\u03c6100<\/span><\/span><\/span><\/span><\/td>\n<\/tr>\n<\/tbody>\n<\/table>\nMatematick\u00fd model cykloidn\u00ed p\u0159evodovky<\/h2>\n
P\u0159evodovka s cykloidn\u00edm rotorem je ide\u00e1ln\u00ed konstrukc\u00ed pro automobil nebo jak\u00e9koli jin\u00e9 vozidlo, proto\u017ee cykloidn\u00ed konstrukce dok\u00e1\u017ee sn\u00ed\u017eit amplitudu vibrac\u00ed, co\u017e je kl\u00ed\u010dov\u00e1 slo\u017eka v\u00fdkonu automobilu. Pou\u017eit\u00ed cykloidn\u00ed p\u0159evodovky je tak\u00e9 skv\u011bl\u00fdm zp\u016fsobem, jak sn\u00ed\u017eit t\u0159en\u00ed mezi ozuben\u00fdmi koly v p\u0159evodovce, co\u017e m\u016f\u017ee pomoci sn\u00ed\u017eit hluk a opot\u0159eben\u00ed. Cykloidn\u00ed p\u0159evodovka je tak\u00e9 velmi \u00fa\u010dinnou konstrukc\u00ed pro vozidla, kter\u00e1 mus\u00ed pracovat p\u0159i vysok\u00e9m zat\u00ed\u017een\u00ed, proto\u017ee p\u0159evodovka m\u016f\u017ee b\u00fdt velmi odoln\u00e1 v\u016f\u010di r\u00e1zov\u00e9mu zat\u00ed\u017een\u00ed.![\"spir\u00e1lov\u00e1](\"https:\/\/img.hzpt.com\/img\/cycloidalgearbox\/t-cycloidalgearbox-4.webp\" "\\"\\"")
<\/p>\n
Z\u00e1kladn\u00ed principy n\u00e1vrhu<\/h2>\n
Cykloidn\u00ed p\u0159evodovky se pou\u017e\u00edvaj\u00ed pro p\u0159esn\u00e9 ozuben\u00ed. Cykloidn\u00ed pohony jsou kompaktn\u00ed a robustn\u00ed a nab\u00edzej\u00ed ni\u017e\u0161\u00ed v\u016fli, torzn\u00ed tuhost a del\u0161\u00ed \u017eivotnost. Jsou tak\u00e9 vhodn\u00e9 pro aplikace s vysok\u00fdm zat\u00ed\u017een\u00edm.
Cykloidn\u00ed pohony jsou kompaktn\u00ed a poskytuj\u00ed velmi vysok\u00e9 p\u0159evodov\u00e9 pom\u011bry. Jsou tak\u00e9 velmi robustn\u00ed a zvl\u00e1daj\u00ed r\u00e1zov\u00e1 zat\u00ed\u017een\u00ed. Cykloidn\u00ed pohony jsou ide\u00e1ln\u00ed pro \u0161irokou \u0161k\u00e1lu technologi\u00ed pohon\u016f. Cykloidn\u00ed ozuben\u00e1 kola maj\u00ed vynikaj\u00edc\u00ed torzn\u00ed tuhost a mohou poskytnout p\u0159evodov\u00fd pom\u011br 300:1. Lze je tak\u00e9 pou\u017e\u00edt v aplikac\u00edch, kde nen\u00ed \u017e\u00e1douc\u00ed stohov\u00e1n\u00ed v\u00edce p\u0159evodov\u00fdch stup\u0148\u016f.
Aby bylo dosa\u017eeno vysok\u00e9ho reduk\u010dn\u00edho pom\u011bru, mus\u00ed b\u00fdt cykloidn\u00ed ozuben\u00e1 kola vyrobena s extr\u00e9mn\u00ed p\u0159esnost\u00ed. Cykloidn\u00ed ozuben\u00e1 kola maj\u00ed zak\u0159iven\u00fd profil zubu, kter\u00fd odstra\u0148uje smykov\u00e9 s\u00edly v jak\u00e9mkoli bod\u011b kontaktu. To zaji\u0161\u0165uje tvarov\u00e9 ulo\u017een\u00ed ozuben\u00e9ho kotou\u010de. Tento profil m\u016f\u017ee b\u00fdt proveden na samostatn\u00e9m vn\u011bj\u0161\u00edm pouzd\u0159e nebo jako vlo\u017eka s vnit\u0159n\u00edm profilem ozuben\u00e9ho kola.
Cykloidn\u00ed pohony se pou\u017e\u00edvaj\u00ed v lodn\u00edch pohonn\u00fdch syst\u00e9mech, kde se nosn\u00e1 deska ot\u00e1\u010d\u00ed kolem os X a Y. Deska je ukotvena z\u00e1vitov\u00fdm otvorem um\u00edst\u011bn\u00fdm 15 mm od st\u0159edu.
V cykloidn\u00ed p\u0159evodovce se k podep\u0159en\u00ed nosn\u00e9 desky pou\u017e\u00edv\u00e1 sekund\u00e1rn\u00ed nosi\u010dov\u00e9 t\u011bleso. Sekund\u00e1rn\u00ed nosi\u010dov\u00e9 t\u011bleso se skl\u00e1d\u00e1 z mont\u00e1\u017en\u00edho nosi\u010dov\u00e9ho t\u011blesa a sekund\u00e1rn\u00edho nosi\u010dov\u00e9ho kotou\u010de.<\/p>\n
N\u00edzk\u00e9 t\u0159en\u00ed<\/h2>\n
Bylo provedeno n\u011bkolik studi\u00ed zam\u011b\u0159en\u00fdch na pochopen\u00ed statick\u00fdch probl\u00e9m\u016f ozuben\u00fdch kol. V tomto \u010dl\u00e1nku se zab\u00fdv\u00e1me matematick\u00fdm modelem cykloidn\u00ed p\u0159evodovky s n\u00edzk\u00fdm t\u0159en\u00edm. Tento model je navr\u017een pro v\u00fdpo\u010det r\u016fzn\u00fdch parametr\u016f, kter\u00e9 ovliv\u0148uj\u00ed v\u00fdkon p\u0159evodovky b\u011bhem v\u00fdroby.
Model je zalo\u017een na nov\u00e9m p\u0159\u00edstupu, kter\u00fd zahrnuje efekt t\u0159en\u00ed a neline\u00e1rn\u00ed charakteristiku t\u0159en\u00ed. Tyto parametry nejsou zahrnuty v konven\u010dn\u00edm pravidle.
Stik\u010dn\u00ed efekt se projevuje p\u0159i zm\u011bn\u011b sm\u011bru rychlosti. B\u011bhem t\u00e9to doby je zapot\u0159eb\u00ed, aby vstupn\u00ed kroutic\u00ed moment p\u0159ev\u00e1\u017eil nad stik\u010dn\u00edm efektem a vyvolal pohyb. Model n\u00e1m tak\u00e9 umo\u017e\u0148uje vypo\u010d\u00edtat velikost stik\u010dn\u00edho efektu a jeho rychlost odtr\u017een\u00ed.
Nejd\u016fle\u017eit\u011bj\u0161\u00ed je, \u017ee model lze pou\u017e\u00edt ke zlep\u0161en\u00ed dynamick\u00e9ho chov\u00e1n\u00ed \u0159\u00edzen\u00e9ho syst\u00e9mu. V tomto ohledu m\u00e1 model vysok\u00fd stupe\u0148 p\u0159esnosti. Model je testov\u00e1n v n\u011bkolika kvadrantech p\u0159evodovky, aby se nalezla optim\u00e1ln\u00ed rychlost odtr\u017een\u00ed od t\u0159en\u00ed. V\u00fdsledky simulace modelu ukazuj\u00ed, \u017ee tento model je efektivn\u00ed p\u0159i predikci \u00fa\u010dinnosti cykloidn\u00ed p\u0159evodovky s n\u00edzk\u00fdm t\u0159en\u00edm.
Krom\u011b stik\u010dn\u00edho modelu jsme tak\u00e9 studovali \u00fa\u010dinnost cykloidn\u00edho reduktoru s n\u00edzk\u00fdm t\u0159en\u00edm. Reduk\u010dn\u00ed pom\u011br t\u00e9to p\u0159evodovky byl odhadnut ze vzorce. Zjistilo se, \u017ee pom\u011br se bl\u00ed\u017e\u00ed z\u00e1porn\u00e9mu nekone\u010dnu, kdy\u017e je to\u010div\u00fd moment motoru bl\u00edzk\u00fd nule Nm.<\/p>\n
Kompaktn\u00ed<\/h2>\n
Na rozd\u00edl od standardn\u00edch planetov\u00fdch p\u0159evodovek jsou cykloidn\u00ed p\u0159evodovky kompaktn\u00ed, s n\u00edzk\u00fdm t\u0159en\u00edm a prakticky nulovou v\u016fl\u00ed. Nab\u00edzej\u00ed tak\u00e9 vysok\u00e9 reduk\u010dn\u00ed pom\u011bry, vysokou nosnost a vysokou \u00fa\u010dinnost. D\u00edky t\u011bmto vlastnostem jsou vhodnou volbou pro \u0161irokou \u0161k\u00e1lu aplikac\u00ed.
Cykloidn\u00ed kotou\u010de jsou poh\u00e1n\u011bny excentrickou vstupn\u00ed h\u0159\u00eddel\u00ed. Ty jsou pot\u00e9 poh\u00e1n\u011bny stacion\u00e1rn\u00edm ozuben\u00fdm v\u011bncem. Ozuben\u00fd v\u011bnec ot\u00e1\u010d\u00ed cykloidn\u00edm kotou\u010dem vy\u0161\u0161\u00ed rychlost\u00ed. Vstupn\u00ed h\u0159\u00eddel se oto\u010d\u00ed dev\u011btkr\u00e1t, aby dokon\u010dila plnou ot\u00e1\u010dku. Ozuben\u00fd v\u011bnec je navr\u017een tak, aby korigoval dynamickou nerovnov\u00e1hu.
Cykloidn\u00ed p\u0159evodovky CZPT jsou navr\u017eeny pro p\u0159esn\u00fd a stabiln\u00ed provoz. Tyto reduktory jsou robustn\u00ed a zvl\u00e1daj\u00ed velk\u00e9 posuny. Nab\u00edzej\u00ed tak\u00e9 vysokou ochranu proti p\u0159et\u00ed\u017een\u00ed. Jsou vhodn\u00e9 pro terapii r\u00e1zov\u00fdmi vlnami. P\u0159evodovky CZPT jsou tak\u00e9 vhodn\u00e9 pro aplikace s kritickou p\u0159esnost\u00ed polohov\u00e1n\u00ed. Vy\u017eaduj\u00ed tak\u00e9 n\u00edzk\u00e9 n\u00e1klady na mont\u00e1\u017e a konstrukci. Jsou navr\u017eeny pro dlouhou \u017eivotnost a n\u00edzk\u00e9 hysterezn\u00ed ztr\u00e1ty.
Cykloidn\u00ed reduktory CZPT se pou\u017e\u00edvaj\u00ed v r\u016fzn\u00fdch pr\u016fmyslov\u00fdch aplikac\u00edch, v\u010detn\u011b CNC obr\u00e1b\u011bc\u00edch center, robotick\u00fdch polohova\u010d\u016f a manipul\u00e1tor\u016f. Nab\u00edzej\u00ed jedine\u010dnou konstrukci, kter\u00e1 zvl\u00e1d\u00e1 vysok\u00e9 s\u00edly na v\u00fdstupn\u00ed ose, a jsou vhodn\u00e9 zejm\u00e9na pro velk\u00e9 posuvy. Tyto p\u0159evodovky jsou vysoce \u00fa\u010dinn\u00e9, sni\u017euj\u00ed n\u00e1klady a jsou k dispozici v r\u016fzn\u00fdch velikostech. Jsou ide\u00e1ln\u00ed pro aplikace, kter\u00e9 vy\u017eaduj\u00ed milimetrovou p\u0159esnost.<\/p>\n
Vysok\u00e9 reduk\u010dn\u00ed pom\u011bry<\/h2>\n
Ve srovn\u00e1n\u00ed s jin\u00fdmi p\u0159evodovkami nab\u00edzej\u00ed cykloidn\u00ed p\u0159evodovky vysok\u00e9 reduk\u010dn\u00ed pom\u011bry a malou v\u016fli. Jsou tak\u00e9 levn\u011bj\u0161\u00ed. Cykloidn\u00ed p\u0159evodovky lze pou\u017e\u00edt v r\u016fzn\u00fdch pr\u016fmyslov\u00fdch odv\u011btv\u00edch. Jsou vhodn\u00e9 pro robotick\u00e9 aplikace. Maj\u00ed tak\u00e9 vysokou \u00fa\u010dinnost a nosnost.
Cykloidn\u00ed p\u0159evodovka pracuje na principu ot\u00e1\u010den\u00ed cykloidn\u00edho disku. Tento disk obsahuje otvory, kter\u00e9 jsou v\u011bt\u0161\u00ed ne\u017e \u010depy na v\u00fdstupn\u00edm h\u0159\u00eddeli. P\u0159i ot\u00e1\u010den\u00ed disku se v\u00fdstupn\u00ed \u010depy pohybuj\u00ed v otvorech a vytv\u00e1\u0159ej\u00ed tak stabiln\u00ed ot\u00e1\u010den\u00ed v\u00fdstupn\u00edho h\u0159\u00eddele. Tento typ p\u0159evodovky nevy\u017eaduje stohov\u00e1n\u00ed stup\u0148\u016f.
Cykloidn\u00ed p\u0159evodovky jsou obvykle krat\u0161\u00ed ne\u017e planetov\u00e9 p\u0159evodovky. Nav\u00edc jsou robustn\u011bj\u0161\u00ed a dok\u00e1\u017e\u00ed p\u0159en\u00e1\u0161et vy\u0161\u0161\u00ed kroutic\u00ed momenty.
Cykloidn\u00ed p\u0159evodovky maj\u00ed excentrickou va\u010dku, kter\u00e1 poh\u00e1n\u00ed cykloidn\u00ed kotou\u010d. Cykloidn\u00ed kotou\u010d se posouv\u00e1 v kroc\u00edch o 360 stup\u0148\u016f\/oto\u010dn\u011b\/po kladk\u00e1ch. Tak\u00e9 se ot\u00e1\u010d\u00ed excentricky. Zab\u00edr\u00e1 s pouzdrem ozuben\u00e9ho v\u011bnce. Tak\u00e9 zab\u00edr\u00e1 s vnit\u0159n\u00edmi zuby pouzdra ozuben\u00e9ho v\u011bnce.
Po\u010det lalok\u016f na cykloidn\u00edm disku nen\u00ed dostate\u010dn\u00fd pro dosa\u017een\u00ed dobr\u00e9ho p\u0159evodov\u00e9ho pom\u011bru. Ve skute\u010dnosti mus\u00ed b\u00fdt po\u010det lalok\u016f men\u0161\u00ed ne\u017e po\u010det \u010dep\u016f obklopuj\u00edc\u00edch cykloidn\u00ed disk.
Cykloidn\u00ed kotou\u010d se ot\u00e1\u010d\u00ed excentrickou va\u010dkou, kter\u00e1 vy\u010dn\u00edv\u00e1 ze z\u00e1kladn\u00ed h\u0159\u00eddele. Va\u010dka se tak\u00e9 ot\u00e1\u010d\u00ed uvnit\u0159 cykloidn\u00edho kotou\u010de. Excentrick\u00fd pohyb va\u010dky pom\u00e1h\u00e1 cykloidn\u00edmu kotou\u010di ot\u00e1\u010det se kolem \u010dep\u016f sk\u0159\u00edn\u011b ozuben\u00e9ho v\u011bnce.![\"spir\u00e1lov\u00e1](\"https:\/\/img.hzpt.com\/img\/cycloidalgearbox\/c-cycloidalgearbox-4.webp\" "\\"\\"")
<\/p>\n
Sn\u00ed\u017een\u00ed amplitudy vibrac\u00ed<\/h2>\n
Byly studov\u00e1ny r\u016fzn\u00e9 p\u0159\u00edstupy ke sn\u00ed\u017een\u00ed amplitudy vibrac\u00ed v cykloidn\u00ed p\u0159evodovce. Tyto p\u0159\u00edstupy jsou zalo\u017eeny na kinematick\u00e9 anal\u00fdze p\u0159evodovky.
Cykloidn\u00ed p\u0159evodovka je p\u0159evodovka, kter\u00e1 se skl\u00e1d\u00e1 z lo\u017eisek, ozuben\u00fdch kol a excentrick\u00e9ho lo\u017eiska, kter\u00e9 poh\u00e1n\u00ed cykloidn\u00ed kotou\u010d. Tato p\u0159evodovka m\u00e1 vysok\u00fd reduk\u010dn\u00ed pom\u011br, \u010deho\u017e je dosa\u017eeno \u0159adou \u010dep\u016f v\u00fdstupn\u00edho h\u0159\u00eddele, kter\u00e9 poh\u00e1n\u011bj\u00ed v\u00fdstupn\u00ed h\u0159\u00eddel p\u0159i ot\u00e1\u010den\u00ed kotou\u010de.
Zku\u0161ebn\u00ed stolice pou\u017eit\u00e1 ve studi\u00edch m\u00e1 \u010dty\u0159i senzory. Ka\u017ed\u00fd senzor sn\u00edm\u00e1 sign\u00e1ly pomoc\u00ed r\u016fzn\u00fdch technik zpracov\u00e1n\u00ed sign\u00e1lu. Krom\u011b toho je zde ot\u00e1\u010dkom\u011br, kter\u00fd sn\u00edm\u00e1 zm\u011bny rychlosti ot\u00e1\u010den\u00ed na vstupn\u00ed stran\u011b.
Kinematick\u00e1 studie robotick\u00e9 p\u0159evodovky byla provedena za \u00fa\u010delem pochopen\u00ed frekvence vibrac\u00ed a ur\u010den\u00ed, zda je p\u0159evodovka vadn\u00e1. Bylo zji\u0161t\u011bno, \u017ee p\u0159evodovka pracuje spr\u00e1vn\u011b, kdy\u017e je amplituda os x a y n\u00edzk\u00e1. Pokud je v\u0161ak amplituda vysok\u00e1, sv\u011bd\u010d\u00ed to o vadn\u00e9m prvku.
Frekven\u010dn\u00ed anal\u00fdza vibra\u010dn\u00edch sign\u00e1l\u016f se prov\u00e1d\u00ed jak pro cyklostacion\u00e1rn\u00ed, tak pro necyklostacion\u00e1rn\u00ed podm\u00ednky. Vybran\u00e9 frekvence jsou ty, kter\u00e9 se objevuj\u00ed v obou typech podm\u00ednek.<\/p>\n
Odoln\u00fd v\u016f\u010di r\u00e1zov\u00e9mu zat\u00ed\u017een\u00ed<\/h2>\n
Ve srovn\u00e1n\u00ed s tradi\u010dn\u00edmi p\u0159evodovkami maj\u00ed cykloidn\u00ed p\u0159evodovky zna\u010dn\u00e9 v\u00fdhody, pokud jde o r\u00e1zov\u00e9 zat\u00ed\u017een\u00ed. Pat\u0159\u00ed mezi n\u011b vysok\u00e1 r\u00e1zov\u00e1 \u00fanosnost, vysok\u00e1 \u00fa\u010dinnost, sn\u00ed\u017een\u00e9 n\u00e1klady, ni\u017e\u0161\u00ed hmotnost, ni\u017e\u0161\u00ed t\u0159en\u00ed a lep\u0161\u00ed p\u0159esnost polohov\u00e1n\u00ed.
Cykloidn\u00ed p\u0159evody lze pou\u017e\u00edt k nahrazen\u00ed tradi\u010dn\u00edch planetov\u00fdch p\u0159evod\u016f v aplikac\u00edch, kde je d\u016fle\u017eit\u00e1 setrva\u010dnost, nap\u0159\u00edklad p\u0159i p\u0159eprav\u011b t\u011b\u017ek\u00fdch b\u0159emen. Maj\u00ed leh\u010d\u00ed konstrukci a lze je vyrobit v kompaktn\u011bj\u0161\u00ed velikosti, co\u017e pom\u00e1h\u00e1 sni\u017eovat n\u00e1klady a n\u00e1klady na instalaci. Cykloidn\u00ed p\u0159evody jsou tak\u00e9 schopny dos\u00e1hnout p\u0159evodov\u00fdch pom\u011br\u016f a\u017e 300:1 v mal\u00e9m proveden\u00ed.
Cykloidn\u00ed p\u0159evodovky jsou vhodn\u00e9 tak\u00e9 pro aplikace, kde je nezbytn\u00e1 dlouh\u00e1 \u017eivotnost. Jejich radi\u00e1ln\u00ed up\u00ednac\u00ed krou\u017eek sni\u017euje setrva\u010dnost a\u017e o 391 TP3T. Cykloidn\u00ed p\u0159evodovky maj\u00ed torzn\u00ed tuhost, kter\u00e1 je p\u011btkr\u00e1t vy\u0161\u0161\u00ed ne\u017e u konven\u010dn\u00edch planetov\u00fdch p\u0159evodovek.
Cykloidn\u00ed p\u0159evodovky mohou p\u0159in\u00e9st v\u00fdznamn\u00e1 vylep\u0161en\u00ed u m\u00edcha\u010dek betonu. Jedn\u00e1 se o vysoce \u00fa\u010dinnou konstrukci, kter\u00e1 umo\u017e\u0148uje d\u016fle\u017eit\u00e9 inovace. Jsou tak\u00e9 ide\u00e1ln\u00ed pro servopohony, obr\u00e1b\u011bc\u00ed stroje a l\u00e9ka\u0159skou techniku. Vyzna\u010duj\u00ed se u\u017eivatelsky p\u0159\u00edv\u011btiv\u00fdmi \u0161roubov\u00fdmi spoji, \u00fa\u010dinnou ochranou proti korozi a efektivn\u00ed manipulac\u00ed.
Cykloidn\u00ed p\u0159evody jsou obzvl\u00e1\u0161t\u011b u\u017eite\u010dn\u00e9 pro aplikace s kritickou p\u0159esnost\u00ed polohov\u00e1n\u00ed. Nap\u0159\u00edklad p\u0159i \u0159\u00edzen\u00ed velk\u00fdch parabolick\u00fdch ant\u00e9n je pro udr\u017een\u00ed p\u0159esnosti vy\u017eadov\u00e1na vysok\u00e1 r\u00e1zov\u00e1 \u00fanosnost. Cykloidn\u00ed p\u0159evody vydr\u017e\u00ed r\u00e1zov\u00e9 zat\u00ed\u017een\u00ed a\u017e do 5001 TP3T jejich jmenovit\u00e9ho to\u010div\u00e9ho momentu.![\"spir\u00e1lov\u00e1](\"https:\/\/img.hzpt.com\/img\/cycloidalgearbox\/b-cycloidalgearbox-4.webp\" "\\"\\"")
<\/p>\n
Inerci\u00e1ln\u00ed efekty<\/h2>\n
Byla provedena \u0159ada studi\u00ed zkoumaj\u00edc\u00edch statick\u00e9 probl\u00e9my ozuben\u00fdch kol. St\u00e1le v\u0161ak existuje pot\u0159eba vhodn\u00e9ho modelu pro zkoum\u00e1n\u00ed dynamick\u00e9ho chov\u00e1n\u00ed \u0159\u00edzen\u00e9ho syst\u00e9mu. Za t\u00edmto \u00fa\u010delem byl vyvinut matematick\u00fd model cykloidn\u00ed p\u0159evodovky. P\u0159edstaven\u00fd model je jednoduch\u00fd, kter\u00fd lze pou\u017e\u00edt jako z\u00e1klad pro slo\u017eit\u011bj\u0161\u00ed mechanick\u00fd model.
Matematick\u00fd model je zalo\u017een na mechanick\u00e9 konstrukci cykloidn\u00ed p\u0159evodovky a m\u00e1 neline\u00e1rn\u00ed t\u0159ec\u00ed charakteristiku. Model je schopen reprodukovat proudov\u00e9 \u0161pi\u010dky a zlomy v klidov\u00e9m stavu. Zohled\u0148uje tak\u00e9 vliv t\u0159en\u00ed. Nezahrnuje v\u0161ak v\u016fli ani torzn\u00ed tuhost.
Tento model se pou\u017e\u00edv\u00e1 k v\u00fdpo\u010dtu proudu generuj\u00edc\u00edho moment a setrva\u010dnosti motoru. Tyto hodnoty jsou pot\u00e9 porovn\u00e1ny s m\u011b\u0159en\u00edm v re\u00e1ln\u00e9m syst\u00e9mu. V\u00fdsledky ukazuj\u00ed, \u017ee v\u00fdsledky simulace se velmi bl\u00ed\u017e\u00ed m\u011b\u0159en\u00ed v re\u00e1ln\u00e9m syst\u00e9mu.
V modelu je pro zlep\u0161en\u00ed jeho dynamick\u00e9ho chov\u00e1n\u00ed zohledn\u011bno n\u011bkolik parametr\u016f. Tyto parametry jsou vypo\u010d\u00edt\u00e1ny z harmonick\u00e9 anal\u00fdzy pohonn\u00e9ho syst\u00e9mu. Pat\u0159\u00ed mezi n\u011b proud generuj\u00edc\u00ed kroutic\u00ed moment, setrva\u010dnost a kontaktn\u00ed s\u00edly rotuj\u00edc\u00edch \u010d\u00e1st\u00ed.
Model m\u00e1 vysokou \u00farove\u0148 p\u0159esnosti a lze jej pou\u017e\u00edt pro \u0159\u00edzen\u00ed motor\u016f. Je tak\u00e9 schopen reprodukovat dynamick\u00e9 chov\u00e1n\u00ed \u0159\u00edzen\u00e9ho syst\u00e9mu.
![\"China](\"https:\/\/img.hzpt.com\/img\/cycloidalgearbox\/cycloidalgearbox-l1.webp\" "\\"\\"")
![\"China](\"https:\/\/img.hzpt.com\/img\/cycloidalgearbox\/cycloidalgearbox-l2.webp\" "\\"\\"")
editor by czh 2022-12-12<\/p>","protected":false},"excerpt":{"rendered":"
Merchandise Description Starshine Push Cycloid Geared Motor\u00a0Traits one. Features:1.\u00a0Smooth working,low sounds gear tooth needle much more engagement.two. Cycloidal tooth profile provides a large make contact with ratio to withstand overload shocks3. Compact measurement: one ratio accessible from 1\/9\u00a0to 1\/87, double phase up from\u00a01\/99 to 1\/7569\u00a0four. Ideal for dynamic purposes: recurrent start-end-reversing obligations satisfies for cyclo […]<\/p>","protected":false},"author":1,"featured_media":0,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"_et_pb_use_builder":"","_et_pb_old_content":"","_et_gb_content_width":"","footnotes":""},"categories":[1],"tags":[4355,1781,1772,1773,52,54,55,56,59,60,1775,61,2320,63,66,24,1804,70],"class_list":["post-2813","post","type-post","status-publish","format-standard","hentry","category-product-catalog","tag-china-gearbox","tag-cycloidal-gear-reducer","tag-cycloidal-gearbox","tag-cycloidal-reducer","tag-gear","tag-gear-gearbox","tag-gear-reducer","tag-gear-reducer-gearbox","tag-gearbox","tag-gearbox-china","tag-gearbox-cycloidal","tag-gearbox-gear","tag-gearbox-input-gear","tag-gearbox-reducer","tag-gearbox-with","tag-reducer","tag-reducer-flange","tag-reducer-gearbox"],"_links":{"self":[{"href":"https:\/\/cyclogearreducer.top\/cs\/wp-json\/wp\/v2\/posts\/2813","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/cyclogearreducer.top\/cs\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/cyclogearreducer.top\/cs\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/cyclogearreducer.top\/cs\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/cyclogearreducer.top\/cs\/wp-json\/wp\/v2\/comments?post=2813"}],"version-history":[{"count":0,"href":"https:\/\/cyclogearreducer.top\/cs\/wp-json\/wp\/v2\/posts\/2813\/revisions"}],"wp:attachment":[{"href":"https:\/\/cyclogearreducer.top\/cs\/wp-json\/wp\/v2\/media?parent=2813"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/cyclogearreducer.top\/cs\/wp-json\/wp\/v2\/categories?post=2813"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/cyclogearreducer.top\/cs\/wp-json\/wp\/v2\/tags?post=2813"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}