while under construction, renders the fear of unseaworthiness, from
either defective construction or equipment, the least reasonable
of all the fears with which ocean navigation is regarded. It is in
later circumstances, and concerning matters of a more extraneous
character, that the most justifiable fears may be entertained
regarding a vessel’s safety. Overloading, improper stowage, bad
management, under-manning, insufficient repair, besides the numerous
inevitable and unforeseen circumstances incidental to sea-voyaging,
may be instanced as the causes to which the greatest losses are
attributable.[4] Few instances of loss from structural defects are
adduceable, and even in these, causes of a more or less extraneous
character are associated with the loss. On the other hand, instances
could be multiplied where vessels sustaining the casualties which
rough weather or rank carelessness make always imminent have come
out of the ordeal with credit to the constructors. One notable case
may be instanced. The _Arizona_, of the Guion Line, some time after
being put on the Atlantic service, while steaming at a speed of 14
knots, and almost in mid-Atlantic, ran into an iceberg of gigantic
dimensions, and notwithstanding that the force of the concussion
smashed her bows for a length of 20 feet into an unrecognisable mass,
she kept afloat, and reached a port of safety.
Where, as has already been indicated, there is such close oversight
and thorough supervision—where, indeed, the real interests of every
party honestly concerned lie so clearly in the high qualities of
construction—nothing short of such results as the foregoing should be
expected. The insurance companies, on whom the burden (monetary at
least) of loss at sea ultimately falls, see it their interest to know
that those registration societies, on whom they rely for guarantee
as to a vessel’s structural and general efficiency, are themselves
efficient and trustworthy authorities. These societies, known as
Lloyd’s, Liverpool Underwriters, and Bureau Veritas, Registries, in
spite of the dread as to business rivalry affecting injuriously their
standards of classification, have still a high criterion, and enjoy
the confidence of insurance societies and shipowners alike.
Shipowners themselves, notwithstanding some examples to the contrary,
are, and have always been, anxious and painstaking seekers after
thoroughness; not merely mercenary grubs, sacrificing considerations
of safety to features promising exemption from tonnage or other
registration dues, and perhaps the extinction of a rival. Some of the
best British vessels, notably those of the Cunard Line, are unclassed
at the registries, but have been built under private survey. The
well known boast of the Cunard Company that not a single life has
been lost by mishap at sea during their long and extensive service,
is eloquent testimony to the care exercised in the construction and
management of ships. It is the practice of some companies to effect
classification in two, sometimes three, separate registries, and
the number of inspectors employed to superintend the work of
construction, over and above the surveyors of the registries and
the overseers of the firms, is in some instances astonishing. The
crowning case of all is that of the building firms themselves—many
shipbuilders unquestionably being conscientious and thorough to a
degree which simply mocks this great array of supervision.
In the outfit of vessels correspondingly close attention is paid to
those features, fixed or portable, which contribute to the safety
of the ship and the welfare of passengers. The universal adoption
of steam winches for working cargo enables the pumps communicating
with the holds to be wrought by steam, through levers attached to
the barrel ends of the winches. Special donkey-engine pumps, in
addition, are now employed in all the higher class vessels, and
automatic means of registering the quantity of water in the holds are
beginning to be introduced. Provision against outbreaks of fire, no
less than against foundering, has been receiving greater attention
than formerly. Many of the first-class mail steamships are fitted
with fire-pipes leading to every compartment, and which convey at the
turning of a valve a charge of steam sufficient to extinguish the
most serious outbreak. Lowering and detaching gear for life-boats is
now a necessary part of every first-class steamer’s equipment. Over a
dozen different apparatuses for effecting this very important purpose
are at present in the market, some of which are admirably adapted for
safe and speedy working, even in the hurry and panic which too often
accompanies cases of shipwreck.
Important as these devices are for saving life and property in event
of casualty, the appliances which contribute to the prevention of
casualty at all, are perhaps more so. This is a gradually increasing
and improving element in ships’ outfit. Conspicuous among this class
of articles are navigational instruments, and of these perhaps the
most noteworthy are the instruments with which the name of Sir
William Thomson is associated, although many others, in use or
awaiting adoption, and designed for equally important purposes, might
be referred to, did space permit.
Within the period covered by this review, this eminent inventor has
introduced an instrument which enables soundings to be taken while
vessels are going at full speed, at depths of 100 fathoms and under.
The sounding line adopted is a fine steel wire, such as is used by
pianoforte makers, which passes through the water with very little
resistance, and can be sent to the bottom by a light weight or
sinker, even when the ship is going full speed. Fastened to a short
length of rope, near the sinker, there is a brass tube, in which is
placed a glass tube two feet long, closed at one end and open at the
other. This glass tube is coated inside with chromate of silver. As
the sinker goes down, the air in the tube becomes compressed, and
sea water rises up inside, the height to which it rises depending on
the depth, from the surface, to which the glass tube goes down. As
the sea water rises in the tube, the salt of the water acts on the
chromate of silver and changes the colour from red to white; thus a
mark is left on the glass tube showing the height to which the sea
water rises, from which the actual depth may be at once measured
by a prepared scale. By means of this sounding machine a ship can
feel her way round a coast in a fog without reducing speed. In later
instruments the inventor has devised another form of automatic gauge,
which obviates the use of glass tubes, and is a decided improvement
on the gauge here described.
The well-known Improved Mariner’s Compass introduced by Sir W.
Thomson enables the magnetism of the ship to be completely corrected
instead of only approximately. This is attained by the use of several
small needles instead of one or two large ones. The requisite
steadiness of the compass card is obtained by means of an aluminium
rim suspended round the edge of the card. The extreme lightness of
the card reduces greatly the wear of the needle point supporting the
compass. Along with the compass the inventor supplies an azimuth
mirror which greatly facilitates observations either on a point of
land or on a star, the whole invention proving from experience an
almost indispensable item of outfit for well-appointed vessels.
The care and ingenuity expended on the question of ship safety must
not, however, be measured simply by the amount of attention and skill
exercised in constructing and outfitting vessels of the common type.
The question has very naturally occasioned many distinct novelties
in ship design. Some of these have been directly designed to secure
safety, but the greater number have aimed at combining with safety
the other qualities of speed and comfort; as in the instances given
in the previous chapter. The success attained in practice, it need
scarcely be said, has hitherto been but partial.
The problem of rendering ships absolutely unsinkable has, from very
early times, received attention from many concerned in shipbuilding
and navigation. Propositions and trials have been made from time to
time, without as yet any very marked success attending any of them.
Various plans have been submitted for safety-ships, the general
principle of which consists in forming the ship into two or more
distinct and entire portions, and in the event of one sustaining
damage by collision or otherwise, those remaining to be disconnected
and sent adrift—presumably with all passengers on board.
Other life-saving devices, while interfering somewhat with the
original structure, have simply been intended to use or modify
existing features or material on board ship. Two of these which have
received attention from the Scientific Societies may be shortly
described as examples of the class of devices referred to. One was
the proposition of Mr Jolly, M.A., of the Royal Navy, laid before
the Institution of Naval Architects in 1874; the other being that
of Mr Gadd, submitted to the Manchester Mechanical Society in 1879.
Mr Jolly’s proposal was to construct what he felicitously termed
the “ark saloon,” an erection on the upper deck, and resembling
very closely an ordinary deck-house, but instead of being built
permanently on the vessel, it was to be an independent structure
capable of being readily disconnected, and “while answering all the
purposes of accommodation found in ordinary deck-houses, to have
within it hidden resources capable of converting it when afloat
into a perfectly navigable vessel.” Mr Gadd’s proposal was to form
the upper portion of the bulwarks of ships of loose sections 12-ft.
long, composed chiefly of hollow, thin metallic tubes. These sections
when immersed in the water would form so many pontoons, and would be
provided with cords and loops along their sides, and in the event
of the ship going down would be lifted out of their place by the
action of the water. Objections on economical grounds to Mr Jolly’s
scheme, fully pointed out by members of the Institute, apply almost
equally to the proposal of Mr Gadd. The expense involved in their
application would far outbalance in the eyes of the shipowner the
possible service they could render. No provision was made by Mr Jolly
for launching his ark saloon, thereby limiting its use to cases of
foundering; and even in event of this, the “ark” was only to be so
in name until the good ship should “go under,” and leave the saloon
serenely floating—presumably with all souls inside. The difficulty in
Mr Gadd’s proposal, of at once making the bulwarks easily floatable
and structurally efficient for the resistance of heavy seas,
seriously detracted from its feasibility.
It would be a somewhat heavy task to make adequate note of all
the varied proposals and patented inventions for the preservation
of life at sea. Some of these, as in the foregoing instances, are
proposals affecting structural features; but others, and by far the
most numerous, are simply adjuncts to the vessel. Ingenuity has
been specially directed of late towards bringing into efficient
requisition, in event of impending shipwreck, the commonest items of
a ship’s outfit. This has been abundantly evidenced in the several
naval exhibitions held within the past three years in various parts
of the country. Firms whose work lies in cork and Indiarubber
manufactures have there exhibited in great profusion various forms
of life-belts, life-buoys, life-saving mattresses and pillows, and
life-saving dresses. Others, availing themselves of larger items,
have shown life-saving adaptations of deck-seats, deck-houses, and
bulwarks made into the form of life-rafts. Not a few of these devices
have received adoption in our passenger-carrying steamships, and
their more general use—especially if accompanied by proper knowledge
of how they may best be taken advantage of—would materially help to
rob shipwreck of some of its terrors at least, if not of its dire
fatalities. It has been urged in this connection—and the plea is
eminently reasonable—that Parliament should invest the Board of Trade
with proper powers—if that Body is not already vested with all that
is requisite—to take the matter of life-saving appliances thoroughly
and practically in hand, and by means of experiments in all kinds of
weather to determine which are the best means of saving life under
different conditions. Having done this, also to draw up rules for
the proper stowage and use of such appliances on board ship, and to
see that such rules are strictly observed, and that no vessel be
permitted to go to sea which is not so equipped.
* * * * *
The development in the size of steamships not only affects the
quality of safety, but also in various ways the element of comfort at
sea. The greater length, for instance, is calculated to neutralise
the longitudinal oscillation, the effects of which are so often fatal
to the comfort of passengers. Again, the great length affords an
advantage in the way of allowing better state-room accommodation; all
the rooms, or a larger proportion of them, being next the vessel’s
side, and consequently more airy and better lighted. It is not,
however, in the increased length so much as in the development of all
three dimensions, and especially in the increased ratio of breadth
to length, that modern types of steamships are enhanced in the
qualities of safety and comfort. Mistaken or imperfect notions as to
the ratio most desirable for speed, have kept in perpetuity types of
steamers which the fuller light of modern scientific investigation
has shown to be undesirable. Great beam is now believed to be not
incompatible with great speed, and even apart from questions of speed
the advantages accruing from breadth are better appreciated.
As an illustration of this movement, one of the more recent of
the many transatlantic mail steamships may be instanced. In the
_Aurania_, of the Cunard Company, the proportions—although perhaps
only in the line along which modern professional ideas tend—are
certainly in advance of the general practice with regard to vessels
of her great size. The dimensions of the _Servia_, the _Alaska_,
and the _City of Rome_—three vessels comparable with the _Aurania_
as constituting the largest merchant vessels afloat—all give a
proportion of 10 beams to the length. The _Aurania’s_ dimensions—470
feet by 57 feet by 39 feet—show her to have only about 8¼ beams to
length. The success of the older type of vessel having proportions
somewhat similar to this “modern instance” has in no material
sense been eclipsed by the narrow types which subsequently for
so long prevailed. Availing themselves of that freedom which
independence of the registration societies yield—their vessels not
being “classed”—the Cunard Coy determined to adopt the old-time
proportions. The step has been justified, in so far as affected by
the matter of speed, the powerful vessel, at her trials on the Clyde,
having attained a mean speed of 17¾ knots, or 20½ statute miles, per
hour. The stable qualities due to the great breadth of the _Aurania_
has in actual service further confirmed the wisdom of the change. The
magnificent vessels presently building on the Clyde for the Cunard
Coy., though between 20 and 30 feet longer, are the same breadth as
the _Aurania_, _i.e._, 57 feet. This is accounted for by the fact
that the breadth of beam fixed for the _Aurania_ was the largest
amount permissible, having regard to the breadth of entrance of the
largest dock in New York. This _en passant_ is worthy of notice as
giving colourable justification to the complaints sometimes made that
civil engineers are urged to progress in dock accommodation only by
shipbuilders treading on their heels.
Coincident with the changes made in the dimensions and structure
of vessels, there are numerous features of enhanced comfort for
passengers and crew which are deserving of notice. Notably is
this manifest in the arrangement of saloons and state-rooms—their
appointment, lighting, and ventilation. The character of steamships
for the great ocean highways in this respect is above and beyond
anything which Board of Trade enactments seek to secure. The amount
of spirited competition itself on those services, acts as an
efficient promoter of excellence in design and equipment.
It is now the prevailing fashion to appropriate that part of a
steamer just before the engine and boiler hatchways for the principal
saloon and first-class berthing, and it has so many advantages over
the old plan of locating these apartments in the poop or after
extremity of the vessel that its adoption in large steamers of the
passenger-carrying trade has become all but general. Some of these
advantages may be briefly enumerated. They are:—ampler and airier
saloon space: the plumbness of the vessel’s sides permitting a
saloon completely athwartship, which is scarcely practicable in
the conventional situation aft, because of the curvature of sides;
increased facilities for ventilation; purer air; freedom from the
noise and vibration caused by propeller; comparative immunity from
the effects of “pitching” or longitudinal oscillation.
Nothing, perhaps, in connection with improved saloon accommodation
strikes one so much as the increased height between decks now
prevalent. While from six-and-a-half to seven-and-a-half feet
was considered sufficient some years ago, it is now the practice
in first-class steamers to make the height as much as from
eight-and-a-half to nine-and-a-half feet. The feeling of spaciousness
this change contributes to the saloons, as well as the scope it
yields for architectural treatment of the walls, are not the least
gratifying results of the improvement. How much the latter result
has been taken advantage of in our modern passenger steamships need
scarcely be told, as their architectural and decorative character is
often and eloquently enlarged upon by delighted voyagers.
[Illustration: FIG. 9.
LONGITUDINAL SECTION OF GRAND SALOON IN _S.S. America_, SHOWING
DOME-ROOF.]
A noteworthy feature in improved saloon accommodation is the
provision of music rooms or social halls, which are usually situated
above the dining saloons, and connected or made one therewith by
means of light and ventilation wells placed in the centre. The
size and ornamentation of these, and the light and air they are
the means of admitting, contribute in a very marked degree to the
spaciousness, beauty, and comfort of the main saloon. By recent
special modifications in the deck structure, several builders on the
Clyde—notably Messrs J. & G. Thomson—are rendering this feature of
greater value than ever. In the National Line Steamship _America_,
just finished by the firm named and to which attention has already
been directed, the Grand Saloon is a splendid apartment, extending
from side to side of the vessel, and measures over eighty feet in
length. Its size and height are augmented in a remarkable degree by
the fitting of a dome-roof extending in height through two tiers
of decks, and embracing about half the length of saloon. This
feature—some conception of which may be gathered from the sketches
shown by Figs. 9 and 10, is altogether free of athwartship beams,
and practically gives to the saloon a clear height of 18 feet. The
crown of the dome is formed of beautifully-executed stained glass,
finished round its base in a richly coloured frieze formed of panels
containing well-executed oil paintings. The whole feature, for
structure, ampleness, and ornamentation, is a noteworthy advance in
the way of rendering the saloons of steamships more comfortable—not
to say palatial—and reflects the utmost credit on the building firm.
[Illustration: FIG. 10.
CROSS SECTION OF GRAND SALOON IN _S.S. America_, SHOWING DOME-ROOF.]
In several vessels built within recent years on the Clyde there has
been adopted—in addition to the athwartship middle length saloon, a
curious and complete reversal of the traditional arrangement with
respect to accommodation for the crew. The plan, one would think,
must shock the orthodox sentiment of our seamen, whatever they may
think of its utility. A few strokes of the draughtsman’s pencil, and
_per saltum_ “Jack” and his “castle” are transported to the poop, and
the precincts so long sacred to his use are prostituted to the lounge
and the tobacco pipe of the pampered “land-lubber”—_i.e._, they form
a luxuriant smoking saloon for passengers.
Of the multifarious ways in which modern invention and skill are laid
under contribution to the end that voyagers shall have the maximum
of safety and comfort on board ship, the system of electric lighting
now so extensively adopted is not the least noteworthy. It is only
about three years ago since the application of the incandescent form
of electric lamp on board ship was first tried. The success of the
system and its rapid extension during the subsequent period has been
remarkable, and is a matter upon which electricians, shipowners, and
sea voyagers are alike to be congratulated. In every well-appointed
passenger ship for ocean service, the electric light has already
supplanted the former method of lighting the saloons, state-rooms,
and machinery spaces, by means of oil lamps, which has so often
proved a fruitful source of annoyance to passengers and crew, if not,
indeed, of positive danger to the vessel herself.
The advantages of the change are such as constitute the electric
light an invaluable acquisition on board every modern passenger
steamship. The light gives off very little heat, there is no smell,
no products of combustion to produce headaches and sickness. No
matches are required, and the danger from fire is absolutely reduced
to a minimum. The light requires little or no attention on the part
of stewards, for it is only requisite that a man be sent round once
a day to see whether any of the lamps require renewal, and the
renewal of a lamp is performed as simply as trimming the wick of an
oil lamp or placing a fresh candle into a candlestick. The danger,
annoyance and time, formerly spent in storing up and dealing out
large quantities of paraffin or other oils, are completely obviated.
The lamps are as easily subject to the control of the passenger as
ordinary gas jets. Instead of the flickering and somewhat clumsy oil
lamps, the electric system presents, encased in neat, tiny, glass
globes, a steady, mellow white light, the adaptability of which to
any conceivable position or design is one of its most beautiful
properties. The artistic grouping of the electric incandescent lamps,
and their combination with the architectural features of saloons,
are matters to which the forms adopted for the best known lamps—the
Edison & Swan types—specially lend themselves. A single Edison lamp
is shown by Fig. 11.
The work in electric lighting on board ship for the year 1883 shows
how firmly the electric system has become established as the only
system for first-class passenger vessels. The report of the Edison
& Swan United Companies embraces the work on thirty-one vessels,
including three Indian troopships (and four more on order), four
vessels for the Clan Line, one for the Peninsular and Oriental
Company, one for the Union Steamship Company, three for the Cunard
Company, three for the British India Steam Navigation Company, three
for the New Zealand Shipping Company, and so on. The list of Messrs
Siemens Brothers amounts to twenty high-class vessels, including the
_Arizona_, the _Servia_, the _Aurania_, the _City of Rome_, the _City
of Chicago_, the _Austral_, the _Germanic_, and the _Massilia_. These
two firms thus give fifty-one vessels, and adding those entrusted to
outsiders—four in all—affords a total of fifty-five, representing an
aggregate of not less than 11,000 incandescent lamps.
[Illustration: FIG. 11.
EDISON LAMP.]
The application of the electric light on board ship to the purposes
of signalling, as a substitute for the ordinary system of oil
lanterns, has been fully shown in theory and already partially
effected in practice, but its development in this direction is
necessarily retarded by considerations which do not affect its
use in the interior of vessels. Vessels traversing the ocean in
darkness are necessarily dependent one on the other for the means
of knowing their proximity, and as the electric light much exceeds
in power and brilliancy that of oil lanterns, it would have the
effect of eclipsing the latter even within a large radius. The
adoption of the electric light for this very important purpose
would, therefore, have to be pretty much a simultaneous and general
movement throughout the ships of the various companies, if not of
the various nations. Apart from such considerations, however, other
objections have been instanced to the appropriation of the electric
light for this purpose. Difficulty, it is said, has been experienced
in distinguishing the colours pertaining to the port and starboard
side-lights, and fears are entertained regarding the liability of
the light, or the machinery employed in generating the current, to
suddenly fail in its action. Few of the objections named, of course,
amount to very serious obstacles, and as the system is yet so much
in its infancy, it may well happen that a few years will witness all
that is here foreshadowed.
Short of this universal and complete appropriation of the electric
light for signalling, however, it has been introduced with gratifying
results in mercantile steamers for various important purposes—_e.g._,
for lighting up the decks and surrounding wharfage during the work
of loading or disembarking cargo; for projecting a flood of light
ahead of a vessel’s course where navigation is difficult, and when
danger in the shape of rocks or icebergs is imminent. The employment
of the light in the way last named has been specially extended in the
case of vessels intended for naval warfare. By its powerful aid the
position and tactics of the enemy, the configuration of forts about
to be assailed, or the nature of the land where it is proposed to
disembark, can all be revealed, with a minuteness almost as perfect
as that due to the light of day.
Another feature on board ship affecting most intimately the
well-being and comfort of passengers—too often, indeed, the safety of
the ship itself—is that of ventilation. The thorough and efficient
ventilation of ships is a feature which only during very recent times
has received from shipowners and shipbuilders the amount of attention
it deserves. The inadequacy of the methods of ventilation existing
in emigrant ships, and as applied to holds for the ventilation of
cargoes, engaged public attention very considerably a few years ago.
The explosion on board the _Doterel_, with other like casualties,
resulted in the appointment of a Royal Commission to inquire into the
ventilation of ships. The prominence thus given to the subject and
the experience then gained, have been fruitful of increased regard
for efficiency in ship ventilation. In the absence for such a long
time, however, of any system capable of universal application and
having at once the merits of efficiency and cheapness, shipowners
have adhered to old-fashioned, unscientific, and ineffective methods
long after the invention of improved systems, one or other of which
would have well repaid adoption.
In ways and to an extent which may perhaps have been made evident
in the previous pages, the introduction of the electric light is
of itself greatly advantageous in this connection. One striking
peculiarity of the change perhaps requires more explicit statement.
This is the curious fact—patent enough to all who know anything of
the properties of the incandescent light—that what is the very life
of oil or other lights, is to it, certain death. The element thus
vitally concerned is, of course, oxygen; and it need not be more than
hinted that in existing so entirely without this element—at all times
a great desideratum in passenger ships—the electric light is a vast
benefactor to all who “go down to the sea in ships.”
Many highly-improved methods of ventilation are now open to the
shipowner; the number of patented systems in use or awaiting
adoption being adequate testimony to the widespread attention
bestowed upon the subject. These divide themselves into two general
classes:—firstly, systems which aim at providing an efficient
self-acting series of ventilating pipes in which the natural current
or that induced by the vessel’s own speed through the atmosphere, is
the only force utilised; and secondly, those in which machines driven
by steam power are employed to produce fresh currents or extract
vitiated atmosphere.
[Illustration: FIG. 12.]
[Illustration: FIG. 13.]
Various forms of ventilators, belonging to the first-named class,
have been introduced into many ocean-going passenger vessels within
recent years, the result being a considerable improvement in the
sanitary condition of the more confined portions of vessels. One of
the most approved of these, receiving specially extended adoption,
amounting as it does to a highly perfected system, may be noticed
a little in detail. This is the form of ventilator patented and
introduced by Messrs R. Boyle & Son, the well known ventilating
engineers of London and Glasgow, consisting of upcast and downcast
shafts fixed above deck, communicating with the interior of vessel by
a system of piping led to the various compartments. The upcast, or
“air pump” ventilator, as the patentees term it, consists of a fixed
head having an ingenious arrangement of louvre webs, whereby the wind
impinging upon it from any direction, creates a current and exhausts
the air from the cylinder of which the head is part, the foul air
from below immediately ascending to supply the place of the air
extracted. A continuous and powerful upward current is thus induced,
and the head is so devised as to effectually prevent down-draught
or the inlet of water. The elevation and plan of this ventilator
is shown by Figs. 12 and 13. In Fig. 13, 1 represents cylindrical
chamber communicating with shaft below; 2, deep lip to prevent the
possibility of water passing into cylinder and down the shaft; 3,
curved plates to deflect and compress the air over outlet openings or
slits; 4, creates an induced current and exhausts the air from the
cylinder; 5, radial plates to deflect air off centre of slits; 6,
curved baffle plate or guard, to concentrate the current, and prevent
the wind blowing through the slits opposite. The downcast ventilator,
though necessarily more simple, is arranged, by means of similar
louvered webs to prevent any water passing below, lodging it on the
open deck instead. By means of up and downcast ventilators of this
type, it is possible to have the ventilation going on between decks
without interruption when there is a storm blowing and seas sweeping
the deck, whereas under ordinary conditions, and in similar weather,
everything would be battened down and the ventilation _nil_. The
inventors, of course, are able to point to other advantages possessed
by these ventilators, but the above are the salient features,
which have won for their system marked recognition and pretty wide
adoption. As evidencing its efficiency, it may be stated that Messrs
Boyle’s system was awarded the “Burt” prize of £50, offered for
international competition by the Shipwrights’ Coy. of London in 1882
for the best system of ship ventilation.
Having regard to the great importance of first providing means
whereby foul air may be extracted from compartments rather than first
attempting to put fresh air in—at least by other than mechanical
means—it has become the practice with several steamship companies
to fit a series of pipes from the rooms throughout the ’tween decks
all leading into a common main, carrying this main into the boiler
funnel, and thus utilising the powerful draught existing there when
the vessel is under way. The efficiency of this method is all that
could be wished, but its action is necessarily impaired when the
vessel is in port and the boilers not in use. For steamships having
long runs its value is very considerable; but in steamers having
short passages and long port delays its merits are not so pronounced,
and it is, of course, of no account when sailing ships are concerned.
Two systems of ventilation much alike in principle and equally
applicable to the steamer and sailing ship may be shortly referred
to. One is the Norton Ventilator, in which the dipping motion of
vessels is utilised in effecting their own ventilation; the action
in ocean-going vessels, of course, being continuous and automatic.
Two cylinders, closed at the upper ends, are placed on each side of
the stern post at such a distance as not to interfere in any way with
the action of the rudder, and sufficiently close under the stern to
be well out of harm’s way. As the vessel rises the water drops in
these cylinders, which are partly submerged, and in its fall causes a
vacuum, to fill which the air is drawn from all parts of the ship.
The sinking motion of the vessel again fills the cylinders and forces
the foul air collected, through the discharge pipes. The ventilator
admits also of being actuated by steam or other power on board
steamships, the exhausting and forcing device in this case consisting
of a water bell or air chamber to which a vertical reciprocating
motion is imparted by a beam or other attachment operated upon by the
mechanical power adopted. The other method referred to is that now
being pretty extensively introduced by Messrs Mosses and Mitchell, of
London. It consists of two small cylinders, placed on either side of
a ship, in-board, and connected by a pipe. The cylinders are partly
filled with water, and, as the vessel rolls, the water rushes from
the elevated to the depressed side of the ship, from one cylinder
to the other, and, by creating a vacuum, draws up the foul air from
between decks, or out of the hold, by pipes leading below. The air
which is pumped up by this self-acting process goes out through a
discharge pipe over the side, and such is the force of its exit that
it serves to blow a foghorn when required. The cylinders can be
placed so as to be worked by the pitching as well as the rolling of
the vessel, and there is always a sufficient movement of the water to
keep these pumps in action.
Systems of the other class—those involving the aid of mechanical
power—are as much available as the automatic systems, but the greater
expense of fitting, maintaining, and working them are considerations,
apart from the question of their greater efficiency, which stand in
the way of their general adoption. In vessels chiefly intended for
passenger or emigrant carrying, artificial ventilation by mechanical
means has been provided, and the practice is greatly on the increase,
but systems in which natural agents are more largely brought into
requisition have advantages which appeal most effectually to ship
owners in general.
In several modern steamships engaged in cargo and passenger service,
hydraulic machinery designed to take the place of the usual deck
steam equipment has recently been introduced with great advantage.
This embraces machinery used for steering the vessel, loading and
discharging cargo, heaving anchors; for performing, indeed, all the
work on board excepting that of propulsion. From experience of the
well proved utility and durability of hydraulic power on shore, it
seems quite a natural consequence that it should take its place on
board ship. Indeed, the system has so many advantages both from
the point of view of the passenger and of the steamship owner,
the wonder is that its introduction has been so long delayed. Its
perfect noiselessness, as compared with the rattling, hissing, steam
machinery now in vogue, is an advantage which will appeal strongly
to the sea voyager. The great speed of the system, as well as the
absence of jar and noise, the reduction in wear and tear, and the
obviating of well-known disadvantages incidental to steam pipes, are
merits of the system which are bound to appeal to the steamship owner.
It has been well pointed out by Mr A. Betts Brown, of Edinburgh, the
patentee and manufacturer of this class of machinery, in a paper read
by him before a recent meeting of the Institution of Naval Architects
that—“With all the noise of steam engines at work on deck, running at
piston speeds of as much as 1000 feet per minute, the cargo is lifted
from the hold at a rate of only from one to two feet per second,
which cannot be considered as keeping pace with the general progress
made in other departments of steamship economy. In short, vast sums
are spent on fuel to gain half a knot extra speed on a passage,
while hours may be wasted in port in consequence of the primitive
nature of the present system of deck machinery for discharging
cargo.” Previous to 1880, Mr Brown had supplied and fitted hydraulic
machinery on board the paddle-steamer _Cosmos_, built by Messrs A.
& J. Inglis, of Glasgow, intended for South American river service,
but it was only in that year that he had an opportunity of fitting a
large ocean-trading steamship with the system. This was the _Quetta_,
built by Messrs Denny, Dumbarton, to whom, with the managers of
the British India Association Steam Navigation Company, who own
the vessel, Mr Brown ascribes credit for the opportunity afforded
him of fitting his firm’s system on a complete scale. The _Quetta_
is 380-ft. in length, 40-ft. breadth, depth of hold 29-ft., and
3,302 tons gross, and is fitted with a complete system of hydraulic
machinery performing the following functions:—Steering, heaving the
anchor, warping by capstans fore and aft, taking in and discharging
cargo, lowering the derricks to clear cargo over side, hoisting
ashes, reversing main engines, and shutting tunnel water-tight
door in engine-room. For detailed descriptions of these various
appliances, the reader is referred to the before-mentioned paper.
The most for which space is here available is a very general outline
of the principle on which they are supplied with motive power. The
prime mover consists of a pair of compound surface-condensing pumping
engines of 100 indicated horse-power, situated in the engine-room
of the vessel. These engines pump water (or in winter non-freezing
fluid) from a tank into a steam accumulator. The pumping engines are
started and stopped by the falling or rising of the steam piston in
the accumulator; and since the piston falls when the hydraulic power
is being utilised, and rises to its former level when the power is
not in use, it follows that the apparatus is perfectly automatic.
Once started, it does not require the supervision of an engineer,
and it maintains a steady pressure of 800-lbs. per square inch in
the hydraulic mains or pressure pipes. These are carried up from
the engine-room, and extend fore and aft the ship. Alongside the
pressure main a similar return main is laid, which discharges into
the tank. From the pressure mains branches are connected to the
various hydraulic machines. After having done its work, the water
is discharged into the return mains, being thus used over and over
again. The experience obtained in the working of the _Quetta_ shows
that a donkey boiler of the usual size, just sufficient for steam
winches, enables the cargo to be discharged in half the time: in
other words, does double the work on a given coal consumpt with
compound surface-condensing pumping engine, and the hydraulic system.
The advantages of hydraulic machinery have been thus summarised:—A
pair of engines in one place do, with no noise and half the
consumption of fuel, the work usually performed by perhaps a dozen
donkey engines, while about £30 or £40 a voyage is saved in wear and
tear. The increase of speed obtained in loading and discharging cargo
practically ensures a quicker voyage. The rapidly working machinery
necessitates double gangs of men in the hold; but though the hands
are more numerous they are paid for a shorter time, and the cost of
labour per ton of cargo is thus less than usual. The prime outlay
is considerably greater than under the ordinary system, but it is
calculated that in at least three years the extra expense will have
been saved.
Notwithstanding the considerable increase in cost (more than double
that of steam equipment) of the hydraulic system, the British India
Association have seen their way to fit the succeeding steamers
they have built, similarly to the _Quetta_, namely, the _Bulimba_,
_Waroonga_, and _Manora_, the two intervening ships having their
emigrant quarters ventilated by fans driven by hydraulic engines, as
well as the usual deck equipment. In addition to the above, there
have already been nine other steamers fitted successfully by Mr
Brown’s firm with hydraulic machinery—including the Union Steamship
Coy.’s _Tartar_, of 4340 tons—and there is every prospect now of its
taking the place of the noisy steam machinery in at least our most
important passenger lines.
* * * * *
The regard which is had to comfort and luxury in modern passenger
steamers has manifested itself—like the attention devoted to
swiftness and safety—in various propositions and designs of a more
or less novel kind. These, indeed, have very often consisted of
designs embracing the whole of the qualities named; comfort and
luxury being coincident with the more important properties of speed
and safety already noticed; but not a few propositions and actual
undertakings have consisted of vessels in which comfort has largely
been the dominant and regulating condition of design. This subject
receives happier illustration from the history of steam service
between England and France, than perhaps from any other service
that could be instanced. The thought and speech expended on “an
efficient Channel service” at the meetings of the various societies
concerned with shipbuilding and marine engineering, and the space
devoted to the subject in the technical journals, has been no more
than commensurate with the number and variety of projects for its
accomplishment, submitted from time to time. Many of the schemes
have not been quite of a marine character, and these, of course,
lie beyond the province of the present review; but so far as ships
are concerned, it is interesting to note to what extent comfort has
been the dominant and regulating condition in the designs. In the
_Castalia_ and the _Calais-Douvres_, employed in Channel service,
features of considerable novelty—notably the double hulls—were
adopted, and it was to the desire for increased comfort as much as
speed that their introduction was owing.
In the steamer _Bessemer_, however, built at Hull in 1875, this
subject finds happiest illustration. This steamer, which involved
some very interesting and novel problems in shipbuilding—in which
the matters of propulsion and steering were largely concerned—was
designed for the special purpose of practically testing an invention
of Mr Henry Bessemer’s, having as its object the alleviation of the
evils of sea-sickness. Mr (now Sir Henry) Bessemer’s invention, as
applied in this case, consisted of a saloon supported on longitudinal
pivots, which was to be made unsusceptible to transverse oscillation
by the application to it of machinery wrought by hydraulic power. It
was the intention of the eminent inventor to have applied this system
to the correction of longitudinal as well as transverse oscillation,
but on considering that the steamer was to be of large dimensions
and performing a service in comparatively small waves it was thought
desirable to limit its application to transverse motion, at the same
time having regard to the longitudinal motion by reducing the height
of the vessel for a distance of 50-ft. at each end, thereby inducing
depression at the extremities, through the vessel’s not rising to,
but being overswept by, the waves.
Although an influential company was formed to work the _Bessemer_
and other vessels embodying her novel features, which it was thought
might follow, she was virtually abandoned after one or two trials
across the Channel. Her failure was assumed without exhaustive and
conclusive trials being made of the many novelties embodied in
her construction, some of which were obviously of an experimental
character. This is the more to be regretted because of the beneficent
issues involved in the project, and also in some degree because of
the extent to which the faith of some intrepid and experienced men
was pledged to its success. Nevertheless, it was always a matter of
grave doubt, even when the fullest measure of mechanical success was
allowed for, whether the idea of the pivoted saloon was calculated to
secure that immunity from the effects of ship motion in a seaway, for
which the celebrated patentee felt induced to hope.
It is maintained by many who profess to have given the subject
attention, that sea-sickness in its most virulent forms, and in the
majority of instances, is less attributable to the transverse and
longitudinal oscillations—known respectively, as the “rolling” and
“pitching” motions—than to the vertical movement termed “dipping,”
which in its descent from the summit of one wave until upborne by the
wave next following, the vessel undergoes. Now, this is a condition
for which, in the Bessemer project, there was no provision, nor
indeed well can be under any circumstances, save in the simple but
costly expedient of adding to the dimensions or bulk of vessels,
irrespective of form. The Czar of Russia’s yacht _Livadia_, built
some years ago, exemplified in her extraordinary dimensions and great
bulk the truth of such reasoning. The actual rolling and pitching of
this remarkable vessel, as observed in the height of a gale in the
Bay of Biscay, and in the midst of very heavy seas, was exceeding
small. This never exceeded four degrees for the single roll, or seven
degrees for the double roll, nor beyond five degrees for the forward
pitch, or nine degrees for the double pitch, so to speak. This
horizontal steadiness appeared to experts, who were on board at the
time, most remarkable, and Sir E. J. Reed, in a communication to the
_Times_, commented amongst other things on the agreeableness of the
contrast the voyage on the _Livadia_ afforded, with his experience of
voyaging at sea in ordinary ships.
After all, it must be acknowledged that attempts hitherto made to
obviate the evils of sea-sickness by novelty in design fall very
far short of attaining the beneficent results sought after. The
_Bessemer_, the _Livadia_, the _Calais-Douvres_, and other _unique_
craft primarily conceived with regard to this end, are now, it
would seem, exemplifying in their latter fate the futility of the
endeavour. Such attempts, however ill-advised they may possibly
appear in the light of the knowledge their very failure or their
partial successes yield, have still their creditable and praiseworthy
aspects. The spirit which has prompted some of them is not wholly
one of money-making, and their histories enrich the general fund of
experience far more than libraries of untried theories. Shipowners
are too ready to shut their minds against everything which seeks
the _acme_ of comfort and safety by other means than those which
guarantee _economical_ success, or those which consist in increasing
the size and power, and enhancing the accommodation of conventional
types of vessels. These novelties and innovations, on the other hand,
represent more of the intrepidity essential to genuine advancement
than is forthcoming in a thousand merchant ships of the conventional
type.
Happily the need for such enterprise as is involved in at once
departing from tried types, has within recent years been largely, if
not altogether, obviated, through improved procedure in the work of
design. The more thoroughly analytic process of investigation and
experiment now in vogue, greatly curtails the number of novelties
introduced, or which reach the constructive stage. Many present-day
projects never get beyond the “paper stage,” which in times not so
far distant would have spelled out “failure” to the very last letter.
Since the system of model experiment has begun to be practised in
a reliable manner, and since theoretical prediction generally has
become better appreciated, over-sanguine inventors have been spared
the penalties of failure in actual practice, and ingenuity has been
reclaimed or warned away from channels that would inevitably have
proved chimerical.
List of Papers bearing on the safety and comfort of modern
steamships, to which readers desiring fuller acquaintance with the
_technique_ and details of the subjects are referred:—
ON THE NECESSITY OF FITTING PASSENGER SHIPS WITH SUFFICIENT
WATERTIGHT BULKHEADS, by Mr Lawrance Hill: Trans. Inst. N.A., vol.
xiv., 1873.
ON WATER AND FIRE-TIGHT COMPARTMENTS IN SHIPS, by Mr Thomas May:
Trans. Inst. N.A., vol. xiv., 1873.
ON CAUSES OF UNSEAWORTHINESS IN MERCHANT STEAMERS, by Mr Benjamin
Martell: Trans. Inst. N.A., vol. xxi., 1880.
ON MODERN MERCHANT STEAMERS, by Mr James Dunn: Trans. Inst. Naval
Architects, vol. xxiii, 1882.
ON BULKHEADS, by Mr James Dunn: Trans. Inst. N.A., vol. xxiv., 1883.
ON PUMPING AND VENTILATING ARRANGEMENTS, by Mr Thomas Morley:
Trans. Inst. N.A., vol. xvii., 1876.
ON SIR WM. THOMSON’S NAVIGATIONAL SOUNDING MACHINE, by Mr P. M.
Swan: Trans. Inst. N.A., vol. xx., 1879.
ON STEAMSHIPS FOR THE CHANNEL SERVICE, by Mr John Grantham: Trans.
Inst. N.A., vol. xiv., 1873.
ON CHANNEL STEAMERS, by Mr John Dudgeon: Trans. Inst. N.A., vol.
xiv., 1873.
ON HIGH-SPEED CHANNEL STEAMERS, by Mr H. Bowlby Willson: Trans.
Inst. N.A., vol. xv., 1874.
ON THE ARK SALOON, OR THE UTILISATION OF DECKHOUSES FOR SAVING LIFE
IN SHIPWRECK, by Rev. W. R. Jolley, R.N.: Trans. Inst. N.A., vol.
xv., 1874.
ON THE BESSEMER STEAMSHIP, by Mr E. J. Reed: Trans. Inst. N.A.,
vol. xvi, 1875.
ON THE BESSEMER CHANNEL STEAMER: Naval Science, edited by Mr E. J.
Reed, 1873.
ON ELECTRIC LIGHTING FOR SHIPS AND MINES, by Mr Andw. Jamieson:
Trans. Inst. Engineers and Shipbuilders, vol. xxv., 1881-82.
ELECTRICITY ON THE STEAMSHIP (Series of Papers): the “Steamship,”
vol. I., 1883.
ON THE VENTILATION OF MERCHANT SHIPS, by Mr Jas. Webb: Trans. Inst.
N.A., vol, xxv., 1884.
ON THE COMPARATIVE SAFETY OF WELL-DECKED STEAMERS, by Mr Thos.
Phillips: Trans. Inst. N.A., vol. xxv., 1884.
ON THE APPLICATION OF HYDRAULIC MACHINERY TO THE LOADING,
DISCHARGING, STEERING, AND WORKING OF STEAMSHIPS, by Mr A. B.
Brown: Trans. Inst. N.A., vol. xxv., 1884.
CHAPTER IV.
PROGRESS IN THE SCIENCE OF SHIPBUILDING.
The appreciation and employment of scientific method and analysis in
designing and building ships have at no previous time been greater
than they are at present. This is already yielding benefits and
ensuring successes which only a few years ago would have remained
ungathered and unachieved, or at best would only have been attained
after wasteful expenditure of money, time, and skill, if not the
sacrifice of human life. Not so long ago endeavours were seldom made
to extract lessons of general value from particular occurrences,
there being a disposition prevalent to accept facts without
accounting for them—“to rejoice in a success and regard a failure as
irreparable”—the outcome, it may at once be said, of indifference,
false ideas of economy, and of a limited conception of the part
scientific methods should play in successful shipbuilding.
Particular occurrences within recent years have without doubt played
a large part in bringing about this more general and intelligent
appreciation of such matters. Some maintain, indeed, that it is
only under pressure of circumstances that anything like proper
regard for fundamental principles has obtained hold among mercantile
shipbuilders. This remissness, even admitting it to be true, is the
more natural and excusable in private commercial concerns, when it
is considered that the bulk of progress made, even in Admiralty
quarters—where ships take several years each to build, and there
is more time for scientific investigation and experiment than is
possible in mercantile work—is more attributable to the awakenings
which have followed upon great disasters than to the natural
improvement of ordinary practice. The terrible loss of the _Captain_
in September, 1870, for example, by which 500 lives were sacrificed,
led to a fuller recognition of the necessity for exact experiment
and calculation to determine thoroughly the conditions of stability
for war vessels; and many war-ships then under construction at the
dockyards—particularly those of the low freeboard type—were altered
in consequence, for the purpose of adding to their safety. The
capsizing of the _Eurydice_ off the Isle of Wight in March, 1878;
the mysterious and mournful loss of her sister ship the _Atalanta_
in 1880; the explosion on board the _Thunderer_ in 1876, by which 45
lives were lost, and the still more calamitous case of the _Doterel_
in April, 1881, by which the ship and 148 lives were destroyed,
are all instances of calamity, the causes of which have formed the
subject of official inquiry, all in their turn teaching important
lessons and yielding subsequent benefits not easily calculable.
Recent occurrences of a very calamitous nature in connection with
merchant ships—some of which will be more explicitly referred to
further on—have been attended with similarly mournful, but, it may
be added, with similarly beneficial results. These disasters and
the resulting inquiries have shown pretty conclusively that the
knowledge of a vessel’s stability and other vital qualities possessed
by ship’s officers is often meagre and erroneous; and that far too
little attention is usually paid to a vessel’s technical qualities
by shipowners or their advisers. They have also tended to prove that
exact knowledge of the principles of ship design, and observance of
scientific method in their construction, are not yet sufficiently
prevalent or thorough in mercantile shipyards.
* * * * *
Progress in the pure science of naval architecture, as distinguished
from the practical application of scientific rules and principles
to shipbuilding, is a great and complex subject, and one which it
would be impossible to do full justice to here. Before attempting
to treat upon these matters as concerned with the period covered by
this review, it may be instructive to trace briefly the progress
made in the past, and take note of the agencies through which such
progress has been effected. In this undertaking, concerned as it
is with matters relating to a period prior to that with which the
present work chiefly deals, the author has availed himself to some
extent of already published works traversing the same ground. As
having afforded the needful assistance in this connection, and as
being a source to which readers may turn for fuller information,
reference may here be made to an article in the _Westminster Review_
of January, 1881, on “The Progress of Shipbuilding in England.” This
article, though unsigned, is from the pen of Mr W. H. White, late
Chief Constructor of the Navy, and author of the well known “Manual
of Naval Architecture.” It furnishes an appreciative and concise
account of the literature and the educational agencies connected
with the theory of naval architecture, and sketches the influence of
science on practice, and _vice versa_ in the profession since the
beginning of the present century.
As has already been indicated, the period during which scientific
knowledge and methods have had any considerable place in merchant
shipbuilding, does not extend back over very many years. In
connection with the Royal Navy, however, the study of scientific
naval architecture has been fostered and promoted under Government
auspices almost from the commencement of the present century; not,
however—it must be added—without alternating periods of regard and
neglect, nor irrespective of pressure from extraneous sources.
Although progress in this matter has not been solely due to
Government agencies, it may be maintained that a large part of the
positive and accurate scientific knowledge which now exists has
grown out of the exigencies of the naval service, and has come from
sources more or less supported by or connected with Government
institutions. It will of course be understood that the science of
naval architecture is a field in which many besides shipbuilders,
and indeed many besides professional naval architects, have laboured
with signal success. The fund of knowledge has been enriched, and
the practice of shipbuilding improved, by men whose association
with the shipyard has been of an indirect and amateur kind, and—it
must be added—whose valuable labours the shipyard has often but
scantily recognised. Mathematicians—“mere theorists,” as they have
been called—have made original investigations and scientific analyses
which have upset many previously received practical notions, and
established principles, the appreciation of which alone, has led to
subsequent progress in actual practice. The part taken by merchant
shipbuilders has consisted in the experimental verification, and
sometimes the practical correction of principles thus evolved, but
even to this extent the service done has been largely incidental.
Those considerations which form the economic basis of every
commercial concern have naturally circumscribed such service, and
only a few notable firms have been able to break through the common
restrictions.
The systematic study of scientific naval architecture may be said
only to have begun in Britain in 1811, in which year, as the outcome
of recommendations made by a Government Commission appointed to
inquire into naval construction in 1806, the first School of Naval
Architecture was established at Portsmouth, under the direction of
Dr Inman, a distinguished member of the University of Cambridge. All
the great advances which had been made previously in the science
of naval architecture were chiefly due to foreigners, and any one
wishing to acquaint himself at first hand with all that was then
most advanced would have to consult the learned treatises of such
distinguished Frenchmen as Bouguer, Dupin, Euler, D’Alembert, and the
Abbé Bossut, of the distinguished Spaniard Don Juan d’Ulloa, and of
Chapman, the celebrated constructor of the Swedish Navy. One or two
English writers, between 1750 and 1800, had published translations
of some of these foreign treatises, but the only original work of
any importance was by Atwood, who contributed a “Disquisition on
the Stability of Ships” to the proceedings of the Royal Society
(1796-98). This contribution was both a criticism and an extension of
flotation and stability investigations by Bouguer, and as an example
of scientific method applied to exact calculations of the qualities
of ships it is still well worthy of study. In 1791 a “Society for the
Improvement of Naval Architecture” had been formed, the membership
being both numerous and influential, and in 1806 the growing sense of
need for improved scientific methods culminated in the appointment of
the Commission above mentioned, and in the establishment five years
later of the first School of Naval Architecture. This institution
existed for over twenty years, over forty students were trained, and
the science of naval architecture was greatly promoted through its
agency. Almost as a body the students of this school, with their
able teacher, deserve the honour of being regarded as the founders
of an English literature of naval architecture. Nevertheless, the
recognition of Dr Inman’s services, and his pupils’ capabilities as
designers, by the naval authorities was of a cold and disappointing
nature. Ultimately, however, many of them attained positions wherein
their talents found worthy exercise.
After the abolition of the School of Naval Architecture, under Dr
Inman, in 1832, no agency for higher education existed until 1848,
when the urgent necessity for a steam re-construction of the Navy
forced attention to the want of trained men, and resulted in the
establishment of a second school at Portsmouth. The principal of
this school was Dr Woolley, an eminent graduate of the University
of Cambridge. From 1848 on to the present time, Dr Woolley has
held a prominent place amongst the promoters of naval science, and
the pupils produced by the institution under his directorship have
given in various ways good practical evidence of his capability as a
teacher. After five or six years of useful work, this second school
was done away with, and a third was established in London in 1864,
after pressure had been brought to bear upon the Government of the
day by the Institution of Naval Architects—an association which was
founded in 1860, and which has since had so flourishing an existence.
The new school was placed for a time under the control of the
Science and Art Department at South Kensington, Dr Woolley being
Inspector-General, and the late Mr C. W. Merrifield, F.R.S.,
Principal. This school, unlike its predecessors, was not nominally a
mere Admiralty establishment, but offered admission to private naval
architects and engineers, and did not exclude foreigners. It remained
in operation at South Kensington until 1873, when the Admiralty
decided to establish the Royal Naval College at Greenwich, and to
train their students of naval architecture and marine engineering
there. Since 1873, therefore, what may be regarded as a continuation
of the third school has been at work at Greenwich, the Admiralty
granting facilities for the entry of private and foreign students,
much as was done at South Kensington.
The small extent to which this institution has been taken advantage
of by private students, or by those whose aim is to equip themselves
for service in merchant shipbuilding, notwithstanding the inducements
existing in the shape of substantial scholarships, has often been
subject of comment. Various reasons have been adduced for this state
of matters, but the true cause would seem to be largely concerned
with the character of the entrance examinations and with the course
of study provided. The subject is well worthy of consideration, and
fuller reference will be made to it further on when some educational
agencies which have been recently established are under consideration.
At such important junctures in the history of shipbuilding as the
introduction of steam power for propulsion in place of sails, and
the employment of iron in place of wood for the hulls, precedent
and experience lost much of their value under the new conditions.
The association of civil and mechanical engineers with shipbuilding
at these crises was of immense advantage. Such men as Fairbairn
and Brunel, who had previously gained high reputations in other
branches, were enabled by their scientific skill in designing bridges
and other structures in wrought-iron, to achieve much, and to take
the lead in ship design and construction. “To men of this class,”
says Mr W. H. White, in the article already alluded to, “careful
preliminary investigation and calculation naturally formed part
of the work of designing ships; ‘rule of thumb’ was not likely to
find favour, even if it had been applicable, which it was not, under
the circumstances. At first, much was done on imperfect methods,
comparatively in the dark; failures were not rare; yet progress was
made, and gradually greater precision was attained, in the attempt
to design steamers capable of proceeding at certain assigned speeds
when laden to a given draught. In fact, the construction of steamers
rendered imperative a careful study of the laws of fluid resistance,
and of the cognate investigation of the mechanical theory of
propulsion—both of which subjects lay practically outside the field
of the designers of sailing ships. The speed of a sailing ship is
obviously dependent upon the force and direction of the wind; her
designer, therefore, chooses forms and proportions which will enable
a good spread of canvas to be carried, on a handy stable vessel.
Questions of resistance to the progress of the ship were therefore
subordinated to sail-carrying power and handiness in sailing ships;
whereas in steamers designed for a certain speed the question of
resistance occupies a primary place, seeing that the engine power
must be proportioned to the resistance. Consequently, while keeping
in view stability, handiness, and structural strength, the designer
of a steamer has a more difficult task than the designer of a sailing
ship, and the difficulty can only be met if faced intelligently by
scientific analysis. Hence it happened, as was previously remarked,
that a more general appreciation of the value of scientific methods
accompanied the development of steam navigation and iron shipbuilding
in the British mercantile marine.”
Another name that must be linked with those already mentioned in
connection with the change from wood to iron in shipbuilding, and
with the new conditions imposed by the transition from sail to steam,
is that of the late Mr John Scott Russell, already referred to at the
beginning of this work. In the fields of inquiry so largely opened
up at the period referred to, Mr Russell was a most distinguished
worker. His advocacy and adoption in practice of special structural
principles, as illustrated not only in the _Great Eastern_ but in
other vessels, has influenced subsequent practice incalculably, and
by his persevering investigations upon the resistance of vessels,
and the “wave-line” theory he advanced, as well as by his inquiry
into the characteristics of wave motion, he laid designers of that
period and subsequent investigators under great indebtedness. His
contributions to the literature of the profession—notably his _magnum
opus_, entitled “Modern System of Naval Architecture”—and the large
share he subsequently took in the deliberations of the Institution of
Naval Architects, and of other societies concerned with shipbuilding
and engineering, enhance that indebtedness and remain as permanent
records of his skill and originality.
Approaching the period with which this review is more particularly
concerned, reference must now be made to the valuable labours of two
eminent men, whose loss the profession has had to mourn within recent
years. These are the late Professor Macquorn Rankine and the late Mr
William Froude, neither of whom was by profession a naval architect,
yet both of whom were led by love of the subject to give their
matured experience as civil engineers and mathematical experts to the
promotion of knowledge in this domain.
Rankine appears to have become specially interested in the problems
connected with ship design, after he became Professor of Civil
Engineering at Glasgow University in 1855. Conjointly with Mr Isaac
Watts, late Chief Constructor of the Navy, and formerly a student of
the first School of Naval Architecture; Mr F. K. Barnes, now Surveyor
of Dockyards, and Chief Constructor of the Navy, and a distinguished
student of the second school; and the late Mr J. R. Napier, a member
of the famous Clyde shipbuilding firm, Prof. Rankine produced in 1866
“Shipbuilding: Theoretical and Practical.” This valuable treatise was
edited, and for the most part written, by Prof. Rankine, and provides
a complete system of information on all branches of shipbuilding
and marine engineering, although subsequent progress in certain
departments of naval science has made a new edition desirable. The
work is also distinguished for its enunciation of several theories
connected with the resistance and propulsion of vessels by Prof.
Rankine, which have become the accepted basis of modern practice.
Of these the mechanical theory of the action of propellers, and
the stream-line theory of resistance, are the best known. His
investigations and writings on the latter subject were most ably
supplemented and confirmed by Mr Froude, whose beautifully-contrived
model experiments, coupled with his discovery of the law by which
such experiments can be made to afford reliable data for the
resistance of full-sized vessels, have laid the profession under even
a heavier load of indebtedness.
This, however, was not the only work of investigation and experiment
with which Mr Froude actively and inseparably identified himself.
Taking up a subject which many authorities before him had studied and
written upon with but little success—that of the phenomena of wave
motion and the oscillation of ships in a seaway—he propounded and
demonstrated at the Institution of Naval Architects in 1861, after
much careful thought and experiment, a theory with respect to it
which at that time was entirely new and striking, but which has since
been firmly established as the sound one.
At first, authorities in the science of naval architecture, like
Moseley and Dr Woolley, regarded the new theory with suspicion and
disapproval; Rankine, on the contrary, warmly supported it, and
helped to develop it and to answer various objections urged against
the hypothesis on which it was based. For nearly twenty years
Mr Froude steadily pursued the inquiry, adding one mathematical
investigation to another, carrying out numerous experiments, and
making voyages for the purpose of studying the behaviour of ships.
Broadly speaking, it may be said that whereas earlier investigations
gave to the naval architect the power of making estimates of the
buoyancy and stability of ships floating in smooth water, they gave
up as altogether hopeless the attempt to predict the behaviour of
ships at sea, or to determine the causes which produce heavy rolling.
On the other hand, thanks to Mr Froude, the designer of a ship now
knows what precautions to take in order to promote steadiness and
good behaviour at sea.
Although the propositions enunciated by Mr Froude were accepted
as laws in a wonderfully short time—considering their startling
nature—their influence on practice, and especially the practical
application of the methods of comparison by which they had been
established, have not even yet been brought to anything like their
full issue. The work is being continued upon the lines laid down
by Mr Froude, amongst others by men whose closer intimacy with the
actual affairs of the shipbuilding yard may be expected to yield
results which will be more immediately reflected in actual practice.
Passing allusion has already been made to the founding of the
Institution of Naval Architects, but an association which has
gathered into its membership so largely of all sections of men
concerned with shipbuilding and shipping, and absorbs so much of the
knowledge and talent in these domains, must have fuller reference
made to it. Regarding its foundation, in 1860, Mr White, in his
article in the _Westminster Review_, says:
“The scheme of the Institution was happily conceived and well
executed. Amongst its earliest members were found the trained naval
architects of the first and second Schools, the leading private
shipbuilders and marine engineers, the principal shipbuilding
officers of the Dockyards, men of science specially interested in
naval architecture, shipowners, merchants, and others connected
with shipping; while a considerable number of sailors from the
Royal Navy and Mercantile Marine showed their appreciation of the
value of naval science by becoming Associates. The list of names
is eminently representative. Sir John Pakington (afterwards Lord
Hampton), then only recently retired from the office of First
Lord of the Admiralty, was the first President. Many experienced
naval officers supported him. There were men like Watts, Read,
and Moorsom, who had been pupils of Dr Inman half a century
before; others, like Fairbairn, Laird, and Grantham, who had been
conversant with iron shipbuilding from its commencement; marine
engineering was worthily represented by veterans like Penn,
Maudslay, and Lloyd; mathematicians and men of science like Canon
Moseley, Dr Woolley, Professor Airy, and Mr Froude appear on the
list. Private shipbuilders and naval architects like Scott Russell,
Samuda, Napier, and White, joined in the movement, so did the
surveying staff of Lloyd’s Register. In fact, there was a general
appreciation of the endeavour to establish an association which
should enable all classes interested in shipping to interchange
ideas and experience with a view to general improvement. Mr Reed
was the first Secretary, retaining that post until he was appointed
Chief Constructor of the Navy, and in that position did much to aid
the progress of the Institution.”
While it is true that the membership list of the Institution in its
early days was of the representative character above indicated, it
should be pointed out that the actual proceedings of the Institution
were not shared in by anything like the variety of talent which the
list comprised, or which now distinguishes its annual meetings.
For many years it was almost the exclusive conference of Admiralty
authorities and members of those shipbuilding and engineering firms
who undertook Government work, and the transactions for a long time
were very largely confined to purely naval matters. The scientific
value of the earlier volumes of the transactions would certainly have
suffered considerably if the papers by Mr Froude and Prof. Rankine
had not formed contributions, and the prosperity and development
of the Institution would have been equally lessened had there not
been general infusion of “new blood” from the mercantile marine in
all parts of the country. This has been going on during the past
twelve years or more, and the scope and utility of the Institution’s
proceedings have increased with the change. Of the later development
of the Institution, the authority already quoted says:—
“Owing to the rapid advances constantly being made in both the
science and the practice of the profession, the ‘Transactions’ have
come to be the chief text-books available. Members and Associates
have joined from all the great maritime nations. Members of the
professional corps of naval architects and engineers of France,
Austria, Italy, Germany, the United States, Russia, Sweden, Norway,
Denmark, Holland, are proud to be numbered with their English
professional brethren, and not a few of these foreign members have
contributed valuable Papers. The meetings of the Institution afford
exceptional opportunities for the discussion of questions having
general interest, as well as others having more special value to
professional men. Different views of the same subject find capable
exponents, and lead to valuable discussions. The latest systems of
construction and most recent changes in _materiel_ are described by
competent authorities. Valuable _data_ are put on record relating
to the designs and performances of war-ships and merchant-ships.
Inventions of various kinds are described and examined. Abstruse
theoretical investigations are by no means rare; and, in many
cases, the contribution of one such Paper by an original thinker
has given a start to others and led to important extensions of
knowledge. In fact, the Institution of Naval Architects has
admirably fulfilled the intentions of its founders, acting as a
centre where valuable information could be collected, and whence
it could be distributed for the general benefit of the profession.
Before it was founded naval science had no home in England; its
treasures lay scattered far and wide in occasional Memoirs and
Papers; but now everything worth preservation naturally finds
its way to the ‘Transactions.’ Any movement affecting shipping
also leaves its record there in Papers and Discussions which will
hereafter have a high historical value.”
As evidencing the change which has latterly come over the Institution
with respect to its annual proceedings, it may be noted that whereas
in the early years there were at some meetings no papers—leaving out
of account those by Froude and Rankine—except by Admiralty members
and others concerned with Government work, there was not a single
paper by an Admiralty man during the meetings of the present year.
* * * * *
With the general reference already made to Mr Froude’s invaluable
labours in connection with the resistance of vessels the brief
statement of the agencies through which progress has been made during
the present century may be considered as brought down to the period
coming within the scope of the term “Modern,” as used in this work.
The more difficult task of chronicling the progress made during the
period in question, both in the science of naval architecture purely,
and in the application of science to practice, must now be attempted.
The plan upon which it is proposed to accomplish this is to show
wherein and to what extent scientific methods in designing and
observing the behaviour of ships have been regarded, and indicating
generally where still further improvement may be looked for. To
accomplish this in such a way as to take appreciative account of the
most salient features, and yet to avoid difficult technical terms
and unnecessary elaboration, may involve some omissions and slight
inaccuracies, important enough from a strictly scientific point of
view, yet which do not materially affect the faithfulness of the
record.[5]
As preparing the way for references to those more special points in
connection with which scientific progress has taken place during
recent years, the following general and elementary outlines of the
principal scientific problems in ship design and construction may be
helpful to many readers:—
DISPLACEMENT AND CARRYING CAPABILITY.
A vessel floating at rest displaces a volume of water whose weight
equals her own total weight.
For vessels floating in sea water the number of cubic feet of water
displaced per ton of weight is, as nearly as possible, thirty-five.
For vessels in fresh water—_i.e._, lakes or rivers—the cubic feet
per ton of weight is thirty-six.
By calculating the volume of under-water portion of the vessel’s
hull, the number of cubic feet displaced by the vessel when
floating at any given draught is obtained. This result, divided by
35 or 36, according as the water is salt or fresh, gives the number
of tons weight displaced, and consequently the total weight of the
vessel.
Calculations being made of the volume of the vessel’s hull to
intermediate distances between the keel and the maximum load line,
it is thus possible to construct a “curve of displacement” from
which the actual amount of displacement at any intermediate draught
can be obtained.
From this curve a set of scales—usually set up alongside a
vertical scale of feet and inches, representing the vessel’s
draught-marks—are constructed, showing—1st, the tons “displacement”
at any draught; 2nd, the tons of “dead-weight” capability—_i.e._,
the tons displacement due to the weight of cargo, coal, ballast,
stores, fresh water, spare gear, &c.—at any draught above the
vessel’s light-draught: “light-draught” being that at which the
vessel floats with holds clean-swept, bilges dry, water in boilers,
and with such spare gear on board as is required by Board of Trade;
and 3rd, the amount of “freeboard”—_i.e._, the distance in feet
and inches from any particular draught line to the top of the deck
amidships.
BUOYANCY AND STABILITY.
A ship floating upright and at rest in still water must fulfil two
conditions—1st, as stated above, she must displace, a weight of
water equal to her own weight; 2nd, her centre of gravity must lie
in the same vertical line with the centre of gravity of the volume
of displacement or “centre of buoyancy.”
The whole weight of the ship may be supposed to be concentrated at
her centre of gravity, and to act vertically downwards, and the
resultant vertical pressure of the surrounding water in the same
way to act upwards through the centre of buoyancy.
When the ship has been inclined from the upright position, by any
force, the downward and the upward forces—weight and buoyancy
respectively—act through two separate but parallel vertical
lines, and form what is technically known as a “couple.” The
perpendicular distance between the vertical lines usually varies
with the inclination, and is called the “arm” of the couple. This
arm measures the leverage with which the weight and buoyancy of the
ship tend either to force her back into the upright position, or
to incline her still further, and, it may be, to capsize her. The
former effect would be the result of what is known as a “righting
couple,” the latter the result of an “upsetting couple.”
[Illustration: FIG. 14. FIG. 15.]
This may be made clearer by illustration. On Figs. 14 and 15,
which show in outline a vessel’s midship section, the vessel being
inclined to a small angle, =G= represents the centre of gravity
of vessel, and =B= the centre of buoyancy. The water line =W.L.=
corresponding to the upright position, in the inclined position
becomes =W_{1}.L_{1}.=, and the centre of buoyancy =B= shifts out
on the immersed side of the vessel to =B_{1}=. Assuming in the case
of Fig. 14 that some external force not involving any shifting of
the centre of gravity has produced the inclination, then the weight
of the vessel acts downwards through =G=, and the buoyancy of her
displacement acts upwards through =B_{1}=, as indicated by the
arrows passing through these points. The combined effect of these
forces, in this case, is to rotate the vessel towards the upright,
_i.e._, it forms a “righting couple.” Fig. 15 illustrates a case
of the opposite kind. The angle of inclination may be supposed to
be greater than in Fig. 14, and the centre of gravity =G= is much
higher in the vessel. The vertical through =B_{1}= is to the left
instead of to the right of the vertical through =G=. The effect of
the forces in this case is to rotate the vessel in the direction
of inclining her still further, and to capsize her—_i.e._, it
forms an “upsetting couple.” A line at =G=, therefore (Fig. 14),
taken at right angles to the new vertical line, gives the distance
which corresponds to the righting arm (=G= =Z=). A similar line at
=G= (Fig. 15) represents the upsetting arm. The lengths of these
arms when multiplied into the displacement, gives the “moments” at
the respective degrees of inclination. The “curve of stability”
for a vessel is simply a graphic representation of these arms or
moments. When calculated for the various degrees of inclination,
they are set off as ordinates along a base line—the righting arms
or moments above, and the upsetting arms or moments below, the
line—at distances corresponding to the number of degrees in the
respective inclinations. A curve drawn through the extremities of
these ordinates is the curve of stability.
The two points above named whose relative positions are vitally
concerned with this subject—_i.e._, centre of buoyancy and
centre of gravity—are determined by shipbuilders for many of
their vessels, although the stability may not be calculated
to its full extent. The position of the centre of buoyancy is
easily ascertained from, and in fact usually forms part of, the
displacement calculation. While the position of centre of gravity
may be found by means of calculation alone, _i.e._—by the process
of estimating the position of the centre of gravity of each of
the component parts, and from this deducing the common centre of
gravity of the whole ship—the work is so laborious, complex, and so
liable to error, that it is scarcely ever adopted at the present
day by mercantile shipbuilders. The position can be ascertained
with comparative ease and greater accuracy by means of “inclining”
experiments with the finished vessel, or closely estimated
before-hand by means of data obtained in the manner alluded to from
previous vessels of similar type.[6]
Another point concerned with stability is that termed the
“metacentre,” which is found by calculation from the lines of
the vessel. Referring to Fig. 14, a vertical line drawn through
the centre of buoyancy =B_{1}= cuts the original vertical line
at =M=. The intersection =M=, when the vessel is inclined to an
indefinitely small angle, is the “metacentre.” It is approximately
the same in all ordinary vessels for inclinations less than say
10°, but varies with greater inclinations. The corresponding
intersections of the consecutive vertical lines for all degrees
of inclination are embraced in the term “metacentrique.” These
features in stability investigations were originated by Bouguer, to
whom reference has already been made. The manner in which they are
concerned with stability will be indicated further on. (See also
footnote on preceding page.)
RESISTANCE POWER AND SPEED.
A ship, in moving through the water, experiences resistance due to
a combination of causes, which combination, according to modern
accepted theory, is made up of three principal elements.
1st—“Frictional” or “skin friction” resistance, due to the
particles of water rubbing against the ship’s hull;
2nd—“Eddy-making” resistance, due to local disturbances or eddies
amongst the particles of water—almost wholly at stern of ship;
3rd—Surface disturbance of the water by the passage of the ship,
resulting in the creation and maintenance of waves: known as
“wave-making” resistance.
The conditions which govern each of these elements, and their
relative importance, may be generally indicated.
Surface-friction resistance, especially for vessels moving at
moderate or slow speeds, is much greater than the resistance due
to other causes—that is if the hull is ordinarily well formed. Its
amount depends upon the area of the immersed surface, upon its
length, upon its degree of roughness, and upon the velocity with
which the water glides over it—_i.e._, upon the speed of the vessel.
Eddy-making resistance only acquires importance in exceptional
cases, _e.g._, in ships having unusually full sterns. In ordinary
well-formed ships it is of small amount, and is caused mainly by
blunt projections such as shaft tubes, propeller brackets, and
stern-posts.
Wave-making resistance is much more variable than surface-friction
resistance. Its amount depends on the form and proportions of
vessels, and on the speed at which they move: being greatest, of
course, in ships of full form and in those moving at high speeds.
The sum of these three main elements of resistance constitutes the
total resistance experienced by a vessel if “towed” through the
water, that is, the resistance considered apart from the action or
influence of the propelling instrument. In the case of a steamship,
however, propelled by a screw or paddle-wheels, the resistance
is augmented, more or less considerably, according to the form,
surface, and disposition of the propelling instrument.
By the employment of various formulæ deduced by scientific
authorities from theory and experiment, an approximation can be
made before-hand to the total resistance of a proposed vessel,
and from this an estimate of the power required to drive her at a
certain speed. Moreover, through the law of comparison propounded
by Mr Froude, the resistance of a ship can at all times be deduced
with fair accuracy from the resistance of her model, certain
corrections well determined by experiment having to be made.
The power of marine engines is expressed either in “nominal” or
“indicated” horse-power. Nominal horse-power is a term practically
obsolete so far as being a measure of the efficiency of engines,
and only exists as a conventional method of commercially measuring
the sizes of engines. Indicated horse-power measures the work
done by the steam in the cylinders during a unit of time, and
33,000 units of work per minute, or 550 units of work per second,
constitute one horse-power. The effective mean pressure of
the steam is ascertained from diagrams drawn by means of the
instrument known as the “Steam Engine Indicator,” and hence the
term “indicated” horse-power.
The development by a vessel’s engines of the power requisite to
drive her at a certain speed is always very considerably more
than the power required simply to overcome her total resistance
at that speed. This excess of power developed over power usefully
employed in overcoming resistance is known as “waste work.” It
amounts in many cases to as much as from 50 to 60 per cent. of the
gross indicated power, and it is absorbed mainly as follows:—In
overcoming frictional and other resistances of the engines and
shafting, working air pumps, &c., and in overcoming the frictional
and edgeways resistance of the propeller. The residue of power
usefully employed is known as the ‘effective’ horse-power. The
respective causes of ‘waste’ and their relative amounts are
problems constantly demanding solution. Progressive speed trials
with actual vessels and experiments with small scale models are
daily contributing to their solution, and to some extent to their
reduction.
STRUCTURAL STRENGTH.
Considering a ship as floating in a state of rest in still water,
the volume of displacement represents a weight of water equal to
the weight of the ship. This equality, however, does not exist
evenly throughout the length of the vessel, or for individual
portions: thus, amidships the weight of water displaced by a
given length—in other words, the buoyancy—is usually considerably
in excess of the weight of that portion of the vessel and her
contents. Similarly at the extremities the ‘weight’ of a certain
length exceeds the ‘buoyancy.’ Between the part or parts of the
vessel in which there is excess of buoyancy over weight, and the
part or parts in which the weight exceeds the buoyancy, there must
obviously be sections of the ship at which the two are equal, and
these are termed “water borne” sections. A ship circumstanced as
described is in a condition similar to that of a beam supported
at the middle and loaded at each end. Such a beam tends to become
curved, the ends dropping relatively to the middle, and the ends of
the ship tend to drop similarly, the change of form being called
“hogging.” On the other hand, if the excess of buoyancy occurred
at the extremities and that of weight amidship, the ship would
resemble a beam supported at the ends and loaded at the middle. In
such a condition the middle would tend to drop relatively to the
ends: a change of form called “sagging.”
These general principles are much more readily and safely
applicable to ships while floating in ‘still water’ than to ships
when at sea—the strains experienced then being necessarily the
results of far more complex and severe influences. The existence of
waves and their rapid motions relatively to that of the vessel, and
the pitching, heaving, and other movements thus caused, increase
the inequality of distribution of weight and buoyancy and affect
more materially the strains brought upon vessels. Consideration of
the problem, therefore, involves a study of waves, both as to their
formation and action, and necessarily leads to a mode of treatment
which cannot have accurate regard for particular cases. Variable
influences of immense importance are also constituted by the state
of loading in vessels for merchant service. For a uniform basis of
comparison in these calculations such vessels are usually assumed
as loaded with homogeneous cargo—_i.e._, cargoes of equal density
throughout.
This fundamental element of relative ‘weight’ and ‘buoyancy’ having
been indicated, the chief strains to which a ship is subjected may
now be stated. This may be done with sufficient regard to general
accuracy, under four heads:—[7]
(1) Strains tending to produce longitudinal bending—“hogging” or
“sagging”—in the structure considered as a whole.
(2) Strains tending to alter the transverse form of a ship,
_i.e._, to change the form of athwartship sections.
(3) Strains incidental to propulsion by steam or sails.
(4) Strains affecting particular parts of a ship, or “local
strains”—tending to produce local damage or change of form
independently of changes in the structure considered as a whole.
To these might be added various other strains, which, however,
are of less practical importance, and are not felt in any
great degree—except in very special cases and under unusual
circumstances—apart from the strains which affect the structure
considered as a whole. The provisions made for the latter are,
under ordinary circumstances, sufficient to cover the demands of
the former, but particular cases may have to be provided for on
their merits, apart from the treatment generally applicable.
The manner of ascertaining the strength of a ship to resist
strains tending to produce longitudinal bending, is to compute
the effective sectional area of all the longitudinal items in the
structure which are brought under compressive or tensile strain,
and from this to calculate the strength in the same manner as for
a girder having an aggregate sectional area and a disposition of
material equivalent to that of the ship.
To ascertain the accurate maximum strains tending to produce
longitudinal bending, or, in excessive cases, to break the ship
across at the transverse section where the strains reach their
maximum, involves a careful and most laborious consideration of
the relative weight and buoyancy of individual sections throughout
the length, and is a task not generally undertaken in mercantile
shipyards.[8]
References to the nature of the transverse and other strains above
enumerated and the extent to which they have been investigated will
be made further on.
With regard to such fundamental properties of vessels as
displacement, weight, and carrying capability, nothing new has
for a long period been added to the fund of scientific knowledge.
One of the conditions now most commonly laid down by the owners
of a proposed ship is that which provides for a certain carrying
capability on a given draught of water and at a certain speed,
the principal dimensions of the vessel also being stipulated. The
problem of determining what total displacement will be required,
involves consideration and an estimate of—1st, The total weight of
hull having regard to structural strength; 2nd, the total weight of
machinery having regard to speed required. By using “co-efficients”
deduced from the weights of vessels of similar type already built,[9]
these are determined; and adding them to the carrying capability
or dead-weight stipulated, the required displacement can be closely
approximated to. For vessels of abnormal proportions or of very
unusual construction careful and detailed calculations of the weight
of materials are undertaken previous to tendering for them. In some
yards, indeed, a like degree of care is observed in ordinary cases:
methods of approximation involving the use of co-efficients such as
that based on cubic capacity being distrusted.
The further problem of determining what form of hull will give the
required displacement is the essential and all-embracing feature of
the work of design, as it involves consideration of almost all other
properties. The methods of designing ships are various, and a very
common method, at one time more followed than it now is, consists
in shaping a block model direct, and from it taking the necessary
measurements for displacement, and for full-size delineation in
the moulding loft. The disadvantages pertaining to this somewhat
antiquated method are becoming more recognised as shortened and exact
methods of linear or “draught plan” design are put forward.
Unless the plan of lines of a similar vessel of nearly the same
dimensions is at hand, the design of a new vessel is in many
instances done without previous calculation being made to ensure at
once obtaining the desired displacement. Special methods of quickly
arriving at this result are, however, not uncommon in mercantile
shipyards, and generally speaking the chief draughtsmen in the employ
of large firms doing a varied class of work have rules derived
from long experience, though not perhaps definitely systematised,
by which they are guided.[10] Irrespective of all such special
methods, however, the work of designing is now greatly shortened and
simplified by means of Amsler’s “planimeter,” an ingenious instrument
for measuring areas now becoming well known.[11] By employing the
instrument in question, the draughtsman need not too laboriously
strive after the exact displacement at first, as the time occupied
in ascertaining what displacement any set of lines gives, and in the
consequent fining or filling out, is very considerably less than by
the ordinary methods.
* * * * *
The question of stability, which has next to be considered, is one
of great difficulty and intricacy, and it was not till the middle of
last century that some of the principles upon which it depends began
to be understood. Bouguer showed in 1746 that the position of the
“metacentre” limits the height to which the centre of gravity of a
floating body may be raised without making it unstable, and that the
righting moments at small angles of inclination from a position of
stable equilibrium are proportional to the height of the metacentre
above the centre of gravity. As the position of the metacentre for
any given draught of water is easily determinable when once the
volume of displacement and the centre of buoyancy at that draught
have been ascertained, it has been the practice for a very long time
to construct a curve representing the height of the metacentre at
all draughts, and to use it for showing the limits above which the
centre of gravity cannot be raised with due regard to the stability
required for the practical working of vessels and for purposes of
safety: By the method of “inclining” vessels, already described (see
outline of fundamental principles, page 98), the determination of the
precise position of the centre of gravity is rendered comparatively
simple.[12]
While the vertical distance between the centre of gravity and the
metacentre—commonly termed the “metacentric height”—forms a measure
of the “initial stability,” or the stability at very small angles of
inclination, it is imperfect by itself, and may be very misleading
as regards the stability at larger angles. This was conclusively
demonstrated by Atwood in his papers read before the Royal Society
in 1796 and 1798, while other grounds for discrediting the standard
of stability furnished by mere metacentric height were discovered
subsequently, and have been signally emphasised, with additional
reasons, by recent occurrences. Atwood, in the papers referred to,
laid down a general theorem for determining the righting moments
at any required angles of inclination possessed by a ship having a
given draught of water and a fixed height of centre of gravity, the
principle of which involved the use of the moments of the volumes
of the “Wedges,” _i.e._, those parts of a vessel (see =W O W_{1}=,
=L_{1} O L=, fig. 15), which become immersed and emerged as she
is inclined. Several methods of simplifying Atwood’s calculations had
been devised previous to 1861,[13] but in that year Mr F. K. Barnes,
in a paper read before the Institution of Naval Architects, described
a method of accomplishing this which until within recent years has
been the one ordinarily adopted in computing the stability of a
vessel at various angles of inclination.[14]
Owing to questions having arisen at the Admiralty in 1867 respecting
the stability of some low freeboard monitors at very large angles
of inclination, Sir E. J. Reed, then Chief Constructor, directed
the matter to be investigated. The work was placed in the hands of
Mr William John, who embodied for the first time the results of the
calculations in the form of a curve of stability, which exhibited
the variations of righting moments with angles of inclination up to
the particular angle at which stability vanished. The entire range
of a vessel’s stability was thus made evident, and in such a form
as enabled the general problem to be far more comprehensively and
accurately treated than before. The results of Mr John’s labours were
described in a paper read by Sir E. J. Reed before the Institution of
Naval Architects in 1868, and a further paper, containing an improved
method of applying Atwood’s theorem to the calculation of stability
upon this extended scale, was read before the same Institution by
Messrs John and W. H. White in 1871. The loss of H.M.S. _Captain_,
in 1870, as already pointed out near the beginning of this chapter,
occasioned an immediate and serious regard for the stability of war
vessels. This disaster, with other losses at sea from instability,
also forcibly directed the attention of mercantile naval architects
to the subject, and investigations on the same complete scale as
those undertaken in the Admiralty have for some years been adopted in
a few leading mercantile shipyards.
In this way the peculiar dangers attaching to low freeboard,
especially when associated with a high centre of gravity, have been
pretty fully made known, but the character of the stability which
is often to be found associated with very light draught appears to
have escaped the attention it demands. Light draught is often as
unfavourable to stability as low freeboard, and in some cases more so.
These truths were forced into prominence at the inquiry held by Sir
E. J. Reed on behalf of the Government into the disaster which befell
the _Daphne_, a screw-steamer of 460 tons gross register, which
capsized in the middle of the Clyde immediately on being launched
from the yard of the builders, Messrs Alexander Stephen & Sons,
Linthouse, on July 3rd, 1883. Sir E. J. Reed, in his exhaustive
report, published in August, 1883, emphasised the lessons adduced at
the inquiry as to the peculiar dangers attaching to light-draught
stability; and Mr Francis Elgar, (now Professor of Naval Architecture
in Glasgow University), who was employed to make investigations
respecting the stability possessed by the _Daphne_ at the time of the
disaster, did much to guide consideration of the subject into this
channel. In a letter to the _Times_ on 1st September, 1883, Mr Elgar,
by way of explaining portions of his evidence at the inquiry, called
attention to the relation which exists between the righting moments
at deep and light draughts in certain elementary forms of floating
bodies, his communication throwing further light on the subject of
light-draught stability. It appears that the fundamental proposition
which underlies the variations in the stability of a floating
body with draught of water had never before been demonstrated or
enunciated.
It will be readily understood that a curve of stability for a
given draught of water and position of centre of gravity ceases to be
applicable if changes are made in the weight and consequent draught
of water of a ship or the position of the centre of gravity, or in
both. Now in mercantile steamers, from the extremely light condition
in which they are launched to the uncertain loaded condition of their
daily service as cargo-carriers, the variation of draught is very
considerable, and imports into the subject considerations which do
not obtain to any great extent in war ships.
To complete the representation of stability as it should be known
for merchant ships, it is now recognised that curves showing the
stability at every possible draught of water and for different
positions of centre of gravity should be constructed. By means of
“cross-curves” of stability, or curves representing the variation
of righting moment, with draught of water at fixed angles of
inclination, this comprehensive want can be met with something like
the necessary expedition. From such curves it is a simple operation,
involving no calculation save measurement, to construct curves of
the ordinary description, showing the righting moment at all angles
for any fixed draught of water and position of centre of gravity.
Professor Elgar was the first to publicly direct attention to this
valuable development of stability investigation of merchant ships,
doing so in an able paper “On the Variation of Stability with Draught
of Water in Ships,” read before the Royal Society on March 13th of
the present year. Simultaneously with Prof. Elgar’s employment of
such curves in actual practice their use had been independently
instituted by Mr William Denny in his firm’s drawing office, and the
mode in which they were worked out in this case was communicated in
a paper read by Mr Denny in April of the present year before the
Institution of Naval Architects.[15] Several important improvements
with respect to simplifying and shortening calculation distinguish
the method employed by Mr Denny, and that gentleman, in the paper
referred to, accords individual credit to members of the scientific
staff in his firm’s employ, who, on being entrusted with the work
of calculation, brought considerable originality to bear upon their
labours. The cross-curves described by Prof. Elgar were constructed
from a series of curves of stability calculated in the ordinary way.
This, however (as pointed out in an after-note to that gentleman’s
Royal Society paper), is less simple and very much less expeditious
than the method carried out under Mr Denny, which consists in
calculating the cross-curves directly by applying Amsler’s mechanical
integrator[16] to the under-water portion of the ship instead of to
the wedges of immersion and emersion, thus determining at once the
positions of the vertical lines through the centres of buoyancy at
the required angles of inclination. As thus carried out a complete
set of cross-curves can be produced with about one-third the labour
involved in employing the older method. The ease and rapidity with
which ordinary curves for separate draughts can be taken from
cross-curves has already been commented upon.
Many other investigators besides those already mentioned have
recently been working at the subject of stability, and a
considerable number have read papers, dealing with the extension and
simplification of stability calculations, before one or other of the
scientific societies concerned with naval architecture, most of the
methods put forward being well worthy of study.[17] To very many
shipbuilders, however, and to others besides them responsible for
the stability of ships, processes of arithmetical calculation—even
allowing for all the simplification which mathematical skill has
recently effected—appear still to be too intricate, or to absorb too
much time for their being entirely followed. As a simple means of
readily, although approximately, arriving at the results attained
more elaborately and reliably by calculation, attention has recently
been directed to an experimental process by which a complete curve
of stability may be constructed almost without the use of a single
figure! The method was first brought forward in 1873 by Capt. H. A.
Blom, chief constructor of the Norwegian Navy, formerly a student of
the South Kensington School of Naval Architecture, who described it
to the United Service Institution. The method has been employed by
shipbuilding firms on the Tyne and Clyde when a curve of stability
had to be produced in a very limited time, and when extreme accuracy
was not a desideratum. As practised by the firms in question, the
_modus operandi_ differs in some slight respects from that described
by Captain Blom, but the changes in no way affect the principles as
first laid down by him. The modern mode of procedure may be briefly
described:—
From the body plan of the ship, _i.e._, that portion of the draught
plan representing the vessel’s form by a series of equidistant
transverse sections—any convenient number of sections lip to the
load water-line are pricked upon and then cut out of a sheet of
drawing paper of uniform thickness. These sections are then gummed
together in their correct relative positions, care being taken
to spread the gum thinly and evenly. This paper model—greatly
foreshortened, of course—represents the immersed portion of the
ship (in other words, the displacement) when she is floating
upright. By suspending this model from two different points, and
taking the intersection of two vertical lines through the points of
suspension—or better still, by balancing it horizontally on a pin
and fixing the point when the model is in equilibrium—the centre
of gravity of the model, or in other words, the actual centre of
buoyancy is obtained.
Water lines at various angles of inclination are then drawn on
the body plan, all intersecting the water line for the upright
condition at the centre line of ship. The displacement represented
by the inclined water lines thus drawn, generally not being equal
to that for the upright position, a correcting layer has to be
added or subtracted for each inclination, in order to obtain this
end. By employing the planimeter the necessary thickness of this
layer can be most readily ascertained. Where a planimeter is not
available the actual floating line may be obtained, after the model
has been made, by cutting off layers, allowance having been made
for this purpose. The same number of sections as before are then
cut out to each of the inclined corrected water-lines, the paper
model prepared and the centre of buoyancy obtained as already
described.
Through this new centre of buoyancy a line is drawn perpendicular
to the inclined water line, and the distance between this line
and the centre of gravity of the ship, already obtained, is the
righting arm. If this process is repeated for each angle of
inclination, it is thus seen a complete curve of stability may be
approximately obtained.
[Illustration: FIG. 16. MODEL IN UPRIGHT POSITION ]
[Illustration: FIG. 17. MODEL IN INCLINED POSITION]
A further method of arriving at results by experiment, involving
principles not unlike those of the “paper section” method just
described, has recently come under the author’s notice, and through
the courtesy of its inventor—Mr John H. Heck, of Lloyd’s surveying
staff at Newcastle—the following general description of the apparatus
and fundamental principles is made public for the first time:—
By means of a “stability balance,” roughly illustrated by Figs 16
and 17, in conjunction with either an outside or inside model of
the vessel, the moments of stability can be practically determined.
In practice, an inside model has been found the most convenient to
employ. This consists of a number of rectangular pieces of yellow
pine of any uniform thickness, out of which a portion has been cut,
respectively to the form of the vessel at equidistant intervals of
say 15 feet. These pieces, together with two end pieces, are kept
together by four or six bolts, thus forming a contracted model, the
inside of which is of a similar form to that of the vessel. If
this model is filled with water to a height corresponding to any
draught, it will represent a volume of water having the same form,
and proportional to the displacement of the vessel at that draught.
The stability balance consists of a frame =A= attached to a steel
bar =Z=, having knife edges working upon the support =C=; a table
=D= attached to a spindle working freely in the bearings =E=, and
capable of being turned through any angle; a sliding weight =F= to
balance the weight of the model when empty; a sliding weight =H=
to balance and measure the weight of the water contained in inside
or displaced by outside models; a sliding balance weight =K= which
by adjustment will locate the centre of gravity of the combined
weights of the table =D=, the model and the weight =K= in the axis
of the table =D=, so that the model will remain when empty in any
inclined position, and be balanced by the weight =F=.
In order to determine the moments of stability, the model is first
fixed on the table =D=, and the weights =F= and =K= so adjusted
that =F= will balance the model at all inclinations. The table is
then brought into the upright position, and water is poured into
the model to the height corresponding to the desired draught of
water, and the weight =H= shifted until the whole is balanced.
The weight of water in the model will evidently be = weight =H= ×
its distance from the fulcrum ÷ distance centre of model is from
fulcrum.
If the table with the model is now turned through any angle, the
distance the centre of gravity of the water has moved from the axis
=E= of the table can easily be determined by shifting the weight
=H= until the whole is balanced, then evidently from the principles
of the lever, =H= × by its distance from fulcrum = weight of water
in model × by the distance the centre of gravity of the water in
the model is from fulcrum. Since the weight of =H= × its distance
from fulcrum ÷ the weight of water in model is known, the distance
that the centre of gravity of the water has shifted from centre
line is easily ascertained and the righting lever determined.
From a lengthened series of experiments, conducted by Mr
Heck—latterly in Messrs Denny’s Works where an apparatus from a
special design by Mr Heck has been constructed for the firm’s use—the
method gives promise of taking a firm place as an extremely simple
and approximately accurate means of arriving at the stability of
vessels.[18]
While a vessel’s qualities with respect to stability may be
determined with great precision by the naval architect, his
investigations are only directly applicable to the ship while empty
or when in certain assumed conditions of loading which may or may
not often occur in actual service. He cannot for obvious reasons
estimate, far less control, the amounts and positions of centre
of gravity of the various items of weight that may make up the
loading.[19] This aspect of the subject has received attention at the
hands of naval architects for a considerable time, but the forcible
way in which it has been brought under view by recent experience
has resulted in special efforts being made to practically meet the
necessities of the case. In 1877 Mr William John read a paper before
the Institution of Naval Architects, in which he dealt with the
effect of stowage on the stability of vessels, and since that time
such authorities as Martell, White, and Denny have given valuable
papers or made suggestive comments bearing on this important matter.
Much has also been done by several builders in the way of devising
diagrams useful for regulating stowage and manipulating ballast with
regard to initial stability. At the last meeting of the Institution,
Professor Elgar read a paper on “The Use of Stability Calculations
in Regulating the Loading of Steamers,” distinguished by its
eminently practical character, and forming an important contribution
to the solution of this problem. The author disapproved of curves
of stability being supplied with vessels, as had been advised and
was then becoming the practice. General notes, giving in a simple
form easily applied in daily practice, particulars respecting the
character of a ship’s stability in different conditions, are what
the author recommended and had found through actual experience to
meet the case most effectually. In the discussion which followed
it was intimated by Mr William Denny that his firm had already
resolved to furnish every new steamer produced by them with a volume
containing general and special notes and diagrams dealing not only
with stability but with several other important technical properties
(see footnote, page 59). After consultation with Professor Elgar,
however, he had abandoned his intention of supplying stability curves.
An arrangement designed to readily find the position of the centre
of gravity experimentally by inclining, and to indicate at once the
stability of loaded vessels as represented by metacentric height, has
been devised and introduced on board several ships by Mr Alexander
Taylor, of Newcastle—already referred to in connection with the
triple expansion principle in marine engines. The instrument and
apparatus, which he appropriately names the “Stability Indicator,”
was described in a paper read by him before the Institution of Naval
Architects at its last meeting. When once an inclining operation
has been made, the degree of inclination is read from a glass gauge
and the position of centre of gravity and corresponding metacentric
height from a previously prepared scale set up alongside the gauge,
or from tabulated figures.
* * * * *
The advance made within recent years in connection with steam
propulsion comprises many matters necessarily left unconsidered in
the chapter on speed and power of modern steamships. Scientific
methods have undoubtedly contributed in no small degree to the
realization of the remarkable results therein outlined. The
achievement of one triumph after another as demonstrated in the
actual performances of new vessels, and especially the confidence
with which pledges of certain results are given and received long
before actual trials are entered upon—and that sometimes with regard
to ships embodying very novel features—are evidences of the truth of
this.
The oldest method of approximating to the horse-power required
to propel a proposed vessel at a given speed is to compare the
new ship with ships already built by the use of formulæ known
as “co-efficients of performance” deduced from the results of
their speed trials. Two such co-efficients have been deduced from
Admiralty practice, the one involving displacement, the other area of
mid-section, with speed as the variable in both cases. Another method
which has been largely used, consists in first determining the ratio
of the indicated horse-power to the amount of “wetted surface,” or
immersed portion of the vessel’s skin, in the exemplar ship, and then
estimating from this ratio the probable value of the corresponding
ratio for the proposed ship at her assigned speed. Inasmuch as these
methods of procedure do not take account of the _forms_ of the hulls,
and consequently of that factor in the total resistance due to
_wave-making_, they cannot be used with any degree of confidence, or
without large corrections, except in connection with vessels whose
speeds are moderate in proportion to their dimensions: those in fact
in which the resistance varies nearly as the square of the speed. A
further method, somewhat resembling the one based upon the relation
between indicated horse-power and the “wetted surface,” was proposed
by the late Prof. Rankine, but has never been extensively employed.
Apart from the unreliable nature of the results which an application
of it gives—except for certain speeds—it is open to several serious
objections in practice.
A method of analysis and prediction, meeting with considerable
acceptance from shipbuilders on the Clyde and elsewhere, has been
introduced within recent years by Mr A. C. Kirk, of Messrs R. Napier
& Sons.[20] The method consists in reducing all vessels to a definite
and simple form, such as readily admits of comparison being made
between their immersed surface, length of entrance and angle of
entrance and their indicated horse-power, and from this judging of
the form and proportions best suited to a given speed or power in
proposed vessels. The form in question consists of a block model,
having a rectangular midship section, parallel middle body, and
wedge-shaped ends; its length being proportioned to that of the ship,
its depth to the mean draught of water, its girth of mid-section
to the girth of immersed mid-section of the ship, and the surface
of its sides, bottom and ends, to the immersed surface of the ship.
By finding from one or more exemplar ships—the selection of which
is obviously governed by the conditions of analysis—the rate of
indicated horse-power required per unit of wetted surface at the
speed assigned for the proposed vessel, the appropriate rate for the
latter may easily be determined.
The data afforded by the modern system of progressive speed trials,
especially when taken in conjunction with that of experiment with
models as systematised by Mr Froude, supplies in a reliable way
much of what is most lacking in the older methods of comparison and
prediction. Progressive speed trials on the measured mile were first
systematically instituted by Mr William Denny about nine years ago,
since which it has been the practice of his firm to make such trials
with all their vessels. The practice has been followed by other firms
on the Clyde and elsewhere, and there is every probability it will
be still more widely adopted in the future. The system consists in
trying the vessel at various speeds, ranging from the highest to
about the lowest of which she is capable. The several speeds are the
mean of two runs—one run with the tide and one against, the object
being to eliminate the tide’s influence from the results.[21]
Essentially noteworthy in connection with the system is the manner
in which the data obtained from the trials is recorded for future
use. This consists of a series of curves, representing the chief
properties of ship, engines, and propeller—_e.g._, “speed and power,”
“revolutions” and “slip”—which show to the eye, more easily and
clearly than bare figures, the whole course and value of a steamer’s
performances. For that of speed and power the various speeds made at
the trials are set off to convenient scale as horizontal distances,
and the indicated horse-power corresponding to those speeds are set
off to scale as vertical distances. The intersection of the offsets
so made, give spots for the curve. The other curves alluded to are
similarly constructed, the requisite data being the direct or deduced
results of the measured mile trials.
From the accumulation of trial results thus graphically recorded
the designer of new ships can proceed to estimate with greater
assurance of attaining satisfactory results than by employing the
older methods. If, for example, a ship is to be built of virtually
similar dimensions and form to one for which such information is
available, but of less speed, the task is simply one of measurement
from the curves, with some allowance for probable differences in
the constant friction of the engines. If the speed is to be greater
than that of the exemplar ship, but still within the limits when
wave-making resistance assumes relative importance, the case is also
one of simple reading from the curves, with slight corrections.
When both the speed and size are different, but the form is
approximately the same, the case is more difficult, but it can be
dealt with approximately by employing the “law of comparison” or of
“corresponding speeds” enunciated by Mr Froude. Formulæ based upon
this law—which will be more fully referred to presently—have been
devised by one or two designers, and applied by them to problems of
the latter class as they occurred in the course of their professional
work. Mr John Inglis, junr., described a method of analysis he had
adopted, involving the use of Mr Froude’s law, in a paper read before
the Institution of Naval Architects in 1877.
When unusual speeds are aimed at, or when novel types of vessels have
to be dealt with, the only available method of making a trustworthy
estimate of the power required lies in the use of direct or
deduced results from model experiments. Mr Froude began the work
of speed experiments with ships’ models on behalf of the Admiralty
at the Experimental Tank in Torquay about 1872, carrying it on
uninterruptedly until his death in May, 1879. Since that lamented
event the work has been continued with most gratifying results by his
son, Mr R. E. Froude. Experiments had, of course, been made by many
other investigators previous to Mr Froude, but none before or since
have made model experiments so practically useful and reliable. Since
the value of the work carried on at Torquay has become appreciated,
several experimental establishments of a similar character have been
instituted. The Dutch Government, in 1874, formed one at Amsterdam,
which, up till his death in 1883, was under the superintendence of
Dr Tideman, whose labours in this direction were second only to
those of the late Mr Froude. It is now superintended by Mr A. J. H.
Beeloo, Chief Constructor, and under him by Mr H. Cop. It was here,
it may be remembered, that experiments were made with a model of the
Czar of Russia’s yacht _Livadia_, previous to the construction of
that extraordinary vessel being begun by Messrs Elder & Co. On the
strength of the data so obtained, together with the results of the
trials made on Loch Lomond with a miniature of the actual vessel,
those responsible for her stipulated speed were satisfied that it
could be attained. The actual results as to the speed of the novel
vessel amply justified the reliance put upon such experiments. In
1877 the French naval authorities established an experimental tank
in the dockyard at Brest, and the Italian Government have formed
one in the naval dockyard at Castellamare. The only experimental
tank hitherto established by a private mercantile firm is that in
the shipyard of Messrs Denny, Dumbarton. This establishment is on a
scale of completeness not surpassed elsewhere, and is fitted with
every appliance which the latest experience in such experiments shows
to be advantageous. A special staff of experimentalists, forming
a branch of the general scientific body, are engaged conducting
experiments and accumulating data, which, besides being of service in
their present daily practice, must ultimately yield fruit of a very
special kind to this enterprising firm.[22]
From mathematical reasoning, and by means of an extended series of
experiments with models and actual ships, Mr Froude determined that
for two vessels of similar form—for instance a ship and her model—the
“corresponding speeds” of ship and model are to one another as the
square roots of the similar dimensions, and at corresponding speeds
the resistance of ship and of model are to one another as the cubes
of the similar dimensions—subject to a correction concerned with skin
friction necessitated by the difference in the lengths of ship and
model.[23] Having obtained the resistance of a model, and from it,
by an application of the above law, deduced the resistance of the
full-sized vessel, the effective horse-power is found by multiplying
the resistance by the speed of the vessel in feet per minute, and
dividing by 33,000. From the effective horse-power an estimate of the
indicated horse-power required can be made by using ratios which the
one bore to the other in former ships, as obtained from a comparison
of their model experiments with their measured mile trial results.
The value of progressive speed trials and of experiments with models
as affording convenient means whereby analysis may be made of the
several sources of expenditure of power in propelling vessels can
scarcely be over-estimated.
From a study of the graphic records of progressive trials, and from
model experiment results, Mr Froude discovered a method whereby the
power expended in overcoming the frictional resistance of the engines
could be determined, and estimates made of the amount of power
absorbed by other elements. The method in question was communicated
in full in a paper read before the Institution of Naval Architects
in 1876, and has since been extensively used. Methods of analysis
resulting from a simultaneous study of this subject, were also
proposed by Mr Robert Mansel, a prominent Clyde shipbuilder and noted
investigator, but they failed in meeting with the acceptance which
was at once accorded to Mr Froude’s propositions.[24]
Although the results obtained by an application of Mr Froude’s
analysis to the trials of a large number of merchant vessels have
undoubtedly thrown considerable light on the relative efficiency of
hull and engines, and of various types of engines, still, for several
reasons adduced by extended experience—most of which, indeed, were
foreseen and perfectly appreciated by Mr Froude himself—the need has
been felt for some means of directly measuring the power actually
delivered to the propellers by the engines when working at different
speeds. One of Mr Froude’s latest inventions, the perfecting of
which was not accomplished until after his death, consisted of a
dynamometric apparatus designed to accomplish this important end.[25]
The construction of the instrument was undertaken for the Admiralty,
and trials were made with it on H.M.S. _Conquest_ in the early part
of 1880. The results of these experiments have not yet in any form
been recorded, but there can be no question as to the benefit that
would accrue to the profession if the Admiralty could be induced to
publish these, as well as the results of other experiments with this
instrument.