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C.P. No. 990 _. MINISTRY OF TECHNOLOGY AERONAUTKAL RESEARCH COUNCIL A Note on some Static Tests of Flexible Skirts for Hovercraft bY W. G. 5. Lester ond F. T. Kiernon LONDON: HER MAJESTY’S STATIONERY OFFICE I 968 PRICE 7s 6d NET

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Page 1: of Flexible Skirts for Hovercraft

C.P. No. 990

_.

MINISTRY OF TECHNOLOGY ’

AERONAUTKAL RESEARCH COUNCIL

A Note on some Static Tests of Flexible Skirts for Hovercraft

bY

W. G. 5. Lester ond F. T. Kiernon

LONDON: HER MAJESTY’S STATIONERY OFFICE

I 968

PRICE 7s 6d NET

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. , L

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U.D.C. No. 52?.136.0 : 629.13."12.12L

C.P. No. 99P February 1466

by

3. G. S. Lester F. 7. K1ermr-L

A series cl" static tests ccnducted tc esteb;lsil an efficient fcrm of flexible skirt for a peripheral Jet type of hot-ercraft is reported. ?11e importance of deslgnmng the peripheral Jet system in conjunction w:th the skirt is demonstrated. The results suggest that the effectlvc w&th oI' a flexible nozzle 1s loss than its ootunl wdth and. the discmrge coefficient requires detcrminlng expermontally for oath confi~atlcn. It is concluded that skirt confqural~.cn ~crfommce is best coqcred on the basis of ?ower mput to a skirt to generate a given cushion pressure fcr a specifzed daylight clearance. The rebulto cont'irm that the skirt inFit pwer per wilt exit area,

based on dnyli&t clearance and Jet lengtn, is directly proprticnal to (cushion pressure)"2.

* Replaces R b.E. Technical Report 66053 - B.R.C. 29356

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3 5 7

IO II

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14 15 17

Fqgres q-37

1 IIVRODUCX'ION 2 T!iE TEST RIG

3 FRELIXINARY TESTS

4 THEDEVELOFWNT OE'ANEFFICIEXT SKIRT

5 GOMPARISONBFXWEEN ~ORYANDEWJ3Rl34ENT 6 ExpERmAL lS%ULTS 7 TESTS WITH A NON-VERTICAL SKLRT FEED SIf3i' 8 coNcLusIoNS Reference Illustrations Detachable abstract cards

t

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I IXTROIXJCTION

In recent years interest has been shv#n in the possSdlltg of iqroving

the overland an& cverwater c&pabz.iity of hcvercraft. It has nov Sec~e apparent that a considerable im~rovemedc in ~eri'crmance can be ac5ieved by fitting hovercraft with flexible extensions to the hull; these ext%lsicns or skirts are capable cf being Seflected Ail& passing over a?? obstacle an2 tien; by virtue of the cushicn pressure ant? the airflow thrcqh the skirt, return to their design ccnfiguration. With the original hovercref't concepticn cf a completely rigid hulled craft the maximum obstacle heq$-d which could be oleare?Iwas governed by the hover height of r.he creft and useful practical cloarawes rleman~ed excessive power; the prcvislon of a flexible wirt !lss

meant that hover heights can be mzinidsed an5 it 1s no lnr.ger necessary to install power sufficient to give a da>~ll~hL clearans~ rqud to the maxtim height of obstacle likely to be encountcrcd. Tl-..c terms daylight clearance, ground nlcarance and hover height are strictly qnonymous but the :'lrst is used generally in tnis Report s==ce tne others arc sometimes use&tc indicate the distance between the grcunil and the lower portion of the had stmotL-e of the hovercraft ratiicr than that of the flexible skirt. For e craft f'itted with flexible skirts the dayllght clearsace beneat:? the skirt need czily be sufflclent to ensure that the mqority of smr.11 surface irregularities arc paSSe< OVPr

without rontact an& larger cbstaccles are accommodated by tnc slart flexibdlty; a reasonable daylight clearance zs desirable in or&r to nunll;iisc skirt v?tRr. The maximum height of obstacle whicn can be accamncdated 1s i&ally the length of the flexible extension below the rzqzd :Jortlon cf the hull plus tne maxu~~m daylight clearance of the craft; in prsctlce this IS not achlcvec because skirt flexibility daes not extend over the whole length of skirt and the skirt beccmes stiffer towards thz hull attachment, maklng ticflectlon more diffzcult and reducing the effective skirt length.

The usual skirt.systcm emplcyed on a pmlpheral jet craft.conslsts of a Double-wall.eFI skirt enclosing the peripheral jet and forming a ntz$ exit nozzle thrcugh which the air su@y is fe& to fg~rm the air cushion beneeth the craft. In addition, if the-basin craft unes 2n array of loqitudd and transverse jets for assisting in main',aining stabiiity, or contr~buting.to ~rqdsion and control, these eze also fltted with double -,valle?. s!;lrts 21 sn attempt to retain the criginalfunet%ens of the jets. The hm skirts have to be derqneci cc) that they can be-defLe&od jlran'is on-csntact \-rlth PJ o5stade; tne aft skirts SO ChnC they can bo deflected nutvards to penrat egress of t,;e o3stacle'

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and the side skirts and longitudinzl stabJllty skirts so that they can be deflected aft. In design allowance must be made for these three dlfr'crent

dxectlons of deflection and provulon also made fcr ccntact with obstacles rr.et whilst the craft is yawing or side-sli?puig. The aft skwt is usually splat

intc sections to facilitate cbstacle egress and prevent scocpu-~g UT cf debris; tc some extent this elxnina tes the necessity fcr rearxard deflecticn cf' t!x aft skuts. In scme cases clcsed inflated baEs have been used lns'cead 4 an aft skirt on craft with ICY dayllght clearsnce and a tendency tc swcpmg.

There are manjr practxal prcblems asscclated with the design of flexrble skirts; the skirt shape and nozzle design mus t b? such that severe flow lo,sses

are not uxluced or contrcl and stablllty of the craft mlpeded; the skut length rrmst allow a reasonable obstacle clearmg cacabillty withwt raxxng the centre of gravity cf the craft tc a height where lnstablllty beccmes manifest; a rcbust though flexible ccnstructlcn is required, and the materials used mst have a high resistance 'cc tear, abrasicn and expnsure tc atmcsoherx cotilti?ns tc

ensure a useful wrkmg life. The .additlcn cf a skirt tc a hcvercrsft will reduce

the dayllght clearance lf the slme payload is tcbe carried as cn an unmcd.1f1ed .

crsft : to minlrmse this reductlw the welg!?t of the skirt and Its attachments must be 1~ but cwsistent vnth durability. Sknts ha-e tc scmc extert beer, 3 regarded as ancillary Items to be added to a ccmpleted waft and deslgnened separately; this is an unfcrixnate situatlcn fcr the skirt shculd be an Integral part of the craft and the ducting from the fin tn the skirt designed in ccnJunc- tlon with the skirt fcr maximum effxlcncy. k vcrt1cs1 discharge Prcm tne fen lntc the skirt is desu-able whereas fcr a craft wthcut skirts the pcrlpheral Jet 3s usually inclued UIWU-& for rnaxxmxn efficiency and xhe ductlng designed accordingly. The skirt 1s effectively a continuation of the ducting m the rigid hull and termrnates in a nozzle dxscharglng auz at an angle to the ground. To malntaln the design shape of zhxs nozzle the skirt contours are determined by fabric diaphragms; m some cases It 1s possible to re~iace these dlaphra@s by strmg ties but, m general, the strmgs vibrate anri cause itutter of the skxrt assembly. The saving m weight through using string ties 1s apprecxdole and the construction 1s also easier. The presence of the skirt alwa;rs leads to an increase jn flow energy losses vhxh can bs mxlmxed by correct noxle and ductlng design and Iinntatlon of the ember of disturbance genvatlng Itens, such

as diaphragms, within the skirt. Diaphragms are however a disadvantage m that they impede the propulsion facility orovlded by the longltud.mal jet systems of some craft and prevent contrcl @f 'the dlrectlcn cf the Jet thrust; the effective- ness of moveable vanes in the rlgld ductmg of tht craft 1s also impawed and there is a need for a skirt control system.

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5

me present r&e is cmnccrned with The reoults of statlC tests Cn ,

various forms cf fabric Skirt. The object has bcell to &sSess the practicability

cf different skirt designs; to find the extent tc which the d~slgn shape of u

flexible nozzle is mintamed, and to determne a fom of s2u-t whxm does not

induce high flmv losses. Little research appears to have been done on the

theoretical aspects of nozzle design fcr skirt application e.rd even the Optimum

jet discharge angle for a peripheral Jet craft I .s a matter for conJecture:

s- designers favour a Jet making w angle of 6O'wlth t?Le ground and. others

use angles of 45’ or less. But, with a flexible fs3ric nozzle, the jet SII.&$C

mSt chmge where the skirt is deflected by an obstacle snd variations in IAN lift am3 stability of the craft will occur; thus ssprrct cm only be ex~mmc?

by full scale trials with a hovercraft and the skmt desig#z can ody ensure

that the nozzle provides a consistmt jet angle when there is complete da;yllght clearance.

The practical aim of the tests has been tc produce flexible extensions for the Britten-Norman Cushionoraft CC-2 of Naval Air DepaJ?tiWnt at R.A.E. Bedfoti and scale dimensions of the skirts tested and the cushicn pressures involved have been directly related to this craft. The peripheral Jet of this partxular

craft is directed vertically dmwSrds fcr feeding the skirt assmbly but some tests have been conducted using the origlnal hull form with the jet dlsc'larging at en angle of JO0 to the underside of the hull. Nuch of the pract~zzl l~wwlcdge gtined is however directly applxablo to flexibla skxrts md nozzles in general.

Sufficient results have now been cbtained for a prelinunary re?rt to be made; the results sd concluSx.ons are by nc means final but a hctter under- SbIIdhg of the problems assoczated with the desl&n of flexible skxrts 1s slowly being achieved. Many of the expertifinxs made have been negative or inconclusive and the test x-i& has suffered from a range of teetixng problems. &n&mental work cn the aerulynamlcs of nozzle design 15 required but this is a long term project anii practical dcvelc~cnts are more urgent; the current progr-e thus consists largely of a number of 'ad hoc' experiments to determine a. skirt iYxth a reasonable perfomoe.

The expertients recorded 111 this Report iwre ccnducted as part cf the research programme at R. & D.E. Cam5ing:on.

2 THF; TEST RIG

A very simple rig was conatmcted. mitmlljr for the testing cf sample skirts. This rig was des~gxd to acco!nnodiate straight sku-t sectlons of 3 ft

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6

breadth and varrable length up to apuroxlmately 16 in. The hull of the hove,rcraft was simulated by a closed reotangular wooden box enclosing a falrlng representmg , the hull sectwn; a rectangular slot 3 ft long and varla3le 111 width from 2 m to 10 111 was cut In the base of the bcx tc form the peripheral Jet orifice. A

c moulding was fltted on the -er Jet edge interlcr to the box to sxnulate the ducting of the flow Into a vertical jet stream as In tile hovercraft. The base of each skirt sample was attached to a rectangular framework which cculd be

clamped to the underside of the box so as to surround the jet orlfica. x circular crlflce, 8 in in diameter, was cut in the rear of tine box and the air supply from a small blower was directed through this tc discharge frcm the

peripheral Jet Into the test skirt and cut via the flexable Jet nozzle. The blower used was capable of delivering abcut 2000 cu ft./man at a nressurt? of up to 8 in water gauge and its output was contrclled by means of a butterfly throttle valve. The wooden box was mounted on top of an open fronted cage with walls of perspex; the region mteno.. * tc tnis cage and benlnd the skxt retained the air cushron formed as a result of the d~%harge from the nozzle. Soft foam rubber was used between the side walls cf the cage and tnc en& caps of the skirt section to prevent loss of cushion pressure. The cage was fltted with a wowlen floor .SdJustable m height usl.lg small jacks to give a contvluous range of daylight clearances between the jet nozsle and the floor; fabric flap seals were then used between the floor and sv5-a walls of tne cage to stop a~ escqc. To give ground sumitatlon the floor orojected well outts1d.e the front of the cage and deer of the nozzle. The rig is illustrated in Plg.l(a) 7~1th a test skirt in posltlon.

,

The apparatus was instrumented so that read,xngs of static and total head could be obtalncd wlthln the box hull and in the cushion area. Total head rea3ings could also be taken within the skirt itself at scvcral stattlons by

perforating the fabric to accept small prcbes made up cf hypodermic tubing for the purpose; by orlentlng the probe s to give a maximum railing on the maxmeter it was poss~blc to obteln fairly accurate mGasuriment.s. Tne stat2 pressurz at any point m the skirt was lmpcsslble to measure accurately as Vera small prtot- statx tubes were net readily available; a rough measurement cculd be ~~ota~ned by holding a pxtot-tube normal to the flow dlrectlon but this was vcq mreliable.

. Prom rat132 flow surveys It was apparen t that z very high prmortlon of

the total head m the box hull -was due to dynemx pressure. The r&tics of cushion pressure to total head at Input,

II -witn any skirt flttcd, twro alwys much

lower than suggested by eqonentlal thecry fcr a given height tc thxkncss rat.10 of the flexible Jet nozzle; a fagure of tne o,-der of 305 of the tneorctlcal value

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was not unconrnon. It was decided tc modify tiw x-cut systm~ tc UIC~CEIS~ the

proportion cf statrc head amI this wss achieved by feedine the output from the blower directly into a iarge settling chamber en?i connectmg the rear of the

box hull directly to this chamber. The settlrng chamber had H volxne cf Cbc~tt

200 cu ft and ccntalned screens of a. fine fabric mesh to reduce the tilrbulence; the entry tc the box hull was rectzngdar instead of circiiLsr as before an?. surveys of the flcvr wlthin thus area showed that the prcpcrtlcn cf velcclty head w&s ncgliglble and the ex- was substantially statx un'cll the discnarge slot intc the skirt was reached and velocity was acquire?. The discharge frcm the jet was fcund tc be uniform alcng Its length to wizhm an inch cr si) cf the side walls.

No mltiel prcvislcn was m-de f?r the measurement CT IXWS flcvr xntc the system but It seen bccrtixe anparent; that, with many cf t!le t.;Tes of skxt emplcyed, it was diffxult tc dctenrnne a true height tc tilidness ratlc fcr the nozzle and compariscn beixeen tneory and experiment cculd net be made by plctting cushion pressure tc tctsl head ratlc against the heqht to thickness ratio with "n;r accuracy. An orifice i>l?te meter was thus mccrpcratzd. in the cutlet frcm the blower tc detcmlne the m?.ss flr7 Lntc the a~ttlmg cnamber and, since the air was virtually staticnary in this chartier a-d the static pressure there wes knr~~, it was pcssible tc deternine tne paver mnpdz t? the skirt as a prduct cf pressure times volume flew per sec~zd. As s. basxs for compariscn the cushlsn pressure achieved ccdd bc plotte? agxnst the

purrer input fcr any daylight cle.arence cr per unit cxlt area tr GIVE a measure cf the efficiency nf different skxts. A sketch cf the flnsl test rq ustd is shown in Fq+l(b).

3 PFSLw;IiU~Y TESTS

The first tmes cf skirt dcsqn cn which experiments were ccnducted are shown in Fig.2. These skirts are charecteriscd by the fact that th?y nave a definite nozzle bcundcd by the cuter and inner walls 1-f' the skirts and the shape is ccntrolled by means cf dlxhragns. Ski&s -f thlr tync were mcxfie

up from a thin twr-ply prvfe$ ccttcn dinghy material and in scm6 c:~scs cf R heavier neoprene-prccfed nylcn materXl. Tc prsvidc a stnnried fcr what might be termed the eptimxn perfcmance cf a given flexible fabric skirt cm?i@ratmn similnr skirts were m3e up firm cardbmz-3 possessmg natural rigdiL,y as qpcsed

to the rigidity cf the flexible skirt achieved thrwgh pressurisaticn.

The initial mcthcd. used fcr cmparing them-y with experiment was the plctting c+f cushim pressze t? total hed ratw, pc/H, zgaxst the nmzle

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a

height above the fleer to the nozzle thickness ratio, b/t, fcr a aven nozzle angle, 8, measured frcm the hcrlcontal. Expcnentlal thecry grvcs the relatxcn between these quantitxes as:-

PC -iT

2(1 + ccs e,t] h J

After some lmtial difficulties m cmpletely sealmg the skirt area cn the rig, the results cf the first tests with cardboerd skmts with 1.33 m wde nczzles shcwed that the values cf pc/3 cbtamed fcr a gzven h/t were cf the crder cf 9@ cf these predxted by the thecry. This was regarded as a satisfactcry demcnstratwn cf the effxlcncy cf the skirt and nozzle shape, which had. been desxgned rather arbitrarliy m the absence of any aercdyllCvnic data m

this type cf nmzle flcv. On replacmg the cardboard skirts by simlar fabric skirts the results were dlsappcmtrng and frequently the measured values cf p,/;i were arcund 5C$ cf the oredlcted values fcr a given h/t. The results vere net affected by altermg the mdth cf the pcrlpheral Jet crlfice feedmg the skirt from 2 m to 10 m or by shortenmg the skirts and retaming the same nozzle configuration. The skirts cf neoprene/nylon fabrx were better than tnose of

proofed cotton and It was believed that the mprovement was due to the ad3iltxxv.3 thickness and rlgldlty of this fabric. Atien@s mere made to stiffen the ccttcn

fabric skmts locally by adding stiff mserts to the dlaphraes m the nozzle, and card strips to the cuter face of the inner wall of the nozzle; thm effectively rlgldised the area but left tne mJcrlty cI c the skxt flexible and the result was an appreciable mcrease in efflclency.

The main reason for the dzscrepancy between t:le efflclencles of the fabric and cardboard skirts was traced as a result cf makmg f1.m surveys mthm the cardboard skirts. It was d.eciuced from the tctal head readmgs and t!le mss flew ccntmn~ty vilthm the tapermg cardbcard skirt that the statx pressure on the insde of the inner wall of the nozzle was less than the cushmn pressure cvcr a region extending upwards from the end of the nozzle for a dletance approxma+,ely equal to the height of the nczele above the flow. The effect of this mth the fabric skirt was that the excess cushlcn pre ssure could ?artlally clcse the nozzle and thus reduce the jet thickness; the momentm amcharge coefficient of the nozzle was effectrvely beme reduced. Narked closure or constrlctmn of the

fabric nozzle was not evdent but it wac, apparent that there was no tensmn 111 the lower part of the diaphragm lnsde the nozzle. Attempts to mcasu1F: the static pressure inside the nozzle and near tc the Inne- - lrrall nChxdxd a ten&zncy for this to be reduced so that a suction efl"ect was produced. The flow surveys

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9

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also shme& that the jot stream closely followed the VertlCal OU%W Wall of

the skirt whatever the wi$th of the discharg.. P dot ~3.133 the trlan&rr- r&on

behind this stresmmas filled w-,th air apparently at rest. In an attempt to visueJ,ise the flov pattern arising a model KW made of the hull and ski?? and

floor m the form of a trough wit II vmlls rmresentmg these outlines; this was

filled with water which could bc released to flov through the skirt, and dye was injected t0 Show the flow pattern. It was evident that the jet clung to

the outer mall of the skirt and there was a standing vertex fcrmatzon between

the jet and inner wall of the skirt; the vclccities in this vcrtcx region mere

much too low to be detected on the proper test rig vnth the instrumentation available.

The design angle of the criginol skirts' nozzles vas either 30c, 65' or 60'but a tendency vas always ncted frr t:ms angle to mcreasc with a skirt fitted on the rig. The exit, .lct was s~?.ely splayed and the zet rcacticn

combined with the cushicn pressure tended to make the cuter wall cf the nozzle kink and change the ncasle angle, par ticuiarly when the nozzle was close to tile flocr and the cushion pressure was reintivelg high. Wmlst this effect Lght be expected its onset is c%'ficult to predict without a prior :2nowlcr~,c of the pressure forces acting on the skirt snd their distribution. It is nra:tioally important that nosele distortion shwld not occur and that the oressurlsation ~ of the skirt should be such that it too is not distorted from the design shaze by cushion pressure, jet reaction cr d.ynam5.c pressur; due to fcr;rard motlrn of the craft. The stiffness attainable with a skirt 1s a functicn of the internal pressure and its stability in buckling &ponds on th; ratic cf its Lngth to base width: the practical limit for this ratio appears tc be about l.j. Jith 16 in lcng skirts on a 10 in base the cuter wall of the skirts nearest the hull attachment points tended to rise up OVW- the hull, effectavely shcrtcning the skirt and causing a change in nczzlc angle independent cf any kinking at the nozzle due tc local buckling. In all the experiments carried cut the wAs Splay cf the noeale exit jet mde it iqossible tc detensinc a true noesle angle and mean values ha3 to be taken,

Many variants of the n!cirts sho.vn in Fig.? have been tried: nozzle angles have been changed and. the width varied; dizqhragrs have been [email protected] or partially replaced by strmg ties; partial diaphra~s end porous diaphragms

instead of full diaphragms have been used: skirts have been shortened in length retaining the ssme nozzle geometry, and the iridth and entry angle of the feed slot have been changed. Yne results obtained from these m&iificaticns to the basic type of skirt witin definite nozzle were not encourag;lng: marginal

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improvements mere sometunes obtained but m many cases the results were conslderably pcorer. Cyhndr~cal skirts with and mthout tapered nozzles am2

horxontal dlaphrap as shown V-I Flg.2 xere also tested and some tpical

results of tests wzth these skirts and the long-noezled skwts are shown In Flg.3.

4 THE DEVELOFMEXC OF A3 EFFICIEXI S:KlRT

It was evident from the prcllmrnary tests that there were serums

di.screpancx,s between the perfcrnwxes of rigld sku-ts a1~3 flexible skltis of the same configuration and that the flexzble skirts vzuld reduce the dalrlight clearance of a craft appreciably. Smce the Object of the tests was to produce a slart approaching maxumx~~ effxlency, ad not Just a skwt glvmg XZglnal

improvement 1x-1 obstacle clearing capablllty, effort vas ccncentrated on flndmg

ho,v a flexible nozzle could be deslgned so that it dxd not dlstcrt or ho;! the problem could be avolded. Although improvement was obtained by locally stiffen- ing the nozzle area thus was not felt to be practicable as It was detrimental to the essentxl feature of flexlblllty and CO&~. be expected to accelerate the wear rate of the skirt.

It was decided to cut back the umer wall 0.. f the 11ozzle 111 stages to find where nozzle closure ceased to occur and the stages cf cuttmg-back cn a long- nozeled skirt are shown in Fig.4. The cuttmng back procew no lcnger allowed the clear definltlon of nozzle width and the plottmg of p,/X against h/t&d not represent a useful means of comparison. A new basis fcr comparlsor, zas sought and the most practzal was found. to be the plotting of cush~cn pressure agaxnst

power for a given clearance height or per unit exit area.

The effect of cutting back the Inner wall of the skxt cf Flg.l+ is shovan m Fig.5 There was a grsd.ual uxrease m the cushicn pressure achieved fcr a given power Input as the skirt was cut back; tms was less marked at the 2 III height but was clearly defined at the 4 in and 6 in daylqht clearances. The improvement levelled off when the curved inner fact; of the nozzle was com&+tely removed and no lmprovemcnt was gained 3n. cilttlng back furt:;er, as 1s shown m the upper curve of Fig.5 rclatmg tc three succcss~~c stages. In the final stages of cutting back it was apparent that the skirt wxtn a single outer wail at its extremity was not practically useful as thus fcrmed a scoot and wds easily dsmaged by the exit of an obstacle. Eowevcr, sLnce the cut-back nozzle gave such an unproved perfcrmance the skut wa s redesqnned so that tne Inner wall of the sku-t was mthout curvature and the cuter mall did not extend to form a scoop. This re-desqned skirt and nczzle 1s shown m Flg.6 where the nozzle

.

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11

is effectively only a slot. Furt'ler experiments were carried out With '&his

skirt by cutting back the straig!lt inner wali; it vas found that once the exit hole size exce&.ed 1.5 m there was r,o im?rovemed m the cushion pressure achieved for e given pcxer and it wzs i,mXderld Wiletiler Cr not thCre ;raS an

inner wall. The results of these tos',s a-e shcr,m in Fig.7 v:hcre the

experimental points follow the full lines with negligible scatter.

The implication of these tests is that the siraplest ty!X Of Skirt 1s

one consistmg of a single outer wail alth its shape retained by dlaD!lragPS attached to the craft hull inboard of the feed :et. :ioxcvcr it has already

been remarked that this type cf skirt tends to scoop up water and debris and catch on cbstaclen, but by making the skirt in small soparate mdividujl sections

or convolutes whiah c-an flex outwards locally, without excessive loss of cushion pressure, much can bc done towards ellminattg the practical Rroblems.

This particular approach has been adopted to sane extent by both 3.D.L. and Vickers in skirting systems.

5 CX.NPARJSG? ShT'NEEX '_'IiEC!RY Am IWl%RIKZNT

It is difficult to obtain a SaiiafactorJ direct method cf comparulg the experimental results wxth theory. It is evident Prcm the results cf cutting

back the inner wall cf the long-noezled skirt and the re-desigued skirt with straight inner wall that the actual jet thickness to be used in any theory is not necessarily the width of the skirt exit nozzle. It oafi easily be show (e.g. Ref.1) that for a given ccnfiguratlcn the p"er required is d~.rectly

proportional to po"*, but the factor cf proaortlcnality is a function cf the jet thickness and ctner georaetric cherzcteristics and its rrag,xtude is different for the tliic principal peripheral ;et tleones currently m use. Yy determlnlng the critical values for t>e factor of ~roportionallty gcoxxctric parameters can be chcscn such that the Rcwer required for a given cushion pressure can be mxxxised. It is with this opttinum situation that the results obtained in the present tests have been coirpared.

Cm the momentum theory, m which It is assumed that the static pressure in the peripheral jet is the ~pesn of the cushion and atmospheric pressures, it can be shocm that

P 22 2x H = 7-E (2)

(3) where x = $( 1 + cos e)

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12

and the power required is

p = ,fin Pc3j2 1 cx 2pF (1 + cos e) iI I --$-

(4)

where 6 1s the Jet length and p the atmxpnerlc density. For given values of the other variables thus power 1s a mmimmm for x = 1, and settmg 0 = 45' it

can be shown that in tms optmum case

PC 3/2 =

3.8a SJ (

where pc is measured III mches of water gauge, P 1s m norse-pcwer and 8 and h are in feet. However, xhen x = 1, p,/" also 1s un1tv a-a t:1x3 1s a SLtuatlon which could not be achieved m practxe.

On expcnential theory It can be sho~m that

P c H I l-e -2x

and the power required is

p = f’+;” (l-e-X)

+ cos 0) (1 - e

-2x)3/2

(6)

In this case the mmmum for paver 1s obtamed when x = 0.7, and agam setting 0 = 45O the optimum case 1s given by

where p, is in mches of mzter gauge, P m horse-po,ver and C ad. h m feet.

At the values of x around unity the exponentxl theory I.S gederzlly regarded as mere satlsfnctory than themomentuin thecry an&, as many expicrunentalists results support this, equdxon (8) 1s used in the preser.t study to give the

optimum sltuatlon sath whxh all the static test resdts ca bc coqared.

It was shown both m flow surveys and by flow vxxalisaticn t:hzt tie main Jet stream closely follavred the vertxal outer wall of the skirt and that the majority of the mass flav occurred in a layer clcse to this outer wall and the

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13

.

velocity dropped rapidly across the Jet as it agproached the inner wall. It was found with cardboard skuts having 1.33 in wide nozzles that the velocity profile was reasonably flat across the Jet, but on widening the nozele to

2 inches and to 3 inches there was no great efi'ective increase u1 jet width because so little flow was occurring towards the inner wall. The card skirts used in these expcrimtdzs with varying nczele widths are shov;n in Fig.8. The plot of p,/H against tit for card skirts with 1.33 in wule nozzles showed reasonable agreement with exponential theory and about 90$ of the theoretical value of pc/H was achieved; the results for the 2 inch and 3 inch nczzles gave progressively lctier values for p,/H as 1s sho#vn ir. Fig.9. The slopes of the three curves passing through the experimental poz.nts .might ha-re been expected to be the same but the effective jet wic?th, which one might ueflne as the width over which a fixed percentage of the mass flow takes $ace, appears also to be a function of the dayllght clearance height. On plotting the cushion pressure against the pp&rer mput to the card skuts nlth diffcrcnt nozzle widths it was found that fcr a given daylight clearance the experimental points fcllcwed substantially the same lines for all threr nozzles; these points are shown plotted in Fig.10 for a rsnge of clearance neights. It was thcught

that the jet streem width could be R functicn of the slot entry size to the skirt end readings were taken for feed slot widths of 2, 5 and IO inches; the results for a 2 inch daylight clearance are shown in Fig.11 an& indicate

that within the range of experimental errcr the feed slot width med.e negllyible difference,

Because the fabric skirt o f the original design shown ~.a Fig.6 was found to have a tendency to catch on cbstaoles it was modified by the addition of a small straight nozzle to the exit slot as snm m Fig.12. Tests with this skirt showed that it ys.ve almost identical results to the unmcdlfied verszon. A further skirt was made up in fabric to a design simdar to the type apparently used by Saunders-Roe on their hovercraft; this skirt is sham in Fig.13 and the test results showed. that it was slightly inferior in pcrformmce to the skirt of Fig.12. A convoluted skirt, similar to the Vickcrs ad. H.D.L. types, was also constructed and this is sho7m in Fig.14; the skirt has no inner well and. is extremely flexible end readdy pcrmlts the ingress of obstzcles, it is also easily deflected outwards by the cgrcss of obstacles. In view of the early experiences with cutting back the inner walls of skirts it was expected that

this skirt would give gocd results: this was confirmed as the results were very

similar tc those obtained with the Saunders-Roe type of skirt. The results of all these tests are given in. Fig.15 where cushion pressure achieved is plotted

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14

against power per unit exit area; Fig.15 also show tne results obtained %lth

cardooard skirts and the optimum theoretical lme plotted frm equatum (8). Mean lines have been drawn through the expermental pomts. It can be seen from Fig.15 that for a given power mput to the skirt there IS a drop of the order of 25% m cushion pressure below the optinum value wltr, the fabric shuts tested. A reasonable fit to the best fabric skirt data is given b;r the expression

where p, is in Inches of water gauge, P In horse-power and C and h in feet. The

expressmn appears to be valid up to p, = 2.0 m and It my be reasorLable to

extrapolate to oonslderably beyond thm pressure; hmever 14, 1s desxrable that tests should be carrled out at more representative cushlcn pressures up to IO incn water gauge usmg a larger blower.

The agreement mlth the optmum %hecry 1s not good but it should be borne

in mind that the theory may be inadequate and it may be jzlpossiblc to achieve optizxm conditions tc comply with its requuenents. For exaqle, the theory is based on a parallel Jet exudir.g from the nozzle whereas in practice the Jet is splayed outwards; p-art of the jet enters the cushion to crovide ewrgy for a vortex motion and the remainder escapes through Lr.e exit area clearance: the simple theories do not take account of this behaviour.

7 TESTS 'JXTH A NON-VERTICAL SKIRT iWJD SLOT

In the course of these tests to deterrmnz a skirt sultable for the Naval

Air DepartmentCC-2hovercraft vrxth a 90' permphcral jet a request was rccelved to explore the posslbilltws of fitting a su~~llar skirt to theCC-2belonglng

to the Fighting Vehicles Research Fad Developent Establlshncnt at Chobham. The F.V.R.D.E. craft has a peripheral Jet xnclmed at 30' to the horizontal and in

order to avoid loss rf cushicn area the conflguratxn shovn in Fig.16 had to be adopted for the scale model to fl'c on the test-rxg. In thu case the peripheral Jet necessarily dxcharges onto the inner wall cf the skirt and IL ::as expected that the flew losscs mould bc ccnsldcrable: thx was confu-med by the tests and the results in comparison with the N.A.D. CC-Zfeed slct conflguratlon are

3 shown UI Flg.17. The results cf these tests served tc erzphasise the LTportance of designing the peripheral Jet feed. system to the skirt 1n conJunction with the skirt itself.

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.

15

a CONCLUSIONS

.

Several simple but important ccnclus~ons can be drawn from the results of this preliminary study:

(1) A flexible fabric skirt nozzle may close locally due to pressure forces and It, 1s advisable tc design the nozzle so that this closure does not ccour. The nozzle design will remain a matter of trial and error until tne flow through a skirt-nozzle ccmbmatlon i s understood and the pressure forces actuq are predlctablc.

(2) Even if a flexible skirt nozzle does not close lowlly its effective width is probably less than its actual width. This implies that there is a discharge coefficient to be included in any calcul~t.tlona and this coefficiect neede determining eqrimentally for czoh hull-skirt-nozzle ccmbmstion.

(3) The discharge coefflolcnt for a flexible skirt nozzle may net be a ccnstant but a function of scvcral varwblcs includu~g dajrlight clearance and cushion pressure.

(4) Withcut kno?ring the discharge coefficient the ccmpariscn between experiment and theory is likely to be meaningless. One can, however, directly oompare particular configurattlons on the basis of pwer inpllt to a skirt to generate a given cushion pressure for a specified dayiqht clearance. Frcm the practical point of view this is the most useful comparlscn awilable and gives a reallstlc estimate of the power requred fcr a give11 static !;CVering performance excluding lcsseo in fans, shaftmg and ductlng to the peripheral jet feed.

(5) The tests conducted conf'irm thlrt the powr per unit cxlt. ,arca is dlrcctly proportional to the cushion pressure to the three halvts for the configurations used.

For the hull-skirt-nozzle configuration employed h s 2.1 where p, is in inches of water gauge, P in horse-power and JZ and h in feet.

(6) It is kierative that the peripherel jet system on a basso hovercraft should be deslmcd in conjunction with the skirt and thc&t the s!clrt should not be regarded as an ancillary if an optimum pcrf'ormance is desired.

Page 18: of Flexible Skirts for Hovercraft

(7) Future work shculd extend the present test results to higher cushion pressures and effort should be devcted tc derlvmg a tPz.oretxxd analyst of the

flow within a typxal skirt to deteranne the pressure dlstrdxhcn and the foxes

acting on the skirt resultmg frcm &ma;na2 effects and cross flow and vortex flaw vrithm the cushmn area.

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17

e No. Author - Title, etc.

1 \?.A. Mair The physical principles cf hcvercreft. J. Roy. Aero. Sot. Vcl. 68 No. 6~~6 October 19GL pp.683-691

Page 20: of Flexible Skirts for Hovercraft
Page 21: of Flexible Skirts for Hovercraft

MOULDING - PROTRACTORS

.

PERSPEX BOX

II I Ill ADJUSTABLE FLOOR I I Ilt-

PROBES I STATIC PRO8E 2 SIDE PROBE - PLENUM CHAMBER 80X 3 FRONT PROBE - PLENUM CHAMBER 80X 4,5.6,7 SKIRT PROBES 8,9,lO,ll COMB PROBE -JET I2 PROBE - OUTER CUSHION 13 PROBE - INNER CUSHION 14,15,16, I7 PROBES - STABILITY CURTAINS I8 WANDERING PROBE - STATIC 19 WANDERING PROBE - DYNAMIC

20 SPARE

.FLOOR JACKS

FIG. l(a) TEST RIG-FLEXIBLE SKIRTS

Page 22: of Flexible Skirts for Hovercraft

ACCESS DOOR,

SKIRT TEST

- -AIR RESERVOIR OR ‘SETTLING’ / CHAMBER. PLYWOOD ON TIMBER

,PRESSURE DIFFERENTIAL ‘U’ TUBE

YRIFICE PLATE

MULTI INCLINED TUBE/ MANOMETER

FIG.1 (b) TEST RIG FOR FLEXIBLE SKIRTS

.

Page 23: of Flexible Skirts for Hovercraft

IMPOROUS ,

DIAPHRAGM

AIR CUSHION

SKIRTS FOR

SCALE XST

LINEN DIAPHRAGM

IE

4; 1, VERTICAL OUTSIDE WALL PROOFED (d) VERTICAL OUTSIDE WALL (a) VERTICAL OUTSIDE WALL DIAPHRAGMS, FOR FULL LENGTH POROUS DIAPHM-9 WITH HOLES POROUS DIAPHM-S WITH HOLES

(a)2 PLY FABRIC SKIN 2 PLY FABRIC SKIN 2 PLY FABRIC SKIN (b)NEOPRENE /NYLON SKIN ALL WITH 45=’ NOZZLE 30“ NOZZLE (c)CARDBOARD SK I RT 49 NOZZLE

FIG.2 (a,b,c,d,e) TYPICAL TYPES OF SKIRT TESTED

Page 24: of Flexible Skirts for Hovercraft

0

.

Page 25: of Flexible Skirts for Hovercraft

. .

NTERVALS

3NLY A PARALLEL 3END OEITAINEO IF RADIAL COROS 3fRUCK FROM :OMMQN CENTRE

FIG. 2 (h)

PANELS ,REGARDED AS FLAT SHEETS

\ BEN0 lNCREA:EO BEN0 INCREASED \ I IN WIDTH

w

t- IO" .

FIG.2(j) FIG. 2 (k)

h FIG 2 (h j sk) SKIRTS WITH CORD TIES 3 SCALE MODEL

Page 26: of Flexible Skirts for Hovercraft

O-7

0.6

0.5

0.4

O-3

0-l

NOZZLE CARD SKIRT 1

B CYUNYDRICAC TYPE FABRIC SKIRT

I

= h/t 6

FIG.3 TYPICAL PERFORMANCE OF EARLY SHAPED NOZZLE

SKIRTS NOZZLE ANGLE 45’WlDTH I.33 INCHES

Page 27: of Flexible Skirts for Hovercraft

MEOIUM LENGTH SKIRT WITH NOZZLE - It” LONG

.

.

FIG.4 STAGES IN CUT BACK OF INNER WALL

Page 28: of Flexible Skirts for Hovercraft

0 196 INCH CUT BACK X 2%6 INCHCUT BAtK 0 2’3/16 INCHcUT BACK t 3546 INCH CUT BACK A 3"/6 INCH CUT BACK 0 496 INCH CUT BACK

0.2 0.3 o-4 0.5 P HORSE POWER

READINGS TAKEN AT A CLEARANCE HEIGHT QF 6 INCHES

0.6

FIG.5 THE EFFECT OF CUTTING BACK THE INNER FACE

OF THE NOZZLE OF A PARALLEL NOZZLED FABRIC SKIRT

Page 29: of Flexible Skirts for Hovercraft

IO” LONG RADIUS OUTER WALL SKIRT

CUT BACK IN Ii&TAGES

.

I FIG. 6 STAGES IN CUT BAC& OF INNER WALL

* 1.

Page 30: of Flexible Skirts for Hovercraft

0.1 0.2 0.s 0.4 o-5 0.6 0.7

I' HORSE POWER

FIG.7 CUTTING BACK THE INNER FACE

OF THE RE-DESIGNED FABRIC SKlRT IN I I

2 INCH STAGES FROM 12 TO 4 INCHES

Page 31: of Flexible Skirts for Hovercraft

16’

IO"

16” LONG, 3* WIDE X 45’ NOZZLE

.

t- IO"

l6”LONG, 2” WIDE X 45’ NOZZLE

. .,

IO”

4S” SHORT PARALLEL NOZZLE, l-33” WIDE

I6

2 45’

\

FIG. 8 CARDBOARD SKIRTS, 16” LONG X 45’ NOZZLES, 3”, 2”i3 1.33” WIDE

Page 32: of Flexible Skirts for Hovercraft

I-0

0.9

0.6

0.7

O-6

0.5

0.4

0.3

0.2

0.1

0

@ t = I.33 INCHES @ t = I.33 INCHES . . t t = = 2.0 2.0 INCHES INCHES A t = 3.0 INCHES A t = 3.0 INCHES

0 I 2 2 3 3 4 4 5 5 6 6 7 7

h/t

FIG. 9 GRAPH OF g L

AGAINST hh FOR CARD

SKIRTS WITH NOZZLE ANGLE OF45*

AND VARYING NOZZLE WIDTHS

Page 33: of Flexible Skirts for Hovercraft

l-6

+ X L - ia INCHi 60 t = 2.0 INCHES

A t = 3.0 INCHES . t = 5.0 INCHES

0 0.1 0.2 0.3 0.4 0.5 0.6

P HORSE - POWER

FIG.10 GRAPH OF CUSHION PRESSURE AGAINST POWER

FOR CARD SKIRTS WITH VARYING NOZZLE WIDTHS

Page 34: of Flexible Skirts for Hovercraft

. 2 INCH FEED SCOT o 5 INCH FEED SLOT A IO INCH FEED SLOT

0.4 0.5 0.6 0.7 0.8 0.9 I-O I-I

'/Lh HORSE POWER / 53 ft EXIT

FIG. II THE EFFECT OF VARYING FEED SLOT WIDTH CARD SKIRT WITH t = I.33 INCHES 8~45~

PARALLEL NOZZLE CLEARANCE HEIGHT =. 2.06 INCHES

Page 35: of Flexible Skirts for Hovercraft

c

:-

Page 36: of Flexible Skirts for Hovercraft

5 R DIAPHRAGMED SKIRTS 5 R CHAIN TYPE SHIRTS ONE IN THIN FABRIC ONE IN THIN FABRIC WlTti CORD TIES ONE IN THICK FABRIC ONE IN THICK FABRIC WITH CHAINS

FIG. 13 SAUNDERS-ROE TYPE SKIRTS

. . I .

Page 37: of Flexible Skirts for Hovercraft

. . . .-

FIG. 14 CONVOLUTED SKIRT-H D L TYPE-60’ INCIDENCE

Page 38: of Flexible Skirts for Hovercraft

PC INCHES WATER GAUGE

-I--

L \ . \ ‘\.

k \

7 Iv

\

\

\

\ \

. .

Page 39: of Flexible Skirts for Hovercraft

.

.

t .Q

4

d. ‘8 \

I

-

. =

-

a - ti ii

Page 40: of Flexible Skirts for Hovercraft

plLh HORSE POWER/ S? ft EXIT

1

FIG.17 COMPARISON OF THE PERFORMANCE OF THE SAME * FABRIC SKIRT COMBINED WITH TWO DIFFERENT

HULL CONFIGURATIONS Pdntad in .@‘hd fw UOT Najasty’s Stotbnwy Office by

, the Roy01 Atnmft Establtshrat, Pamborough. W.lZMRR. K.S.,

Page 41: of Flexible Skirts for Hovercraft

. . .

A.R.C. C.P. NO. 990 Pebntwy 1966

Lester. W.G.S. Kleman, F.T.

629.136.8 I 629.13.ul21a4

629.136.8 I 629.i3.012.124

Lester, W&S. Klcma”. F.T.

A series or Static tests conducted to establish a” erflclent rolp or flexlbl~ skirt ror a peripheral jet type of hw’etcraft Is reported. The importance or deslylng the prlpheral jet system In conjunetlon slth the skirt 1s dernonstrared. The ms”lts su6~eSt that the eflectlve sldth or a rlexlble m,zzIe Is less t,m” its actual rddth and the dischal‘gc coerflclent ~cqulres determini” experlnnfally lo,- each conf iguratlon. It 1s coneluded that skirt conllguratlon perfonmnce 1s best compwed on the basis of power Input to a skirt to ~.“erate a Slve” cushlo” pressure for a speclfled Qyllght c1eammm. The rea1ts co”flrn trat the ski!% 1”p.a pOKeI‘ p-al- unit ex1c a.~, based on dayl@ht clearence and jet length. 1s dlreetly pruportloral to kuahlon pressun)312.

A series or static tests conducted to estahllsh an errlclent folll or rloxlb skirt ror a perlphcrel jet typ or honreraft 1s z.qa’%ed. T%? l.wItB”e~ or desl@“g the prlphsral jet system In con,““ctlo” With tha skllt Is demonstrated. The rrsults s”z&Eest tlmt the erreetlre Width of a rlexlble nozzle 1s la3 than Its .sCCI!al width and the dl.?&aIx* coerridenc requires determining expr1mnta11y r0r each .mri.5umi0n. II 1s ooneluded chat skirt c0nriguration prromm 1s best eomrared on the tmsls 0r pow 1”~ to a skirt to Senexata a Slve” cushlo” pnsrwe rw a spalrled tiyll&ht ClCX=XlCe. The results wnrlm tlmt Lhe skirt input povar per unit exit area, based on dxyll@,t clearance and jet 1-h. 1s dlrntly propo,%lonl to (cushion ~rr~)3’~.

A&C. C.P. No. 993 February 1966

629.136.8 : 629.13.ol2.12Ll

Lester, W.G.S.

Kler”a”, F.T.

Page 42: of Flexible Skirts for Hovercraft

i

Page 43: of Flexible Skirts for Hovercraft
Page 44: of Flexible Skirts for Hovercraft

C.P. No. 990

Q Crown Copyrrght 1968

Published by HER MAJESTY'S STATIONERY OFFICE

To be purchased from 49 High Holborn, London wc.1 423 Oxford Street. London w.1 13A Castle Street. Edmburgh 2

109 St. Mary Street. CarddI Brazennose Street, Manchester 2

50 Fairfax Street. Bristol 1 258-259 Broad Street, BlmGngham 1

7-11 Lmenhall Street, Belfast 2 or through any bookseller

C.P. No. 990 S.O. CODE No. 23-9017-90