تبليغاتX

برای تعجیل در فرج وسلامتی آقا صلوات:اللهم صل علي محمد وآل محمدو عجل فرجهم

اپان


اپان

یالطیف


International Journal of Offshore and Polar Engineering (ISSN 1053-5381)

Copyright © byThe International Societyof Offshore and Polar Engineers

Vol. 15, No. 2, June 2005, pp. 109–116

Roll Motion of Ro-Ro Passenger Ship with Flooded Vehicle Deck

Toshifumi Fujiwara and Tomihiro Haraguchi

Advanced Maritime Transport TechnologyDepartment, National Maritime Research Institute

Tokyo, Japan

This paper tries to confirm the effectiveness of an estimation method of roll motion on a Ro-Ro passenger ship with

a flooded vehicle deck. Atime domain simulation of roll motion expressed by the 2-dimensional lump mass concept was

applied to the Ro-Ro passenger ship with no water ingress, but with a flooded vehicle deck. Measurements of the motion

of the ship with different amounts of water on deck were carried out in regular beam waves in order to compare with

calculated results. The trend of the calculated results on roll amplitude generally represents the experimental results.

INTRODUCTION

After the disaster of the Ro-Ro passenger ship Estonia in the

Baltic Sea in 1994, the safetyof damaged Ro-Ro passenger ships

has been discussed at the International Maritime Organization

(IMO). Because Ro-Ro passenger ships have large, flat vehicle

decks with no watertight bulkheads, large amounts of water can

enter the decks through damage holes causing the ship to lose stability.

To prevent such kinds of disasters, it is necessary to assess

the static and dynamic effect of the water on deck for ensuring

the stabilityof such kinds of ships.

Manye xperimental investigations of the Ro-Ro passenger ships

with a hole from damage and a flooded deck have been conducted

(Ishida et al., 1996; Hamano et al., 1997; Haraguchi et al.,

1998; Vassalos et al., 2000; and others). It is, however, difficult

to capture all dangerous conditions of a flooded ship deck using

limited sample ships and experimental conditions. Although calculation

methods on ship motion have been presented to predict

the capsize of the ships (Dillingham et al., 1986; Zaraphonitis et

al., 1997; Hasegawa et al., 2000; Papanikolaou et al., 2000), there

are manyuncertain points of applicabilityand detail.

To exactlyestimate ship motion with a deck flooded with water

entered from damaged holes, it is necessaryto deal with 2 subjects:

(1) to estimate the amount of water coming from damaged

holes, and (2) to estimate ship motion with flooded vehicle decks,

which means to calculate the dynamic influence of the water on

deck. In past investigations, both subjects were treated at the same

time. To be clear about the problems of the estimation method of

the Ro-Ro passenger ships with flooded decks, each subject must

be treated separately.

In this paper, the calculation method of roll motion for the sample

Ro-Ro passenger ship with the flooded vehicle deck is presented

from the viewpoint of subject (2). The 2-dimensional lump

mass concept for the flooded deck used byIshida et al. (1996)

and Murashige et al. (1997, 1998) that is applied to the flooded

box is used for the Ro-Ro passenger ship in the calculation. The

calculated results are compared with the experimental ones. The

Received March 16, 2003; revised manuscript received bythe editors

May4, 2005. The original version (prior to the final revised manuscript)

was presented at the 12th International Offshore and Polar Engineering

Conference (ISOPE-2002), Kitakyushu, Japan, May 26–31, 2002.

KEY WORDS: Ro-Ro passenger ship, Estonia, estimation method, roll

motion, flooded vehicle deck, model experiment, damage stability.

trend of the calculated results on the roll amplitude sufficiently

represents the experimental results.

MATHEMATICAL MODEL OF ROLL MOTION ON

RO-RO SHIP WITH FLOODED DECK

The Ro-Ro passenger ship is assumed to have a large, flat vehicle

deck flooded with water and no forward speed in beam waves.

In this case, it is assumed that the ship rolling and water moving

effects are main components of ship motion. The equation of 2

degrees of freedom for ship rolling and water moving is used in

the calculation, neglecting the effect of swayand heave motion.

Fig. 1 defines the coordinate system of the ship and water. The

ship breadth, draft and height of the free-board are denoted by B,

ds , fr . When the ship is upright, the water of width bw and depth

dw is on the vehicle deck. Each position of the center of gravity,

buoyancyof the ship and the water is respectivelydesignated Gs ,

Gw and Bs . Using the suffixes Gw the horizontal and vertical

position xGW

, yGW

of the gravitycenter of the water is defined

from the origin, that is, the Gw position when the ship is upright,

while the roll angle of the ship and the water surface slope are

defined as and . The vehicle deck is one compartment without

partitions such as a central casing, and the center of gravityof the

water Gw transfers 2-dimensionallyin the midship section on the

vehicle deck, not moving with respect to the longitudinal direction

of the ship.

The kinetic energy K, potential energy P and dissipation energy

D of the ship and water can be expressed with and in the

Fig. 1 Coordinate system on Ro-Ro passenger ship with flooded

deck

نویسنده: مهدی ׀ تاریخ: پنجشنبه دهم دی 1388 ׀ موضوع: ׀ لینک این پست ׀


نویسنده: مهدی ׀ تاریخ: سه شنبه بیست و چهارم آذر 1388 ׀ موضوع: ׀ لینک این پست ׀


سال ها دل طلب جام جم از ما می کرد          

 آنچه خود داشت ز بیگانه تمنا می کرد

نویسنده: مهدی ׀ تاریخ: یکشنبه پانزدهم شهریور 1388 ׀ موضوع: ׀ لینک این پست ׀


© All Rights Reserved to epan.Blogfa.com / Theme by:
bahar-20

انواع کد های جدید جاوا تغییر شکل موس