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wheel¡¡at¡¡certain¡¡speeds¡£



A¡¡TANGENT¡£When¡¡an¡¡object¡¡is¡¡thrown¡¡horizontally

the¡¡line¡¡of¡¡flight¡¡is¡¡tangential¡¡to¡¡the¡¡earth£»

or¡¡at¡¡right¡¡angles¡¡to¡¡the¡¡force¡¡of¡¡gravity¡£¡¡Such

a¡¡course¡¡in¡¡a¡¡flying¡¡machine¡¡finds¡¡less¡¡resistance

than¡¡if¡¡it¡¡should¡¡be¡¡projected¡¡upwardly£»¡¡or¡¡directly

opposite¡¡the¡¡centripetal¡¡pull¡£



_Fig¡¡1¡£¡¡Tangential¡¡Flight_



TANGENTIAL¡¡MOTION¡¡REPRESENTS¡¡CENTRIFUGAL

PULL¡£A¡¡tangential¡¡motion£»¡¡or¡¡a¡¡horizontal

movement£»¡¡seeks¡¡to¡¡move¡¡matter¡¡away¡¡from¡¡the

center¡¡of¡¡the¡¡earth£»¡¡and¡¡any¡¡force¡¡which¡¡imparts

a¡¡horizontal¡¡motion¡¡to¡¡an¡¡object¡¡exerts¡¡a¡¡centrifugal

pull¡¡for¡¡that¡¡reason¡£



In¡¡Fig¡£¡¡1£»¡¡let¡¡A¡¡represent¡¡the¡¡surface¡¡of¡¡the

earth£»¡¡B¡¡the¡¡starting¡¡point¡¡of¡¡the¡¡flight¡¡of¡¡an¡¡object£»

and¡¡C¡¡the¡¡line¡¡of¡¡flight¡£¡¡That¡¡represents¡¡a

tangential¡¡line¡£¡¡For¡¡the¡¡purpose¡¡of¡¡explaining

the¡¡phenomena¡¡of¡¡tangential¡¡flight£»¡¡we¡¡will¡¡assume

that¡¡the¡¡missile¡¡was¡¡projected¡¡with¡¡a¡¡sufficient

force¡¡to¡¡reach¡¡the¡¡vertical¡¡point¡¡D£»¡¡which

is¡¡4000¡¡miles¡¡from¡¡the¡¡starting¡¡point¡¡B¡£



In¡¡such¡¡a¡¡case¡¡it¡¡would¡¡now¡¡be¡¡over¡¡5500¡¡miles

from¡¡the¡¡center¡¡of¡¡the¡¡earth£»¡¡and¡¡the¡¡centrifugal

pull¡¡would¡¡be¡¡decreased¡¡to¡¡such¡¡an¡¡extent¡¡that¡¡the

ball¡¡would¡¡go¡¡on¡¡and¡¡on¡¡until¡¡it¡¡came¡¡within¡¡the

sphere¡¡of¡¡influence¡¡from¡¡some¡¡other¡¡celestial

body¡£



EQUALIZING¡¡THE¡¡TWO¡¡MOTIONS¡£But¡¡now¡¡let¡¡us

assume¡¡that¡¡the¡¡line¡¡of¡¡flight¡¡is¡¡like¡¡that¡¡shown

at¡¡E£»¡¡in¡¡Fig¡£¡¡2£»¡¡where¡¡it¡¡travels¡¡along¡¡parallel

with¡¡the¡¡surface¡¡of¡¡the¡¡earth¡£¡¡In¡¡this¡¡case¡¡the

force¡¡of¡¡the¡¡ball¡¡equals¡¡the¡¡centripetal¡¡pull£»or£»

to¡¡put¡¡it¡¡differently£»¡¡the¡¡centrifugal¡¡equals¡¡the

gravitational¡¡pull¡£



The¡¡constant¡¡tendency¡¡of¡¡the¡¡ball¡¡to¡¡fly¡¡off¡¡at

a¡¡tangent£»¡¡and¡¡the¡¡equally¡¡powerful¡¡pull¡¡of

gravity¡¡acting¡¡against¡¡each¡¡other£»¡¡produce¡¡a

motion¡¡which¡¡is¡¡like¡¡that¡¡of¡¡the¡¡earth£»¡¡revolving

around¡¡the¡¡sun¡¡once¡¡every¡¡three¡¡hundred¡¡and

sixty¡­five¡¡days¡£



It¡¡is¡¡a¡¡curious¡¡thing¡¡that¡¡neither¡¡Langley£»¡¡nor

any¡¡of¡¡the¡¡scientists£»¡¡in¡¡treating¡¡of¡¡the¡¡matter¡¡of

flight£»¡¡have¡¡taken¡¡into¡¡consideration¡¡this¡¡quality

of¡¡momentum£»¡¡in¡¡their¡¡calculations¡¡of¡¡the¡¡elements

of¡¡flight¡£



_Fig¡£¡¡2¡¡Horizontal¡¡Flight_



All¡¡have¡¡treated¡¡the¡¡subject¡¡as¡¡though¡¡the

whole¡¡problem¡¡rested¡¡on¡¡the¡¡angle¡¡at¡¡which¡¡the

planes¡¡were¡¡placed¡£¡¡At¡¡45¡¡degrees¡¡the¡¡lift¡¡and

drift¡¡are¡¡assumed¡¡to¡¡be¡¡equal¡£



LIFT¡¡AND¡¡DRIFT¡£The¡¡terms¡¡should¡¡be¡¡explained£»

in¡¡view¡¡of¡¡the¡¡frequent¡¡allusion¡¡which

will¡¡be¡¡made¡¡to¡¡the¡¡terms¡¡hereinafter¡£¡¡Lift

is¡¡the¡¡word¡¡employed¡¡to¡¡indicate¡¡the¡¡amount

which¡¡a¡¡plane¡¡surface¡¡will¡¡support¡¡while¡¡in¡¡flight¡£

Drift¡¡is¡¡the¡¡term¡¡used¡¡to¡¡indicate¡¡the¡¡resistance

which¡¡is¡¡offered¡¡to¡¡a¡¡plane¡¡moving¡¡forwardly

against¡¡the¡¡atmosphere¡£



_Fig¡£¡¡3¡£¡¡Lift¡¡and¡¡Drift_



In¡¡Fig¡£¡¡3¡¡the¡¡plane¡¡A¡¡is¡¡assumed¡¡to¡¡be¡¡moving

forwardly¡¡in¡¡the¡¡direction¡¡of¡¡the¡¡arrow¡¡B¡£¡¡This

indicates¡¡the¡¡resistance¡£¡¡The¡¡vertical¡¡arrow¡¡C

shows¡¡the¡¡direction¡¡of¡¡lift£»¡¡which¡¡is¡¡the¡¡weight

held¡¡up¡¡by¡¡the¡¡plane¡£



NORMAL¡¡PRESSURE¡£Now¡¡there¡¡is¡¡another¡¡term

much¡¡used¡¡which¡¡needs¡¡explanation£»¡¡and¡¡that¡¡is

normal¡¡pressure¡£¡¡A¡¡pressure¡¡of¡¡this¡¡kind

against¡¡a¡¡plane¡¡is¡¡where¡¡the¡¡wind¡¡strikes¡¡it¡¡at

right¡¡angles¡£¡¡This¡¡is¡¡illustrated¡¡in¡¡Fig¡£¡¡4£»¡¡in

which¡¡the¡¡plane¡¡is¡¡shown¡¡with¡¡the¡¡wind¡¡striking

it¡¡squarely¡£



It¡¡is¡¡obvious¡¡that¡¡the¡¡wind¡¡will¡¡exert¡¡a¡¡greater

force¡¡against¡¡a¡¡plane¡¡when¡¡at¡¡its¡¡normal¡£¡¡On¡¡the

other¡¡hand£»¡¡the¡¡least¡¡pressure¡¡against¡¡a¡¡plane¡¡is

when¡¡it¡¡is¡¡in¡¡a¡¡horizontal¡¡position£»¡¡because¡¡then

the¡¡wind¡¡has¡¡no¡¡force¡¡against¡¡the¡¡surfaces£»¡¡and

the¡¡only¡¡effect¡¡on¡¡the¡¡drift¡¡is¡¡that¡¡which¡¡takes

place¡¡when¡¡the¡¡wind¡¡strikes¡¡its¡¡forward¡¡edge¡£



_Fig¡£¡¡4¡£¡¡Normal¡¡Air¡¡Pressure_



_Fig¡£¡¡5¡£¡¡Edge¡¡Resistance_





HEAD¡¡RESISTANCE¡£Fig¡£¡¡5¡¡shows¡¡such¡¡a¡¡plane£»

the¡¡only¡¡resistance¡¡being¡¡the¡¡thickness¡¡of¡¡the

plane¡¡as¡¡at¡¡A¡£¡¡This¡¡is¡¡called¡¡head¡¡resistance£»

and¡¡on¡¡this¡¡subject¡¡there¡¡has¡¡been¡¡much¡¡controversy£»

and¡¡many¡¡theories£»¡¡which¡¡will¡¡be¡¡considered

under¡¡the¡¡proper¡¡headings¡£



If¡¡a¡¡plane¡¡is¡¡placed¡¡at¡¡an¡¡angle¡¡of¡¡45¡¡degrees

the¡¡lift¡¡and¡¡the¡¡drift¡¡are¡¡the¡¡same£»¡¡assumedly£»¡¡because£»

if¡¡we¡¡were¡¡to¡¡measure¡¡the¡¡power¡¡required

to¡¡drive¡¡it¡¡forwardly£»¡¡it¡¡would¡¡be¡¡found¡¡to¡¡equal

the¡¡weight¡¡necessary¡¡to¡¡lift¡¡it¡£¡¡That¡¡is£»¡¡suppose

we¡¡should¡¡hold¡¡a¡¡plane¡¡at¡¡that¡¡angle¡¡with¡¡a¡¡heavy

wind¡¡blowing¡¡against¡¡it£»¡¡and¡¡attach¡¡two¡¡pairs¡¡of

scales¡¡to¡¡the¡¡plane£»¡¡both¡¡would¡¡show¡¡the¡¡same

pull¡£



_Fig¡£¡¡6¡£¡¡Measuring¡¡Lift¡¡and¡¡Drift_



MEASURING¡¡LIFT¡¡AND¡¡DRIFT¡£In¡¡Fig¡£¡¡6£»¡¡A¡¡is¡¡the

plane£»¡¡B¡¡the¡¡horizontal¡¡line¡¡which¡¡attaches¡¡the

plane¡¡to¡¡a¡¡scale¡¡C£»¡¡and¡¡D¡¡the¡¡line¡¡attaching¡¡it¡¡to

the¡¡scale¡¡E¡£¡¡When¡¡the¡¡wind¡¡is¡¡of¡¡sufficient¡¡force

to¡¡hold¡¡up¡¡the¡¡plane£»¡¡the¡¡scales¡¡will¡¡show¡¡the¡¡same

pull£»¡¡neglecting£»¡¡of¡¡course£»¡¡the¡¡weight¡¡of¡¡the

plane¡¡itself¡£



PRESSURE¡¡AT¡¡DIFFERENT¡¡ANGLES¡£What¡¡every

one¡¡wants¡¡to¡¡know£»¡¡and¡¡a¡¡subject¡¡on¡¡which¡¡a

great¡¡deal¡¡of¡¡experiment¡¡and¡¡time¡¡have¡¡been¡¡expended£»

is¡¡to¡¡determine¡¡what¡¡the¡¡pressures¡¡are¡¡at

the¡¡different¡¡angles¡¡between¡¡the¡¡horizontal£»¡¡and

laws¡¡have¡¡been¡¡formulated¡¡which¡¡enable¡¡the¡¡pressures

to¡¡be¡¡calculated¡£



DIFFERENCE¡¡BETWEEN¡¡LIFT¡¡AND¡¡DRIFT¡¡IN¡¡MOTION¡£The

first¡¡observation¡¡is¡¡directed¡¡to¡¡the¡¡differences

that¡¡exist¡¡between¡¡the¡¡lift¡¡and¡¡drift£»

when¡¡the¡¡plane¡¡is¡¡placed¡¡at¡¡an¡¡angle¡¡of¡¡less¡¡than

45¡¡degrees¡£¡¡A¡¡machine¡¡weighing¡¡1000¡¡pounds

has¡¡always¡¡the¡¡same¡¡lift¡£¡¡Its¡¡mass¡¡does¡¡not

change¡£¡¡Remember£»¡¡now£»¡¡we¡¡allude¡¡to¡¡its¡¡mass£»

or¡¡density¡£



We¡¡are¡¡not¡¡now¡¡referring¡¡to¡¡weight£»¡¡because

that¡¡must¡¡be¡¡taken¡¡into¡¡consideration£»¡¡in¡¡the

problem¡£¡¡As¡¡heretofore¡¡stated£»¡¡when¡¡an¡¡object

moves¡¡horizontally£»¡¡it¡¡has¡¡less¡¡weight¡¡than¡¡when

at¡¡rest¡£¡¡If¡¡it¡¡had¡¡the¡¡same¡¡weight¡¡it¡¡would¡¡not

move¡¡forwardly£»¡¡but¡¡come¡¡to¡¡rest¡£



When¡¡in¡¡motion£»¡¡therefore£»¡¡while¡¡the¡¡lift£»¡¡so

far¡¡as¡¡its¡¡mass¡¡is¡¡concerned£»¡¡does¡¡not¡¡change£»¡¡the

drift¡¡does¡¡decrease£»¡¡or¡¡the¡¡forward¡¡pull¡¡is¡¡less

than¡¡when¡¡at¡¡45¡¡degrees£»¡¡and¡¡the¡¡decrease¡¡is¡¡less

and¡¡less¡¡until¡¡the¡¡plane¡¡assumes¡¡a¡¡horizontal¡¡position£»

where¡¡it¡¡is¡¡absolutely¡¡nil£»¡¡if¡¡we¡¡do¡¡not¡¡consider

head¡¡resistance¡£



TABLES¡¡OF¡¡LIFT¡¡AND¡¡DRIFT¡£All¡¡tables¡¡of¡¡Lift

and¡¡Drift¡¡consider¡¡only¡¡the¡¡air¡¡pressures¡£¡¡They

do¡¡not¡¡take¡¡into¡¡account¡¡the¡¡fact¡¡that¡¡momentum

takes¡¡an¡¡important¡¡part¡¡in¡¡the¡¡translation¡¡of¡¡an

object£»¡¡like¡¡a¡¡flying¡¡machine¡£



A¡¡mass¡¡of¡¡material£»¡¡weighing¡¡1000¡¡pounds¡¡while

at¡¡rest£»¡¡sets¡¡up¡¡an¡¡enormous¡¡energy¡¡when¡¡moving

through¡¡the¡¡air¡¡at¡¡fifty£»¡¡seventy¡­five£»¡¡or¡¡one¡¡hundred

miles¡¡an¡¡hour¡£¡¡At¡¡the¡¡latter¡¡speed¡¡the¡¡movement

is¡¡about¡¡160¡¡feet¡¡per¡¡second£»¡¡a¡¡motion¡¡which

is¡¡nearly¡¡sufficient¡¡to¡¡maintain¡¡it¡¡in¡¡horizontal

flight£»¡¡independently¡¡of¡¡any¡¡plane¡¡surface¡£



Such¡¡being¡¡the¡¡case£»¡¡why¡¡take¡¡into¡¡account¡¡only

the¡¡angle¡¡of¡¡the¡¡plane£¿¡¡It¡¡is¡¡no¡¡wonder¡¡that

aviators¡¡have¡¡not¡¡been¡¡able¡¡to¡¡make¡¡the¡¡theoretical

considerations¡¡and¡¡the¡¡practical¡¡demonstrations

agree¡£



WHY¡¡TABLES¡¡OF¡¡LIFT¡¡AND¡¡DRIFT¡¡ARE¡¡WRONG¡£

A¡¡little¡¡reflection¡¡will¡¡show¡¡why¡¡such¡¡tables¡¡are

wrong¡£¡¡They¡¡were¡¡prepared¡¡by¡¡using¡¡a¡¡plane

surface¡¡at¡¡rest£»¡¡and¡¡forcing¡¡a¡¡blast¡¡of¡¡air¡¡against

the¡¡plane¡¡placed¡¡at¡¡different¡¡angles£»¡¡and¡¡for¡¡determining

air¡¡pressures£»¡¡this¡¡is£»¡¡no¡¡doubt£»¡¡correct¡£

But¡¡it¡¡does¡¡not¡¡represent¡¡actual¡¡flying¡¡conditions¡£

It¡¡does¡¡not¡¡show¡¡the¡¡conditions¡¡existing

in¡¡an¡¡aeroplane¡¡while¡¡in¡¡flight¡£



To¡¡determine¡¡this£»¡¡short¡¡of¡¡actual¡¡experiments

with¡¡a¡¡machine¡¡in¡¡horizontal¡¡translation£»¡¡is¡¡impossible£»

unless¡¡it¡¡is¡¡done¡¡by¡¡taking¡¡into¡¡account

the¡¡factor¡¡due¡¡to¡¡momentum¡¡and¡¡the¡¡element

attributable¡¡to¡¡the¡¡lift¡¡of¡¡the¡¡plane¡¡itself¡¡due¡¡to¡¡its

impact¡¡against¡¡the¡¡atmosphere¡£



LANGLEY'S¡¡LAW¡£The¡¡law¡¡enunciated¡¡by

Langley¡¡is£»¡¡that¡¡the¡¡greater¡¡the¡¡speed¡¡the¡¡less¡¡the

power¡¡required¡¡to¡¡propel¡¡it¡£¡¡Water¡¡as¡¡a¡¡propelling

medium¡¡has¡¡over¡¡seven¡¡hundred¡¡times

more¡¡force¡¡than¡¡air¡£¡¡A¡¡vessel¡¡having£»¡¡for¡¡instance£»

twenty¡¡horse¡¡power£»¡¡and¡¡a¡¡speed¡¡of¡¡ten

miles¡¡per¡¡hour£»¡¡would¡¡require¡¡four¡¡times¡¡that

power¡¡to¡¡drive¡¡it¡¡through¡¡the¡¡water¡¡at¡¡double¡¡the

speed¡£¡¡The¡¡power¡¡is¡¡as¡¡the¡¡square¡¡of¡¡the¡¡speed¡£



With¡¡air¡¡the¡¡conditions¡¡are¡¡entirely¡¡different¡£

The¡¡boat¡¡submergence¡¡in¡¡the¡¡water¡¡is¡¡practically

the¡¡same£»¡¡whether¡¡going¡¡ten¡¡or¡¡twenty¡¡miles¡¡an

hour¡£¡¡The¡¡head¡¡resistance¡¡is¡¡the¡¡same£»¡¡substantially£»

at¡¡all¡¡times¡¡in¡¡the¡¡case¡¡of¡¡the¡¡boat£»¡¡with¡¡the

flying¡¡machine¡¡the¡¡resistance¡¡of¡¡its¡¡sustaining

surfaces¡¡decreases¡£



Without¡¡going¡¡into¡¡a¡¡too¡¡technical¡¡description

of¡¡the¡¡reasoning¡¡which¡¡led¡¡to¡¡the¡¡discovery¡¡of¡¡the

law¡¡of¡¡air¡¡pressures£»¡¡let¡¡us¡¡try¡¡and¡¡understand

it¡¡by¡¡examining¡¡the¡¡diagram£»¡¡Fig¡£¡¡7¡£



A¡¡represents¡¡a¡¡plane¡¡at¡¡an¡¡angle¡¡of¡¡45¡¡degrees£»

moving¡¡forwardly¡¡into¡¡the¡¡atmosphere¡¡in¡¡the

direction¡¡of¡¡the¡¡arrows¡¡B¡£¡¡The¡¡measurement

across¡¡the¡¡plane¡¡vertically£»¡¡along¡¡the¡¡line¡¡B£»

which¡¡is¡¡called¡¡the¡¡sine¡¡of¡¡the¡¡angle£»¡¡represents

the¡¡surface¡¡impact¡¡of¡¡air¡¡against¡¡the¡¡plane¡£



In¡¡Fig¡£¡¡8¡¡the¡¡plane¡¡is¡¡at¡¡an¡¡angle¡¡of¡¡27¡¡degrees£»

which¡¡makes¡¡the¡¡distance¡¡in¡¡height¡¡across¡¡the¡¡line

C¡¡just¡¡one¡­half¡¡the¡¡length¡¡of¡¡the¡¡line¡¡B¡¡of¡¡Fig¡£¡¡7£»

hence¡¡the¡¡surface¡¡impact¡¡of¡¡the¡¡air¡¡is¡¡one¡­half¡¡that

of¡¡Fig¡£¡¡7£»¡¡and¡¡the¡¡drift¡¡is¡¡correspondingly¡¡decreased¡£



_Fig¡£¡¡7¡£¡¡Equal¡¡Lift¡¡and¡¡Drift¡¡in¡¡Flig
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