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
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_Fig¡¡1¡£¡¡Tangential¡¡Flight_
TANGENTIAL¡¡MOTION¡¡REPRESENTS¡¡CENTRIFUGAL
PULL¡£A¡¡tangential¡¡motion£»¡¡or¡¡a¡¡horizontal
movement£»¡¡seeks¡¡to¡¡move¡¡matter¡¡away¡¡from¡¡the
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a¡¡horizontal¡¡motion¡¡to¡¡an¡¡object¡¡exerts¡¡a¡¡centrifugal
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In¡¡Fig¡£¡¡1£»¡¡let¡¡A¡¡represent¡¡the¡¡surface¡¡of¡¡the
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and¡¡C¡¡the¡¡line¡¡of¡¡flight¡£¡¡That¡¡represents¡¡a
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EQUALIZING¡¡THE¡¡TWO¡¡MOTIONS¡£But¡¡now¡¡let¡¡us
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gravitational¡¡pull¡£
The¡¡constant¡¡tendency¡¡of¡¡the¡¡ball¡¡to¡¡fly¡¡off¡¡at
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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
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Drift¡¡is¡¡the¡¡term¡¡used¡¡to¡¡indicate¡¡the¡¡resistance
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_Fig¡£¡¡3¡£¡¡Lift¡¡and¡¡Drift_
In¡¡Fig¡£¡¡3¡¡the¡¡plane¡¡A¡¡is¡¡assumed¡¡to¡¡be¡¡moving
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indicates¡¡the¡¡resistance¡£¡¡The¡¡vertical¡¡arrow¡¡C
shows¡¡the¡¡direction¡¡of¡¡lift£»¡¡which¡¡is¡¡the¡¡weight
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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
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_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
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if¡¡we¡¡were¡¡to¡¡measure¡¡the¡¡power¡¡required
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the¡¡weight¡¡necessary¡¡to¡¡lift¡¡it¡£¡¡That¡¡is£»¡¡suppose
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scales¡¡to¡¡the¡¡plane£»¡¡both¡¡would¡¡show¡¡the¡¡same
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_Fig¡£¡¡6¡£¡¡Measuring¡¡Lift¡¡and¡¡Drift_
MEASURING¡¡LIFT¡¡AND¡¡DRIFT¡£In¡¡Fig¡£¡¡6£»¡¡A¡¡is¡¡the
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the¡¡scale¡¡E¡£¡¡When¡¡the¡¡wind¡¡is¡¡of¡¡sufficient¡¡force
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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
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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
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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
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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
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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
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flight£»¡¡independently¡¡of¡¡any¡¡plane¡¡surface¡£
Such¡¡being¡¡the¡¡case£»¡¡why¡¡take¡¡into¡¡account¡¡only
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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
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unless¡¡it¡¡is¡¡done¡¡by¡¡taking¡¡into¡¡account
the¡¡factor¡¡due¡¡to¡¡momentum¡¡and¡¡the¡¡element
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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¡£
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moving¡¡forwardly¡¡into¡¡the¡¡atmosphere¡¡in¡¡the
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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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