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Ttk&& ........ .. ..=fw’ @x ‘~ 7 TECHNICAL NOTES ... . . NATIONAII ADVISORYCOWITTEEFORAERONAUTICS . No.247 t’ I O km rfdtlrnm-j to ihe fifes of thfi ~~flgl~y , Mtmorial Aeronautical FOR REEEZEi& MXWatory ,. Washington Scptemb.er, >926 .. . .— a-. J

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Ttk&&........ ....=fw’@x ‘~7 TECHNICALNOTES

. . . . .

NATIONAIIADVISORYCOWITTEEFORAERONAUTICS.

No.247

t’I O km rfdtlrnm-j to

ihe fifes of thfi ~~flgl~y ,

Mtmorial AeronauticalFOR REEEZEi&MXWatory ,.

WashingtonScptemb.er,>926

.. .

.—

a-. J

.

NATIGNAL

Summary

in ordertobegiaressarchon thedragofairshipsitwas

firstnecessarytor,akea logicaldigestof therepGrtedpast

performancesanddatagivenon decelerationtestsfora large

numberofairships.TY=tthesedata~a:rbecomea~~ailablefor

airshipdes~.gnersina compactformis thepurposeof thisr-

port,as wellas to sezve as thebasis on w’~ichtheauthoris

continuinghisresearches,yhic”nmill‘DegivenlaterinPartII

(TechnicalNoteHo.24S).

Thisdirestas givenhereinPartZ was,begunin Sqtember,........

1923,and‘rorkedon intermittentlyuntilDecember,1325.

Theoutstaildingresultsareas follows:

1. In genexal,themaximumspeedofmostairshipswas.re– _

portefla-oout5 per centhigherthanobte.insdin thisreport.

9U* Totalmaximumhorsepowerwaszeportedinmanycases

higherandina fewcaseslower,thanobtainedin thisreport= r

3. Propulsivecoefficientsat =ximum speed&are in Wn-

erallowert-banthereportedvalues.Coefficient“C’fis con-

N.A.C~A.TechnicalNoteNo.247%

stantandthepropellerefficiency

mum speedthatthepropulsivecoeffi

2

1111E is reducedas at maxi-

cient 1!K!!fallsoff.~.- Itwasfurthernotedthatseveralshipsof widelydif–

fere~tdesigns‘tednearlythesamedragcoefficientforthe.

vholeship. However,thisis lookeduponas a coincidencein

thecaseswherethetypeof hull,cars,andsurfacesdiffered

midely.

5. That

aboutfifteen

ler‘@dshout

in gene~alan idlingprcpellerwasfoundto lhave

squarefeetareaof dragwhilea stoppedpropel-

sixsquarefeeta~eaof .:ra.g.Thiswasfcundby

workingouttheareaofd=agfromtheshipisperformanceand

comparingitwith.theareaofd~agas cbtainedon thedecelera-

tiontestwitheitherstoppedor idlingpropellersas thecase

wasreported.In somecasesthisdifferenceofareaworkedout

tobe 8 or9 sq=re feetperpropeller,but withcertaint~~es :.of enSinesit ispossiblethatall engineswerenot stoppedbut

thatoneor twowereleftidlingduringthedecelerationtests.

Appliedvaluesofprincipledataand resultsare givenin ‘

TableZ andFig.3.

Introduction

At thebeginningof theresearch- “TheDragofAirships!’-

it was immediatelydiscoveredthattherewasmuchconflicting

dataon recordconcerningany givenparticularship. Dccelera-W %iontests had ‘Deenperformedon someship6,yettheresultsof

Y.A.C.A.TechnicalNoteNo.247 3

.

#-

thesetestsdidnotalwaysagreewiththatheldon exactlysimi-

larships.Thereportednm.ximumspeeds,propellerefficiencies,

andmaximum horsepowermauldgivea dragcoefficientthatdif- --

feredwidelyfromthatreportedor foundon thedeceleration

-tests.Or,again,usingthedragcos:ficientfm.rkiondeceler-

ationteststogetherwiththemaximumhorsepowerand reported

maximumspeedwouldinmanycasesgivea propellerefficiency

thatuashighlyimprobable.

A digestby Lipkfs enpiricalmetho~of digestinginconsist-

entd~.tawasappliedto thefoliomfigquantitiessmaxinurnspeed,

maximumtotalhorsepowerjprop-~lsivecoefficicnhat uaxjmum

speed,propc;llerefficienc}-at maximumspee~,areaofdrag

(poner02), anddrapcoefficientforthe-wholeship. This~S

donenotml.yfoxthedatacor.ct?i~i.ng %ch individwdlshipbut

takingintoaccountthsre”!.c.tionbetv”ccrzshipson thetwoquan–

titiesofdragcocfficientend-propCIZ.QTefficicncyUPOnwhich.manyquantitiesd.~,ended.Thenethodof hou thisrelationwas

obtainedisexplain~lfull-yin thee~~lanationof Lipkais method

as givenlaterin thisrepozt.

The reasonsforundertakingthisproblemwasprimarilyto

digesttheresultsalr~adycbtainedin flighton full-sized

shipsso tll’.tt-heres’fitscouldbe usedforfurtherresmrch ..

norkas will be givenlaterinPartII (TethnicalNoteNo.248).

Thescopeof theworkextendsovernearlyall theZeppelin

shipstogetherwithfivctypesof nonrigidairships.Themethod

N.A.c.Ac TechnicalNoteNo.247 ~%

usedisLipka~sempiricalmethodofdigestinginconsistentdata

and is explainedas follows:

Themethodchosenfor~hedigestionof inconsistentdata —

is theinventionof thelateProfessorJosephLipka. It isde-

scribedas the‘Imethodof selectedpoints”iriProfessorLiplka!s

book“GraphicalandMechanicalComputation.ilThisnethodis

fran’kly.axpirical,andhasnot iherigidmathematicaljustifi-

cationof the

ious,and‘has

datavhichis

be givenmore

metkodof leastsq~res,but it is farlesslabor-

thegrec.tadvantageforthepresentproblemthat

kQowntobe especiallyceliablecanarbitrarily

weightthanotherdataof lesscertainaccuracy.

Lip~*Gmethoddoesnotalnaysgiveresultsconverging

to consistency.If thesumof theerxorsisverylarge,each

aPProx~ationS~OWS~cr~sing di~er~cncefromConsistentval– .

Ucs,showingt-hatthedatais toounreliabletobe considered.

Explq.nationof LipkalsEmpiricalMethod

fortheDigestof InconsistentData

Lipkalsempirical~ethodofmakinginconsistentdatacon–

sistentniththetheoreticalmathematicalrelationt-hatexists.

As a stipleexample,Case1:

A rectar@eactuallyexistsas inFig.1. T1--l4

An observerz~nsuresside~[a!landrepo~ts5.1 a=5d=20

k. —[1 If 1! II !Ib!![1 1! 3.9 Fb=q+,II 1! lr a~~a llAlf 1! II 20.11 Fig.1

* N.A.C”A” TechnicalNoteNo.247 5

Thesereportedvalueshavebeenmeasuredperhapsby differ-J entobserversat differenttinesand theaccuracy-of theirdata

isnotknownas yet;forthepurposeof research,letus thers- .foreassumethat ab = A nustholdtrueto four(4)signifi~nt

figures. Thisisanalogousto thereporteddataconcerninga .-..singleairship.Yetwithairships,thereportedvaluesof drag

coefficient,horsepower,naximunspeed,propellerefficiencies

at naximuii speed,andpropulsivecoefficientareinterconnected

by rmthemc-ticalrelationsandwouldonlyserveto complicate

the explanationof ther.lethod.The relationbetweendifferent

ships‘;rill be later explainedanalogoustousingtwo rectangles.

. Reportedvalues :AssumeA andb correct,then a = ~ = 5.146● ,b.

a. 5.1 ,IAssumeA anda co~rect,then b = ~ = 3.943

b = 3.9 .,+ A= 20.11 : Assumea andb correct,then A = ab =.. 5.1X 3.9= 19.89

,b!

Thesemlues of a,b, andA are theMt approximation:

1stapproximation:Reporteda =’ 5.1●

a = 5.146 ~ 1stapprox.a = ~b= 3.943 : 2:10.246A = 19.89 : 54123= 1stmeanvalueofa

Reportedb = 3.901stapprox.b = 3.S43

2: 7.8433.922= 1stmeanvalueofb

ReportedA = 20.111stapprox.A = 19.89—.

2:40,0020.GO= 1st mean valueofA

-kN.A.~”A-TechnicalNoteNo.247 6

Testforconsistencyab = 5.123X 3.922= 20.092= A, calculated“4 value. -.

lstneanvalueof A.. .O . . ..-. =20>00.092

..-.

Consistentto onlythreesignificantfigures.

Nowconsidertheseraear~valuesas newreportedvaluesandcon–

tinuetheprocessto thesecondapproximation.

Similartonetho&of firstapproximation:

.

i’

a = 1staeanA = 20s001st meanb 3.922= a, 2d approx.= 5.099

A = {Z.stmeana) (lstmeanb) = 5.123X 3.922= 20.092= A,2d appro~.

(Checlzfor consisten~y,A= 5.099X 3*903= 190901*)

Lastncanvalue

2d approx.“

2d m@n II

Xeanvalue=

b =2dlXea?lA=2d meana

A = (2C!meana)

La,stmeanvalue

3d aqprox.‘~

3d,aem 1!

20.0465.Ill= 3.922= b, 3d “

(2dmeanb) = 5*111 X 3.908

a b A5.111 3.908 20.046

5.129 3.922 19.9737

5.120 3*~15 20.0098

= 19.9737= A,3d approx.

N.A.c.A” TechnicalEoteYo.247 7

b= 3&meanA = 20.oG98= 3 908= b 4tn ‘f3dmeana ~“ >

A= (3dmeana) (3dme-anb) = 5.120X 3.93.5= 20.0448= A,4thap-prox=(Checkfor consistency, 5.111X 3.9C?8= 19.9738.)

a b ALastmean value 5.120 3.915 20,C098

4thapprox.II 5.111 3.308 20,0448

4thmean ~’ 5.115 3,932 20.0273

4thmeanA s 2~:~~;3= 5.119a= —— = a, 5thapprox.4thmeanb

~thmeanA 20.@273_b _— = 3.915= a, 5th “= 4thmeana 5.115

A= (4thmeana) (4thnem b) =‘5-Z15X 3=912= 2°~~~9~~r~~.20.040s.) —‘Checkfor consistency( 5.119x 3.215=

a b ALastm~.nvalue 5.115 3.912 20SW73

5thapprox.“ 5“119 3*915 20.0998

5thmean l! 5.117 3.914 20*o1185

~t~m-n A = 20.01E15a = 5.114= 6thapprox., a= 5ihmeanb 3.914

.

– 5t~.tieanA= 2~.~1~5b— —— = 3.912= 6thapprox~,b5tnmeana ● “

A= (5thmeana) (5th‘-n b) = 5=217x 30g1& ::;:;:,=A

(Checkfor consistency,5.114X 3=912= 20.0059=)

a b ALastman value 5●117 3.914 20.0185

6thayprox.“ 5.114 3.912 20.0279,m

6thmean 1’ 5.1155 3.913 20.0237

N.A.C-ADTec~fi .NOteNo. 247

. GthmeanA . 20._o&3zs 5.1170= a, 7thapp~ox=a ~thmeanb 3.913

6thm-n ~ = 20.02S7= 3.9143= b, 7~~ 1!b= 6thman b

5a~~55,20.olw=

A = (6th~ealla) (6thmeanb) = 5“1155x 3‘913A:7thapp~~x.

(Checkfor cmsistency,5.117X 3.9143=20.0294.)

a b A

5.1162 3.91S6 20.0203Last~lean~a~ue

8thapproxa“ ~.1155 3.s131 20.02276

The

—-

8thman “ E.1M8 5.9134 20.02153

gthappro~=

8thmean~ = ~~og~152= 3.9136= “o,9th1!

-D= 8thmesaa —50~158 ..”.20.02017=

A= (8thneana) (athn-n b, = 50Z1W ‘“3“g1~ ‘gthapprox.

(Checkforconsis~~ency,5.1161X 3.S136=20,0~236.)

Consistencyexiststo four(4}sigaifigantfi~resm

desixedvaluesarethentakenfromthe9thapproxtiationas

= 5.116;b = 3=914;..A.f0210ws: a .= 20.02;

as check,ab = A = 5.116X 3.914= 20.0240.

.-

Case 2.

Nowletus consideras

exist,as fOllol.vs:

h~=4I

al=6 Al = 24

I-J

247 9

exampletworectanglesw-nichactuall~;-.

Fig.2

I\A2= 19.5Ii

.-

a2=5

It }sknown(letus say)thathumanendeavortriedtomakeside

bz = sideb2.“Thisisanalogousto twotypesof shipsbuilt

sayin thesameyear,withr.o apparentadvancementin theartof

. propellerLesignc~~passcd to -t-heshipsjustbeforeandjust

afterthebuildingof tkese twoships. It thenis safeto say &_thatthese-two ships-wouldh~veas faza.sis knownthesanepro-

4pellerefficiencies.Cr.thisrelationthatside b~ = sideb=

thefollowingwillbe workedout:

Therepcrt6dvaluesare .

istrectangle 2d rectangle Mathermticalrelationsin thiscase

bz = 3.95 ba = 3=99 al’02= .42

~z= 6.08 a2 = 4.94 a2b2 = Aa.A~ = 24.95 A. = 19.80 h~ = b2

f/

.

4

.

N..\.C’1~*Tcc.ki@l~OtcNo.247 10

ered

Asstiingconsistencyto threesignificantfiguresis consid-

sufficient.?roceedLsimilsrlyto Case1.

b+= Igoac)——- = 4..OG8= b=,4.94 1st !l

Al = ZI ‘~ = 6.08X 3.95= 24.016= AZ, Istapprox.

ITOWuonsitie~therelationbl = bz :

-b1> 1sta-pprox.= 3.955 -.

b H 1[29 = 4.~Q8 ,-..

+-

(ZT.anvalue j CELI. = 3.982tobe a~:eragedintothemeanvalues.

Lestman (inthiscasereporteddata):.21 bl L$-l % % 4?

Lastnean 6.08 3.95 24.05 4*94 3.99. 19.80

1stapprox. 6.CM8 3.955 24.016 4.952 4,008 19.710

(c.eanval’le)cal. 3.982 3.382

1stman value 6.084 3.962 24.033 4.951 3.993 19.755

It is tobe notedthattheasmmptionthat ~ = k based.

on hunanendeavoris givenequalweightwithreporteddataand

hencee-ntersthe~eanvalueonlyonce,havingthusone-ttiirdef-,“

feet on themeanvaluesof bl andbz* However,if (inthecase

N.A.C.A.TechnicalNoteNo.247 11w

O.fships)2 certaindata,sayaE3obtainedfromdeceleration

.-

-tests

4 is acsucd.to be highlycorrect,thiscanbe givengreaterweight __

by averagingit ona weightedmeanprinciple.On shipswherethe _

decelerationdatalookedreasona’oleit wasgiventhreetinesthe

weightof otherrepel-tcdvaluesandwasaveragedin on eachap-

proximation,therebyforcingthedependentvariablesto closely

conforuto theactualdecelerationtest. To continuethecase

at hand-

Checkforconsistency:

(a,,1stapprox.)(3:, 1stapprox.)R 6.038X3.355y 2~a078

(%, II II )(%, 1’ “ ) = 4.962X4.008 = 19.887

Cornpared,,againstthemeanvalues;f

Z4*033

19.755

1stmeanAl ~4,033= 6.065 = al, 2d approx=

lst’meanbl= 3-962. ...

1stmeanAl ~~.033—= 3.950== 6.084

bl, 2d 11l.stneanal

(lst r~ean al)(lst mean bl)= 6.084 X 3.9:2 = 24.1048=I,.2d~pprox.

IstmeanAs 19.755= 4.947= aa, 2d approx= “

1stmeanbz = 3.993

1st neailAa 19.7!55— = 3.990= bz, 2d “

1stmeanaa = 4=951 ....

(lstmeana~)(lstmeanba)= 4.951X 3.S93= 19.7693= --AZ,2d ELpprOX-

4N.A.C.A.TechuicalNoteNo.247 12

4Checkforcons.istencj~; . . ,. .,

(al,2d approx.)(b.,2d approx.),=At=6.065X 3-?~W3-956~,

(aa,2d 1’ )(52,2d “ ) = Jlz=4.947X 3.990=19.738=,.

as comparedab=instAl = 24=10~8 b~,2d approx.= 3m950

AZ = 19.7693 ba,2d 1’ = 3.990mean= 3.970

bl k ba-‘1 -1 a~ &Lastman 6.:84 3.962 24.G33 4.951 3.993 19.755.

2d a-pprox.6.065 5.950 24.1048 4.947 3.990 19.7693

Mmulvalueofbl&& 3.970 5.970

2d ncan 6.074 3.961 24.0689 .4.949 3.984 19s7622

.2dmeanAl 24.0689: 6 ~764

al=-.2CLrmanal = 3.951 “= cl> 3d approx.

.

bl = 2d EleanAI= 24.0G59= 3096~6= bl 3d II2dneanal ?.074 > ..

Al = (2dmeanal)(25ntiznbl).= 6.074X 3.961= 24.0591= Al,3d ZLppTOys

2d meanAZ%!=

= 19.7622= 496032d neanba

= aa, 3d approx.3.984 “

bz =2dmeanAa = 19.7622‘= 3.9931= ba, 3d IIZd tieanaa 4.949

A= (2dmeanaa)(2dmeanb,)= 4.949X3,984= 19.7168=A~,3d appr~x,Checkfor~onsistency: .. .. ..

(al,3d approx.)(b~, 3d approx.)=A1=6.0764X3.9626=24.0783

(%, “ “ )(~, I* II )=A2=4.9603X3.9931=19.8069.+

as comparetlaLaMst

13

Al = 24.0591

4Aa ==19.7168.

b1>2d approx.= 3.9626

b 11 II2> = 3.9931

mean = 3.9??8al bz A3 % bz AZ

Lastmean 5.(j74 3.961 24. om9 4.9’49 S.984 19. ‘7622

3d approx. ~.0764 309&6 24,05314>9603 3<993 19.7168

meanvaluebl & ba 3.9778 3.Z778 ‘ “3dmean 6.0752 3.9571 24.~5404.9546 3.9$34919.7395

X!.meanAl 24.~64~% ‘>- = 6.~558= al,

= 3.9671 4thapprox.OQ meanbl

bl = 3dmeanAl = 24.0640= 3.9510 = bl,b.~7~2 4th “Sdmeanal ‘“ .,

AZ = (W. meanaa)(Zdmeanb,)==4.9546X3.9849=19 .7436 = A.,4thapp~~x.

bheckfor consistency: .,.

(al,~thapprox.)(b.,4thapprox.)=AZ=6.0658X3.9610=24.0266(a2, II II )(ba, “ “ )=A,=4.9535x3.984&13.7347

acj apjainst.i .“ .-

A1 = 24 ●1009.,,

....~<1 ...,

.. -----

N..4.C..!!..TechnicalNoteHo.247* 14

It isseenthctrect2nqle1{0.2 hasreachedconsistencyto

4 threesignificantfigure~as specified,whicharefor engineer-

ingpurpo~es.-—.

aa= 4.95 b 3.S3‘Az13.7,“

Forch~ck4.95X 3,98= ~9.71310

Thw thevalueof ba = 3.98 canbe averagedintothenext

approxtiatim,thesa~eas theweanof bl and ba wasformer–

ly. Theilextapproximationneedonlybe carriedouton rectangle

No. 1.-

Thus:

Lastaean = 6.0752 3.96’71

4thapprox.= 6.0658 3.9610

ba = 3.98

~thn~an = 6.0?’25 3.9649

al = A 4th ~e~n _ 24.~~25 = 6.0670b 4thK,e~- 3.9594

24.0825

= ~1> 5thapprox.

Al = (4thneana:)(4ti~meanbl)= 6.0705x3.9694=24.0962=Aa,5thap rox.

7Checkfor consistency(al, 5thapprox.)(bl,5thapprox.-=6.067X3.9671=24.068.

It is seen‘~hatrectangleNo. 1 ti2sreaclmd.consistencyto three

“ significantfig’~resas specifiedwhichareforengineeringpur- _

poses.

al = 6.07 bl ==3.37 Al = 24.09 cr 24.1for3 figurer

2hGCk6.07x 3.97= 24.C979r

.

*

i?.A.C.A.TechnicalNoteNo.247 “ 15

It isherewelltonotethatalthoughhumanendeavortried

tomake bl = bz itwasso tempered.by thereportedvaluesof

1)~and ba thattheyneverdid

finalvaluesbl = 3.97 and bz

So itcanbe seenthateven

thatthepropellerefficiencyof

anothez,theydo notnecessarily

quiteequaleachothez.ThUS

= 3.99.

thoughan assumptionwasmade

oneshipis equal to t-atof,in thefinalvaluesequaleach

otherunlessthereporteddataagreescloseenoughtomakeit —Soo

● The interconnectingquantitiesbetweenshipswhereno data

we~availablewerepropellerefficaciesanddragcoefficients.

Thedataobtainedby directobserr~tionaremaximumspeed

andhorsepower;dragcoefficient(withdeador $dlingpropellers

as wasthecaseat thegivendecelerationtest).

Thedatacalculatedfromobserveddataaredragcoefficient

withengines‘havingnoprcpellczdrag,propellerefficiency,

maximumspeedandpropulsive

Thedataobtainedwhere

wereto consi&eras reported

betweentheshipsbuiltjust

finenessratio,typeof cars

coefficient.

no decelerationtesthadbeenrun

dataa dragcoefficientthatlay .beforeandafterwithdue regardtO.

and surfaces,contoursof hull,etc.

Thisassumeddragcoefficientwasforcedby IJipka~smethodto

varyifnecessaryto accommodatethedragcoefficientas calcu-

latedfronmaximumspeed,hors~~owerandpropellerefficiency

or fromareaof drag. Likewise,in shipswherepropellereffic’i- ,

,. .

N.A.C.A.TechnicalNoteHo.247 16.

.

*

endywasnotknownby anydata,it wasassumedas betweenthe

shipson eithersideof it. Thiscouldnotbe muchin error.as

propellerefficiencyat maximumspeedwasalmosta centinucus

fw.no’tiion. Thenagaintheareaofdragas foundfor shipson’

whichdecelerationtestMd beenrun,wasseentobe nearlya

centinuousfunctionfmm onedesignto anothez.So wherercport-

C3datancrcnissing(twocasesonly)tncsca~sumptionswere

made,

Greatweightwas given to thedxagcoefficientsandpropel-

ler efficienciesas obtainedfroman actualknowndeceleration

test. Thiswasdoneby averagingthisobserveddatain oneach

successivemeanvalue;therebyforcfilgthe conflictingreported

datato conformto thedecelerationtestdata. In sonecases

twodecelerationtcctso: thesaneshipwerefoundand theydif- .

feredindragcoefficientandpropellerefficiencies.Insuch

casesan averagevaluewasusedforthe initialreporteddata= . _.

Afterthefifthapproxirntiontherelativevalueof ~ch q~n~itY ._._

comparedto thesamevalueof shipson eachsideof itwasnain-

taincdby avora.gingin thisinterpolatedvalueofdragcoeffici-

entandpropellerefficiency.Thesetwoquantitiesdetcrnincd

all therestforeachindividualshipso gavetwicethen~ber . ..

of calculatedvaluesforquantities.Thus, ona particularship

a valueofdragcoefficientwouldbe arrivedat fromthedata

pertainingto thatparticularship’andanothervalueof itsdrag

co~ffici.ent~O~l&be arrivedat by its relation to theship~S

. ~~~~.C*A.TechnicalNote?iOo247

1!ita~-:Gllon eachsideof it,whichanounts

i portedobserveddata(givinggreatweight

17

to this:digestall re-

todecelerationtests}

forfiveapproximations,thencalculatetherelativevaluesof

sinilarquantitiesbetweeneaohitenin succession.Thenon each

successiveapproximation,averagein to itsmeanthe interpolated

valuesofdragcoefficientsandpropellerefficiencies.Thusthe .—relativevaluesof quantitieswouldhavenearlythemme relation

betweenshipsas foundto existon thefifthapproximationand

wouldbe foundto existin thefinalanafiysis.

BodyofReport

.

Preliminarycalculationsof data,and empixicaldigestof

reportedanddecelerationtestdatato obtzinconsistentvalues

of allnecessaryquantities.

*Liplatsenpiricalnethodwasused. Thismethod,as ex-

plainedin theintroduction,gi~e~consistentresultsby chang-

ingvaluestlmtlieoffther.eanby arbitrarilyuoving(byaver-

aging)theulmlfwayto thatMeanandthencalculatingthede-

.

~ pendentvariables.ThisJmsdoneforsixdependentquantities:

r:laxitnu.1airs~eed,horsepowerat naximumspeed,propulsivecoef-

ficientat~aximumspeed,-nropellerefficiencyat naximumspe~sd,

areaof drag,andwholeship’sdragcoefficient.

Itwa~foundthatthedatathoughtreliableoftenr~oved

slightlyas itwasnotalwaysconsistent.

N.A.CDA.Tcchni.calNoteNO.247 18.

4

.

Prclininaryapproxiuat~cc.lculationsweremadeon therela–

tivetotaldLr~g of eachship,itsapproximateskinfriction,re-

sistanceof thebarehull,etc. Thiswasdonepurelyto geta

convenientarrangementof theships,andnotintendedtobe the

basisfo~thesubdivisionof a ship;s dragintoitscomponent

parts,asbarehullresistanceand skinfrictionare onlyvery

approxtitc. Part11 (TechnicalNoteNo.248)dealsentirely

witht“ncsubdivisionof thedragofairships. -.—

ThequantityS = IIcharacteristiclength[’withpoweronand

poweroff, was carriedalongthroughthreeapproximations

primarilyto givea moreaccuratestart tothesystemofapprox- ._

imatione.

Consistentres-~ltswereobtainedin elevenapproximations —

whenrtostquantitiesshcmd a rapidlyconvergingscriosof their.

differenceswiththepreviousapproxizz.ation,andthedifferences

yet tobe sosaallas-toshowsucha mall rmclericalthan.=in

thedepcndontquantitiest’hatthoIiaitsof theseserieswere

takenas thefinalconsistentvalues.Thefinalvalueswere

thencheckedagainst

tions (SeeTablesI

Thejustifice,tion

eachotkcrby theforiulasof theirrcl&-

toVIIIgivenat theendof report).

Asstmptions

forth~relationsbetweenshipsisbased

Theartofpropellerdesi~nforairships ._L

s-nowcdnearlya continuousfunctionoverthetime. The!propel-.

. U-A.C.A,Teclhni.calNoteNo.247 19

lerefficienciesgaveseveralpointson thisfunction.It then

“+ was safetoassumethatthepropellerefficiencyof a shipon

.whichno decelerationdataoouldbe foundwasbetween-Thatob- -----

tainedon theshipsbeforeand theshipsafter. Thisassumed

propellerefficiencywasgivenequalweightwithreported(not

decelerationtestdata)dataon thefirstapproximateion. The

samewasdoneforwholeship?sdragcocfficienton theships

no decelerationtestc ‘hadbeenran,taklinginto.accounttype

hull,volue, typeof cars,surfaces,etc., and so,in fact,

becamean

thefirst

Each

interpolatedvalueof thedragcoefficientforuse

approximation.

where

of

it

on

ship$s datawerethenrunindependentlyof otherships

forfivcapproximations,giving~reaterweighttodeceleration

tcstdatawhe~eavailchlc.At theendof thefifthapproxima-

tionthevaluesof C and E werecomparedto theitemson each

sideof itandthisrelativepositionwaskeptby averagingin

these.,newinterpolatedvaluesonalltheapproximationsthat

follom.

. 1{.A.C.A.TechnicalNoteNo. 247 20

Sym’bOlsand DefinitionsUsedinPazt14 d

L,

= Lengthof shipin feet.

w = Airspeedinft./3ec.

umax.= Ai~speedat fullthrottleall engines.

A = Kaximm crosF sectional Zreain sq.ft.

—.

k = Cylindricalcocfficient..

x= EiGtar.ce fromnosetomax+imumdiareeter in feet.. x Alt30usedto indicatet-ypeof seriesas in X,~,~.....O.

—.r Uaxifi.umrcbtl,iuaof hullinfeet.

e = Zccentriaityofnoseellipse.b.4~ = Tot~lsurf~ceazeaof h-ullin sq.ft.

S.F.= SkinfriCtiGn.

Kp = Approx.dragcoef. 1duetopresmredifference.U~e&or~yin fir~t

Ks = l! 11 II II II skin :Ziction●

1

approxi-r.ations.

K = II II. II II 11 hl.11~.

K= Fropulsivecoefficientinl.z.st approximationsandfinalfiumarie~.

PO = PullTatedhorsepower.

T = A ternt’hatapproache~propellerefficiencyE.● .-.

E = Propellerefficiencyforwi~oleship.

.

. R.A. C*A.TechnicalNoteNo.,247 21

Emax.= propellerefficiencywith Wmax.and~~max”

* P = Densityof theair;consistentlyusedas a constantof.00237sWgs/c-u>ft.

I$J . Tfi&ualvolume

s= Characteristic

Sp = II

in.cuoft.

lengthinfeet.II with poweron in feet,.

A= .4rcaof draginSq.ft.

~p ~ H II II with pcnvezon infeet.

c = D~a&,coefficientof wholeshipinabsoluteunits.

Note.-Subscriptnumeralsdenotethem],a’aezof theapproximation.

Pximcs(as K’,K\’,W’)” “ II II 1! H

in thefirstfewapproximations. —

Wherethereareanyapproximationsona sheet,thewhole

6heetislabeled“Prelim.tnary Calculations%”Thisisto

preventmisuseof thisarticle.

FinalresultsofPartI aresummarizedonPage3.

* }T.A.C.A,TechnicalNoteNo.247

Formulas

HP. P )( ?~ol.2’3V3available= cx~ 550z

HP.r =

E

K

Ap

Ap

c.

c

c

K

Ap

Horsepowerusefulinlineof fliglht.

-HP.* SD-d

‘available =Q HP.available2/3 2/3

Propulsivecoeff.= ~ = 2E(1”01-) = p V3(VQ1Ap 550+.r

Areaof dragwithpoweron (sq.ft.).

Draginpounds P = slups/’cu.ft.p ~2 v = ft.,?sec. .

2 Ap = Sq.ft.

Dragcoefficiei~t(absoluteunits).

gr~,g “iIl -p CKl?ds.=K; vyvol.)2”3

T?M= virtialvolumein cu,ft.. Vol,+ N.3

ST) (r = max. radiusof crosssection).Sp = characteristiclength,poweron (ft.).

.—

.-.

. .2VM

‘poweroff= ‘powerofffoundfrondecelerationcurve..● ‘poweroff

Ap - Aponeroff= Areaofdrag,dueto idlepropellers.

P = .00237 slugs/cu.ft.(Allforegoingdatabasedon theu standarddensityof air.)

. N.A.C.A.

v

D

.HF.*

T~chnicalNoteNo, 247

Formulas(Cont.)

Velocity;alr,speed.inft./see.

HP.X2X55-OXE (HI?.= Max.EP.available.)c g (701.)2i3 (E = PzopoEff.at v~ax.

andEP.max.).,.,.,,... . .

w ft./see.D = pounds

@t=d-o &- ‘s=characteristicieng~fl);

-t‘poweroff= *_ ~ (7Tom slopeof$ plotted

V. -J . L t duringdecele~~%;;fi~est.)

.

Conclusion

.

.

1—-* Theconsistentvaluesobtainedin thebody

portandgivenagainin theSummarymustbe usedin

24

of thisre–

theligiltOf

themethodby whichtheywereobtained.ThilS, itmustbe real– —

izcdt“=tthenet errozsen rcpoctcddatacomparedtowhatactu-

allyexists,arepm-xitedaroundand that~rrorsin deceleration

testdataarelikmjsepro–rzztc~arounduntilconsistencyis ob-

tained.It cantkenbe saidthatthe~alueshereinobtainedare

theprobablerelat:vevaluesandttus:ordcsigmand research

purposescanbe c~rl~~d~r~d as a digestof past

decelerationdata.

?d. partII (T.1~.IYo.24S)dealswiththe

performance

subdivision

Emd

of

theDragofAirshipsandthisworkpresents(bytheauthor)the

pointofpreliminarycalculationsanda first VL curvefor

fullsizeb~l”eairshipb.ullsc

3. Therangeofapplicationof thedataobtainedinPartI

c~mnotIogicaIlybe appliedto ilewdesignsthatarenotnarlY

similartoairshipsfromwhichthosedatawereobtained.Ho’i7-

Cvcr> on thejud~entof thedesi.~.er,certainq~ntitiessuch .+

as d~~gcocfftcientandpropellerefficiencymaybe usedfor

shipsoflargervolumes,theaccuracyof theresultswilllarge-

ly dependon theassumptions~,ade.Part11 (?.N.No.248)en-

deavorstodevisea methodof calculatingquantitiesconcernin~

a newdesign.

K..4.C.A+TechnicalNoteNo. 247-

“\References

● N.A.C.A.TechnicalMemorandumNo.237*’-by FriedrichStahl,November,1923.

N.A,C...4.TechnicalReportNo.117- I’TheAirships!!by MaxM. Lti.nk,1S21.

N.A.CaA,Technical~e~ortNo.184- “The

25

“RigidAirships”

Dragof Zeppelin ..—-

Aerod~@amicForcesinAirshipEullsi’by KaxM. M-uk,1924. - -.

N.A*C.A.TechnicalNoteito.194-‘;AMethodofDeterminingtheDimensions~ndHorse-powerofan AirshipforanyGivenPerformance1~by G. P. Burgess,1924.

BureauofAeronautics(U.S.Navy)DcsigmMemosNos.30,41,~~,44and47,by C.p. ~~~~ess. .

VariousPapersby Prandtl,Furmanj31asiusandS’@nton. ..

U.S.NavyBu. Cl.&’R.BulletinITo.101,Dec.1919.

llThcRigidAirship,ZR-3[[by C.P. Burgess,publishedin. JournalA.S.N~tis,~ovembe~,1924.

ReportsonAirshipUodels,by ~iffel,1918.

ClassroomNotesfrcxnProfessorsE. P. Warnerand Lipka,Kass. Instituteof

Inadditiontodataand

‘s ‘followingdataobtainedfrom*

Tcchnolo~.

formulastaken

Germanscurces

fromtheabove,the

sireconsidered.

(Wheredataformorethanoneshipin an itemww given,theav-

erageis tabulatedhere.)

*

* N..’,A.A.Technical 26

AdditionalReportedDataI 1

9 i Air Dist.max.Prop.Prop.1DragIter~VolurlcOyd.from Coef.Eff\ I.Coef.

Nose I] at. .

~ length I~.ax., Cu.ft. Klz C*

a; 17● 50 16~361

9 I 572000 25.80 20 I

I28I.05610 I 23.62 16 33 ~.C4411 ! 25.00 19 66 ;.G71121 24.61 ~ 2613 ! 22.40 ; i9

59 1.052. 57 1.048

14 I858000, 22.19 24 55 I.J055

24I

I9 30.80 i 59 65 .02025 2400000I 24.40 56 65 ●020

Remarks —

Forr.ulaC = ~ doe= .notalwaysholdtruewiththisdata.

Cn thisiteu,datastatesskinfric$ion= 82%hulldrag. —.—

Ingenexalthisdataconflictswiththatgivenin therefer-ences. It is thusconsideredas reporteddata.

A statement‘intheabovereporteddata,thatskinfriction~constantX V-*047=fiefhulldrag(~he~eV=\-oUme of hull)isnotconsistentwithCiatareported,for.ita22.

*FOTwholeship,

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