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1,266,175 minimizingleakage,andinthusactingasa beingstruckisdecreasedbythepresenceof quasi-repellanttoincreaseenormouslythe myprotector,whereasitwouldbeincreased safetyfactor. bythepresenceoftheFranklinrod,forrea Forthebestandmosteconomicalinstala sonsthatIwilnowexplain. An understanding of but part of the O invention,thosefactorsandphenomenathat truthsrelativetoelectricaldischarges,and tionofprotectivedevicesaccordingtomy dictatesize,numberofprotectorsandphys theirmisapplicationduetothewantof icalqualitiesoftheapparatusmustbe fulerappreciationhasdoubtlessbeenre graspedbytheinstallingengineer,andpre sponsiblefortheFranklin,lightningrod. OFEEEforfulEiofthetakingitsconventionalpointedform,but75 principlesofmyinvention,theseshouldbe theoreticalconsiderations,andtheimportant brieflyexplained. discoveries that have been made in the Economicalinstalation,ofcourse,de courseofinyestigationswithawireles mandsthattheprotectivecapabilityofany transmitterofgreatactivitybywhicharcs 5 givenequipmentbenotnedleslygreater ofavolumeandtensioncomparabletothose80 thanisrequiredtomeetthemaximumex occurringinnaturewereobtained(“Prob pectanciesundertheconditionssurroundin lemsofIncreasingHumanEnergy”Century theparticularbuildingtobeprotected,E. MagazineJune1900andPatents645,576, thesedepend,partialy,asIshalshow, 649,621,787,412and1,19,732)atonceestab 20 uponthecharacterofthelandscapeproxi lishthefallacyofthehithertoprevailing85 mate to the building site. notion on which the Franklin type of rod Inthedrawings,Figures1to4inclusive, isbased,showthedistinetivenoveltyofmy arediagramsrequisitetoillustrationofthe lightningprotector,andguidetheconstruc factsandconditionsrelevanttothedeter torintheuseofmyinvention. f 25minationofspecificinstalationsofmyin InFig.2,5isasmallsphereincontact90 vention,andFigs.5to.8ilustrateconstruc withalargeone,6,partlyshown. Itcan tionandaplicationoftheprotectors.Spe beprovedbythetheoryofelectricimages cificaly: that when the two bodies are charged the Fig.1isalandscapesuitedforpurpose meandensityonthesmallonewilbeonly 30 ofexplanation;Figs,2,3and4aretheoreti caldiagrams;Figs.5and6ilustrateforms , ofimprovedprotectors;andFigs.7and8 showbuildingsequipedwiththesame. 35 ducedareaoftheregion,whichisvirtualy.Maxwell).InFig.3,thetwospheres7and100 partoftheextendedunruffledocean-surface. 8areplacedsomedistanceapartandcon (Se“PapersonElectrostaticsandMagnet nectedthroughathinwire9. Thissystem timesgreaterthanthatontheother, (See InFig.1,1representsLordKelvin’s“re “Electricity and Magnetism' by Clerk ism”bySirWilliamThomson). Underor havingbeenexcitedasbefore,thedensityon dinaryWeatherconditions,whentheskyis theSmallsphereislikelytobemanytimes 40 clear,thetotalamountofelectricitydis thatonthelarge-one. Sincebothareat105 tributedoverthelandisnearlythesameas thesamepotentialitfolowsdirectlythat thatwhichwouldbecontainedwithinits thedensitiesonthemwilbeinverselyas horizontal projection. But in times of theirradiiofcurvature. Ifthedensityof storm,Owingtotheinductiveactionofthe 7bedesignatedasdandtheradiusr,then 5clouds,animmense E.maybeaccuthechargeq=47'd,thepotentialp=4Trd10 mulatedinthelocality,ithedensitybeing andtheoutwardforce,normaltothesur greatestatthemostelevatedportionsof face,fe-2td'.Asbeforestated,whend theground.Assumingthis,underthecon surpasses20C.G.S.units,theforcefbe ditionsexistingatanymoment,letanother comessuficientlyintensetobreakdownthe 50 Sphericalsurface2,concentricwiththe-dielectricandastreamerorcoronaappears. 5 earth,bedrawn-whichmaybecaled“elec Inthiscasep=80ter. Hence,withasphere trical niveau'l-Such that the quantities ofonecentimeterradiusdisruptionwould storedoyerandunderitareequal.Inother takeplaceatapotentialp=807-251.328 Words,theiralgebraicsum,takenrelatively E.S.units,or75,398.4volts. Inreality,the 55totheimaginarysurface,inthepositiveand dischargeoccursatalowerpressureasa 20 negativesense,isnil. Objectsabovethe consequenceofunevendistributiononthe G 99 Inlveau areexposedtoeversomuch more Smallsphere,thedensitybeinggreateston riskthanthosebelow.Thus,abuildingat thesideturnedawayfromthelargeone. 3,onasiteofexcesivedensity,isapttobe Inthisrespectthebehaviorofapointed 80 hitsoonerorlater,whileoneinadepresion conductorisjustthereverse. Theoreticaly, 2 4,wherethechargeperunitareaisvery itis: erroneouslybeinferredfromthe smal,isalmostentirelysafe. Itfolows preceding,thatsharpprojectionswouldper thattheonebuilding3requiresmoreex mitelectricitytoescapeatthelowestpo tensiveequipmentthandoestheother. In tentials,butthisdoesnotfollow. Therea 65 bothinstances,however,theprobabilityof.sonwilbeclearfromaninspectionofFig. 30 =1.6493 95PDF Image | Nikola Tesla Lightning Protector 1266175
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