View source for Engineering:Ship stability

{{Short description|Ship response to disturbance from an upright condition}}
[[File:Ship stability.svg|right|thumb|upright=1.35|Ship stability illustration explaining the stable and unstable dynamics of buoyancy (B), center of buoyancy (CB), center of gravity (CG), and weight (W)]]

'''Ship stability''' is an area of [[Engineering:Naval architecture|naval architecture]] and ship design that deals with how a ship behaves at sea, both in still water and in waves, whether intact or damaged. Stability calculations focus on [[Physics:Center of mass#center of gravity|centers of gravity]], [[Physics:Buoyancy|centers of buoyancy]], the metacenters of vessels, and on how these interact.

== History ==
[[Image:NewcastleTowingTank.jpg|thumb|A model yacht being tested in the towing tank of Newcastle University]]
Ship stability, as it pertains to naval architecture, has been taken into account for hundreds of years.  Historically, ship stability calculations relied on [[Rule of thumb|rule of thumb]] calculations, often tied to a specific system of measurement.  Some of these very old equations continue to be used in naval architecture books today. However, the advent of calculus-based methods of determining stability, particularly Pierre Bouguer's introduction of the concept of the metacenter in the 1740s [[Ship model basin|ship model basin]], allow much more complex analysis.

Master shipbuilders of the past used a system of adaptive and variant design. Ships were often copied from one generation to the next with only minor changes; by replicating stable designs, serious problems were usually avoided. Ships today still use this process of adaptation and variation; however, [[Computational fluid dynamics|computational fluid dynamics]], ship model testing and a better overall understanding of [[Engineering:Ship motion test|fluid and ship motions]] has allowed much more analytical design.

Transverse and longitudinal waterproof [[Engineering:Bulkhead (partition)|bulkheads]] were introduced in [[Engineering:Ironclad warship|ironclad]] designs between 1860 and the 1880s, anti-collision bulkheads having been made compulsory in British steam [[Engineering:Merchant vessel|merchant ships]] prior to 1860.<ref>''From Warrior to Dreadnought'' by D.K. Brown, Chatham Publishing (June 1997)</ref>  Before this, a hull breach in any part of a vessel could flood its entire length. Transverse bulkheads, while expensive, increase the likelihood of ship survival in the event of hull damage, by limiting flooding to the breached compartments they separate from undamaged ones. Longitudinal bulkheads have a similar purpose, but damaged stability effects must be taken into account to eliminate excessive heeling. Today, most ships have means to equalize water in sections port and starboard (cross flooding), which helps limit structural stresses and changes to the ship's heel and/or trim.

==Add-on stability systems==
Add-on stability systems are designed to reduce the effects of waves and wind gusts. They do not increase a vessel's stability in calm seas. The International Maritime Organization International Convention on Load Lines does not cite active stability systems as a method of ensuring stability. The hull must be stable without active systems.

===Passive systems===
====Bilge keel====
[[Image:bilgekeel.jpg|right|thumb|A bilge keel]]
A bilge keel is a long, often V-shaped metal fin welded along the length of the ship at the turn of the bilge.  Bilge keels are employed in pairs (one for each side of the ship). Rarely, a ship may have more than one bilge keel per side. Bilge keels increase hydrodynamic resistance when a vessel rolls, limiting the amount of roll.

====Outriggers====
[[Engineering:Outrigger|Outrigger]]s may be employed on vessels to reduce rolling, either by the force required to submerge buoyant floats or by hydrodynamic foils. In some cases, these outriggers are of sufficient size to classify the vessel as a [[Engineering:Trimaran|trimaran]]; on other vessels, they may simply be referred to as stabilizers.

====Antiroll tanks====
[[Engineering:Antiroll tanks|Antiroll tanks]] are interior tanks fitted with baffles to slow the rate of water transfer from the tank's port side to its starboard side. It is designed so that a larger amount of water is trapped on the vessel's higher side. It is intended to have an effect counter to that of the [[Physics:Free surface effect|free surface effect]].

====Paravanes====

[[Engineering:Paravane (water kite)|Paravane]]s may be employed by slow-moving vessels, such as fishing vessels, to reduce roll.

===Active systems===
Active stability systems, found on many vessels, require energy to be applied to the system in the form of pumps, hydraulic pistons, or electric actuators. They include stabilizer fins attached to the side of the vessel or tanks in which fluid is pumped around to counteract the vessel's motion.

====Stabilizer fins====


Active fin stabilizers reduce the roll a vessel experiences while underway or, more recently, while at rest. They extend beyond the vessel's hull below the waterline and alter their angle of attack depending on heel angle and the vessel's rate-of-roll, operating similarly to airplane [[Engineering:Aileron|aileron]]s. [[Engineering:Cruise ship|Cruise ship]]s and [[Engineering:Yacht|yacht]]s frequently use this type of stabilizing system.

When fins are not retractable, they constitute fixed appendages to the hull, possibly extending the beam or draft envelope and requiring attention for additional hull clearance.

While the typical "active fin" stabilizer effectively counteracts roll for ships underway, some modern active fin systems can reduce roll when vessels are not underway. Referred to as zero-speed, or Stabilization at Rest, these systems work by moving specially designed fins with sufficient acceleration and impulse timing to create effective roll-cancelling energy.

====Rudder Roll Stabilisation====
In case a ship is underway, a fast rudder change will not only initiate a heading change, but it will also cause the ship to roll. For some ships such as frigates, this effect is so large that it can be used by a control algorithm to simultaneously steer the ship while reducing its roll motions. Such a system is usually referred to as "Rudder Roll Stabilisation System". Its effectiveness can be as good as that of stabiliser fins. However, that depends on the ship speed (higher is better) and various ship design aspects such as position, size and quality of the rudder positioning system (behaves as fast as a stabiliser fin). Also important is how quickly the ship will respond to rudder motions with roll motions (quick is better) and rate of turn (slow is better). Despite the high costs of high-quality steering gear and strengthening of the ship's stern, this stabilisation option offers better economics than stabiliser fins. It requires fewer installations, is less vulnerable and it causes less drag. Even better, the required high-quality components provide excellent steering properties also for those periods when roll reduction is not required and a significant reduction of underwater noise.  Known navy ships with this stabilisation solution are F124 (Germany), M-fregat and LCF (both of Dutch Navy).

====Gyroscopic internal stabilizers====
[[Image:Ship stabilizing gyroscopes USS Henderson 1917.jpg|thumb|The first stabilizing gyroscope to be fitted on a ship, USS Henderson (AP-1) (1917).]]
[[Engineering:Gyroscope|Gyroscope]]s were first used to control a ship's roll in the late 1920s and early 1930s for warships and then passenger liners.  The most ambitious use of large gyros to control a ship's roll was on an Italian passenger liner, the SS ''Conte di Savoia'', in which three large [[Company:Sperry Corporation|Sperry]] gyros were mounted in the forward part of the ship. While it proved successful in drastically reducing roll in the westbound trips, the system had to be disconnected on the eastbound leg for safety reasons. This was because with a following sea (and the deep slow rolls this generated) the vessel tended to 'hang' with the system turned on, and the inertia it generated made it harder for the vessel to right herself from heavy rolls.<ref>[https://books.google.com/books?id=Y-IDAAAAMBAJ&dq=popular+mechanics+1932&pg=PA626 "Italian Liner To Defy The Waves"] ''Popular Mechanics'', April 1931</ref>

Gyro stabilizers consist of a spinning flywheel and gyroscopic [[Physics:Precession#Torque-induced|precession]] that imposes boat-righting [[Physics:Torque|torque]] on the hull structure.
The [[Physics:Angular momentum|angular momentum]] of the gyro's flywheel is a measure of the extent to which the flywheel will continue to rotate about its axis unless acted upon by an external torque. The higher the angular momentum, the greater the resisting force of the gyro to external torque (in this case more ability to cancel boat roll).

A gyroscope has three axes: a spin axis, an input axis, and an output axis. The spin axis is the axis about which the flywheel is spinning and is vertical for a boat gyro. The input axis is the axis about which input torques are applied. For a boat, the principal input axis is the longitudinal axis of the boat since that is the axis around which the boat rolls. The principal output axis is the transverse (athwartship) axis about which the gyro rotates or precesses in reaction to an input.

When the boat rolls, the rotation acts as an input to the gyro, causing the gyro to generate rotation around its output axis such that the spin axis rotates to align itself with the input axis. This output rotation is called [[Physics:Precession#Torque-induced|precession]] and, in the boat case, the gyro will rotate fore and aft about the output or gimbal axis.

Angular momentum is the measure of effectiveness for a gyro stabilizer, analogous to horsepower ratings on a diesel engine or kilowatts on a generator.  In specifications for gyro stabilizers, the total angular momentum ([[Physics:Moment of inertia|moment of inertia]] multiplied by spin speed) is the key quantity. In modern designs, the output axis torque can be used to control the angle of the stabilizer fins (see above) to counteract the roll of the boat so that only a small gyroscope is needed. The idea for gyro controlling a ship's fin stabilizers was first proposed in 1932 by a [[Company:General Electric|General Electric]] scientist, Dr Alexanderson. He proposed a gyro to control the current to the electric motors on the stabilizer fins, with the actuating instructions being generated by thyratron vacuum tubes.<ref>[https://books.google.com/books?id=7-EDAAAAMBAJ&dq=popular+mechanics+1932+the+president+of+a+big&pg=PA251 "Fins Purposed For Big Liners To Prevent Rolling"] ''Popular Mechanics'', August 1932</ref>

==Calculated stability conditions==
When a hull is designed, stability calculations are performed for the intact and damaged states of the vessel.  Ships are usually designed to slightly exceed the stability requirements (below), as they are usually tested for this by a classification society.

===Intact stability===
[[File:MetacentricHeight.svg|thumb|Ship stability diagram showing center of gravity (G), center of buoyancy (B), and metacenter (M) with ship upright and heeled over to one side. As long as the load of a ship remains stable, G is fixed. For small angles M can also be considered to be fixed, while B moves as the ship heels.]]
Intact stability calculations are relatively straightforward and involve taking all the centers of mass of objects on the vessel which are then computed/calculated to identify the center of gravity of the vessel, and the center of buoyancy of the hull.  Cargo arrangements and loadings, crane operations, and the design sea states are usually taken into account.  The diagram at the right shows the center of gravity is well above the center of buoyancy, yet the ship remains stable.  The ship is stable because as it begins to heel, one side of the hull begins to rise from the water and the other side begins to submerge.  This causes the center of buoyancy to shift toward the side that is lower in the water.  The job of the naval architect is to make sure that the center of buoyancy shifts outboard of the center of gravity as the ship heels. A line drawn from the center of buoyancy in a slightly heeled condition vertically will intersect the centerline at a point called the metacenter.  As long as the metacenter is further above the keel than the center of gravity, the ship is stable in an upright condition.

===Damage stability (Stability in the damaged condition)===
Damage stability calculations are much more complicated than intact stability.  Software utilizing numerical methods are typically employed because the areas and volumes can quickly become tedious and long to compute using other methods.

The loss of stability from flooding may be due in part to the free surface effect. Water accumulating in the hull usually drains to the bilges, lowering the center of gravity and actually increasing the [[Metacentric height|metacentric height]]. This assumes the ship remains stationary and upright. However, once the ship is inclined to any degree (a wave strikes it for example), the fluid in the bilge moves to the lower side. This results in a list.

Stability is also reduced in flooding when, for example, an empty tank is filled with seawater. The lost buoyancy of the tank results in that section of the ship lowering into the water slightly. This creates a list unless the tank is on the centerline of the vessel.

In stability calculations, when a tank is filled, its contents are assumed to be lost and replaced by seawater. If these contents are lighter than seawater, (light oil for example) then buoyancy is lost and the section lowers slightly in the water accordingly.

For merchant vessels, and increasingly for passenger vessels, the damage stability calculations are of a probabilistic nature. That is, instead of assessing the ship for one compartment failure, a situation where two or even up to three compartments are flooded will be assessed as well. 
This is a concept in which the chance that a compartment is damaged is combined with the consequences for the ship, resulting in a damage stability index number that has to comply with certain regulations.

==Required stability==
In order to be acceptable to classification societies such as the [[Organization:Bureau Veritas|Bureau Veritas]], [[Organization:American Bureau of Shipping|American Bureau of Shipping]], Lloyd's Register of Ships, Korean Register of Shipping and Det Norske Veritas, the blueprints of the ship must be provided for independent review by the classification society. Calculations must also be provided which follow a structure outlined in the regulations for the country in which the ship intends to be flagged.

Within this framework different countries establish requirements that must be met. For U.S.-flagged vessels, blueprints and stability calculations are checked against the U.S. Code of Federal Regulations and International Convention for the Safety of Life at Sea conventions (SOLAS). Ships are required to be stable in the conditions to which they are designed for, in both undamaged and damaged states.  The extent of damage required to design for is included in the regulations.  The assumed hole is calculated as fractions of the length and breadth of the vessel, and is to be placed in the area of the ship where it would cause the most damage to vessel stability.

In addition, United States Coast Guard rules apply to vessels operating in U.S. ports and in U.S. waters.  Generally these Coast Guard rules concern a minimum metacentric height or a minimum righting moment.  Because different countries may have different requirements for the minimum metacentric height, most ships are now fitted with stability computers that calculate this distance on the fly based on the cargo or crew loading. There are many commercially available computer programs used for this task.

Depending upon the class of vessel either a stability letter or stability booklet is required to be carried on board.<ref>[https://www.govinfo.gov/content/pkg/CFR-1999-title46-vol7/pdf/CFR-1999-title46-vol7-sec170-110.pdf 46 CFR Ch. I (10–1–99 Edition)] govinfo.gov</ref><ref>[https://wwwcdn.imo.org/localresources/en/KnowledgeCentre/IndexofIMOResolutions/MSCResolutions/MSC.267(85).pdf Resolution MSC.267(85)] wwwcdn.imo.org</ref>

== See also  ==
* {{annotated link|Engineering:Capsizing}}
* {{annotated link|Physics:Free surface effect}}
* {{annotated link|Engineering:Inclining test}}
* {{annotated link|Engineering:Kronan (ship)}}
* {{annotated link|Engineering:Niobe (schooner)}}
* {{annotated link|Engineering:Pamir (ship)}}
* {{annotated link|Engineering:Ship motions}}

==References==
{{reflist}}

==External links==
* [http://www.access.gpo.gov/nara/cfr/cfr-table-search.html  Title 46 U.S. Code of Federal Regulations] {{Webarchive|url=https://web.archive.org/web/20070701212021/http://www.access.gpo.gov/nara/cfr/cfr-table-search.html |date=2007-07-01 }}
* [http://www.eagle.org/absdownloads/listdetails.cfm?id=349 ABS Rules for Building and Classing Steel Vessels 2007]
* [http://www.kastenmarine.com/roll_attenuation.htm  Overview of a few common Roll Attenuation Strategies]


[[Category:Shipbuilding]]

{{Sourceattribution|Ship stability}}