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inner ends ‘ofthe blades P of the outer mem ber. Theinnerendsof‘saidbladesvScon The inner member not only acts as a de—' ?ector in the manner which has thus far been .“768.,116' .3. ,passing between the various blades or vanes ‘trialchamber'1‘and createsaradial‘out?ow the intermediate portions of said bolts are iwhich hassimultaneous actionwiththec0u~ ?attened, as at 11, said ?attened portions ?t ting snugly against the convexed side of the - by the outer ‘revolving _n1ember.. :‘This out blades. Thebladesofboth’theouterandin ?ow may be ‘readily proportioned, whereby normembersareofcoursearrangedincircu-'thesamewill‘bearapropervelocityrelation , ,larseries,and theouterendsofthebladesb‘ vrequired to secure almost compiete energy - terminateatatangentreverseofthatofthetransfer. - ' - verge‘intotheradiiofthecircleinwhich pointedout,butthesameisalsoassociated theyare-set.-'ThedisksQandRoftheinner withcertainotherinstrumentalitieswhereby member aresolidand constituteand inclose itactsasahighly-sensitivegovernor. ‘an interiorcentrally-locatedchamberT,into is.which the'in?ow of ?uid is forced by the en Referring now more particularly to Figs. 2, 3,and5,aiwormW issecuredtotheshaftV, ergyit‘maycontainaftertheinitialimpact soastorotatetherewith,saidworm beingar-' withthe.outermember. Thisin?owiscon 'ductedradiallyinwardbyde?ectionwiththe byatransversely-arrangedshafth,which‘con staticbladesoftheinnermember(itbeingun stitutelstheoperating-stemforthe'valveHin caved surfaceof alof the blades Pwcarried' rangedtoengagewithagear-wheelX, carriedi derstoodthattheinnermemberisnormally the-?uid-supplypipeG,hereinbef'orereferred85 stationary)andconvergingtothe‘centercre to. Theouterendofthe‘shafthisrotatably atesacompression commensurate with its‘ve locity,resultinginanout?owinaldrections.'fromthebaseA. Thegear-wheelXis'loose ‘Theout?owinturnisde?ectedbycontact upontheshaftIt,wherebythe.shaftmaybe‘ withtheinnervanes,soastodirectthe?ow operatedindependentlyof.-thegear-wheel tangentiallytotheinnerterminioftheactive whenfoundexpedient. Aroundtheshafth vanes .1’, whereby an additional impact is se is acoiledspring Z, the outer'endof which _ curedupon-theouterrevolvingmember.'It is‘rigidlysecuredtothebracketY,whilethe. willthusbeseenthattheinnermemberserves -innerend thereof isconnected tothe-armor 30 thedualfunctionofdirectingboththein?ow projectionh’oftheshaft7L. Thisspringis and out?ow from ‘thechamber T.v Itisalso for the purposeof creating a tension in the ‘ ‘tobeappreciatedthattheinitialimpactfrom direction of the arrow,'Fig.2,wherebythe _ _thenozzleisathighvelocityandthatitisa armIt’.forciblycontacts-apinit’,projecting physicallawthatenergytransferbyimpact laterallyfromthe,faceof.thegearX. -Out or,collision can never be complete where dis parityofmass obtains unlessthe impelled theprotrudingendoftheshaftorvalve-stem‘ component'is invested with a velocity su'i? cientlynearthatoftheimpellingcomponent thebracketY,thesamebeingprovidedwith" as to bring the two components to the correct» a bearing for a thumb-screw 3, the function _- 40 relation. Therefore in a turbine in which a. of which-is to act as a stop whereby the limit 105 simpleimpact'onlyissecuredthevelocityor ofdownward‘movementof'thelever.1isad-I rate'oflrevolutionswouldofnecessity‘beso adjusted,consequentlyrestricting'themove i“high/inordertobeartheproperrelationto mentoftheshaft/LandthevalveH,‘carried. thespoutingvelocityoftheworking?uidas thereby,asisobvious. 4 isafspringcoiled 45 ’togenerateadestructiveordangerouscentrif abouttheshaftqV,designedforreceiving,I10 u -ugal force. the slow-speed type in order tosecure an _eco—' bine and in this capacity actsas a counter-.v beforedescribed,inconnectionwithwhichlat teritmay be-furtherpointedout thatinthe. initialimpactwhentheengineissogearcdas to ‘allow a high rate of-revolution the .dis—. paritybetweenthe'spoutingvelocityof the; working ?uid and the peripheral velocity of. the wheel issogreatas toleaveaconsider able percentage~of energy conserved by then working ?uichand itis this energy, as has iby the adjusted tension of thesprmgAc may been explained, which converges into the 0on1 .be indicated, a scale 9 beingshown in , ig. 2 supportedinabracketY_,projectingupwardly sideof thebracket3'.’and rigidly-securedto,[00 i1.isa‘lever1. 2isanoffsetarmsecuredto Ontheotherhand,,a‘turbineof thestressof-theinnermember.of.thetur nomi'calenergy-transferfromacommensu balance.aswillmoreclearlyhereinafterapi. ratelylowspoutingvelocitymust.ofnecessity pear. Oneendofthisspringisrigidly'se~ 5carry a cumbersome or structural complica». cured to the worm W, and theopposite end, - tionof1variesinorderthattherequiredarea thereofiscorrespomlinglyattachedtoadisk ofactionmaybesecuredtoaffordaconstant 5,theshaftVworkinglooselythroughthis stresssu?ieientlygreattocarefortheload. disk.‘ Thedisk5mayberotateduponthe Itisameanbetween‘thesetwoprinciplesor. shaft-V'toproperlyregulatethetensionofthe .55.typesthat1havedev'isedatheengineherein-..spring4bymeans‘ofanopposingdisk6;rig [20 idlymountedupontheuprightB,andthe-bolted‘ and-nutfastening,device7,adapted‘to,pass : throughasuitableapertureinthedisk6and- any one of a series.Obapez‘tures.8 in the disk‘ 5,arranged incircularseries,wherebythey 15' may duly register with said aperture in the dish 6. .The disk 5may carry any convenient . __ orpreferredscaleorregisteringvdevlcewhereiPDF Image | STEAM TURBINE Dutton
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