Rc t--E
THIRD SV!POSIUM ON NAVAL RYDRODYNAMIC8 1960.
Ir. 3. GEE2ITSMA
1. Introduction,
The Third Symposium on Naval Hydrodynamics was organized
by the Office
of Naval Research (U.s.A.) in cooperation
with the Netherlands Ship Model Basin, and held at the
Zurbaus in Schéveningen froa the 19th to the 22nd of
September 1960.
The Symposium was dedicated to 31r Thomas Bavelock, the
well-known English scientist in recognition of his
valua-ble contributions to naval hydrodynamics.
The greater part of the Symposium was devoted to "high
performance craft": vessels which in one way or another
have outstanding qualities when compared with conventional
ships.
Hydrofoil craft, ground effect machines (usually
abbrevia-ted: GEM's) submarines, semi-submerged ehipa and
deep-divine oceanographic submarines were reviewed. Theoretical
investigations, economical aspects, actu&l and possible
applications of these craft were diecuesed as well as
ex-perimental research on models, prototypes and special
de-tails.
Also some aub1ecta connected with stiipmotione in waves,
resistance and power in smooth water were discussed.
The Symposium was opened with addresses of welcome by
Frot.Ir. L. Troost (Central Organisation of Industrial
Research TPN,O. Netherlands) and by Dr. Killian (Office
of Naval Research U.$.A.)
Dr. von flrmèri then dedicated the Symposium to Sir Thomas
Havelock and drew the attention to the valuable work in
the field of naval hydrodynamics carried out by this
scientist.
He expressed the general feeling of regret that $ir Thomas
was prevented to attend the Symposium.
The lis-t-o.t' participants mentioned 347 persons,
represen-tixig 21 nationalities.
die-
2-cussed.
The proram was as follows
Session 1: Chairman: Prof.DrIr W..A. van Iamrneren. (Netherlands Ship Model Basin)
1. O.H. Oakley (Bureau of Ships, United States Navy) "High performance ships - promises and problems". 3.0. van Mann (Netherlands Ship Model Basin) "Size, type and speed of ships in the future" Session
2: Chairman: Prof.J.K.
Lunde.(Skipamodelitanken, Troridbeiiu)
3. J.A. Sparenberg (Netherlanda Ship Mod.el Basin)
"On the efficiency of a verticalaxia propeller11.
k. B. Timman and G. Vossers (Netherlands $bip Model Basin)
"A solution of the minimum wave resistance ,problem"
3. Zarp, 3. Kotik and J. Lurye.
(Technical Research Group Inc.,Syoaset, New York) 'On the problem of minimum wave resistance for strut and atrut-ifle dipole distributions'
Session 3: Chairman: P. Eisenber.
(Hydronautics Inc., Rookvtlle, raryland) M.P. Tulin (Hydronautos Inc., Rookville, Maryland')
"The bydrodynamios of hib speed bydrofoil craftt' 5, Schuster and H. Schwanecke
(Versuhaanstalt' fur
Waaserbau und. Schiffbau, Berlin)
"On bydrofoils running near a free surface"
A. Hadidakis (Aquavion Holland N.Y., The Hague)
"The effect of size on the seaworthiness of hydrofoil
craft".
G.J. Wenxxagel (Dynamic Development Inc., Babylon, New York)
"Design and inittal tests of our supercavitating
easion 4: Chairman J.A. Obermeyer..
(David. Taylor Model Basin, Washington)
H. von Schertel (Supramar A.G. Luzern)
Design and operatir
problems of commercial
hydro-foil boate'.
LB. Chaplin Jr. (David Taylor' Model Baein,Washingtoxi
"Ground effect machine research and development in
the United States"
12,
P. Mandel (Massachusetts
Institute of Technology)
"Hydrodynantic aspects of a deep.-diving oceanographic
submarine"
Session
5:
Chairman: Dr.
. Brard.
(Basein d'Essais
des Carènes, Lrance)13.
F.Ji. Todd (National Physical Laboratory,Teddiiiton)
"Submarine cargo ships and tankers"14,
A. Goodman (David
Taylor Model Basin, Washingto]1)"experimental techniques and methods of
analysis
used in submerged body refearch"F.W. Bogge
and N. Tokita.(United States
ThibberCompany, Wayne, New Yersey)
"A theory of the stability of laminar flow along
compliant plates"
P.H, Wilirn (Service Technique do Construction et
Armee Navalee, Paris)
"The French bathysoaphe program"
Session 6: Chairman: Prof.d.r. GP. Weinbium.
(InBtitut fur Schiffbau der Universitt,Eamburg,
. Grim,
(Hamburgiache Scbiffbau Verausobeanstalt)
"A method for a more precise computation of beevizigand. pitching motions, both in amooth water and in
E.V. Lewis and J.P. Breslind
(Stevens Institute of Technoio, Hoboken).
"Semi submerged ships for high speed
operation in
rough seas".
A.. 8ilver].eaf and W.J, Marwood.
(National Physical Laboratory, eddington)
"Design data :tor high speed displacement type hulls
and a comparison
with hydrofoil craft".In the following pages, an attempt will be made to sun a-'
rize briefly the contents of the papers which were presen-'
ted.
2. Summary of the papers.
It will be clear that military demands conoernin speed,
manoeuvrability, limits of sbipmotions and accelerations etc., are a driving force for the development of high performance ships.
Oakley gave in his paper some particulars about the research work in this field which is carried out by the United States Navy.
An interesting part of this research concerns the develop mont of a high speed destroyer, It is known that in cer-tain circumstances the speed of a modern nuclear powered submarine can exceed that of the destroyer. In a heavy seaway the conventional destroyer cannot maintain full speed because
slamming and the
shipping of green water become too dangerous. The submarine however is not much affected by the seaway and a higher sustained speed can result. Therefore, new wye have to be ecplored to give the bunter a better chance to capture his prey.One of the proposed solutions is a vessel Of which the mainhull travels under water, whereas a relatively small superstructure penetrates the surface,
-5-This combination is much less affected. by surface waves
and probably such a vessel is able to maintain higher
speeds in a seaway than the conventional type. Several
modifications of this idea are
considered., an eztreine casebetng the "spar ship": a vessel with its largest dimension
in the vertical direction and only a small part piercing
the surface.
Another posSibility je the use of hydrofoil boats where
hydrostatic buoyancy is replaced by the lift force of
relatively small wings' attached to the bull, The bull
itself does not touch the water surface when the veasel
is at speed and. in this way the wave resistance, which
forms an important
part of the total resistance of Last
diap,lacemant
type vessels
is practically eliminated.Therefore hydrofoil craft are particulaily well aui.ted
for high speeds. Many problems however arise when these
vessels are operating in waves.
These problems are diacuased in detail in some *f the
other papers.
Van Manen drew the attention to the fact that generally
owners and builders of merchant ships are too well aware
of the expenses and. Linanc&al risks associated with the
development and. applications of vessels which differ
radically from
conventional types. Therefore £t is notsurprtaing that research work on progressive ship types
is mai.nly stimulated and supported by military
organisa-.tions. Obviously the need for a htgb performance balances
the financial. consequences.
It is made clear that untill now, naval architecture
always had, a more or less ernpirióal character. In the
future however more ecientifc and. tuud.amental metboda
have to be employed in the research and design methods
for new sbp types.
Ãìóó the
!àrói
iior
eOntcntl
1tip
aid.the
increase of power per ahaft are sometimes a source of
-6-The high power per shaft and the £uU, form of supertankers
for instance can result in severe cavitation.- and vibra
tion phenomena, Van Manen proposed. in this respect the
use of the cigarshaped. Hognex' afterbody in connection
with a complete ring nozzle propeller system. A somewhat
better propulsive efficiency, a 25% smaller propeller
diameter and. notably better vibration and cavitation
charaoteristioa may be obtained.
In general it is expected that the speed of normal
nor-chantshipB will not inorease beyond 20 to 2 knots.
Perhaps in the future the nuclear powered submarine WiU
offer a djstinet advantage for speeds exceeding 25 knots.
The dimensions of this type of vessels are restricted.
because of the limited harbour depths and. the available
dry-docking facilities, At this moment the maximum draught
seems to be limited to approximately 35 feet.
A study carried. out by the Electric Boat Division of the
General Dynamics Corporation showed. that the largest
nuclear propelled submarine merohantehip wich could be
built with the present state of powerplant technology
would have the following dimensions:
cargo deadweight
41565
tone
speed
37
knots
circular cross-section
maximum diameter
80
feet
surface displacement
91903
tons
submerged displacement
101000
tons
loaded draught
6?
feet.
length
936
feet
power
240000
sbp
number of screws
4
The "most conservatIve" of the 27 designs carried out,
-7-cargo deadweight
21189 'tons
speed
20 knota
surface displacement
38791 tone
submerged displacement
42671 tone
loaded draught
35 feet
length
583feet
beam
80 feet
dptb
40 feet
rectangular cross section
power
50O0 sh,p
number of screws
I
Neither military nor economic considerations were
consider-ed in thi
otudy.
With the aid of some reasonable and realistic estimations
concerning power and weight coefficients, Van Manen oon
eludes that the displacement of hydrofoil boats and G]M's
will be restricted to about 100 tons and the speed will
probably not exceed 100 knots,
A mathematical st*dy on the efficiency of a vertical-axis
propeUer (Voith-Schneid.er type) was given by parenberg.
The blades of such a propeller are forced to oscillate by
a system of rods and hinges. The angle of incidence of
each blade is prescribed by this system and varies in
such a way that the propeller as a whole can deliver a
tb.rus1 in any 'direction perpendicular to the vertical axis
In this study a number of simplifying assumptions are made:
the blades axe infinitely thin, top effects are ignored
and the chord of the blades is assumed to be small with
respect to the aallest xadius of curvature of the orbits
of' the blades (these orbits are oycloide)'.
The optimum angle of incidence as a function of the poi.
tion of the blade along the circumference of the propeller
is found with the conitton that the kinetic energy left
-behind---jn-the -wake--of th
ropefler-is
tn1y1 mum., Phi-
'kinetic energy i-e-- expzessei -in terms
f the-bound vortiea
-8-Also the case of avertical-axis propeller witbma
blades
or a high rotational velocity is considered. Here the bound
vortioity and. the vortex layers in the wake are approximated
by continuous vortex densities.
In this case the angle of incidence with respect to the
tangent at the cycloid can be expreased explicitly as a
function of the position of the blade alou
the
circumferen-Ce.
In the future numerical calculations based upon this theory
will be compared with experimental results.
The determination of ship builforms with minimum wave
resis-tance has been the eubjeot of the paper given by T1.rnman and
Voseers.
As is known the wave resistance of relatively slow ships
amounts to 20 to kO percent of the total resistance tn
smooth water. The problem of the determination of optimal
hull forms in view of minimum wave resistance can be
con-sidered as solved for this type o
ship as a result of the
experimental research carried out by the towing tanks
througho4t the years.
For fast ships much remains to be done; here theoretical
work can give valuable indications for experimental research
even if the theory is based upon a number of simplifying
assumptions
such as the linearization of the problem.
8eaides the condition that the wave resistance should be a
minimum, an additional condition is necessary, because
otherwise a hull with zero beam would result. A natural
additional condition is the requirement that the
displace-ment should have a given value4
Timman and. Vossers use this condition and give a method to
minimize the wave resistance resulting from Michell's inte-.
gral. By considering a certain class of hull forms for
which the additional condition can be expressed as a quadra-.
tic functional the problem is reduced to i
tion of the second kind. In order to obtain a simple
inte-gral equation the influenoG of the bottom in the evaluation
Numerical results were not yet available, but will be
given in the near future.
Kari, Kotk and. Lure treated a
similar problem; the
minimizing of the wave resistance of a strut of
fixed
length and volume per unit depth at a given
Proude number.
(by length is meant; the dimension of the strut in the
direction of travel).
They formulated the problem by using the dipole die tn-bution rather than the form as the unknown function. The
optimizing dipole d,istnibv.tiona have been found. Although the dipole densities turn out to be infinite at the ends,
the corresponding shapes can be found for large depths. These optimum shapes have rounded enda with
a relatively
large radius and make one think of the lower waterlines of a ship having a bulbuous bow.The authora
remark that three-dimensional etecte andother corrections on the linearized theory are
not COnr
sdered in their paper.
me following five lectures were devoted to
hydrofoil ortt
and investigations on the behaviour of hydrofotle.
Tulin summarized the hydrodynamical probleriaasootated with the de8ign of hydrofoil
bots.In general there are
also problems in the design of power plants transmissions,structures etc. but these are not considered
in the paper.
Wing loadings are very large. A hydrofoil boathAvingTa
speed of 60 knots experiences a static wing loadingwhich
is 20 to 50 times as large as that of supersonic aircrafttravelling at 600 knots. At the same time the demands
con-certiing resistance and cavitation characteristics result
in toils as thin as those of the supersonic aircraft. For high speede a aupercavitating propeller can be used.
with advantage (efficiency 65-72%), because serious
-10-Por speeds beyond 70 knots the supporting foiTh will expe-rienee serious cavitation accompanied. by drag rise and buffeting.
The only way to overcome these difficulties seems to be
the use of supercavitating foils. The first hydrofoilcraft designed with this prineiple in mind io being tested this year. The cavities behind the foils are not filled with water vapor but are ventilated by air paths to the atmosphere.
In addition to the static wing loading the hydrofoil c'aft experiences severe variable loads caused by the sea waves. A comparison of the vertical velocity components in the North Atlantic (5 ft.beneath the swfaoe) and. the vertical velocities in the atmosphere at low altitutes (0-10000 ft)
and moderate altitudes (30 to 50.000 ft)Is made,
It
iB
shown that a root meansquare
value of one foot persecond Is cxceeded only 17%
of the time at moderate alt±tudes in the atmosphere 53% at low altitudes and. 89% of the
time at the depth QZ 5 feet in the North Atlantic.In general it is
desired that hy&rcf oil craft maintain their distance from the sea surface and. follow the wavecontours when the wave length equals or exceeds the length of the boat. With increasing frequency of encounter (high speeda) however the experienced accelerations will become to severe. In that case a foil with variable angle of incidence has to be used, which is controlled in ouch a way, that the seacraft ploughes through the waves. The fully submerged wing seems to be the most suitable in contrast with the surfaee-piercing foil.
The use of controllable flaps in order to adjust the lift is discussed and some results 0± calculations on the be-haviour of two-dimensional flaps for both subcavitatIng and supercavitating foils, operating at high speeds are
given.
In- pra ha e1iessiiou1d.. b&inodi1ied. t& take into
- 11
magnitude of the influence of the surface proxiiity
however is clearly demonstrated..
For speeds exceeding kO knots the danger' of cavitation bn toils, vertical strLlte and propulsion macsilas in-..
creases rapidly.
because of its erosive effects1
local cavitation BbQUld.
be suppressed and also more extensivecavitation (short
of superoavitation) should be avoided,f or this type of flow is often not stable and may be accompanied by buff e
ting.
The designer must thus strive to suppresecavitation, a
process which leads to very thin underwater structures.
For speeds exceeding 70 knots eupercavitating toils mu3t
be used as mentioned earlier.
Finally lift-drag ratios of eupercavitating hdroZoils
and the influence of the free surface on these ratios
are discussed.
Schuster and Scbwanecke presented the results of theore.
tical and experimental research on two types of
hydro-foils: a fully submerged
wingand a dihedral toil.
For the steady state flow the pressure distribution
along the chord of the foils was measured as a function
of speed, depth of submergence, anglO of incidence and
roll angle.
For two dihedral foils the total forces and moments are
also given. For speeds below
7/R
(b means waterdepth)
the pressure distribution is influenced. by shallow water
effects as was already known from the work of Laitone
Plesset
nd Parkin.
Above this critical velocity no dependency on speed
exists, Here the pressure distribution ii influenced -only
by the distance of the bydrotoil
tothe surface in
rela-tion to the chord length. For this situarela-tion which is
- o
dorOrlWfttthd'er serviceondiUons ,
12
-mic forces are given.
'inally the relations for the vertical and lateral stability
of the two types of kzydrofoila are derived as well as the
influence of side slip motion,
Had3jidaki discussed the effect of size on the seaworthiness
of hydrofoil craft.
The behaviour of the hydrofoil craft in waves was compared
with a simple linear maas.aprixig system, excited with forces
and moments in the frequency of encounter of the waves. Assuming that wave length and wave heigth are propQrtional
to the length of the boat the author draws the following conclusions:
In a following sea the maximum pitching angle is the criti. cal factor. The danger exists that the combined effect of
a large negative pitch angle and the moment
caused by the
orbital motion of the waterpa.rticles can make the bow touch
the water with the
result that the craft is slowed down. It is shown that the seaworthiness of the hydrofoil craft in a following sea is nearly unaffected by size. Actuallythe seaworthiness improvee slightly with decreasing E'roude number.
In a head.sea the vertical accelerations are critical.
They decrease more than proportionally with the Froude
number.
From these considerations the author concludes that the 8eaworthineee and comfort of hydrofoil boats increase with
increasing dimensions,
Wennagel mentioned the research. and development programs
concerning the improvement of hydrofoil craft in which
dynamic Developments Inc.
nd Grumman Aircraft Enginee.
xtng Corp. are engaged.. Three of the testprograms were consIdered of special
interest to the symposium. !ew
çPl7ed. to teat bydofot1s. The first was
13
-the mnnerside is open. The centrifugal force caused by
the high speed of rotation forces the water against the
outer boundaries and. the free surface becomes nearly
vertical. In this way a model hydrofoil attached to a
strut and placed in the flow1 can be tested at speeds
up to 100 knots. Froes and moments
experienced by the
model can be measured electronically.
The second program utilizes a pendulum apparatus, in
which model foils attached to the end of a pendulum
swing through
watertank of variable water temperature
and. variable vapor pressure. Instantaneous measurements
of speed, forces and moments can be done.
The third teatprogram utilizes a research and test craft
the XCR6 with a gasturbine powerpiant aud. a
supercavi-tating propeller.
The propeller has a diameter of 10 inches and develops
a thrust of 77. lbs at a speed of 62 knots and
6000 r.p.m.
With this number of revolutions of the propeller, the
engine runs at 19500 r.p.m. and has a continuous normal
output of 765 bp, which is greatly in excess of the
required power.
Forward of the center of graitity the boat is sup:ported
by two surface piercing dihedral foil systems (one at
each side) and aft of the transom by a fully submerged
foil.
Each of the forward foilsystemo eonsists of a vertical
strut attached to the hull, a cruise foil pointing
out-ward and up attached. to the bottom of the s'brut and a
diagonal foil element connecting the upper end of the
cruise foil with the upper region of the strut. The
cruise foil is designed with a supercavitating cross
section. The diagvnal foil, which is only used during
low speeds, has a ubcavitating cross section with a
blimttraiiing edge.
The tail foil einploys a subeavitatiñg eross étin
The cavity regions of foils and struts are ventilated..
'or intermediate speeds forced ventilation is provided.
When operating at a speed of 62 knots the lift-drag ratio
of the forward bydrofoils is estimated to be approximate
Ly 10.
Initial tests have a].ready been performed.
An extensive paper about the different aspects of the
design and. operation of hydrofoil boats was read by
Von Schertel. He compared this type of vessel with other
fast water craft and aircraft.
A calculation of the specific power requirements for planing
craft and hydrofoil boats in the speed range of 40 to 60
knots showed that for the same length of 160 ft. and the
same displacement of
0O ta the hydrofoil boats need only
55% of the power of planing vessels. Por this epeed range
comparablö with the Epeeds of trains and. automob1.les,
hydrofoil craft can be expected to operate economically.
The airplane attains much higher speeds with lower specific
power and therefore represents an economical means of
trans-portation. However the extensive and expensive ground
organisation makes the airp]ane far lees suitable for relative short distances, This does not hold in the case
of helicopters; these require a high specific power and
the operating and
maintenance costs are several times as high as forhydrofoil boats.
Planing vessels do not provide the necessary comfort when
travelling in waves, because of high vertical accelerations (actually accelerations of 6g have been measured). It can be stated that hydrofoil craft can maintain higher speeds with less vertical and. transverse motions than any other type of seacraft of comparable size.Then Vos Schertel discussed the characteristics of the two basic foil systems: the surface-piercing 3ysteni,
eon-gjtin either of aaingle dihedral foji or of several
emll f 01. ls arrange on top of each other and the fully
15
-The first system is automatically stable because any deviation from the position of equilibrium of the craft Causes a change of the lift producing wetted area and
this creates restoring forces.
The fully submerged foil does not have natural stability. The depth of submergence must be controlled by mechanical or electronical devices which measure for instance the distance between the water surface and the bull. These sensing elements are used to command a mechanism which changes the angle of incidence of the foil or of a flap.
Therefore this last type can offer better seariding
qualities and. conz.tort.
However the complicated controlling devices form a serious drawback. A new self-controlling system has been developed by the author and a teetboat equiped with this device is
already being tested.
At cruising speed both foilsyatems have
approximately
thesame lift-drag ratio of
1L.
3eyond this speed the condi-tions change in favour of the surface-piercing foil because of the decreasing wetted area.In general the fully submerged foil will offer in the
future some advantages for long distances and ieee
protec-ted sea areas.
Experience with commercial
passenger services baa shown that the hydrofoil lxat can be operated entirely success-ful and profitable if there is a sufficient high passengerfrequency.
With PT 20 and PT 50 hydrofoil boats approximately ten, mainly coastal, services are established.
One of the
most prosperous services
exists between Maracal-bo and Cabimas; annually.over 6O00OO passengers arecar-ried. over a distance of 20 miles.
The str.ngth, reliability and seaworthiness of these ves-sels proved to be entirely satisfactory.
he author concludes with the statement that-
under-the-present circumstances hydrofoil boats can compete economi-cally with aircraft over distances not exceeding 300 to
-. 16
OO miles.
Ohaplin read a paper about ground effect machines (GiM's)
and the development of these vehicles in the United atates.
At present some forty commercial firms are engaged in
ground effect investigations. The diversity of the
count-lees variations in approach makes a comprehensive review
impractical. Therefore only the more significant concepts
are discussed. With 'he aid of the elementary principles
of fluid mechanics the performance of the various GEM eye.
teme are estimated and the outstanding advantages and pro
bl.ems are revealed.. With our present knowledge of ground
cushion effects however, it is as yet not poeible to say
which of thasystema will prevail.
Seven concepts to maintain the air cushion pressure are die-.
cussed. The first system, the air curtain or "annula' jet"
has received by far the most attention. The ground cushiOn
is generated and contained by a jet of air exhausted
down-ward and indown-ward from a nozzle at the periphery of the base.
The eeoond concept is only auttable when the GEM operates
exclusively over water. In that case a part o
the air
curtain can be replaced by sideplates or skegs, which extend
into the water. Compared with the complete air curtain
oon-cept a substantial reduction in power can be obtained at
moderate speeds
The third system: the integrated air curtain is related to
the first concept. Here the integrated air curtaXn provides
for propulsion by directing the peripheral jet at a rear
ward inclined angle by means of vanes.
In principle the air cushion can be contained by a per$.pbe
ral jet of water as is done in the fourth system.
In theory a large reduction in power compared with the
irst concept is effected
but it is not clear at present
bow much of this advantage is left in practice.
The most simple system is the "plenum cbambex'. The
under-rsoesne
aa -adorns and air
i-aimpl-pumped jnto the recess; the ar is allowed toleak out
17
along the ground.
Probably the "ramwing" is the oldest system, having
been
inbx'oduced in Finland by Kaario in 1935. The vehicle has
the form of a box with the bottom and the frontside removed. At a speed V
the
ram pressure +,
Vzis built up beneath the base, giving a lift force LFinally there is the academic possibility to sustain a
GM at a finite height above the
ground withoutdissipa-ting energy. This concept is called the "diffuser-recircu-lation" system. It consists of a recirculating flow, rather like a standing vortex ring which is maiutsined within and under the vehicle. The average static pressure under the base can exceed the atmoaperic pressure and so a net lift Zrce is created. Under the assu*ption of an inviscid flow
this system has no energy dissipation. Practical appl±ca-tion will meet large difficulties.
The author offered the following
conclusions. The
perfor-mance of a GM depends directly on the ratio size-height, in which height means the distance between the base of the GM and the ground or the water surface.
Since laud. areas are
in general insuitable for the
opera-tion of large, high speed vehicles at low heights,
one is
inclined to think of the large ocean going GEM as. a
possi-bility in the future.
In the meantime however, moderate-sized GEM's could be attractive for special purposes. There seem to be two
fields of application:
Passenger- and cargo ferries, emergency craft, sports
craft, etc. on flat inland areas and protected waters,
where extremely low operating heights guarantee good
performance.
Limited militarr applications where requirements for
speed, amphibious capability and load-carrying ability
outweigh the conventional economic performance criteria.
Mèitid the
ódic iáti fdedfvii
This vesoel is designed for operation at depths down to
15.000 ft.
The Aluminaut differs in basic concept from the
bat1yeoaphes
RT8 and
rieste, which were developed by Auguste Piocard..
It will be recalled that it was the Trieate
which made the
record.breaking dive on January 22 1960, to a depth of
3?.800 ft.
The buoyancy of the pressure bull of the
Aluminaut supports
over 80% of the total weight, whereas the buoyancy
of the
small pressure cabins of the batbyscaphas support
only 5%
of the weight. The remainder of the batbysoaphe's
weight
is carried b' a non pressure hull filled with a buoyant
liq4d..
With a total submerged. displacement of slightly more than
half that of the Trieste, the Alurninaut baa about 9
times
the
aeful volume and possesses a superior mobility
and
enduranoe.
The ballast intended for routine ascent consists
of 1,8 ta
of iron shot contained in two amidebip external
saddle
tanks. The tanks can be emptied through hollow solenoids.
When the solenoids are eriergizàd they magnetically solidi-.
ty the iron shot; when the current to thesolenoids
is cut
the iron shot flows out at.ay depth of
operation.
In addition there are tanks for 1,35 ta. of water
ballast
ar4 provision is made for jettisoning 3,18 to. Of
a3.uxniniuinwrapped lead, in oases of emergency.
The remaining ballast of over 3 ta. is fixed. This ballast
io partly needed for stabiItr pux'poees and.
partly forma
a margin available for design, construction or suture
growth.
Special attention has been given to the motions of
the
vessel when rising vertically. In order to avoid violent
oscillations the natural rolling period was chosen so that
the probability of resonance with the psriód of
the shedding
ofvorticeawould remain very smalid In addition
large
19
-Modeltests were carried out In order to
be certain
that theexpeimental
data confirmed the computed values.The submarine is equiped. with two screw propellers of which one, mounted on top of a email superstructure, has
to
provide thrust in vertical direction, the other Is a swivel-ling propeller which can deliver a
thrust in
the horizontalplane.
With the two propellers working Bimultaneous].y it is
possi-ble to descend. to 15.000
ft.
in 40 minutes (without propul-sion it would take about 4+ hours).An emergency ascent from a depth of 15.000 ft. takes 22 minutes. With no power available
it
would take 44 mInutes.Todd. discussed extensively the possibilities of submarine cargoships.
In order to have some figures s a basis for
comparison
between surface ships end submarines, calculations have been made of
the horsepower required for
displacements ranging from 25.000 tons to 150.000tone.
The comparison is made on the base of equal deadweight, For the lower speeds (10-15 kn.) there appears to be no difference In the power requirements between the surface
tanker and. the submarine tanker
with circular cross
sectionAt higher speeds the submarine with circular section
re-quires less power.
For large dead.weighte the draught of this type of ship becomes excessive. When the
section La made elliptical
with a beam equal to four times the draught, the gain in power is lost.For all shiptypee nuclear propulsion is
assumed.For speeds up to 25 to 50 knots, the limit to
which surface
ships can be built and operated economically the advantage
of the submarine tanker is not sufficiently large to
justi-fy its use.
In addition it would require expensive new
building facilitieB, now dry docking fai1itiesandnew
20
-Por speeds beyond 30 knots the gain in power would be
sub-stantial. The weight
and the required volume of the power plant however increase considerably and thiB would result in a deadweight-displacement ratio which will be rathersmall.
It depends on. a number of economic factors whether it would be justifiable to build submarine cargoahips. It is possi-ble that in the future the coat of nuclear fuel will
de.-crease, at present the conventional fuel is considerably less expensive.
The author mentions an interesting comparison made by
Teasdale. With
the assumption that a small aumbarine tanker of 26.000 tons deadweight because of its higher speed could deliver yearly the same quantity of oil as a surface tankerof 7.000 tons deadweight, Teasdale estimated that
the fuel
consumption of the submarine tanker would be about four times as large asthat of its
surface counterpart. Bothships were supposed
to be nuclear powered.There is no doubt that for military use the submarine is of great value for the transport of valuable cargoes in
wartime, with little
chance of detection. It is possible that some government will build a craftof this type
very soon, both for its military potential and national prestigeThe paper of Goodman
dealt with the various experimental techniques and methods of analysis which are either preaenb-ly being ued or are contemplated in the near future atthe David
Taylor Model Basin inthe field of dynamic
stabi-lity and. control of submerged
bodies.The D.T.M.B. has
in
operationthe
"Planar Motion Meohaniam' system, a device which allows the experimental determina-tion of the coefficients of the linearized equadetermina-tions of motion for a submerged body with six degrees of freedom. Brief deacriptions of the newRotating
ArmFacility
21
-The paper of Bogga and. Tokita contained a contribution
to the theory of boundary layer flow, namely: a treatise
on the stability of laminair flow along compliant plates.
It seems that the use of a flexible skin (for instance a
skin Of rubber with liquid backing) may have a favourable
effect on the stability o± laminar flow, because the onset
of turbulence is damped out and transition is prevented.
The paper of Bogge and Tokita unde±takes the development
of a theory which will predict the stability conditions
of the boundary layer
in contact with a flexible wail.
Onethe cono.usions of the authors is that the
condi-tionsof stabtliztn
a flow are rather critical and that
all flexeb3.e coatings do not necessarily have a favourable
effect on the flow.
Wilim presented a paper concerning the history of the
batbyscaphes, the principles of their destgn and the
contribution of trance in the development of each craft.
The pressure bull of the batbyscapho is a sphere because
this is the beet shape to wttbatand high external
pres-sures. The shell of this sphere has a certain thickness
which is so large that the weight of the sphere is far
in excess Of its
buoyaoy.
This pressure hull is suspended underneath a float filled
with extra light petrol directly exposed to the external
pressure to proide the necessary buoyancy. This system
is comparable with the principle
of the free balloon.
Vertical movement is effected. by jettisoning ballast:
ateelehot for rising and petrel for sinking. The steel
shot is bld magnetically and the petrol can be replaced
by seawater.
The use of petrol has a serious drawback: its
compressibi-lity is substantaily rnore than that of seawater. Thiring
the descent the loss of buoyancy due to øompresion of
Vtirol-iB morehant1ie gain due to t
nceafli
22
Once the bathyacaphe has started to sink, it descends
quicker and quicker. On the other band., once the
batbyscaphe starts going up, its speed will increase
progressively and it is impossible to stop it.
The maximum speed under these conditions is approximately
one meter per second..
Short descriptions were given of the bathysoaphes 'IB8 III
and 11.000. The last one is designed for a depth of 11.000
metres.
The FNI8 III baa been used for five years and during this
period more than 80 dives were made. Biologists,
geolo-giats, oceanographers and other scientists have had the
opportunity of carrying out their respective
investiga-tions.
Wilim concluded with a plea for international cooperation
of all the research workers who are interested in
oceano-grapby.
Grim discussed the computation of the hydrodynatnic forces
associated with the pitching and. heaving motions of a
ship. In general the methods which have been applied to
the theoretical treatment of this problem may be
sub-divided crudely into two groups.
The first group employs the representation Of the moving
s
hull form by perodioal singularities.
The disadvantage of these methods is that the boundary
condition on. the surface of the body is insufficiently
satisfied. Therefore only qualitative information
concer-nine the influence of the main parameters may be expected.
The methods used in the second group assume solutions
to be known for two-dmensionslbodtes of which the
seetions correspond with the cross sections of the ship,
The results for the three-dimensional body can be
obtatned
by integraUng the two-dimensional solutions over the23
influence of three-dimensional floW can scarcely be taken into account and that the influence of the speed of the
shi:p caxmot exactly be established.
Grim combines the two methods: a strip method will be applied for the distribution of the singularities, i.e. fOr each
eecton of the ship the similarity will first
be chosen to satisfy the condttion on the cuiface of a two dimensional body of the section inquestion. An
im-proved distribution of singularities to allow for threedimensional flow is
then obtained with the help of anintegral euatiou.
The following problems
re treated.
The heaving motion, the pitching motion and the forces
generated by the waves in a vertical direction. In thepaper only the case
of zero speed is considered. however it is possible to carry out the calculations for a ship with forward speed. Numerical results for this case were not yet available.Lewis and Breslin discussed the possibilities of obtating high speed in a seaway with ships of normal displacement. As is mentioned earlier, the submarine which is not
affec-ted by the seaway, baa a poet&ve advantae over th
destroyer. The speed of the submarine is in principle only limited by the weight and volume of the rower plant.
The resistance oZ this type of vessel is directly
proper.-tional to the square of the speed, whereas the resistance of the destroyer is proportional to a much higher power of the speed.
Research has been carried out to arrive at ship types having reasonable dimensions and a higher sustained speed
in waves than the present destroyers in order to meet the challenge of the submarine.
To this enda number of possible eolutiirns of the problem
is reviewed. bydrof oil cra1,planing vessels, long slender
shipa and semi-stthmerged craft, which are neither pure
-21l-.
These craft potentially
ean exceed submarine speeds becausof their low resistance, good sea performance and. relative.
ly low power.
An interesting conoept is a ship which operates at the
surface in fair weather; in bad weather large peak
bal-last tanks can be filled to enlarge the natural pitching period by increasing the displacement and the radiue of gyration. In addition the waterplane area is reduced as a consequence of the hull form. In this way it is possible to avoid synchronism at high speeda and head seas.
Another interesting type is a long slender hull, with large bow and. etern bulbs. The radius of gyration i large and consequently the natural pitching period is large, where-.
as the resistance is not excessive. In comparison with the semi-submerged design it has the advantage of leas
uU.-volume limitatione.. Sufficient freeboard and flare can be provided forward to keep the water ol't the foredeck
The last group discussed consisted of semi-submarines,
which oan be considered as the next step in the transition
from surface ship to submarine.
The main hull of the semi-submarines is fully or nearly submerged, while a fin or strut pierces the surface. The
advantage of thIs type when compared with the true sub-.
iarine lies in the fact that conventional air-breathing power plants can be used. The weight of a nuclear
power-plant is at present still far- in excess of that of a
con-ventioxial plant.
The behaviour of the semi-submarine as regards depth sta-bility is interesting, for it cannot be expected to rwi at a constant depth below the surface without controlling
devices because of surface interaction effects and. lack
of natural vertical stability. Simplified lineair equa-tions of motion have been set up and solved with the aid of an analog computer. The influence of the distribution
aud area of the stabtitsation fins
as
iveetiated.
PiiverleaI and Marwood presented .eaign data for small high speed displacement type hulls (Froude number betweoi