part I. F. X. P. Soejadi, 1965.

67 5 Heat-transfer in cargotanks of a 50,000 DWT tanker. D. J. van der Heeden and L. L. Mulder, 1965.

68 M Guide to the application of method for calculation of cylinder liner temperatures in diesel engines. H. W. van Tijen, 1965. 69 M Stress measurements on a propeller model for a 42,000 DWT

tanker. R. Wereldsma, 1965.

70 M Experiments on vibrating propeller models. R. Wereldsma, 1965.

71 S Research on bulbous bow ships. Part Il. A. Still water

perfor-mance of a 24,000 DWT bulkcarrier with a large bulbous bow. W. P. A van Lammeren and J. J. Muntjewerf, 1965.

72 S Research on bulbous bow ships. Part II. B. Behaviour of a 24,000 DWT hulkcarrier with a large bulbous bow in a seaway. W. P. A. van Lammeren and F. V. A. Pangalila, 1965.

73 S Stress and strain distribution in a vertically corrugated bulkhead. H. E. Jaeger and P. A. van Katwijk, 1965.

74 S Research on bulbous bow ships. Part 1. A. Still water investiga-tions into bulbous bow forms for a fast cargo liner. W. P. A. van Lammeren and R. Wahab, 1965.

75 S Hull vibrations of the cargo-passenger motor ship "Oranje

Nassau", W. van Horssen, 1965.

76 S Research on bulbous bow ships. Part I. B. The behaviour of a fast cargo liner with a conventional and with a bulbous bow in a sea-way. R. Wahab, 1965.

77 M Comparative shipboard measurements of surface temperatures

and surface corrosion in air cooled and water cooled turbine outlet casings of exhaust driven marine diesel engine

turbo-chargers. R. W. Stuart Mitchell and V. A. Ogale, 1965.

78 M Stern tube vibration measurements of a cargo ship with special afterbody. R. Wereldsma, 1965.

79 C The pre-treatment of ship plates: A comparative investigation on some pre-treatment methods in use in the shipbuilding

industry. A. M. van Londen, 1965.

80 C The pre-treatment of ship plates: A practical investigation into

the influence of different working procedures in over-coating

zinc rich epoxy-resin based pre-construction primers. A. M. van Londen and W. Mulder, 1965.

81 S The performance of U-tanks as a passive anti-rolling device.

C. Stigter, 1966.

82 S Low-cycle fatigue of steel structures. J. J. W. Nibbering and J. van Lint. 1966.

83 S Roll damping by free surface tanks. J. J. van den Bosch and

J. H. Vugts, 1966.

84 S Behaviour of a ship in a seaway. J. Gerritsma, 1966.

85 S Brittle fracture of full scale structures damaged by fatigue.

J. J. W. Nibbering, J. van Lint and R. T. van Leeuwen, 1966. 86 M Theoretical evaluation of heat transfer in dry cargo ship's tanks

using thermal oil as a heat transfer medium. D. J. van der

Heeden, 1966.

87 S Model experiments on sound transmission from engineroom to accommodation in motorships. J. H. Janssen, 1966.

88 S Pitch and heave with fixed and controlled bow fins. J. H. Vugts, 1966.

89 S Estimation of the natural frequencies of a ship's double bottom by means of a sandwich theory. S. Hylarides, 1967.

90 S Computation ofpitch and heave motions for arbitrary ship forms. W. E. Smith, 1967.

91 M Corrosion in exhaust driven turbochargers on marine diesel

engines using heavy fuels. R. W. Stuart Mitchell, A. J. M. S. van Montfoort and V. A. Ogale, 1967.

92 M Residual fuel treatment on board ship. Part II. Comparative

cylinder wear measurements on a laboratory diesel engine using filtered or centrifuged residual fuel. A. de Mooy, M. Verwoest and G. G. van der Meulen, 1967.

93 C Cost relations of the treatments of ship hulls and the fuel

con-sumption of ships. H. J. Lageveen-van Kuiik, 1967.

94 C Optimum conditions for blast cleaning of steel plate. J.

Rem-melts, 1967.

95 M Residual fuel treatment on board ship. Part I. The effect of cen-trifuging, filtering and homogenizing on the unsolubles in residual fuel. M. Verwoest and F. J. Colon, 1967.

96 S Analysis of the modified strip theory for the calculation of ship motions and wave bending momcnts. J. Gerritsma and W. Beu-kelman, 1967.

97 S On the efficacy of two different roll-damping tanks. J. Bootsma and J. J. van den Bosch, 1967.

98 S Equation of motion coefficients for a pitching and heaving des-troyer model. W. E. Smith, 1967.

99 S The manoeuvrabilíty of ships on a straight course. J. P. Hooft,

1967.

100 S Amidships forces and moments on a CB = 0.8(1 "Series 60" model in waves from various directions. R. Wahab, 1967. 101 C Optimum conditions for blast cleaning of steel plate. Conclusion.

J. Remmelts, 1967.

102 M The axial stiffness of marine diesel engine crankshafts. Part I. Comparison between the results of full scale measurements and

those of calculations according to published formulae. N. J.

Visser, 1967.

103 M The axial stiffness of marine diesel engine crankshafts. Part li. Theory and results of scale model measurements and comparison with published formulae. C. A. M. van der Linden, 1967. 104 M Marine dieselengine exhaust noise. Part I. A mathematical model.

J. H. Janssen, 1967.

105 M Marine diesel engine exhaust noise. Part II. Scale models of

exhaust systems. J. Buiten and J. H. Janssen, 1968.

106 M Marine diesel engine exhaust noise. Part III. Exhaust sound

criteria for bridge wings. J. H. Janssen en J. Buiten, 1967.

107 S Ship vibration analysis by finite element technique. Part I.

General review and application to simple structures, statically loaded. S. Hylarides, 1967.

108 M Marine refrigeration engineering. Part I. Testing of a decentraI-ised refrigerating installation. J. A. Knobbout and R. W. J.

Kouffeld, 1967.

109 S A comparative study on four different passive roll damping tanks. Part I. J. H. Vugts, 1968.

IIOS Strain, stress and flexure of two corrugated and one plane

bulk-head subjected to a lateral, distributed load. H. E. Jaeger and

P. A. van Katwijk, 1968.

Ill M Experimental evaluation of heat transfer in a dry-cargo ships'

tank, using thermal oil as a heat transfer medium. D. J. van der Heeden, 1968.

112 S The hydrodynamic coefficients for swaying. heaving and rolling cylinders in a free surface. J. H. Vugts, 1968.

113 M Marine refrigeration engineering. Part li. Some results of testing a decentralised marine refrigerating unit with R 502. J. A. Knob-bout and C. B. Colenbrander, 1968.

114 S The steering of a ship during the stopping manoeuvre. J. P.

Hooft, 1969.

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