\n <\/i>P\u0159izp\u016fsoben\u00fd po\u017eadavek
\n <\/a>\n <\/div>\n<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\nCyklonoidn\u00ed p\u0159evodovka<\/h2>\n
Cykloidn\u00ed p\u0159evodovka je v podstat\u011b p\u0159evodovka, kter\u00e1 k prov\u00e1d\u011bn\u00ed rota\u010dn\u00edho pohybu vyu\u017e\u00edv\u00e1 cykloidn\u00ed pohyb. Jedn\u00e1 se o velmi jednoduchou a efektivn\u00ed konstrukci, kterou lze pou\u017e\u00edt v r\u016fzn\u00fdch aplikac\u00edch. Cykloidn\u00ed p\u0159evodovka se \u010dasto pou\u017e\u00edv\u00e1 v aplikac\u00edch, kter\u00e9 vy\u017eaduj\u00ed pohyb t\u011b\u017ek\u00fdch b\u0159emen. Oproti planetov\u00e9 p\u0159evodovce m\u00e1 n\u011bkolik v\u00fdhod, v\u010detn\u011b schopnosti zvl\u00e1dat vy\u0161\u0161\u00ed zat\u00ed\u017een\u00ed a vy\u0161\u0161\u00ed rychlosti.![\"spir\u00e1lov\u00e1](\"https:\/\/img.hzpt.com\/img\/cycloidalgearbox\/t-cycloidalgearbox-5.webp\" "\\"\\"")
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Dynamick\u00e9 a setrva\u010dn\u00e9 \u00fa\u010dinky cykloidn\u00ed p\u0159evodovky<\/h2>\n
Bylo provedeno n\u011bkolik studi\u00ed dynamick\u00fdch a setrva\u010dn\u00fdch \u00fa\u010dink\u016f cykloidn\u00ed p\u0159evodovky. N\u011bkter\u00e9 z nich se zam\u011b\u0159uj\u00ed na principy fungov\u00e1n\u00ed, zat\u00edmco jin\u00e9 se zam\u011b\u0159uj\u00ed na matematick\u00fd model p\u0159evodovky. Tento \u010dl\u00e1nek zkoum\u00e1 matematick\u00fd model cykloidn\u00ed p\u0159evodovky a porovn\u00e1v\u00e1 jej\u00ed v\u00fdkon s re\u00e1ln\u00fdmi m\u011b\u0159en\u00edmi. Pro n\u00e1vrh a \u0159\u00edzen\u00ed cykloidn\u00ed p\u0159evodovky je d\u016fle\u017eit\u00e9 m\u00edt vhodn\u00fd matematick\u00fd model. Cykloidn\u00ed p\u0159evodovka je dvoustup\u0148ov\u00e1 p\u0159evodovka s cykloidn\u00edm kotou\u010dem a ozuben\u00fdm v\u011bncem, kter\u00e9 se ot\u00e1\u010d\u00ed kolem vlastn\u00ed osy.
Matematick\u00fd model se skl\u00e1d\u00e1 z v\u00edce ne\u017e 1,6 milionu prvk\u016f. Ka\u017ed\u00fd p\u00e1r ozuben\u00fdch kol je reprezentov\u00e1n redukovan\u00fdm modelem s 500 vlastn\u00edmi m\u00f3dy. Vlastn\u00ed frekvence pro \u010deln\u00ed ozuben\u00e9 kolo je 70 kHz. Mod\u00e1ln\u011b redukovan\u00fd model je vhodn\u00fd pro cykloidn\u00ed p\u0159evodovku.
Matematick\u00fd model je validov\u00e1n pomoc\u00ed softwaru ABAQUS. Cykloidn\u00ed kotou\u010d byl diskretizov\u00e1n pro vytvo\u0159en\u00ed velmi jemn\u00e9ho modelu. Vy\u017eaduje 400 element\u00e1rn\u00edch bod\u016f na zub. Byl tak\u00e9 ov\u011b\u0159en pomoc\u00ed statick\u00e9 metody kone\u010dn\u00fdch prvk\u016f (MKP). Tento model byl pot\u00e9 pou\u017eit k modelov\u00e1n\u00ed t\u0159en\u00ed ozuben\u00fdch kol ve v\u0161ech kvadrantech. Jedn\u00e1 se o nov\u00fd p\u0159\u00edstup k modelov\u00e1n\u00ed t\u0159en\u00ed v cykloidn\u00ed p\u0159evodovce. Uk\u00e1zalo se, \u017ee poskytuje v\u00fdsledky srovnateln\u00e9 s v\u00fdsledky modelu EMBS. V\u00fdsledky jsou tak\u00e9 porovn\u00e1ny s elastick\u00fdm simula\u010dn\u00edm modelem v\u00edce t\u011bles. To dob\u0159e odpov\u00edd\u00e1 kontaktn\u00edm sil\u00e1m a velikosti cykloidn\u00edho ozuben\u00e9ho kotou\u010de. Bylo tak\u00e9 zji\u0161t\u011bno, \u017ee p\u0159esnost p\u0159enosu mezi cykloidn\u00edm ozuben\u00fdm kotou\u010dem a ozuben\u00fdm v\u011bncem je p\u0159ibli\u017en\u011b 98,51 TP3T. Tato hodnota je v\u0161ak ni\u017e\u0161\u00ed ne\u017e p\u0159esnost p\u0159enosu p\u00e1ru ozuben\u00fdch v\u011bnc\u016f. Chyba p\u0159enosu korigovan\u00e9ho modelu je p\u0159ibli\u017en\u011b 0,31 TP3T. P\u0159esnost p\u0159enosu je men\u0161\u00ed kv\u016fli men\u0161\u00ed velikosti elastick\u00e9 deformace na boc\u00edch zub\u016f.
Je d\u016fle\u017eit\u00e9 poznamenat, \u017ee nejp\u0159esn\u011bj\u0161\u00ed kontaktn\u00ed s\u00edly pro ka\u017ed\u00fd zub cykloidn\u00ed p\u0159evodovky nejsou plynul\u00e9. Kontaktn\u00ed s\u00edla na jednotliv\u00e9m zubu za\u010d\u00edn\u00e1 line\u00e1rn\u00edm n\u00e1r\u016fstem a pot\u00e9 kon\u010d\u00ed prudk\u00fdm poklesem. Nen\u00ed tak plynul\u00e1 jako kontaktn\u00ed s\u00edla na bodov\u00e9m kontaktu, a proto byla srovn\u00e1v\u00e1na s kontaktn\u00ed silou na eliptick\u00e9m kontaktu. Kontakt na eliptick\u00e9m kontaktu je v\u0161ak st\u00e1le relativn\u011b mal\u00fd a model EMBS to nedok\u00e1\u017ee zachytit.
Model kone\u010dn\u00fdch prvk\u016f pro cykloidn\u00ed kotou\u010d obsahuje p\u0159ibli\u017en\u011b 1,6 milionu prvk\u016f. Nejd\u016fle\u017eit\u011bj\u0161\u00ed \u010d\u00e1st\u00ed modelu kone\u010dn\u00fdch prvk\u016f je diskretizace cykloidn\u00edho kotou\u010de. Je velmi d\u016fle\u017eit\u00e9 prov\u00e9st diskretizaci cykloidn\u00edho ozuben\u00e9ho kotou\u010de velmi pe\u010dliv\u011b kv\u016fli vysok\u00e9mu stupni vibrac\u00ed, kter\u00fdm je vystaven. Cykloidn\u00ed kotou\u010d mus\u00ed b\u00fdt diskretizov\u00e1n jemn\u011b, aby v\u00fdsledky byly srovnateln\u00e9 s v\u00fdsledky statick\u00e9ho v\u00fdpo\u010dtu kone\u010dn\u00fdch prvk\u016f. Mus\u00ed se jednat o co nejp\u0159esn\u011bj\u0161\u00ed model, aby bylo mo\u017en\u00e9 p\u0159esn\u011b simulovat kontaktn\u00ed s\u00edly mezi cykloidn\u00edm kotou\u010dem a ozuben\u00fdm v\u011bncem.![\"spir\u00e1lov\u00e1](\"https:\/\/img.hzpt.com\/img\/cycloidalgearbox\/c-cycloidalgearbox-5.webp\" "\\"\\"")
<\/p>\n
Kinematika cykloidn\u00edho pohonu<\/h2>\n
Pomoc\u00ed libovoln\u00e9ho sou\u0159adnicov\u00e9ho syst\u00e9mu m\u016f\u017eeme pozorovat pohyb sou\u010d\u00e1st\u00ed cykloidn\u00ed p\u0159evodovky. Pozorujeme, \u017ee cykloidn\u00ed kotou\u010d se ot\u00e1\u010d\u00ed kolem pevn\u00fdch \u010dep\u016f po kruhu, zat\u00edmco h\u0159\u00eddel un\u00e1\u0161e\u010de se ot\u00e1\u010d\u00ed kolem excentrick\u00e9 va\u010dky. D\u00e1le vid\u00edme, \u017ee vstupn\u00ed h\u0159\u00eddel je ulo\u017een excentricky vzhledem k valiv\u00e9mu lo\u017eisku.
Tak\u00e9 pozorujeme, \u017ee cykloidn\u00ed kotou\u010d se ot\u00e1\u010d\u00ed nez\u00e1visle kolem excentrick\u00e9ho lo\u017eiska, zat\u00edmco h\u0159\u00eddel un\u00e1\u0161e\u010de se ot\u00e1\u010d\u00ed kolem osy symetrie. M\u016f\u017eeme konstatovat, \u017ee cykloidn\u00ed kotou\u010d hraje kl\u00ed\u010dovou roli v kinematice cykloidn\u00ed p\u0159evodovky.
Pro v\u00fdpo\u010det \u00fa\u010dinnosti cykloidn\u00edho reduktoru pou\u017e\u00edv\u00e1me model, kter\u00fd je zalo\u017een\u00fd na neline\u00e1rn\u00ed tuhosti kontakt\u016f. V tomto modelu je nelinearita kontaktu d\u00e1na nelinearitou s\u00edly a deformac\u00ed v kontaktu. Uk\u00e1zali jsme, \u017ee \u00fa\u010dinnost cykloidn\u00edho reduktoru se zvy\u0161uje se zvy\u0161uj\u00edc\u00edm se zat\u00ed\u017een\u00edm. Krom\u011b toho je \u00fa\u010dinnost z\u00e1visl\u00e1 na kluzn\u00e9 rychlosti a deformac\u00edch norm\u00e1lov\u00e9ho zat\u00ed\u017een\u00ed. Tyto faktory jsou pova\u017eov\u00e1ny za kl\u00ed\u010dov\u00e9 prom\u011bnn\u00e9 pro ur\u010den\u00ed \u00fa\u010dinnosti cykloidn\u00edho pohonu.
Tak\u00e9 zohled\u0148ujeme \u00fa\u010dinnost cykloidn\u00edho reduktoru se vstupn\u00edm to\u010div\u00fdm momentem a vstupn\u00ed rychlost\u00ed. \u00da\u010dinnost m\u016f\u017eeme vypo\u010d\u00edtat vyd\u011blen\u00edm \u010dist\u00e9ho to\u010div\u00e9ho momentu v ozuben\u00e9m v\u011bnci v\u00fdstupn\u00edm to\u010div\u00fdm momentem. \u00da\u010dinnost lze upravit tak, aby vyhovovala r\u016fzn\u00fdm provozn\u00edm podm\u00ednk\u00e1m. \u00da\u010dinnost cykloidn\u00edho pohonu se zvy\u0161uje se zvy\u0161uj\u00edc\u00edm se zat\u00ed\u017een\u00edm.
Cykloidn\u00ed p\u0159evodovka je v\u00edcestup\u0148ov\u00e1 p\u0159evodovka s mal\u00fdm a velk\u00fdm h\u0159\u00eddelov\u00fdm \u010depem. M\u00e1 19 zub\u016f a mosazn\u00e9 podlo\u017eky. Vn\u011bj\u0161\u00ed kotou\u010de se pohybuj\u00ed proti sm\u011bru pohybu prost\u0159edn\u00edho kotou\u010de a jsou posunuty o 180 stup\u0148\u016f. Prost\u0159edn\u00ed kotou\u010d je dvakr\u00e1t masivn\u011bj\u0161\u00ed ne\u017e vn\u011bj\u0161\u00ed kotou\u010d. Cykloidn\u00ed kotou\u010d m\u00e1 dev\u011bt lalok\u016f, kter\u00e9 se p\u0159i jedn\u00e9 ot\u00e1\u010dce hnac\u00ed h\u0159\u00eddele posunou o jeden lalok. Po\u010det \u010dep\u016f v kotou\u010di by m\u011bl b\u00fdt men\u0161\u00ed ne\u017e po\u010det \u010dep\u016f v okoln\u00edch \u010depech.
Vstupn\u00ed h\u0159\u00eddel poh\u00e1n\u00ed excentrick\u00e9 lo\u017eisko, kter\u00e9 je schopno p\u0159en\u00e1\u0161et v\u00fdkon na v\u00fdstupn\u00ed h\u0159\u00eddel. Vstupn\u00ed h\u0159\u00eddel nav\u00edc p\u016fsob\u00ed na cykloidn\u00ed kotou\u010d prost\u0159ednictv\u00edm mezilehl\u00e9ho lo\u017eiska silami. Cykloidn\u00ed kotou\u010d se pot\u00e9 posouv\u00e1 v kroc\u00edch o 360 stup\u0148\u016f\/ot\u00e1\u010den\u00ed\/kladka. \u010cepy v\u00fdstupn\u00edho h\u0159\u00eddele se pot\u00e9 pohybuj\u00ed v otvorech, \u010d\u00edm\u017e se v\u00fdstupn\u00ed h\u0159\u00eddel nep\u0159etr\u017eit\u011b ot\u00e1\u010d\u00ed. Vstupn\u00ed h\u0159\u00eddel vykon\u00e1v\u00e1 sinusov\u00fd pohyb, aby udr\u017eovala konstantn\u00ed ot\u00e1\u010dky z\u00e1kladn\u00edho h\u0159\u00eddele. Tato sinusov\u00e1 vlna zp\u016fsobuje mal\u00e9 zm\u011bny ot\u00e1\u010den\u00ed h\u0159\u00eddele un\u00e1\u0161e\u010de. S\u00edly p\u016fsob\u00edc\u00ed na vnit\u0159n\u00ed pouzdra jsou sou\u010d\u00e1st\u00ed rovnov\u00e1\u017en\u00e9ho mechanismu.
D\u00e1le m\u016f\u017eeme pozorovat, \u017ee cykloidn\u00ed pohon je schopen p\u0159en\u00e1\u0161et v\u011bt\u0161\u00ed to\u010div\u00fd moment ne\u017e planetov\u00e9 soukol\u00ed. To je d\u00e1no v\u011bt\u0161\u00ed axi\u00e1ln\u00ed d\u00e9lkou cykloidn\u00edho soukol\u00ed a men\u0161\u00edm pr\u016fm\u011brem otvoru v ozuben\u00e9m v\u011bnci. Je tak\u00e9 mo\u017en\u00e9 dos\u00e1hnout tvarov\u00e9ho ulo\u017een\u00ed mezi pevn\u00fdm krou\u017ekem a kotou\u010dem, \u010deho\u017e je dosa\u017eeno ozuben\u00edm mezi pevn\u00fdm krou\u017ekem a kotou\u010dem. Cykloidn\u00ed kotou\u010d je obvykle navr\u017een s kr\u00e1tkou cykloidou, aby se minimalizovaly nevyv\u00e1\u017een\u00e9 s\u00edly p\u0159i vysok\u00fdch rychlostech.![\"spir\u00e1lov\u00e1](\"https:\/\/img.hzpt.com\/img\/cycloidalgearbox\/b-cycloidalgearbox-5.webp\" "\\"\\"")
<\/p>\n
Srovn\u00e1n\u00ed s planetov\u00fdmi p\u0159evodovkami<\/h2>\n
Ve srovn\u00e1n\u00ed s planetov\u00fdmi p\u0159evodovkami m\u00e1 cykloidn\u00ed p\u0159evodovka n\u011bkolik v\u00fdhod. Mezi tyto v\u00fdhody pat\u0159\u00ed: n\u00edzk\u00e1 v\u016fle, lep\u0161\u00ed p\u0159et\u00ed\u017eitelnost, kompaktn\u00ed konstrukce a schopnost pou\u017e\u00edvat v \u0161irok\u00e9 \u0161k\u00e1le aplikac\u00ed. Cykloidn\u00ed p\u0159evodovka se stala popul\u00e1rn\u00ed na trhu s v\u00edceosou robotikou. P\u0159evodovka se tak\u00e9 st\u00e1le \u010dast\u011bji pou\u017e\u00edv\u00e1 v prvn\u00edch kloubech a polohova\u010d\u00edch.
Cykloidn\u00ed p\u0159evodovka je p\u0159evodovka, kter\u00e1 se skl\u00e1d\u00e1 ze \u010dty\u0159 z\u00e1kladn\u00edch sou\u010d\u00e1st\u00ed: cykloidn\u00edho kotou\u010de, v\u00fdstupn\u00ed p\u0159\u00edruby, ozuben\u00e9ho v\u011bnce a pevn\u00e9ho v\u011bnce. Cykloidn\u00ed kotou\u010d je poh\u00e1n\u011bn excentrickou h\u0159\u00eddel\u00ed, kter\u00e1 se ot\u00e1\u010d\u00ed o 360 stup\u0148\u016f\/oto\u010dn\u011b\/v\u00e1le\u010dn\u011b. V\u00fdstupn\u00ed p\u0159\u00edruba je kotou\u010d s pevn\u00fdm \u010depem, kter\u00fd p\u0159en\u00e1\u0161\u00ed v\u00fdkon na v\u00fdstupn\u00ed h\u0159\u00eddel. Ozuben\u00fd v\u011bnec je pevn\u00fd v\u011bnec a vstupn\u00ed h\u0159\u00eddel je p\u0159ipojen k servomotoru.
Cykloidn\u00ed p\u0159evodovka je navr\u017eena pro \u0159\u00edzen\u00ed setrva\u010dnosti ve vysoce dynamick\u00fdch situac\u00edch. Tyto p\u0159evodovky se obecn\u011b pou\u017e\u00edvaj\u00ed v robotice a polohova\u010d\u00edch, kde se pou\u017e\u00edvaj\u00ed k polohov\u00e1n\u00ed t\u011b\u017ek\u00fdch b\u0159emen. B\u011b\u017en\u011b se tak\u00e9 pou\u017e\u00edvaj\u00ed v \u0161irok\u00e9 \u0161k\u00e1le pr\u016fmyslov\u00fdch aplikac\u00ed. Maj\u00ed vy\u0161\u0161\u00ed hustotu to\u010div\u00e9ho momentu a n\u00edzkou v\u016fli, d\u00edky \u010demu\u017e jsou ide\u00e1ln\u00ed pro t\u011b\u017ek\u00e1 b\u0159emena.
V\u00fdstupn\u00ed p\u0159\u00edruba je tak\u00e9 navr\u017eena pro to\u010div\u00fd moment a\u017e 500 Nm. Jej\u00ed ot\u00e1\u010dky jsou ni\u017e\u0161\u00ed ne\u017e u planetov\u00e9 p\u0159evodovky, ale v\u00fdstupn\u00ed to\u010div\u00fd moment je mnohem vy\u0161\u0161\u00ed. Je navr\u017eena jako vysoce v\u00fdkonn\u00e1 p\u0159evodovka a lze ji pou\u017e\u00edt v aplikac\u00edch, kter\u00e9 vy\u017eaduj\u00ed vysok\u00e9 p\u0159evodov\u00e9 pom\u011bry a vysokou hustotu to\u010div\u00e9ho momentu. Cykloidn\u00ed p\u0159evodovka je tak\u00e9 levn\u011bj\u0161\u00ed a m\u00e1 men\u0161\u00ed v\u016fli. Cykloidn\u00ed p\u0159evodovka m\u00e1 v\u0161ak nev\u00fdhody, kter\u00e9 je t\u0159eba p\u0159i n\u00e1vrhu p\u0159evodovky zohlednit. Hlavn\u00edm probl\u00e9mem jsou vibrace.
Ve srovn\u00e1n\u00ed s planetov\u00fdmi p\u0159evodovkami maj\u00ed cykloidn\u00ed p\u0159evodovky men\u0161\u00ed celkov\u00e9 rozm\u011bry a jsou levn\u011bj\u0161\u00ed. Cykloidn\u00ed p\u0159evodovka m\u00e1 nav\u00edc velk\u00fd reduk\u010dn\u00ed pom\u011br v jednom stupni. Obecn\u011b maj\u00ed cykloidn\u00ed p\u0159evodovky jeden nebo dva stupn\u011b, p\u0159i\u010dem\u017e t\u0159et\u00ed stupe\u0148 je m\u00e9n\u011b \u010dast\u00fd. Cykloidn\u00ed p\u0159evodovka v\u0161ak nen\u00ed jedin\u00fdm typem p\u0159evodovky s t\u00edmto typem konfigurace. B\u011b\u017en\u011b se tak\u00e9 vyskytuje planetov\u00e1 p\u0159evodovka s jedn\u00edm stupn\u011bm.
Existuje n\u011bkolik r\u016fzn\u00fdch typ\u016f cykloidn\u00edch p\u0159evodovek a \u010dasto se ozna\u010duj\u00ed jako cykloidn\u00ed reduktory rychlosti. Tyto p\u0159evodovky jsou ur\u010deny pro jak\u00e9koli odv\u011btv\u00ed, kter\u00e9 pou\u017e\u00edv\u00e1 serva. Jsou krat\u0161\u00ed ne\u017e planetov\u00e9 p\u0159evodovky a maj\u00ed v\u011bt\u0161\u00ed pr\u016fm\u011br pro stejn\u00fd to\u010div\u00fd moment. N\u011bkter\u00e9 z nich jsou k dispozici i s p\u0159evodov\u00fdm pom\u011brem ni\u017e\u0161\u00edm ne\u017e 30:1.
Cykloidn\u00ed p\u0159evodovka m\u016f\u017ee b\u00fdt dobrou volbou pro aplikace s vysok\u00fdmi ot\u00e1\u010dkami a po\u017eadavky na vysok\u00fd to\u010div\u00fd moment. Tyto p\u0159evodovky jsou tak\u00e9 kompaktn\u011bj\u0161\u00ed ne\u017e planetov\u00e9 p\u0159evodovky a jsou vhodn\u00e9 pro aplikace s vysok\u00fdm to\u010div\u00fdm momentem. Krom\u011b toho jsou robustn\u011bj\u0161\u00ed a zvl\u00e1daj\u00ed r\u00e1zov\u00e1 zat\u00ed\u017een\u00ed. Maj\u00ed tak\u00e9 n\u00edzkou v\u016fli a vy\u0161\u0161\u00ed \u00farove\u0148 p\u0159esnosti a polohov\u00e1n\u00ed. Pou\u017e\u00edvaj\u00ed se tak\u00e9 v \u0161irok\u00e9 \u0161k\u00e1le aplikac\u00ed, v\u010detn\u011b pr\u016fmyslov\u00e9 robotiky.
![\"\u00da\u010dinnost](\"https:\/\/img.hzpt.com\/img\/cycloidalgearbox\/cycloidalgearbox-l1.webp\" "\\"\\"")
![\"\u00da\u010dinnost](\"https:\/\/img.hzpt.com\/img\/cycloidalgearbox\/cycloidalgearbox-l2.webp\" "\\"\\"")
editor od czh 2023-01-18<\/p>","protected":false},"excerpt":{"rendered":"
Merchandise Description HangZhou Gearbox R K F S Sequence Helical Equipment Motors Company Information\u00a0 \u00a0\u00a0\u00a0HangZhou Gearbox Producing Co., Ltd.\u00a0registered in\u00a01979. The organization is situated at national higher-tech growth zone, HangZhou, ZheJiang , China, with a lot more than\u00a038\u00a0years\u00a0experience to specialize in reserch and advancement equipment transmission products. The manufacturing facility covers an location of\u00a087,000\u00a0square meters. […]<\/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":[4355,4362,2253,4518,1772,2256,52,2257,4519,54,1170,4520,4521,1612,59,60,1775,61,4467,717,4522,1378,4468,4469,1845,4523,1846,4364,4472,4470,4471,4366,4524],"class_list":["post-2846","post","type-post","status-publish","format-standard","hentry","category-product-catalog","tag-china-gearbox","tag-china-motors","tag-cycloidal-drive","tag-cycloidal-gear-motors","tag-cycloidal-gearbox","tag-drive-gear","tag-gear","tag-gear-drive","tag-gear-drive-motors","tag-gear-gearbox","tag-gear-motors","tag-gear-motors-drive","tag-gear-motors-gearbox","tag-gear-s","tag-gearbox","tag-gearbox-china","tag-gearbox-cycloidal","tag-gearbox-gear","tag-gearbox-motors","tag-helical-gear","tag-helical-gear-motors","tag-helical-gearbox","tag-helical-motors","tag-helical-motors-gearbox","tag-k-gearbox","tag-k-series-gear-motors","tag-k-series-gearbox","tag-motors","tag-motors-drive","tag-motors-gearbox","tag-motors-gearbox-china","tag-motors-motors","tag-r-series-gear-motors"],"_links":{"self":[{"href":"https:\/\/cyclogearreducer.top\/cs\/wp-json\/wp\/v2\/posts\/2846","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=2846"}],"version-history":[{"count":0,"href":"https:\/\/cyclogearreducer.top\/cs\/wp-json\/wp\/v2\/posts\/2846\/revisions"}],"wp:attachment":[{"href":"https:\/\/cyclogearreducer.top\/cs\/wp-json\/wp\/v2\/media?parent=2846"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/cyclogearreducer.top\/cs\/wp-json\/wp\/v2\/categories?post=2846"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/cyclogearreducer.top\/cs\/wp-json\/wp\/v2\/tags?post=2846"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}