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NC\L 1P80

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Deift

DAVID W. TAYLOR NAVAL SHIP

RESEARCH AND DEVELOPMENT CENTER

Bethesda,Md.

20084

PREDICTION OF EXTREME AMMUNITION CARGO FORCES AT SEA

by

A. Erich Baltis

S. L. Bales

W. R. McCreight

V. G. Meyers

APPROVED FOR PUBLIC RELEASE:

DISTRIBUTION UNLIMITED

SHIP PERFORMANCE DEPARTMENT

(2)

MAJOR

OTNSRDC ORGANIZATIONAL COMPONENTS

OFFICER.IN.CHARGE

CARDEROCK

05

SYSTEMS

DEVELOPMENT

DEPARTMENT

11

SHIP PERFORMANCE

DEPARTMENT

15

STRUCTURES

DEPARTMENT17

SHIP ACOUSTICS

DEPARTMENT

19

MATERIALS

DEPARTMENT

28

DTNSRDC

COMMANDER

TECHNICAL DIRECTOR

01

OFF ICE P. IN-C WA PG E

ANNAPOLIS

04

AVIATION AND

SURFACE EFFECTS

DEPARTMENT

COMPUTAT1 ON

AND MATHEMATICS

DEPARTMENT

is

PROPULSION AND

AUXILIARY SYSTEMS

DEPARTMENT

27

CENTRAL

INSTRUMENTATION

DEPARTMENT

(3)

Bibliotheek vn

AfdeIig

SF-

e

Techrc..e

bOCUMN1ATE

:

DATUMI

b

PREDICTION OF EXTREME AMMUNITION CARGO FORCES AT SEA

PROJECT FOR UNITED STATES COAST GUARD

by

A, E. BaItTs

S. L. Bales

W. R. McCreght

W, G. Meyers

de

aarne

o, Di

SHIP PERFORMANCE DEPARTMENT

(4)

UNCLASSIFIED

-i

cci lrATIr.L f

THIS PACF (When Data

ntOr

FORM

1 JAN 73

1473

EDITION OF INOV 651$ OBSOLETE

SiN 0102-014- 6601

UNCLASS IFi ED

LA

E"

A 1ItLI

I

rVv

U I1U.UM II IMI IJfl U

READ INSTRUCTIONS

-BEFORE COMPLETING FORM

I. REPORT NUMBER

SPD7OkO1

2. GOVT ACCESSION NO. 3. REcIPIENrS CATALOG NUMBER

- -

-4. TITLE (and Subtitle)

PREDICTION OF EXTREME AMMUNITION CARGO FORCES

-

-S. TYPE OF REPORT & PERIOD COVERED

Final

6. PERFORMING ORG. REPORT NUMBER

8. CONTRACTORGRANTNUMBER(I)

7. AUTNOR(a)

A. Erich Baitis, S. L.Ba.les, W. R. McCreight,

and W. G.Meyer.s

9. PERFORMING ORGANIZATION NAME AND ADDRESS

Ship Performance Department

David W. Taylor Naval Ship R&D Center

...

-petnesga, ridrylanu

LUUU

PROGRAM ELEMENT. PROJECT. TASK

I_irQ11 iirn7.nn

.

an

l-1-612-1c6

-I -I. CONTROLL-ING OFF-ICE NAME AND ADDRESS

United States Coast Guard

'OO Seventh Street, S.W.

Washington, D.C.

20590

.

12. REPORT DATE

July 1476

13. NUMBEROFPAGES

-279

14. MONITORING -AGENCY NAME a ADDRESS(II different

fran,

ContrOfliná Office)

IS. SECURITY CLASS. (of title report)

Unclassified

15a. DECLASSIFICATIONIDOWNGRADING

-SCHEDULE

16. DISTRIBUTION STATEMENT (of thu

Report)

- - -

-APPROVED. FOR PUBLIC RELEASE: DISTRIBUTION UNLIMITED

-17. DISTRIBUTION STATEMENT of the ab.tract ant.r.d in Block 20;

ii dlfforit front Raãf)

18. SUPPLEMENTARY NOTES

-.

-

-19. KEY WORDS (Continui bit reiire iidó ii nec.e.y and Identt

by block

ñiber)

Cargo shoring forces, Ammunition cargo ships, Design sea conditions,

Design

ship operating conditions, 20-year storms, Effect of storm severity on

cargo shoring, Time domain shoring loads, Upper

bounds of shoring loads,

Shoring load estimates from roll, vertical and lateral accelerations,

Ship

response data base, Ship speed

degradation In storms

20. ABSTRACT (Continue on revere. aid if n.c.a.y and ld.ntlt by

block manb.r)

Progress and results from a research project devoted to the

determina-tion of extreme amunitlon cargo forces at sea are presented.

The work was

undertaken by the David W..Taylor Naval Ship Research and Development Center

(DTNSRDC) and sponsored by the U.S. Coast Guard (USCG) for assistance in Its

hazardous cargo safety program.

Four ships, representative of ammunition

cargo ships entering and leaving U.S. ports with ammunition cargo

capacities

ranging from about 6,300 to 19,200 tons, were examined.

(5)

UNCLASSI FlED

LIJITY CLASSIFICATION OF THIS PAGE(When Data Enter.d

-Ship motions and accelerations were' developed in the frequency domain for

a wide range of ship load conditions, headings, speeds, and Sea conditions by

applying procedures developed during the USCG LNG Cargo Tank Research Program

recently conducted at DTNSRDC.

The Influences of storm severity and ship operator strategies In storms

on

the magnitude of the resulting ship responses and cargo shoring loads were

examined using a math model of the ship traversing the North Atlantic Ocean.

The ship is- under control of various voluntary operator decisions as to how to

best proceed in rough weather to the port of destination without- incurring

either excessive Ship response levels or unacceptably long time delays.

The suitability of developing a single design vector from which design

loads of cargo shoring could be easily derived was examined and found to be not

particularly useful because for large time periods components of the shoring

forces are equal to zero, I.e., time periods, when gravIty or friction

are

adequate to prevent the occurrence of shoring forces.

A cargo shoring model was developed to establish both lateral and normal

forces that shoring must withstand to prevent shifting of amunitlon

cargo.

The model consists of a time simulation developed in the coordinate system of

the ship.

A pilot study applied the model to a single ship and results Include

the range of loads to be expected, the time periods associated with particular

loading cycles1 the amount of time cargo shoring will experience loads, the

sensitivity of shoring loads to changes In speed, heading, position in ship,

and Ship GM, the relative magnitudes of lateral and tomming loads, as well as

the degree of conservatism inherent In the use of the worst possible 20 year

storm, a typical 20 year storm, and a normal storm to specify shoring design

loads.

Results suggest that cargo shoring

loads

based on frequ,cy domain ship

response predictions will be very much greater than results based on the more

accurate time domain simulations.

It was concluded, therefore, that in order

to prevent the predictions of unrealistically large desIgn shoring loads, the

shoring loads should be developed directly in the time domain.

It is considerec

crucial to explore the cargo shoring model application further, e.g., to other

ships, In any efforts to develop a simple shoring load rule which may be used

by regulatory agencies.

(6)

ADMINISTRATIVE INFORMATION

APPENDIX B

-APPENDIX C

APPENDIX D

APPENDIX E

APPENDIX F

APPENDIX G

APPENDIX H

APPENDIX

I

TABLE OF CONTENTS

ABSTRACT

INTRODUCTION

SHIP RESPONSE PREDICTION COORDINATE SYSTEM

DATA BASE GENERATION

DEFINITION OF DESIGN RESPONSES

DISCUSSION OF RESULTS

Operating Conditions at Which Design Responses

Modal

Encounter Periods Associated with Design

GM and Load Effect on Design Responses

Bilge Keel Effect ofl Lateral Acceleration and

Page

13

13

15

16

18

REFERENCES

276

SIMULATED SHI.P TRIP

.

.

20

DISCUSSION OF RESULTS

22

CARGO SHORING LOADS

26

DESIGN VECTOR

26

SLAMMING LOADS

31

CARGO SHORING MODEL PARTICULARS.

33

MAJOR CHARACTERISTICS AND LIMITATIONS OF SHORING MODEL

35

DEFINITION OF DESIGN SHORING LOADS

37

Scope 'of Shoring Load Calculations

38

DISCUSSION OF SHORING MODEL RESULTS

40

CONCLUSIONS

. . . .

.

59

RECOMMENDATIONS

62

ACKNOWLEDGEMENTS

63

APPENDIX A - PREDICTION OF EXTREME AMMUNITION CARGO. FORCES AT

SEA - STATEMENT OF WORK

. . .

91

DATA BASE OF SHIP MOTIONS AND POINT 0 ACCELERATIONS .

.

97

DESIGN ACCELERATiONS AT ANY POINT IN THE SHIP

'

221

PREDICTION OF CARGO SHORING LOADS

231

DESIGN VALUE DETERMINATION VIA WORST HEADING,

JAMES SPEED REDUCTION STRATEGY

.

241

SPEED LOSS CRITERIA DISCUSSION

245

ROLL PREDICTION PROCEDURE

'

249

'SIMULATED SHIP TRIP IN EXTREME AND NORMAL SEAS

259

IDENTIFICATION OF SHORING LOAD DESIGN OPERATING

CONDITION .

. . .

275

2

3

6

8

11

Occur

Responses

Roll

(7)

LIST OF FIGURES

MAIN TEXT

Figure

1

- Geometry of AMMO Ship Series

Figure

2 - Design Sea Conditions

FIgure

3 - Recommended Design Accelerat ions for AMMO

Ship Series

. . . .

...

66

Figure

4 - Design Value Data Base for Ship A

...67

Figure

5 - Typical Response Amplitude Operator Predictions.

. . .

68

Figure

6 - Typical RMS Response versus Encountered Period

Predictions (Density Graph)

69

Figure

7 - Effect of Bilge Keels on Lateral Ship Response

Predictions

-70

Figure

8 - Operator Strategy Influence on Motions and

Accelerations in Random Seas and a Normal Storm

Encountered at Various Relative Headings to the

Desired Course.

71

Figure

9 - Operator Strategy Influence. Oh Motions and

Accelerations in a 20-Year Design Storm Encountered

atVàrious Relative Headings to the Desired Course

.

72

Figure 10 - Maximum Shoring Loads for 1/2-Hour and 21i-Hour

Operations in Design Seas As Well As. the Associated

Wave Height, Ship Responses, and ComponentS of

Accelerations Acting on Cargo and Shoring...73

Figure 11 - Maximum Port and Starboard Shoring Loads for 24-Hour

Operations in Design Seas As Well As Associated

Torning Loads, Wave Height, and Ship Responses

. . . .

74

Figure 12 - Influence of Ship Heading, GM, and Coefficient of

Friction Between Deck and Cargo on Lateral

Shoring Loads

. . .. . . ..,. . .

75

Figure 13 - Motion and Acceleration Levels at Which Lateral

Shoring Loads Occurred at Various Ship Headings.

. . .

.

76

Figure 14 - Typical Samples of Ship Orientation While Shoring

or Deck Loads OccUrred

. . .

77

Page

64

(8)

'I,

Page

Figure 15 - Variations in Maximum Nomal, S

, and Lateral Shoring..

Loads, SL, and Associated LOädurations for 6-Hour

Operation of Ship C in Bow Seas at Design Sea

Conditions

78

Figure 16 - Identification of Areas where Toming of Ammunition

Cargo Required

. . . ., . . . .. .

79

Figure 17 - Effect of Speed, Heading,. and Longitudinal Cargo

-Location on Shoring Loads of Ship A and C

80

Figure

18 -

Degree of Conservatism Inherent in Specification of

Design Lateral Shoring Load from Use of Worst. Possible

20-Year Storm, TypIcal 20-Year Design Storm, and

Normal Storm .

. . .-

81

Figure 1.9 - Effect of Stacking Cargo Pallets on Loads Experienced

by Lowest and End Pa.11ets.

.. . .

... .

.

. 82

APPENDIX B

Figure B.1. - Ship A, Full Load, GM1, Root Mean Square Responses

versus EAcountered Modal Periods

106

Figure B.2 -

Ship

A, 50% Load, GMI, Root Mean Square Responses

versus Encountered Modal Periods

107

Figure B.3 -

Ship

B, Full Load, GM1, Root Mean Square Responses

versus Encountered Modal Periods

.

108

Figure B.1i -

Ship

B, 50% Load, GM1, Root Mean Square Responses

versus Encountered Modal Periods

109

Figure B.5 -

Ship C,

Full Load, GM1, Root Mean Square Responses.

versus Encountered Modal Periods... .110

Figure B.6 - Ship C, 50% Load, Gill,, Root. Mean Square-Responses

verSus Encountered Modal Periods

111

Figure B.7 -

Ship

D, Full Load,, Gill, Root Mean Square Responses

versus Encountered Modal Periods

. . .

.112

Figure B.8 - Ship D, 50% Load, Gill, Root Mean Square Responses

.

(9)

Page

APPENDIX C

Figure C.1 - Location of Points for Proposed Point Variation

Investigation

. . . ,. .

. 227

Figure C.2 - Data Base for Design Acceleration Deterniinatión of

Any Point Along Ship

228

Figure C.3 - Effect of Load on Design Accelerations for.Ship A

.

229

Figure C.4- Design Value Data Base for Ship A.

23o

APPENDIX D

Figure D.1, - Coordinate System, Earth

.

. 237

*

*

*

Figure D.2 - Forces on Cargo Box at Location (

,y ,z.),

Earth Coordinates

237

Figure D.3 - Forces on Cargo Box at Location

(x*,y*,z*),

Ship Coordinates

.

237

Figure D.4 - Computational Scheme for Cargo Shoring LOads.

. .

238

Figure D.5 - Upper Bounds for Shoring Loads

239

APPENDIX E

Figure E.1 - Sample Extreme Response Surface for Ship A

Vertical Accelerations, LNG Ship Series

2144

APPENDIX .F

Figure. F.l

Definition of James Speed Loss Criteria Used to

Predict Extreme AcceleratiOnS of AMMO Series.

. . 2147

Figure F.2 - Comparison of Speed Loss Criteria for the AMMO

and LNG Series ...248

APPENDIX G

Figure G.1 - Data Base of Largest Measured Roll Amplitudes

(10)

Figure 6.2

Figure

Figure

Figure

-

Effect of Bilge Keels on Largest Measured Roll

for Typical Naval Oil Tanker in BeamWaves

G.3 - Comparison of Largest Measured Roll for All

Ship Conditions of Typical Naval Oil Tanker

in Beam Waves

256

G.4 - Calibration of a Ship's Roll Inclinometer

257

6.5 -

Effect of Wave Steepness on Lateral Ship

Response Predictions

.

258

APPENDIX H

.

Figure H.1 - Overall Flowchart for TRIP.

268

'Figure. H.2 - Ship Navigation Logic

269

Figure H.3 - Wave Selection Logic

. . ..

270

Figure H.i - Operator Strategy Selection Logic

.

271

Figure H.5 - Sample Trip Results:

Histograms and Probabilities

of Exceédaflce...272

Figure H.6 - Operator Strategy Influence on Motions and Accelerations

in Random Seas and a Normal Storm Encountered at Various

Relative Heading,s to the Desired Course...273

LIST OF TABLES

Page

255

AMMO Series Ship Particulars ...

83

Point Locations for Predicted Accelerations of

AMMO Ship Series

84

AMMO Series Design Motions

85

AMMO Series Design Accelerations

.

86

Operating Conditiofls at Which Design Responses Occur.

. . .

87

Components of Lateral Shoring Loads

88

Shoring Timbers Required in Various Storms

89

MAIN TEXT

Table 1

Table 2

Table 3

Table

1I

Table

5

Table 6

Table .7

(11)

Page

APPENDIX B

Table

B.1 - Description of AMMO Series Data Base Presentation

. . .

.114

Tables B.2 to B7

-Ship A, Full Load, GM1, Root Mean Square

Heave, Roll, Pitch, and Longitudinal,

Lateral, and Vertical Accelerations at

POint 0, UnIt Significant Wave Height

115

Tables B.8 to B.11

- Ship A, Full Load, GM2, Root Mean Square

Roll and Longitudinal, Lateral and Vertical

Accelerations at Point 0, UflIt Significant

Wave Height

121

Tables B.12 to B.17 - Ship A, 50% Load, GM2, Root Mean Square

Heave, Roll, Pitch, and Longitudinal,

Lateral, and Vertical Accelerations at

Point 0, Unit Significant Wave Height

125

Tables B.18 to B.21 - Ship A, 50% Load, GM2, Root Mean Square

Roll and Longitudinal, Lateral and

Vertical Accelerations at PoInt 0, Unit

Significant Wave Height

131

Tables B.22. to B.27 - Ship B,FU1i Load, GM1, Root Mean Square

Heave, Roll, Pitch, and Longitudinal,

Lateral, and Vertical Accelerations at

Point 0, Unit Significant Wave Height

135

Tables B.28to B.3l

Ship B, Full Load,GM2, Root Mean Square

Roll, and Longitudinal, Lateral, and

Vertical Accelerations at Point 0, Unit

Significant Wave Height

. .

.141

Tables B.32 to B.35

Ship B, Full Load, GM3, Root Mean Square

Roll, and Longitudinal, Lateral, and

Vertical Accelerations at POint 0, UnIt

Significant Wave Height

Tables B.36 to B.41 - Ship B, 50% Load, GM1, RoOt Mean Square

Heave, Roll, Pitch, and Longitudinal,

Lateral, and Vertical Aâcelertions at

Point 0, Unit Significant Wave Height

149

Tables B.42 to B.45 - Ship B, 50% Load, 6M2, Root Mean Square

Roll, and Longitudinal, Lateral, afld

Vertical Accelerations at Point 0, Unit

(12)

Page

Täblès 3.46 to B.49

ShtpB, 50%. Load, GM3, Root Mean Square

Roll, and Longitudinal, Lateral, and

VerticalAcceleratlons at Point 0, Unit

Significant Wave HeIght

159

Tables B.50 to B.53

Ship B, 50% Load.,.GM4, Root Mean Square

Roll, and Longitudinal, Lateral, and

Vertical Acceleratibnsat Point 0, Unit

Significant Wave Height

.

.163

Tables B.54 to B.59

Ship C, Full Load, GMI, Root Mean Square

Heave, Roll, Pitch, and Longitudinal,

Lateral, afldVertical Accelerations at

Point0,UnitSfgnlficant Wave Height

167

tables B.60. to B63 - Ship C, Full Load, GM2, Root Mean Square

Roll, and Longitudinal, Lateral, and

Vertical Accelerations at Point 0, Unit

Significant Wave Height

. .

173

Tables B.6L to B.67

Ship C, Full Load, GM3, Root Mean Square

Roll? and Longitudinal, Lateral, and

Vertical Accelerations at PoInt 0, Unit

Significant Wave Height

177

Tables B.68 to B.73 - Ship C, 50% Load, GM1, Root Mean Square

Heave, Roll, Pitch, and Longitudinal,

Lateral, and Vertical Accelerations at

Point 0, Unit Significant Wave Height

1 81

Tables B.74 to B.77 - Ship C, 50% Load, GM2, Root Mean Square

Roll, and Longitudinal, Lateral, and

Vertical Accelerations at Point 0, Unit

Significant Wave Height

. . .

.187

Tables B.78 to B.83 - Ship D, Full LOad, GM1, Root Mean Square

Heave, Roll, Pitch, and Longitudinal,

Lateral, and Vertical Accelerations at

Point 0, Unit Significant Wave Height

. . .

.191

Tables B.84 to B.87 - Ship D, Full Load, GM2, Root Mean Square

Roll, and Longitudinal, Lateral, and

Vertical Accelerations at Point 0, Unit

significant Wave Height

197

Tables B.88 to B.91 - Ship D, Full Load, GM3, Root Mean Square

Roll, and Longitudinal, Lateral, and

Vertical Accelerations at Point 0, Unit

(13)

Page

Tables B.'92 to B.97 - Ship.D, 50% Load, GMI,. Root Mean Square

Heave, Roll, Pitch, andLongitudinal,

Lateral., and Vertical Accelerations at

Point 0, Unit SigniflcantWave Height..

. .

205

Tables B.98 to B.10l

Ship D, 50% Load., GM2, Root Mean Square

Roll, andLongitudt'nal., Latral, and

Vertical Accelerations at Point 0, Unit

Significant Wave Height...

- .

211

Tables B.102 to B.105

Ship D, 50%. Load, GM3, Roo.t Mean Square

Roll, 'and Longitudinal., Lateral, and

Vertical Accelerations at...Point 0,, Unit

Significant Wave Height... ...21.5

Table B.106 - Constants .for, Single-Amplitude Statist1s

. . . . .. .

219

Table B.107- Sample Linear Interpolation of Data BaSe Tables

. . .

220

APPENDIX H

Table H.1

- Normal Yearly Storm and 20-Year Storm Used in

(14)

NOTATION

AR

Aft perpendicular

BL

Baseline

Bx

Maximum beam

CL

Centerline

CB

Block coefficient

Longitudinal prismatic coefficient

CT

Confidence factor

Cx

Maximum transverse section coefficient

FP

Forward perpendicular

FL

Lateral acceleration,, in the ship system, acting on the cargo

FN

Normal acceleration, in the ship system, acting on the cargo

F

Froude number

n

-

-GM

Transverse metacentric height

2

g

..

Acceleration due to gravity, 321725 ft/sec

KG

Height of center of gravity above baseline

KM

Height Of transverse metacenter above baseline

K0,K,K

Pitch, roll, and yaw radii of gyration

LCG

Longitudinal location of center of gravity

LNG

Liquid Natural Gas

Length between perpendiculars

L,L(L),L-(V) LongitudiAál, lateral, and vertical accelerations at a

specified point along the ship

N

Number of cycles; also number of successive amplitudes

Number of times a response level

is exceeded

(15)

-T,

V

TOE

XA,yA,ZA

*

*

*

x ,y ,z

ws.

wl/3

Maximum draft

Modal wave period, period corresponding to peak of wave

spectrum

Natural periods of heave., pitch, and roll

Ship speed

Extreme ship response

Surge, sway, and heave amplitudes

Coordinates of any point, measured from the origin of the

coordinate system

-..

Wave steepness,

. .

Response level

Ship displacemnent

Wave amplitude

single amplitude

Significant wave height - average of oneathird highest

dOuble amplitudes

RMS

Root mean square, square root of variance.

Starboard side

Lateral load to be sustained by cargo shoring

Upper bounds of!iateral Shoring: loads

Normal load to be sustained by cargo, shoring

SN

Upper bounds of normal shoring loads

-SN

+

Taming lo2d$

SN+

Deck or sheathing, loads

SXX(cA))

Spectral density function of response X

T

Time variable

TAp.,T,TFp

Ship draft at aft perpendicular, amidships., and forward

perpendicular

Modal response period, period corresponding to peak of

encountered response spectrum

(16)

eA,A,JA

Pitch, roll, and yaw amplitudes

A

Wavelength

Ship heading angle, predominant wave direction with

respect.

to the ship; also coefficient of friction

Wave direction

RMS or standard deviation Of ship response

Roll amplitudes in earth coordinates

Arbitrary ship response

.

Wave frequency

(17)

ABSTRACT

Progress and results from a research project devoted to the

determination of extreme amunition cargo forces at sea are presented.

The work was undertaken by the David W. Taylor Naval Ship Research

and Development Center (DTNSRDC) and sponsored by the U.S. Coast Guard

(USCG) for assistance In Its hazardous cargo safety program.

Four 'ships,

representative of ammunition cargo ships entering and leaviing U.S. ports

fld with ammunition cargo capacities ranging from about 6,300 to 19,200

tons, were examined.

Ship motions and accelerations were developed for a wide range

of ship load conditions, headings, speeds, and sea conditions by applying

procedures developed during the USCG LNG Cargo Tank Research Program recently

conducted at DTNSRDC.

These results, calculated in the frequency domain,

were taken as the core data base from which other aspects of the project

drew basic ship response data.

The influence of storm severity and ship operator strategies in

storms on the magnitude of the resulting ship responses were examined by

developing a model of the ship traversing the North Atlantic Ocean.

The

ship is under control of various voluntary operator decisions as to hOw to

best proceed in rough weather to the port of destination without incurring

either excessive ship response levels or unacceptably long time delays.

Results provide the number of individual ship response cycles that exceed

specified levels on a per trip basis depending on the various operator

decisions employed.

The suitability of developing a single design vector from which

design loads of cargo shoring could be easily derived was examined.

It

was found that state-of-the-art ship motion prediction techniques, which

are traditionally based on the earth coordinate system, cannot be used

directly to accomplish this.

It was concluded that the concept of a single,

cargo shoring force vector Is not particularly useful because for large time

periods components of the shoring forces are equal to zero, i.e., time

period, when gravity or friction are adequate to prevent one occurrence

(18)

the transverse and normal directions do not occur simultaneously.,

A cargo shoring model was developed to establish both

lateral and

normal: forces that shoring mustwithstand to prevent shifting of ammunition

cargo.

The model consists of a time simulation, and was developed in the

coordinate system of the ship.

A pilot study applied the model to a single

ship and results include the range of loads to be expected, the

time periods

associated with particular loading cycles, the amount of time cargo

shoring

will experience loads, the sensitivity of shoring loads to changes

in speed,

heading, position in ship, and ship GM, the relative magnitudes

of lateral

and tomming loads, as well as the degree of conservatism inherent

in the

use of the worst possible 20 year storm, a

typical 20 year storm, and a

normal storm to specify shoring design loads.

Results suggest that cargo shoring loads based on frequency domain

ship response predictions will be very much greater than results based

on the more accurate time domain

simulations.

It Was concluded, therefore,,

that in order to prevent the predictions of unrealistically

large design

shoring loads, the shoring loads should be developed directly in

the time

domain.

By predicting in the time domain the components of the

forces

which produce. the shoring loads in the coordinate system of the ship,

phasing uncertainties in combining these acceleration and friction

related

forces are avoided.

In other words, it is not necessary in a time domain

shoring model to assume that the àomponeflt forces will

combine in the worst

possible fashion.

Therefore, it Is considered crucial to explore the cargo

shoring model application further, e.g., to other ships, in any

efforts to

develop a simple shoring load rule which may be used by regulatory

agencies.

ADMINISTRATIVE INFORMATION

The work was conducted at the David W. Taylor Naval Ship Research

and Development Center (DTNSRDC) by Ship Performance Department

Code

1568

upon request of, the U.S. Coast Guard

(USCG), MIPR

Z-70099-443330-B.

It is

identified as Work Unit Number

1-1568-011.

A statement of work is contained

in Appendix A

The developrnentandpredictions effort made with the Cargo

Shoring Model was also partialIy.supported byU.S.Navy tasks Identified as

Work Unit Numbers

1-1507-200-84

of the Navy Seakeeping Research and

(19)

INTRODUCTI ON

The United States Coast Guard (USCG) has

authority1' for ensuring the

safety of all hazardous càrgo'shipments entering or leaving U.S. ports.

This

design safety responsibility encompasses all ownership categories of ships,

foreign or domestic, Including some ships owned, operated, or chartered

by the U.S. Armed Forces.

Safety of hazardous matertal cargo shIpments concerns itself,

anong other topics, with the structural integrity of the containment systems

within which the cargo Is transported on the ships.

The USCGtherefore

contracted the David W. Taylor Naval Ship Research and Development Center

(DTNSRDC) to predict Extreme Ammunition -Cargo Forces at Sea based on

pre-vious LNG Cargo Tank Load procedures.

These predictions are intended to

improve the validity and realism of existing cargo shoring and torrilling

regulations,

A summary of these Ammunition Cargo Force predictions is presented

based on a DTNSRDC research program conducted on an intermittent basis over

a two year period.

The research program Is based on ship motion

accelera-tion and shoring load predicaccelera-tions for a series of representative U.S.

Ammunition Cargo ships specified by the USCG.

This Ammunition Cargo Ship

series consists of four ships ranging in ammunition cargo capacities from

about 6,300 to 19,200 tons.

The results of this research and program are

presented in terms of the extreme lifetime g-loads to which the cargo will

be exposed and which If appropriate*

the shoring is expected to

with-stand.

These. so-called design g-loads are presented in terms of

in-dependently derived vertical, lateral, and longitudinal

accelerations at

the most forward and highest position In each ship where amunition cargo

may occasionally be loaded.

Simple methods for translating these design

loads to other desired positions in the ship are provided (See Appendix B

and C).

Similarly simple expressions for the upper bound of the cargo

'shoring forces that can result when the design g-loads and the associated

roll motions are experienced are also provided (See Appendix D).

cRêferePces are denoted by superscripts. A complete listing is given on

pages 276-279.

.

(20)

The order of presentation of data and recomended actions in this

report is based on the recommendations and conclusions of the National

Transportation Board and USCG

report15

on the sinking of the ammunition

cargo ship SS BADGER STATE in the North Pacific in December 1969.

Since

the development of realistic cargo shoring forces depends essentially on

the ranges of ship responses that result when a large number of variables*

occur in various combinations, it was considered appropriate to subdivide

the research program into a number of distinct tasks, each with a specific

goal.

The Ammunition Cargo Force Research Program has been conducted

there-fore, as six separate, roughly, related tasks as originally outlined i.n the

statement of work, see Appendix A.

The first task was the development of

the basic ship motions and accelerations Using the procedures developed

during the USCG LNG Cargo Tank, Research Program at

DTNSRDC.2'3'4

This

first task thus was considered to be the data base task from which

all

other

tasks would draw the basic ship response data developed in the frequency

domain.

The second task was Intended to examine the influence of Storm severity

and operator strategies In storms on the magnitude of the resulting ship

responses.

Thus, this second task essentially consisted of the development

of a model of the ship traversing the ocean in arbitrary directions under

the control of various voluntary operator decisions as to how to best

pro-ceed in rough weather to the destination without Incurring either excessive

cargo shoring loads or unacceptably long time delays.

The

results of this

task provide the number of individual ship response cycles that exceed

specified levels and how these are Influenced by operator decisions in a

storm.

This number of response cycles Is of significant interest because

it represents a realistic load history to develop the fatigue

characteris-tics of the shoring.

The third task consisted of an investigation into the suitability of

the concept that a single unique design vector can be develped from which

all of the loads on the cargo shoring can be derived quite simply.

Thus

*These'vari.ablëslnclüde.the'deadweight, load distribution, roll

stabili-zation status of ship, trade route ship operates on, storm severity (wave

hefght and modal period), size and speed of the storms, their frequency of

occurrence, voluntary strategies of the operators employed when they

en-counter storms, levels of probability that specific motion levels will not

be exceeded, the different lOcations within the ship.where cargo is secured,

as well as the particular shoring or securing configuration employed.

(21)

this third task may be regarded as an attempt to present the cargo design

loads in as simple and concise a form as possible for use by designers and

shoring regulation purposes.

The fourth task consisted of th&deièloprnent of a so-called slamming

force magnification factor.

This factor was to be drawn essentially from

a comparison of the magnitude of the rigid body vertical acceleration of

the WOLVERINE STATE and the sti'uctural impact response to slamming.

The fifth and most demanding task was to select for a particular

example of cargo location, the shoring required to keep the cargo from

shifting.

This example shoring Is then exposed as part of the ship trip

to design extreme seas to verify the selected shoring.

The degree of

con-servatism inherent in the design shoring when the ship encounters a normal

rather than design storm is expressed in terms of the number of timbers

that might be saved if the shoring regulation required Only normal yearly

extreme rather than 20 year extreme storms.

The sixth task Is to summarize the results in the form

of

a report

that can be read, Understood, and used by members of the regulatory agencies

as well as various ammunition shipping activities,

in order to accomplish

this last task, the text

of

this report deals primarily with the results

of the individual tasks rather than on the details of how they were derived.

Appendices are included to provide some of the procedural details, as well

as to present some

of the voluminous

results of Task 1.

It should be pointed out that implicit in the structure of the

re-search program was the assumption that design ship responses as developed

in Tasks

1 and 2 could be employed to develop accurate shoring loads in the

frequency domain.

The inability to employ the frequency domain results for

this purpose led to a substantial increase in the research effOrt In Tasks

3 and 5 whIch dealt with time domaIn representations of the ships motions

and the resulting shoring forces.

Before proceeding with the results of the individual program tasks,

however, it must be noted that the results of the shoring example of Task

5 have Indicated that some of the accelerations developed in the first task

are not considered to be appropriate for the accurate determination of

cargo loads or shoring requirements.

The next section discusses the reasons

(22)

SHIP RESPONSE PREDICTION COORDINATE SYSTEM

The reasons that lateral acceleration loads developed in Task 1

are inappropriate for the accurate determination of cargo shoring loads

are associated with the basic coordinate system within which the ship

motion prediction equations have been Written.

The Task 1

ship responses

were calculated by the state-of-the-art prediction procedures employed

during the USCG LNG work of Reference 2.

These procedures employ equations

developed in the earth coordinate system.

The major practical concern in the LNG tank research was to

es-tablish the pressure loads acting on the tank structure due to the rigid

body ship motions.

Since the

igid body motions of the ship were con

sidered to augment the internal pressure loads by acting along the direction

of acceleration design vector; and the. magnitude of this vector was dominated

by the vertical acceleration In earth coordinates, the importance of lateral

accelerations in the development of shoring loads was not initially recognized.

It became obvious., however, once the shoring example of Task 5 was

initiated that the individual components of the shoring load could be

de-termined in several different ways, and that each would result in different

Shoring loads.*

For example, the gravity force component, which is a function

primarily of roll, attains its maximum value at a different heading and/or

ship speed than do the inertia force components whlc.h are due primarily to

ship heave, yaw, and pitch, respectively.

Therefore, since shoring loads

depend on components which attain their individual maximum values for

different ship operating conditions, the relative phasing between the

corn-poneñts become of considerable concern.

There are specifically two sets

Of phasin9 uncertainties; one is associated with the ship operating

condi-tions that produce maximum values for particular Shoring load components,

and the second uncertainty is associated with the maximum values of the

components when the ship Is operating at any given set of speed, heading,

etc. Operating conditions.

.. . . ..

The above considerations lead to the conclusion that both sets of

phasing uncertainties can best be avoided by. develOping the shoring loads

*The components consist of inertia, gravity, and friction forces as de

tailed in later sections of the report and Appendix D.

(23)

directly in the coordinate system in which'the shoring loads are most

appropriately described, i.e., in ship coordinates rather thanthe

con-ventionally employed earth coordinates.

Ship coordinates are most appropriate because the three principal

force components of the shoring loads, namely the lateral, normal and

fric-tion forces, are defined* in terms of the lateral and normal axes of the

ship.

Since lateral forces or accelerations in earth coordinates cannot

be substituted for lateral forces or accelerations in ship coordinates

with-out encountering phasing difficulties in considering gravity, it was also

concluded that a coordinate system transformation might have to be performed

at some stage on the responses previously calculated.

The resultant

in-vestigation Into a conversion procedure for the lateral accelerations de

rived in the earth system quickly revealed tha,t there was little hope for

even a reasonable engineering estimate of how this conversion might proceed.

On this basis, the feasibility of developing the necessary response amplitude

operators in the ship system was examined.

The results indicated that there

appeared to be no quick, efficient way in which such a cOnversion might be

accOmplished.

It was decided, after consultations with the IJSCG R&D

per-sonnel' tO report the results áttainedand to develop the basic transformation

expressions for the forces and accelerations in the time domain.

The time

domain transformation expressiOns were subsequently developed and a

relative-ly extensive Series of time history investigations was then conducted.

Ammunition Cargo Force Program results consist of frequency domain

based design ship motions and accelerations in earth coordinates, procedures

for establishing upper bounds of shoring loads** 'based on such results, as

well as the significantly more accurate, lower design shoring loads'

devel-oped in ship coordinates in the time domain.

That is, the uppe

bound

shoring loads based on earth system accelerations were much larger than the

time domain shoring loads.

Consequently, the frequency domain based

accelera-tions calculated in earth coordinates are not considered to be appropriate

for determining realistic shoring loads suitable for design or regulatory

purposes.

*It isnotédin this context that 'lateral force,in'the ship system consist

of the sum of the inertial and gravity force components parallel to the

deck, FL, whereas the comparable force components perpendicular to the deck

are designated as the normal force, F.

See pages 33-37 and Appendix D.

**The upper bound shoring load expressions were developed on a related Navy

(24)

DATA BASE GENERATION

The development of realistic cargo shoring forces suitable for

design or regulatory purposes depends on the largest cargo accelerations

that result when a realistic range of present and fUture potential

amuni-tion cargo ships Is exposed to the full range of variables that influence

their cargo loads.

The AMMUNITION Ship Series (AMMO Ships) specified by the USCG

contains C3, Ck, C5, and LASH cargo ships whose particulars are given in

Table 1

and Figure 1.

Since for a given ship type, the responses and

thus the cargo loads may vary substantially with dead weight and load

distribution, the AMMO ship's responses were developed for the widest

practical range of dead weight, i.e., 100 percent of full load to 50 percent

of full load.

The shipment of aninunitlon on ships loaded to less thafl

-50 percent of full load was considered to be impractical by

defini-tion!

In addition, at each of these dead weights, the location of the

ship's vertical center of gravity, or equivalently the vertical distribution

of the anununition cargo, was varied over the widest practical range.

The highest vertical center of gravity locations corresponded essentially

to the lowest allowable safe metacentric heights, GMs, specified by the

USCG; and the lest center of gravity locations corresponded to the

largest GMs that are likely to be employed in loading these ships under

any circumstances.

As a result, by calculating the responses of each

of the four ships at essentially four to seven Individual dead weight and

load 'distribution combinations, the possible range in ship responses

and dynamic cargo loads due to dead weight/load distribution variability

was established.

In order to consider the variations In the cargo accelerations

experienced because of the location within the ship where the cargo is stored,

the cargo accelerations were calculated at the location which would produce

the worst acceleration loads on the cargo, i.e., the furthest forward and

highest position (Point 0,. see Figure 1

and Table 2) at which the cargo

(25)

might occasionally be stowed.

Results are given in tabular form in

Appendix B.,

Simple, numericai interpolation methodsare then required

to translate these "worst-cargo-accelerations-on-the-ship" to a desired

location, i.e., to reduce them to the appropriate value for other locations

along the ship.

Appendix C provides details of these interpolation

procedures.

It should be noted that at the outset of this research project,

had been intended to employ the graphical trend procedures developed

during the LNG project to translate the accelerations at PoInt 0 toother

points in the ship.

However, as the practical implications of the cargo

force sensitivity* to spatial variations became apparent in the Cargo

Shoring. Task, it was considered essential to upgrade the accuracy, of the

acceleration translation procedure.

Design accelerations were thereforf

calculated for five points in. the centerline plane at. the same vertical

locations as Point 0, i.e., the highest practical vertical location at

which amuflition cargo might becarried.

Table 2 illustrates the positions

of these five points.

Thus effectively, one may now estimate the acceleratiOnS at any

point in the ship at any heading, speed, ship load condition, and sea

conditiOn by shifting the Point

0

acceleratIons of Appendix B In accordance

wIth the design acceleration trends given in Table 4.

These trends In the

accelerations with longitudinal centerline shifts produce the most

sig-nificant variations i'n the most important compoflents** of the cargo force

accelerations.

It is to be nOted that shifts in the somewhat less

important vertical and lateral direction, respectively, are

ignored.2'3'4

To further improve the accuracy of the predicted accelerations at

arbitrary points in the ship, requires properly taking the vertIcai and

lateral shift trends into account.

Such additional accuracy, however,

requlres many. more data points in the ship, and is clearly beyond the scope

*Restricted longitudinal ranges where tonning is required to suppress upward

motion of the cargo and ranges where large lateral loads and thus

signifi-cantly stronger lateral cargo shoring is required.

(26)

of the present project.

It is recomended that these calculations

be performed.

Appendix C has been prepared to further elaborate. On this

recommendation and to 'demonstrate the numerical procedureby 'which

accelerations'may then be attained accUrately for any point in the 'ship.

The design accelerations and associated ship motions are developed

by means of a flexible, four stage building block procedure.

This procedure

was recently documented in references 2,3, and 4.

HistorIcal wave data;

a complete set of ship response amplitude operators,* i.e., for all possible

speed, heading, and ship load conditions;' and short term statistics are

then employed to :predict the entire range or universe of extreme ship

responses that the ShIp.Is likely to encounter during lts"li"fetlme.

From

this' unIverse Of posslble** ship reSponses and accelerations, the design

accelerations are selected by excluding physically unrealizable ship

conditions that may occur In a computer' prediction but not at sea.

That

is, physical limitations such as deck wetness, slaming, the vol'untary

speed loss resulting therefrom, as well 'as the' involuntary, speed loss due

to the added drag caused by motions of 'the ship, the added drag due to'wind,

the loss of propulsive efficiency due to ship motions., etc. are considered

to limit the speed of a ship in a seay.. The James speed criterion

reflects implicitly the voluntary speed losses due to operator strategies

In

many storms as well as the unavoidable Involuntary speed losses,

A

brief comparison of this speed loss criterion with the more recent speed

loss formulation of

Aertssen8

is given in Appendix F!

The empirical speed

loss data of

James7

was used to limit the physically realizable speed of the

ship In extreme seas.

It is to be noted that the design seas .are

con-sidered to be Seas, see Figure 2, that.threaten the survival of the ship.

James' empirical speed' loss data for the C4 cargo ship was applied to all

ships in the AMMO series.

FunctIons which descr1b

the response of a ship to wave excitations as

a functIon 'of frequency.

These RAO's were calculated using the DTNSRDC

Ship Motion and Sea Loads Program of.references 5. and 6.

c*f the power installed in the ship is assumed to be unlimited

(27)

Load and GM variations.

AppendixE describes, In outline.form, theindividual stages

involved in the development of the design ship responses which, In turn,

produce the cargo shoring, loads.

The following section will discuss the

definition of these design responses before the results of the data

genera-tion task are presentedin the last part of the Data 'Base Generagenera-tion

Section.

DEFINITION OF DESIGN RESPONSES

The term design responses implies responses derived from the ship

operating in design seas by a procedure Outlined in Appendix E and discussed

in Appendix H.

Basically, design responses are defined to be the worst

responses that the ship will produce when encountering, at the worst

possible heading, the design seas of Figure 2 at a speed determined by the

James speed loss criterion.

The speed loss criterion serveS to exclude

from the universe of possible ship responses the speeds that are physically

unrealizable at each heading.

When ship load conditions are not explicitly considered, the term

design responses then means, additionally, that the worst responses

indepen-dent of load condition are selected.,

Figure 3 presents recommended design

accelerations for the AMMO Ship Series obtained

by

the above procedure.

These accelerations are given for three different longitudinal locations

on the ship.

' "

This latter type of design response requirement that Is independent

of ship' load condition, may be decreased when specifying ammunition shoring

requirements if, ,and, only if, the permissible ship load conditlons* are

specifically incorporated in the shoring regulations.

Figure 4 clearly

illustrates the large reductions, particularly for lateral accelerations,

that can be achieved when the regulations specify ship load conditions

as well as the shoring loads to be withstood.

The importance of load

conditions on the vertical and lateral accelerations are brought out further

in following sections.

(28)

The selection of design sea cOnditions equally strongly affects

the magnitudes of the design responses.

This selection process is discussed

in some deta1lin Appendix H.

If, for example, design seas are based on

normal 1- to 5-year instead of 20-year storms, it appears that design

responses can be reduced by approximately 20 percent.

Similarly;, if

design seas are selected as representing the most probable design seas,

that is, seas with relatively longer modal periods (> 14 seconds), design

responses can be additionally lowered by anywhere from 10 to 34 percent from

the values given in Figure 3.

It is important. to note, however, that the selection of design

accelerations and motions are performed independently for each response.

That

is, ship conditions that produce design lateral acceleration will not

necessarily be the same ones that yield the maximum vertical accelerations.

It was considered Important for design and regulatory purpose to develop

the maximum or design values for each response separately Inasmuch as the

ships and their cargo will certainly experience these individual responses

or accelerations in exactly this fashion.

The attempt to develop a design

condition that simultaneously results In maximum shoring loads for all

responses will be examined for the cargo accelerations in a following section

on the Design Vector.

It was assumed implicitly at the outset of the current research

program that predicted frequency dothain ship responses could be used

directly to establish the selected cargo shoring loads.

That Is, it was

assumed that if the probable maximum values of three components of the

acceleration an6, also, the ships roll, pitch and yaw could be established,

then these values could be combined into realistic cargo shoring forces.

Procedures for developing an upper bound on the cargo forces based on

the frequency domain ship responses are discussed in the Design Vector

section.

In addition, this section develops the quality of such "upper

bound" shoring loads by contrasting them to time domain shoring loads.

Before proceeding with that discussion, however, a summary of the

(29)

DISCUSSION OF RESULTS

The results of the Data Base Generation Task for the various ships,

ship load conditions and cargo locations Within the ship are presented

in terms of design responses in Tables 3 and 4.

Motions are given in Table

3 and accelerations in Table 4.

Overall trends in the responses as they are affected by ship size,

GM, load condition, and spatial variation within the ship, may be developed

directly from this tabulated data.

Similarly, the influence of the design

wave heights as well as the relative magnitudes of the three basic components

of theacceleratlon may be deduced from these data tabulations.

It is

noted that the various factors mentioned are all interrelated.

The

Implica-tions of the tabulated results are considered in terms of:

OperatIng cOnditions at which design responses occur,,

Modal encounter periods associated with design responses,

GM and load effect on design responses,

The influence of the location of the cargo In the ship on the

operating conditions at which design responses occur, and

Bilge keel effect on lateral accelerations and roll.

Operating Conditions at Which Design Responses Occur

Table 5 was prepared from Tables 3 and 4 to summarize the operating

conditions, I.e., ship speeds, headings, and modal periods of the seas

at which design responses occur.

A few of the more important results are

noted.

First, GM and load variations do not appear to influence the speeds

and headings at which design pitch, heave, and lateral accelerations

occur--irrespective of ship size.

Ship size appears to Influence only slightly the

modal periods of the seas at which design pitch, heave, and vertical

accel-erations occur.

That is, there is only a slight tendency for the larger

ships to encounter design responses In longer period seas, i.e., up to

two seconds longer than do the smallest ships.

(30)

Second, the modal period of the seas that produce design respons

vary from response to response, wIth motions tending to reach their design

values In somhat longer seas thahis the case for accelerations.

Third, design pitch Invariably occurred in head seas, whereas design

heave occurred In essentially beam seas

(900

to

1050).

These values occurred

at speeds of 0 to 5 knots,. independent of the ship type or loading.

Fourth, design roll, on the other hand, occurred at speeds ranging

from 0 t015 knots, depending strongly on the

GM.

Large

GMs,

which result

In a relatively stiff ship, produce design roll values in beam seas at low

speeds ranging up to 5 knots

independent ofship's type or dead weight.

On the other hand, small

GM

values which result In a relatively, slow, rolling

comfortable ship, tended to produce design roll values at relatively high ship

speeds, i.e., 10 to 15 knots In quartering or following seas.

Thus, It is quite

apparent that

GM

values will very much dictate the operating conditions

in which design roll motiOhs occur.

Low

GM

values thus induce roll response

behavior that may result in conditions that are conducive to capsizing,

even

though the magnitudes of such roll motions are, in fact, less than the

ones

attained with higher

GMs.

To

further emphasize the importance of

GM

and

load, rather than excessive roll, on the occurrence of capsizing,

a relevant

section, of the conclusion of reference 18 is quoted.

"Out of a total of 136

mOdel experiments, 21 capsizes were experienced.

All of these capsizes

occurred In quartering or following seas, i.e., conditions In which the

stability is strongly affected by the relative position of ship and

wave.

No capsizes occurred in beamseas.

All

capsizes except one occurred in

the heavy displacement (low freeboard) condition.

This is the condition

most sensitive tothe reduction Of stability in a wave crest."

In the capIzing cofltext, it is noted, of course, that the tested

GMs

of reference 18 are very much lower, i.e.,

GMs

on the order of 0.5 to 1.5

percent of the ship's beam compared to

GM

values of 3.7 to about 15 percent

of the ship's beams in the

AMMO

series.

The trend in the operating

con-ditions with

GM Is

noted to illustrate that the occurrence of design roll

In operating conditions conducive to capsizing may limit the lower acceptable

GM

conditions rather than the magnitude of roll and associated lateral

(31)

Modal Encounter Periods Associated with Design Responses

The natural pitch, heave, and roll periods of Table

1 were

selected according to the procedure of reference 19.

That is, the

periods selected correspond to the peak of the zero speed transfer

func-tions in beam seas for roll and heave, and head seas for pitch.

Figure

5 illustrates the behavior Of the responseamplitude Operators at 0 knots

for Ship C, Full Load, GM2.

When the modal periods at which design roll, pitch, and heave

responses occur (see Tables 3 and 1+) are compared to the. natural periods

of these responses (see table I),

It becomes evident that design roll

always occurs at the natural frequency, even when the ship Is operatin.g

in quartering or following seas, independent of load, GM or ship size.

This essentially reSOnant roll behavior-of the various ships is particularly

well illustrated by the roll response density graphs of Appendix B.

Figure 6 is presented to demonstrate this resonant roll behavior for

Ship B.

Design pitch, on the other hand, occurs at. periods that are up

to 1.9 seconds shorter than the natural pitch periods, again independent

of ship load and GM.

Design heave occurs at periods that are much longer than the

corresponding natural heave periods.

Based on the heave density graphs,

however, it may be noted that large heave responses occur for a very

wide rangeof modal. encounter periods.

Thus heave, unlike roll, exhibi:ts

a distinctly nonresonant motion response.

Thus it is noted that, whereas

the désigh roll period is strongly dependent on GM, comparable pitch and

heave periods are essentially unaffected by GM.

The vertical, lateral1 and longitudinal design accelerations

exhibit distinctly different behavior as far as their design periods are

concerned, i.e., modal periods corresponding to design responses.

This

(32)

difference is attributable to the fact that the accelerations are made

up of various combinations of heave, roll, and pitch depending entirely

on the location within the ship where the accelerations are considered,

i.e., the relative import'nce of the heave, roll and pitch

components

varies With location on the ship.

In referring to .the.sample. response density graph for Ship B of

Figure 6, the sharply peaked vertical acceleration graph demonstrates

the essentially resonant behavior of this

response at this particular

ship location.

At large GMs, design lateral accelerations

occur at or near. the

resonant roll periods,..suggesting that for these conditions roll is a

dominant component of the lateral acceleratIon.

At the small GMs, however,

design lateral acceleration periods tend to occur flear the roll

resonance

only at a point near midship (Point 3).

Clearly, at the ends of the ship

sway and yaw with shorter periods than roll produce the dominant components

of lateral acceleration In the earth reference system,

that Is.

.

It should

be noted that, unless otherwise specified, earth reference

system

accelera-tions are always considered.

Finally, the relative magnitude of design

vertical and lateral accelerations are so much greater than design

longi-tudinal accelerations that the latter are not explicitly discussed since

they are effectively Unimportant

GM and Load Effect on Design Responses

There .iSessentia!ly.no GM and.load effect on designpitch and

heave.

The same, however, cannot be. said for roll

Increasing the GM.

through the range of. 3.7 to about.l5..percent of the beam increased roll.

for every ship.

The ship with the smaller GM will have the lowest roll.

The roll of Ship C was particularly sensitive to GM variations since roll

increased by as. much as 57 percent.

The roll of the fully loaded ship

was more sensitive to GM variation than the same ship with a lighter load.

increasing the displacement at the low GMs decreases roll by as

much as 17 percent for Ships A and D, but only 4 percent or less for

(33)

Increasing the displacement atthe high GMs had very little

influence on the design roll for Ships A, B and C, though Ship D decreased

its roll by 14 percent for this condition.

-It is clear that GM has a far stronger influence on the roll'

performance of the ships than does load variations.

In addition, the

indIvidual. shipsare not equally sensitive to either GM or load variations.

Increasing GM at either the full load or the 50 percent load

condition has a negligible effect on the vertical accelerations.

On the

other hand, Increasing GM at full load results in 47 and 50 percent

increases in lateral accelerations for Ships B and C, respectively.

At

the 50percent load condition, similar GM increases result in slightly,

lower

increases in lateral accelerations, i.e., 21 to 29 percent.

Regardless of GM, Increasing the displacement from the 50 percent

load condition to the full load condition decreases vertical

accelera-tions by as much as 12 percent for Ship A, and by as little as 2 percent

for the largest ship, Ship D.

At the low GM, increaslngthe displacement decreases lateral

accelerations by no more than 6 percent, whereas the high GM Ships B

and C show a similar reduction in the lateral accelerations.

Ships A

and D, on the other hand, actually Increase their lateral design

accelerations by 15 and 10 percent..

In summarizing the GM and load effect on the accelerations, it

is noted that only the lateral accelerations and thus lateral shoring

loads are significantly affected by GM variations.

Displacement

varia-tions result in

much lower acceleration variations'.

The Influence of Location on the Operating Conditions at Which Design

Responses Occur

Angular motions, are the same for any location on the ship*

(see Table 3) because the ship is considered to be a rigid body.

*Note

that heave, definedto be the vertical motion near the CG, is only

one component of the vertical motion at an arbitrary point in the

ship.

The other components result from the angular motions of the ship.

Cytaty

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