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°´¼üÅÌÉÏ·½Ïò¼ü ¡û »ò ¡ú ¿É¿ìËÙÉÏÏ·­Ò³£¬°´¼üÅÌÉ쵀 Enter ¼ü¿É»Øµ½±¾ÊéĿ¼ҳ£¬°´¼üÅÌÉÏ·½Ïò¼ü ¡ü ¿É»Øµ½±¾Ò³¶¥²¿£¡

machine¡¡could¡¡ever¡¡fly£»¡¡would¡¡be¡¡by¡¡propelling¡¡it

through¡¡space£»¡¡like¡¡the¡¡ball¡¡was¡¡thrown£»¡¡or¡¡by

some¡¡sort¡¡of¡¡impulse¡¡or¡¡reaction¡¡mechanism¡¡on

the¡¡air¡­ship¡¡itself¡£¡¡It¡¡could¡¡get¡¡no¡¡support¡¡from

the¡¡atmosphere¡£



LIGHT¡¡MACHINES¡¡UNSTABLE¡£Gradually¡¡the

question¡¡of¡¡weight¡¡is¡¡solving¡¡itself¡£¡¡Aviators¡¡are

beginning¡¡to¡¡realize¡¡that¡¡momentum¡¡is¡¡a¡¡wonderful

property£»¡¡and¡¡a¡¡most¡¡important¡¡element¡¡in

flying¡£¡¡The¡¡safest¡¡machines¡¡are¡¡those¡¡which¡¡have

weight¡£¡¡The¡¡light£»¡¡willowy¡¡machines¡¡are¡¡subject

to¡¡every¡¡caprice¡¡of¡¡the¡¡wind¡£¡¡They¡¡are¡¡notoriously

unstable¡¡in¡¡flight£»¡¡and¡¡are¡¡dangerous¡¡even

in¡¡the¡¡hands¡¡of¡¡experts¡£



THE¡¡APPLICATION¡¡OF¡¡POWER¡£The¡¡thing¡¡now¡¡to

consider¡¡is¡¡not¡¡form£»¡¡or¡¡shape£»¡¡or¡¡the¡¡distribution

of¡¡the¡¡supporting¡¡surfaces£»¡¡but¡¡HOW¡¡to¡¡apply

the¡¡power¡¡so¡¡that¡¡it¡¡will¡¡rapidly¡¡transfer¡¡a¡¡machine

at¡¡rest¡¡to¡¡one¡¡in¡¡motion£»¡¡and¡¡thereby¡¡get

the¡¡proper¡¡support¡¡on¡¡the¡¡atmosphere¡¡to¡¡hold¡¡it

in¡¡flight¡£



THE¡¡SUPPORTING¡¡SURFACES¡£This¡¡brings¡¡us¡¡to

the¡¡consideration¡¡of¡¡one¡¡of¡¡the¡¡first¡¡great¡¡problems

in¡¡flying¡¡machines£»¡¡namely£»¡¡the¡¡supporting

surfaces£»not¡¡its¡¡form£»¡¡shape¡¡or¡¡arrangement£»

£¨which¡¡will¡¡be¡¡taken¡¡up¡¡in¡¡their¡¡proper¡¡places£©£»¡¡but

the¡¡area£»¡¡the¡¡dimensions£»¡¡and¡¡the¡¡angle¡¡necessary

for¡¡flight¡£



AREA¡¡NOT¡¡THE¡¡ESSENTIAL¡¡THING¡£The¡¡history

of¡¡flying¡¡machines£»¡¡short¡¡as¡¡it¡¡is£»¡¡furnishes¡¡many

examples¡¡of¡¡one¡¡striking¡¡fact£º¡¡That¡¡area¡¡has

but¡¡little¡¡to¡¡do¡¡with¡¡sustaining¡¡an¡¡aeroplane¡¡when

once¡¡in¡¡flight¡£¡¡The¡¡first¡¡Wright¡¡flyer¡¡weighed

741¡¡pounds£»¡¡had¡¡about¡¡400¡¡square¡¡feet¡¡of¡¡plane

surface£»¡¡and¡¡was¡¡maintained¡¡in¡¡the¡¡air¡¡with¡¡a¡¡12

horse¡¡power¡¡engine¡£



True£»¡¡that¡¡machine¡¡was¡¡shot¡¡into¡¡the¡¡air¡¡by¡¡a

catapult¡£¡¡Motion¡¡having¡¡once¡¡been¡¡imparted¡¡to¡¡it£»

the¡¡only¡¡thing¡¡necessary¡¡for¡¡the¡¡motor¡¡was¡¡to

maintain¡¡the¡¡speed¡£



There¡¡are¡¡many¡¡instances¡¡to¡¡show¡¡that¡¡when

once¡¡in¡¡flight£»¡¡one¡¡horse¡¡power¡¡will¡¡sustain¡¡over

100¡¡pounds£»¡¡and¡¡each¡¡square¡¡foot¡¡of¡¡supporting

surface¡¡will¡¡maintain¡¡90¡¡pounds¡¡in¡¡flight¡£



THE¡¡LAW¡¡OF¡¡GRAVITY¡£As¡¡the¡¡effort¡¡to¡¡fly

may¡¡be¡¡considered¡¡in¡¡the¡¡light¡¡of¡¡a¡¡struggle¡¡to

avoid¡¡the¡¡laws¡¡of¡¡nature¡¡with¡¡respect¡¡to¡¡matter£»

it¡¡may¡¡be¡¡well¡¡to¡¡consider¡¡this¡¡great¡¡force¡¡as¡¡a

fitting¡¡prelude¡¡to¡¡the¡¡study¡¡of¡¡our¡¡subject¡£



Proper¡¡understanding£»¡¡and¡¡use¡¡of¡¡terms¡¡is¡¡very

desirable£»¡¡so¡¡that¡¡we¡¡must¡¡not¡¡confuse¡¡them¡£

Thus£»¡¡weight¡¡and¡¡mass¡¡are¡¡not¡¡the¡¡same¡£¡¡Weight

varies¡¡with¡¡the¡¡latitude£»¡¡and¡¡it¡¡is¡¡different¡¡at¡¡various

altitudes£»¡¡but¡¡mass¡¡is¡¡always¡¡the¡¡same¡£



If¡¡projected¡¡through¡¡space£»¡¡a¡¡certain¡¡mass

would¡¡move¡¡so¡¡as¡¡to¡¡produce¡¡momentum£»¡¡which

would¡¡be¡¡equal¡¡at¡¡all¡¡places¡¡on¡¡the¡¡earth's¡¡surface£»

or¡¡at¡¡any¡¡altitude¡£



Gravity¡¡has¡¡been¡¡called¡¡weight£»¡¡and¡¡weight

gravity¡£¡¡The¡¡real¡¡difference¡¡is¡¡plain¡¡if¡¡gravity

is¡¡considered¡¡as¡¡the¡¡attraction¡¡of¡¡mass¡¡for¡¡mass¡£

Gravity¡¡is¡¡generally¡¡known¡¡and¡¡considered¡¡as¡¡a

force¡¡which¡¡seeks¡¡to¡¡draw¡¡things¡¡to¡¡the¡¡earth¡£

This¡¡is¡¡too¡¡narrow¡£



Gravity¡¡acts¡¡in¡¡all¡¡directions¡£¡¡Two¡¡balls¡¡suspended

from¡¡strings¡¡and¡¡hung¡¡in¡¡close¡¡proximity

to¡¡each¡¡other¡¡will¡¡mutually¡¡attract¡¡each¡¡other¡£

If¡¡one¡¡has¡¡double¡¡the¡¡mass¡¡it¡¡will¡¡have¡¡twice¡¡the

attractive¡¡power¡£¡¡If¡¡one¡¡is¡¡doubled¡¡and¡¡the¡¡other

tripled£»¡¡the¡¡attraction¡¡would¡¡be¡¡increased¡¡six

times¡£¡¡But¡¡if¡¡the¡¡distance¡¡should¡¡be¡¡doubled¡¡the

attraction¡¡would¡¡be¡¡reduced¡¡to¡¡one¡­fourth£»¡¡and

if¡¡the¡¡distance¡¡should¡¡be¡¡tripled¡¡then¡¡the¡¡pull

would¡¡be¡¡only¡¡one¡­ninth¡£



The¡¡foregoing¡¡is¡¡the¡¡substance¡¡of¡¡the¡¡law£»

namely£»¡¡that¡¡all¡¡bodies¡¡attract¡¡all¡¡other¡¡bodies

with¡¡a¡¡force¡¡directly¡¡in¡¡proportion¡¡to¡¡their¡¡mass£»

and¡¡inversely¡¡as¡¡the¡¡square¡¡of¡¡their¡¡distance¡¡from

one¡¡another¡£



To¡¡explain¡¡this¡¡we¡¡cite¡¡the¡¡following¡¡illustration£º

Two¡¡bodies£»¡¡each¡¡having¡¡a¡¡mass¡¡of¡¡4

pounds£»¡¡and¡¡one¡¡inch¡¡apart£»¡¡are¡¡attracted¡¡toward

each¡¡other£»¡¡so¡¡they¡¡touch¡£¡¡If¡¡one¡¡has¡¡twice¡¡the

mass¡¡of¡¡the¡¡other£»¡¡the¡¡smaller¡¡will¡¡draw¡¡the¡¡larger

only¡¡one¡­quarter¡¡of¡¡an¡¡inch£»¡¡and¡¡the¡¡large¡¡one

will¡¡draw¡¡the¡¡other¡¡three¡­quarters¡¡of¡¡an¡¡inch£»

thus¡¡confirming¡¡the¡¡law¡¡that¡¡two¡¡bodies¡¡will¡¡attract

each¡¡other¡¡in¡¡proportion¡¡to¡¡their¡¡mass¡£



Suppose£»¡¡now£»¡¡that¡¡these¡¡balls¡¡are¡¡placed¡¡two

inches¡¡apart£»that¡¡is£»¡¡twice¡¡the¡¡distance¡£¡¡As

each¡¡is£»¡¡we¡¡shall¡¡say£»¡¡four¡¡pounds¡¡in¡¡weight£»¡¡the

square¡¡of¡¡each¡¡would¡¡be¡¡16¡£¡¡This¡¡does¡¡not¡¡mean

that¡¡there¡¡would¡¡be¡¡sixteen¡¡times¡¡the¡¡attraction£»

but£»¡¡as¡¡the¡¡law¡¡says£»¡¡inversely¡¡as¡¡the¡¡square¡¡of

the¡¡distance£»¡¡so¡¡that¡¡at¡¡two¡¡inches¡¡there¡¡is¡¡only

one¡­sixteenth¡¡the¡¡attraction¡¡as¡¡at¡¡one¡¡inch¡£



If¡¡the¡¡cord¡¡of¡¡one¡¡of¡¡the¡¡balls¡¡should¡¡be¡¡cut£»¡¡it

would¡¡fall¡¡to¡¡the¡¡earth£»¡¡for¡¡the¡¡reason¡¡that¡¡the

attractive¡¡force¡¡of¡¡the¡¡great¡¡mass¡¡of¡¡the¡¡earth¡¡is

so¡¡much¡¡greater¡¡than¡¡the¡¡force¡¡of¡¡attraction¡¡in

its¡¡companion¡¡ball¡£



INDESTRUCTIBILITY¡¡OF¡¡GRAVITATION¡£Gravity

cannot¡¡be¡¡produced¡¡or¡¡destroyed¡£¡¡It¡¡acts¡¡between

all¡¡parts¡¡of¡¡bodies¡¡equally£»¡¡the¡¡force¡¡being

proportioned¡¡to¡¡their¡¡mass¡£¡¡It¡¡is¡¡not¡¡affected¡¡by

any¡¡intervening¡¡substance£»¡¡and¡¡is¡¡transmitted

instantaneously£»¡¡whatever¡¡the¡¡distance¡¡may¡¡be¡£



While£»¡¡therefore£»¡¡it¡¡is¡¡impossible¡¡to¡¡divest¡¡matter

of¡¡this¡¡property£»¡¡there¡¡are¡¡two¡¡conditions

which¡¡neutralize¡¡its¡¡effect¡£¡¡The¡¡first¡¡of¡¡these¡¡is

position¡£¡¡Let¡¡us¡¡take¡¡two¡¡balls£»¡¡one¡¡solid¡¡and

the¡¡other¡¡hollow£»¡¡but¡¡of¡¡the¡¡same¡¡mass£»¡¡or¡¡density¡£

If¡¡the¡¡cavity¡¡of¡¡the¡¡one¡¡is¡¡large¡¡enough¡¡to¡¡receive

the¡¡other£»¡¡it¡¡is¡¡obvious¡¡that¡¡while¡¡gravity¡¡is¡¡still

present¡¡the¡¡lines¡¡of¡¡attraction¡¡being¡¡equal¡¡at

all¡¡points£»¡¡and¡¡radially£»¡¡there¡¡can¡¡be¡¡no¡¡pull¡¡which

moves¡¡them¡¡together¡£



DISTANCE¡¡REDUCES¡¡GRAVITATIONAL¡¡PULL¡£Or

the¡¡balls¡¡may¡¡be¡¡such¡¡distance¡¡apart¡¡that¡¡the¡¡attractive

force¡¡ceases¡£¡¡At¡¡the¡¡center¡¡of¡¡the¡¡earth

an¡¡object¡¡would¡¡not¡¡weigh¡¡anything¡£¡¡A¡¡pound

of¡¡iron¡¡and¡¡an¡¡ounce¡¡of¡¡wood£»¡¡one¡¡sixteen¡¡times

the¡¡mass¡¡of¡¡the¡¡other£»¡¡would¡¡be¡¡the¡¡same£»absolutely

without¡¡weight¡£



If¡¡the¡¡object¡¡should¡¡be¡¡far¡¡away¡¡in¡¡space¡¡it

would¡¡not¡¡be¡¡influenced¡¡by¡¡the¡¡earth's¡¡gravity£»

so¡¡it¡¡will¡¡be¡¡understood¡¡that¡¡position¡¡plays¡¡an

important¡¡part¡¡in¡¡the¡¡attraction¡¡of¡¡mass¡¡for¡¡mass¡£



HOW¡¡MOTION¡¡ANTAGONIZES¡¡GRAVITY¡£The¡¡second

way¡¡to¡¡neutralize¡¡gravity£»¡¡is¡¡by¡¡motion¡£¡¡A

ball¡¡thrown¡¡upwardly£»¡¡antagonizes¡¡the¡¡force¡¡of

gravity¡¡during¡¡the¡¡period¡¡of¡¡its¡¡ascent¡£¡¡In¡¡like

manner£»¡¡when¡¡an¡¡object¡¡is¡¡projected¡¡horizontally£»

while¡¡its¡¡mass¡¡is¡¡still¡¡the¡¡same£»¡¡its¡¡weight¡¡is¡¡less¡£



Motion¡¡is¡¡that¡¡which¡¡is¡¡constantly¡¡combating

the¡¡action¡¡of¡¡gravity¡£¡¡A¡¡body¡¡moving¡¡in¡¡a¡¡circle

must¡¡be¡¡acted¡¡upon¡¡by¡¡two¡¡forces£»¡¡one¡¡which¡¡tends

to¡¡draw¡¡it¡¡inwardly£»¡¡and¡¡the¡¡other¡¡which¡¡seeks¡¡to

throw¡¡it¡¡outwardly¡£



The¡¡former¡¡is¡¡called¡¡centripetal£»¡¡and¡¡the¡¡latter

centrifugal¡¡motion¡£¡¡Gravity£»¡¡therefore£»¡¡represents

centripetal£»¡¡and¡¡motion¡¡centrifugal¡¡force¡£



If¡¡the¡¡rotative¡¡speed¡¡of¡¡the¡¡earth¡¡should¡¡be¡¡retarded£»

all¡¡objects¡¡on¡¡the¡¡earth¡¡would¡¡be¡¡increased

in¡¡weight£»¡¡and¡¡if¡¡the¡¡motion¡¡should¡¡be¡¡accelerated

objects¡¡would¡¡become¡¡lighter£»¡¡and¡¡if¡¡sufficient

speed¡¡should¡¡be¡¡attained¡¡all¡¡matter¡¡would¡¡fly¡¡off

the¡¡surface£»¡¡just¡¡as¡¡dirt¡¡dies¡¡off¡¡the¡¡rim¡¡of¡¡a

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¡¡
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