{"id":2381,"date":"2026-06-26T03:40:24","date_gmt":"2026-06-26T03:40:24","guid":{"rendered":"https:\/\/helicalcutgears.top\/?p=2381"},"modified":"2026-06-26T03:40:24","modified_gmt":"2026-06-26T03:40:24","slug":"helical-gear-profile-shift-addendum-modification","status":"publish","type":"post","link":"https:\/\/helicalcutgears.top\/tr\/helical-gear-profile-shift-addendum-modification\/","title":{"rendered":"Profil Kayd\u0131rmal\u0131 Helisel Di\u015fliler \u2014 Alt Kesimi \u00d6nlemek ve Merkez Mesafesini D\u00fczeltmek \u0130\u00e7in Ek Par\u00e7a Modifikasyonunun Kullan\u0131m\u0131"},"content":{"rendered":"
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Profil Kayd\u0131rmal\u0131 Helisel Di\u015fliler \u2014 Ek De\u011fi\u015fiklik, Alt Kesme \u00d6nleme ve Merkez Mesafesi D\u00fczeltmesi<\/h1>\n

Profil de\u011fi\u015fikli\u011fi helisel di\u015fli<\/strong> \u2014 di\u015fli frezeleme s\u0131ras\u0131nda kesici tak\u0131m\u0131n di\u015fli bo\u015flu\u011funa g\u00f6re kas\u0131tl\u0131 olarak yer de\u011fi\u015ftirmesi \u2014 en g\u00fc\u00e7l\u00fc ancak en az anla\u015f\u0131lan tasar\u0131m ara\u00e7lar\u0131ndan biridir. helisel di\u015fli<\/strong> Do\u011fru uygulanan bir profil kaymas\u0131, d\u00fc\u015f\u00fck di\u015f say\u0131s\u0131na sahip pinyonlarda di\u015f k\u00f6k\u00fc a\u015f\u0131nmas\u0131n\u0131 \u00f6nleyebilir, standart d\u0131\u015f\u0131 bir mod\u00fcle ba\u015fvurmadan standart d\u0131\u015f\u0131 bir merkez mesafesini d\u00fczeltebilir ve aksi takdirde e\u015fit olmayan hizmet \u00f6m\u00fcrlerine sahip olacak bir pinyon ve di\u015fli \u00e7ark aras\u0131ndaki e\u011filme yorulma \u00f6mr\u00fcn\u00fc dengeleyebilir.<\/p>\n

Helisel Di\u015fliniz \u0130\u00e7in Profil Kaymas\u0131n\u0131 Belirtin \u2192<\/a><\/p>\n<\/div>\n<\/div>\n

Profil Kaymas\u0131 Nedir? \u2014 Kesici Tak\u0131m Yer De\u011fi\u015ftirme Kavram\u0131<\/h2>\n

Standart olarak helisel di\u015fli<\/strong> \u00dcretimde (x = 0), kesici tak\u0131m referans \u00e7izgisi, frezeleme veya \u015fekillendirme s\u0131ras\u0131nda di\u015flinin hat dairesine te\u011fettir. Profil kaymas\u0131 bu referans \u00e7izgisini radyal olarak hareket ettirir: pozitif kayma (x > 0), kesiciyi d\u0131\u015fa do\u011fru -di\u015fli ekseninden uza\u011fa- hareket ettirir; bu da ek b\u00f6lgeden daha fazla malzeme \u00e7\u0131kar\u0131r ve alt b\u00f6lgede daha fazla malzeme b\u0131rak\u0131r. Sonu\u00e7 olarak, ek b\u00f6lgede daha y\u00fcksek (daha uzun invol\u00fct yan y\u00fczey) ve k\u00f6k dolgusunda daha kal\u0131n bir di\u015f elde edilir:<\/p>\n

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Pozitif Profil Kaymas\u0131 (+x)<\/p>\n

Kesici, di\u015fli ekseninden d\u0131\u015far\u0131 do\u011fru hareket etti. helisel di\u015fli<\/strong> Di\u015f \u015fu \u00f6zelliklere sahip olur: k\u00f6k k\u0131sm\u0131nda daha kal\u0131nla\u015f\u0131r (b\u00fck\u00fclme yorgunlu\u011funa kar\u015f\u0131 daha g\u00fc\u00e7l\u00fc); aktif invol\u00fct yan y\u00fczeyi daha uzun olur; ucu biraz daha daral\u0131r. \u0130nvol\u00fct, taban \u00e7emberine daha yak\u0131n ba\u015flar; bu da d\u00fc\u015f\u00fck di\u015f say\u0131s\u0131na sahip pinyonlarda alt kesme riskini azalt\u0131r.<\/p>\n<\/div>\n

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Negatif Profil Kaymas\u0131 (\u2212x)<\/p>\n

Kesici, di\u015fli eksenine do\u011fru i\u00e7e do\u011fru hareket ettirilir. Di\u015f \u015fu hale gelir: k\u00f6kte incelir (daha zay\u0131f); aktif invol\u00fct yan y\u00fczey k\u0131sal\u0131r; u\u00e7 daha geni\u015f olur (sivri u\u00e7 riski azal\u0131r). Alt kesme riskini art\u0131r\u0131r. Esas olarak \u015fu ama\u00e7larla kullan\u0131l\u0131r: x\u2081 + x\u2082 = 0 oldu\u011funda ve yaln\u0131zca bir di\u015fli de\u011fi\u015ftirildi\u011finde \u00e7al\u0131\u015fma merkezi mesafesini azaltmak; veya e\u015fle\u015fen pinyonda pozitif bir kayma oldu\u011funda do\u011fru merkez mesafesini korumak (toplam d\u00fczeltme).<\/p>\n<\/div>\n<\/div>\n

Kullan\u0131m Durumu 1 \u2014 D\u00fc\u015f\u00fck Di\u015f Say\u0131s\u0131na Sahip Pinyonlarda Di\u015f K\u00f6k\u00fc A\u015f\u0131nmas\u0131n\u0131n \u00d6nlenmesi<\/h2>\n

Di\u015f k\u00f6k\u00fc alt\u0131 oyulmas\u0131, k\u00f6k dolgusundan materyal uzakla\u015ft\u0131rarak k\u00f6k\u00fc zay\u0131flat\u0131r. helisel di\u015fli<\/strong> Di\u015f say\u0131s\u0131, belirli bas\u0131n\u00e7 a\u00e7\u0131s\u0131 ve helis a\u00e7\u0131s\u0131 i\u00e7in minimum de\u011ferin alt\u0131na d\u00fc\u015ft\u00fc\u011f\u00fcnde ortaya \u00e7\u0131kar. helisel di\u015fli<\/strong> Normal bas\u0131n\u00e7 a\u00e7\u0131s\u0131 \u03b1_n = 20\u00b0 ve helis a\u00e7\u0131s\u0131 \u03b2 ile x = 0 noktas\u0131nda alt kesme olmaks\u0131z\u0131n minimum di\u015f say\u0131s\u0131 \u015f\u00f6yledir:<\/p>\n

z_min (x=0) = 2 \u00d7 cos \u03b2 \/ sin\u00b2\u03b1_t
\nburada \u03b1_t = arctan(tan \u03b1_n \/ cos \u03b2)<\/p>\n

\u03b2 = 20\u00b0 i\u00e7in: \u03b1_t = 21,17\u00b0, sin\u00b2\u03b1_t = 0,1303
\nz_min = 2 \u00d7 cos 20\u00b0 \/ 0.1303 = 2 \u00d7 0.9397 \/ 0.1303 = 14.4 \u2192 z_min'i yukar\u0131 yuvarlayal\u0131m = 15<\/p>\n

\u03b2 = 25\u00b0 i\u00e7in: \u03b1_t = 22,80\u00b0, sin\u00b2\u03b1_t = 0,1500
\nz_min = 2 \u00d7 cos 25\u00b0 \/ 0,1500 = 2 \u00d7 0,9063 \/ 0,1500 = 12,1 \u2192 z_min = 13<\/p>\n

Pozitif bir profil kaymas\u0131 x ile, alt kesme olmaks\u0131z\u0131n minimum di\u015f say\u0131s\u0131 azal\u0131r. Sanal (normal d\u00fczlem) di\u015f say\u0131s\u0131 z_v = z \/ cos\u00b3\u03b2 i\u00e7in helisel di\u015fli<\/strong>x kayd\u0131rmas\u0131yla alt kesme olmaks\u0131z\u0131n minimum z_v de\u011feri yakla\u015f\u0131k olarak \u015f\u00f6yledir:<\/p>\n

z_vmin (x kayd\u0131rmas\u0131yla) \u2248 2 \u00d7 (1 \u2212 x) \/ sin\u00b2\u03b1_n = 17.1 \u00d7 (1 \u2212 x) [\u03b1_n = 20\u00b0 i\u00e7in]<\/p>\n

Helisel di\u015fli \u00e7ark\u0131n minimum ger\u00e7ek di\u015f say\u0131s\u0131: z_min_actual = z_vmin \u00d7 cos\u00b3\u03b2<\/p>\n

\u03b1_n = 20\u00b0, \u03b2 = 20\u00b0 i\u00e7in \u00f6rnekler:
\nx = 0: z_vmin = 17,1 \u2192 z_min = 17,1 \u00d7 cos\u00b320\u00b0 = 14,2 \u2192 z_min = 15
\nx = 0,25: z_vmin = 12,8 \u2192 z_min = 12,8 \u00d7 0,830 = 10,6 \u2192 z_min = 11
\nx = 0,50: z_vmin = 8,55 \u2192 z_min = 8,55 \u00d7 0,830 = 7,1 \u2192 z_min = 8<\/p>\n

Pratik faydas\u0131:<\/strong> A helisel di\u015fli<\/strong> z\u2081 = 10 di\u015fli pinyon, x = 0'da ciddi bir alt kesme olmadan \u00fcretilemez; k\u00f6k yuvarlatmas\u0131 kesilir ve di\u015f k\u00f6k\u00fc \u00f6nemli \u00f6l\u00e7\u00fcde zay\u0131flar. x\u2081 = +0,50 ile ayn\u0131 z\u2081 = 10 pinyon, alt kesme olmadan \u00fcretilebilir ve k\u00f6k kal\u0131nl\u0131\u011f\u0131 standart x = 0 k\u00f6k\u00fcnden yakla\u015f\u0131k 15% daha fazlad\u0131r. Bu, pinyon di\u015f say\u0131s\u0131n\u0131n z = 15'in alt\u0131na d\u00fc\u015fmesi gereken alan k\u0131s\u0131tlamal\u0131 uygulamalarda \u00e7ok kompakt di\u015fli oranlar\u0131na olanak tan\u0131r.<\/div>\n

Kullan\u0131m Durumu 2 \u2014 Standart Olmayan Merkez Mesafesinin D\u00fczeltilmesi<\/h2>\n

Bir yedek par\u00e7a oldu\u011funda helisel di\u015fli<\/strong> Bir \u00e7ift, standart d\u0131\u015f\u0131 bir merkez mesafesine sahip (g\u00f6vde a\u015f\u0131nmas\u0131, tasar\u0131m varyasyonu veya emperyalden metrik sisteme d\u00f6n\u00fc\u015ft\u00fcrme nedeniyle) mevcut bir g\u00f6vdeye uymal\u0131d\u0131r; profil kayd\u0131rma, standart d\u0131\u015f\u0131 bir mod\u00fcl belirtmeden do\u011fru \u00e7al\u0131\u015fma merkez mesafesinin elde edilmesini sa\u011flar. Kayd\u0131r\u0131lm\u0131\u015f bir profil i\u00e7in \u00e7al\u0131\u015fma merkez mesafesi a_w helisel di\u015fli<\/strong> (x\u2081 + x\u2082 \u2260 0) \u00e7ifti \u015f\u00f6yledir:<\/p>\n

a_w = (z\u2081 + z\u2082) \u00d7 Mn \/ (2 \u00d7 cos \u03b2) \u00d7 cos \u03b1_t \/ cos \u03b1_wt
\n\u00c7al\u0131\u015fma enine bas\u0131n\u00e7 a\u00e7\u0131s\u0131 \u03b1_wt a\u015fa\u011f\u0131daki ko\u015fulu sa\u011flar:
\ninv \u03b1_wt = inv \u03b1_t + 2 \u00d7 (x\u2081 + x\u2082) \u00d7 tan \u03b1_n \/ (z\u2081 + z\u2082)<\/p>\n

Merkez mesafesi d\u00fczeltmesi i\u00e7in: Ger\u00e7ek g\u00f6vde merkez mesafesi a_act = 130,5 mm ise ancak M5 i\u00e7in standart merkez mesafesi (z\u2081=24, z\u2082=72, \u03b2=20\u00b0) a_std = 128,0 mm ise, fazlal\u0131k \u0394a = 2,5 mm'dir. Bunu sa\u011flamak i\u00e7in gereken profil kayd\u0131rmalar\u0131n\u0131n toplam\u0131:<\/p>\n

\u0394a = a_w \u2212 a_std = (z\u2081+z\u2082) \u00d7 Mn\/(2cos\u03b2) \u00d7 (cos \u03b1_t\/cos \u03b1_wt \u2212 1)<\/p>\n

\u0394a = 2,5 mm ve z\u2081+z\u2082 = 96, Mn=5, \u03b2=20\u00b0 i\u00e7in:
\ninv \u03b1_wt yinelemeli olarak bulunabilir \u2192 (x\u2081+x\u2082) \u2248 \u0394a \u00d7 cos \u03b2 \/ (Mn \u00d7 tan \u03b1_n) = 2,5 \u00d7 0,940 \/ (5 \u00d7 0,364) \u2248 1,29<\/p>\n

Bu, iki di\u015fli aras\u0131nda x\u2081 + x\u2082 \u2248 1,29'un da\u011f\u0131t\u0131lmas\u0131 gerekti\u011fi anlam\u0131na gelir.
\nPratik bir ayr\u0131m: x\u2081 = +0,70, x\u2082 = +0,59 \u2014 her ikisi de pozitif, her iki di\u015fli de k\u00f6k kuvveti kazan\u0131yor.<\/p>\n

\"Profil<\/p>\n

Hassas ta\u015flanm\u0131\u015f profil kayd\u0131rmal\u0131 helisel di\u015fli<\/strong> \u2014 Pozitif profil kaymas\u0131 (x > 0), daha geni\u015f di\u015f k\u00f6k\u00fc yuvarlatmas\u0131 ve hafif\u00e7e daralm\u0131\u015f di\u015f ucunda g\u00f6r\u00fclebilir. Profil kayma katsay\u0131s\u0131 x, \u00e7izimin di\u015fli veri tablosunda belirtilmi\u015ftir ve \u00f6l\u00e7\u00fclen W_k a\u00e7\u0131kl\u0131k \u00f6l\u00e7\u00fcm\u00fc ve taban te\u011fet uzunlu\u011fu sapmas\u0131ndan di\u015fli analiz\u00f6r\u00fc taraf\u0131ndan do\u011frulanm\u0131\u015ft\u0131r.<\/p>\n

Kullan\u0131m Durumu 3 \u2014 Pinyon ve Di\u015fli Aras\u0131nda Dengeli E\u011filme Yorulmas\u0131 (Niemann Y\u00f6ntemi)<\/h2>\n

Bir helisel di\u015fli<\/strong> u = z\u2082\/z\u2081 > 1 oran\u0131nda tahrikte, pinyon di\u015f k\u00f6k\u00fc, di\u015fli di\u015f k\u00f6k\u00fcne g\u00f6re birim zamanda u kat daha s\u0131k y\u00fcklenir. Bu nedenle pinyon, e\u011filme yorulma s\u0131n\u0131r\u0131na daha erken ula\u015f\u0131r - pinyona k\u00f6k kal\u0131nl\u0131\u011f\u0131n\u0131 ve k\u00f6k kiri\u015f gerilme d\u00fczeltme fakt\u00f6r\u00fcn\u00fc (Y_Sa) art\u0131rmak i\u00e7in pozitif bir profil kaymas\u0131 verilmedi\u011fi s\u00fcrece, di\u015fli ise e\u015fit b\u00fcy\u00fckl\u00fckte negatif bir kayma al\u0131r (merkez mesafesi de\u011fi\u015fmeden kal\u0131rsa x\u2081 + x\u2082 = 0). Dengeli e\u011filme i\u00e7in Niemann y\u00f6ntemi, ISO 6336-3 e\u011filme g\u00fcvenlik fakt\u00f6rleri S_F1 (pinyon) ve S_F2 (di\u015fli) yakla\u015f\u0131k olarak e\u015fit olacak \u015fekilde profil kaymas\u0131 da\u011f\u0131l\u0131m\u0131n\u0131 se\u00e7er:<\/p>\n

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Di\u015fli Oran\u0131 u = z\u2082\/z\u2081<\/th>\n\u00d6nerilen x\u2081 (di\u015fli)<\/th>\nx\u2082 (di\u015fli) = \u2212x\u2081 s\u0131f\u0131r toplaml\u0131<\/th>\nEtki<\/th>\n<\/tr>\n<\/thead>\n
u = 1,0 (e\u015fit di\u015f say\u0131s\u0131)<\/td>\nx\u2081 = 0 (kayd\u0131rma gerekmiyor)<\/td>\nx\u2082 = 0<\/td>\nHer iki di\u015fli de e\u015fit \u015fekilde y\u00fcklenmi\u015f; d\u00fczeltilmesi gereken bir dengesizlik yok.<\/td>\n<\/tr>\n
u = 2.0<\/td>\nx\u2081 \u2248 +0.15 ila +0.25<\/td>\nx\u2082 \u2248 \u22120.15 ila \u22120.25<\/td>\nPinyon k\u00f6k\u00fc g\u00fc\u00e7lendirilmi\u015f; di\u015fli k\u00f6k\u00fc hafif\u00e7e zay\u0131flam\u0131\u015f; net S_F1 \u2248 S_F2<\/td>\n<\/tr>\n
u = 3,0\u20134,0<\/td>\nx\u2081 \u2248 +0.30 ila +0.45<\/td>\nx\u2082 \u2248 \u22120.30 ila \u22120.45<\/td>\nPinyon di\u015flisinde \u00f6nemli k\u00f6k g\u00fc\u00e7lendirmesi; genellikle i = 3\u20134 end\u00fcstriyel tahrik sistemleri i\u00e7in standart \u00f6neridir.<\/td>\n<\/tr>\n
u = 5.0+<\/td>\nx\u2081 \u2248 +0,45 ila +0,60<\/td>\nx\u2082 \u2248 \u22120,45 ila \u22120,60<\/td>\nTekerlek \u00fczerinde yeterli u\u00e7 kal\u0131nl\u0131\u011f\u0131n\u0131 korumak i\u00e7in \u00f6nerilen maksimum aral\u0131k (u\u00e7 kal\u0131nl\u0131\u011f\u0131 \u2265 0,2 \u00d7 Mn gereklidir)<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<\/div>\n
1. Kontrol \u2014 U\u00e7 kal\u0131nl\u0131\u011f\u0131:<\/strong> Pinyon \u00fczerindeki pozitif bir kayma (x\u2081 > 0), di\u015f ucunu daralt\u0131r. Keskin u\u00e7 k\u0131r\u0131lmas\u0131n\u0131 \u00f6nlemek i\u00e7in, ek daire \u00fczerindeki minimum di\u015f ucu kal\u0131nl\u0131\u011f\u0131 \u2265 0,2 \u00d7 Mn olmal\u0131d\u0131r. Korea Ever-Power, her profil kaymas\u0131 i\u00e7in u\u00e7 kal\u0131nl\u0131\u011f\u0131n\u0131 hesaplar. helisel di\u015fli<\/strong> Sipari\u015f incelemesinin bir par\u00e7as\u0131 olarak, bu s\u0131n\u0131r\u0131n \u00f6tesinde daralan bir u\u00e7, kayd\u0131rmay\u0131 azaltmay\u0131 veya k\u00fc\u00e7\u00fck bir u\u00e7 pah\u0131 eklemeyi gerektirir.<\/p>\n

Kontrol 2 \u2014 Temas oran\u0131:<\/strong> B\u00fcy\u00fck bir toplam profil kaymas\u0131 (x\u2081 + x\u2082 > 0), \u00e7al\u0131\u015fma bas\u0131n\u00e7 a\u00e7\u0131s\u0131 \u03b1_wt'yi art\u0131r\u0131r ve bu da enine temas oran\u0131 \u03b5_\u03b1'y\u0131 azalt\u0131r. Korea Ever-Power, profil kaymas\u0131 uyguland\u0131ktan sonra toplam temas oran\u0131 \u03b5_\u03b3 = \u03b5_\u03b1 + \u03b5_\u03b2'nin \u2265 1,2 olarak kald\u0131\u011f\u0131n\u0131 do\u011frulam\u0131\u015ft\u0131r.<\/div>\n

Di\u015fli \u00c7iziminde Profil Kaymas\u0131 Nas\u0131l Belirtilir?<\/h2>\n

Profil kaymas\u0131, vites veri tablosunda belirtilir. helisel di\u015fli<\/strong> Boyutsuz katsay\u0131 x (normal d\u00fczlem referans\u0131) olarak \u00e7izim. Standart g\u00f6sterim:<\/p>\n

Di\u015fli veri tablosu sat\u0131r \u00f6rnekleri:
\nNormal mod\u00fcl: Mn = 5
\nNormal bas\u0131n\u00e7 a\u00e7\u0131s\u0131: \u03b1_n = 20\u00b0
\nHelis a\u00e7\u0131s\u0131: \u03b2 = 20\u00b0 RH
\nDi\u015f say\u0131s\u0131: z = 24
\nProfil kaymas\u0131: x = +0,35 \u2190 pinyon i\u00e7in pozitif kayma
\nMerkez mesafesi: a = 255,6 mm (\u00e7al\u0131\u015fma, kayd\u0131r\u0131lm\u0131\u015f \u00e7ift i\u00e7in a_w de\u011fil a_std)
\n\u00c7al\u0131\u015fma bas\u0131n\u00e7 a\u00e7\u0131s\u0131: \u03b1_wt = 22,4\u00b0 \u2190 x\u2081+x\u2082 \u2260 0 oldu\u011funda de\u011fi\u015fir<\/p>\n

E\u015fle\u015ftirilmi\u015f bir \u00fcr\u00fcn i\u00e7in helisel di\u015fli<\/strong> \u00c7ift di\u015fli ve pinyon \u00e7izimlerinde, her birinin x de\u011ferleri ve \u00e7iftin \u00e7al\u0131\u015fma merkezi mesafesi a_w belirtilmelidir. x\u2081 + x\u2082 toplam\u0131 ve elde edilen \u03b1_wt, her iki \u00e7izim aras\u0131nda tutarl\u0131 olmal\u0131d\u0131r. Korea Ever-Power, x\u2081 ve x\u2082'nin \u00e7apraz uyumlulu\u011funu do\u011frular. helisel di\u015fli<\/strong> \u00dcretimden \u00f6nce iki \u00e7izimin kendi i\u00e7lerinde tutarl\u0131 oldu\u011fundan emin olmak i\u00e7in e\u015fle\u015ftirme yap\u0131lmal\u0131d\u0131r; bu, profil kaymas\u0131 olan \u00e7iftler i\u00e7in m\u00fc\u015fteriye g\u00f6nderilen \u00e7izimlerde s\u0131k yap\u0131lan bir hatad\u0131r.<\/p>\n

Do\u011frulama \u2014 Di\u015fli Analiz Cihaz\u0131 Profil Kaymas\u0131n\u0131 Nas\u0131l Do\u011fruluyor?<\/h2>\n

\"Korea<\/p>\n

Korea Ever-Power di\u015fli analiz\u00f6r\u00fc, profil kaymas\u0131n\u0131 do\u011fruluyor. helisel di\u015fli<\/strong> \u2014 Analiz raporundaki a\u00e7\u0131kl\u0131k \u00f6l\u00e7\u00fcm\u00fc W_k (taban te\u011fet uzunlu\u011fu) ve di\u015f kal\u0131nl\u0131\u011f\u0131 b\u00f6l\u00fcm\u00fc, uygulanan profil kaymas\u0131 x'in \u00e7izim spesifikasyonuna uygun oldu\u011funu do\u011frular. Standart (x=0) nominal de\u011ferden daha y\u00fcksek bir W_k de\u011feri, pozitif bir kayman\u0131n uyguland\u0131\u011f\u0131n\u0131 g\u00f6sterir.<\/p>\n

Profil kaymas\u0131, a\u00e7\u0131kl\u0131k \u00f6l\u00e7\u00fcm\u00fc W_k ile dolayl\u0131 olarak do\u011frulan\u0131r: profil kaymas\u0131 olan bir profil i\u00e7in nominal W_k de\u011feri. helisel di\u015fli<\/strong> Di\u015f kal\u0131nl\u0131\u011f\u0131 teriminde kayma katk\u0131s\u0131n\u0131 i\u00e7erir. Korea Ever-Power, belirtilen her x de\u011feri i\u00e7in nominal W_k de\u011ferini hesaplar ve muayene sertifikas\u0131nda izin verilen W_k aral\u0131\u011f\u0131n\u0131 (profil kaymas\u0131 i\u00e7in d\u00fczeltilmi\u015f) bildirir; bu da m\u00fc\u015fterilerin gelen muayene s\u0131ras\u0131nda dijital kumpas ile x uyumlulu\u011funu do\u011frulamas\u0131na olanak tan\u0131r. Do\u011frudan bir helisel di\u015fli \u00fcreticisi<\/a>Korea Ever-Power, m\u00fc\u015fterilerinin tahrik parametrelerini ve g\u00f6vde merkez mesafesini vermeleri ko\u015fuluyla, alt kesme \u00f6nleme, merkez mesafesi d\u00fczeltme veya dengeli b\u00fckme i\u00e7in x\u2081 ve x\u2082 se\u00e7imi yaparak profil kayd\u0131rma tasar\u0131m\u0131 ger\u00e7ekle\u015ftirir. Daha fazla bilgi i\u00e7in inceleyin. helisel di\u015fli \u00fcr\u00fcn yelpazesi<\/a> T\u00fcm standart ve profil kayd\u0131rmal\u0131 konfig\u00fcrasyonlar i\u00e7in.<\/p>\n

S\u0131k\u00e7a Sorulan Sorular<\/h2>\n
Profil kaymas\u0131, helisel di\u015flinin taban dairesini veya mod\u00fcl\u00fcn\u00fc de\u011fi\u015ftirir mi?<\/strong><\/p>\n

\u0130kisi de de\u011fil. Profil kayd\u0131rma, taban dairesinin \u00e7ap\u0131n\u0131 (d_b = d \u00d7 cos \u03b1_t sabit kal\u0131r) veya mod\u00fcl\u00fc (Mn kesici taraf\u0131ndan belirlenir ve kayd\u0131rma ile de\u011fi\u015fmez) de\u011fi\u015ftirmez. De\u011fi\u015fen \u015fey, ad\u0131m dairesinin taban dairesine g\u00f6re konumu ve dolay\u0131s\u0131yla di\u015f oranlar\u0131d\u0131r (ek y\u00fckseklik, eksi derinlik, ad\u0131m dairesindeki di\u015f kal\u0131nl\u0131\u011f\u0131). Di\u015f yan y\u00fczeyinin invol\u00fct e\u011frisi, profil kayd\u0131rmadan \u00f6nce ve sonra ayn\u0131d\u0131r; kayd\u0131rma sadece ayn\u0131 invol\u00fct\u00fcn farkl\u0131 bir b\u00f6l\u00fcm\u00fcn\u00fc kullan\u0131r. Bu, profil kayd\u0131rmal\u0131 bir di\u015fin helisel di\u015fli<\/strong> Mn = 5 mod\u00fcl\u00fc ile, ayn\u0131 Mn ve \u03b1_n de\u011ferlerine sahip standart bir x = 0 di\u015flisiyle yine de do\u011fru \u015fekilde e\u015fle\u015febilir; profil hala ayn\u0131 taban \u00e7emberinin bir invol\u00fct\u00fcd\u00fcr, sadece onun boyunca kayd\u0131r\u0131lm\u0131\u015ft\u0131r.<\/p>\n<\/div>\n

Helisel di\u015fli pinyonu i\u00e7in maksimum g\u00fcvenli profil kaymas\u0131 nedir?<\/strong><\/p>\n

Kullan\u0131labilir maksimum pozitif profil kaymas\u0131, di\u015f ucu kal\u0131nl\u0131\u011f\u0131 ile s\u0131n\u0131rl\u0131d\u0131r: x artt\u0131k\u00e7a, di\u015f ucu daral\u0131r ve sonunda sivri hale gelir (u\u00e7 kal\u0131nl\u0131\u011f\u0131 \u2192 0). Pratik s\u0131n\u0131r, di\u015f ucu kal\u0131nl\u0131\u011f\u0131 s_a \u2265 0,2 \u00d7 Mn (Korea Ever-Power'\u0131n minimum standard\u0131) olacak \u015fekilde x_max't\u0131r. \u03b1_n = 20\u00b0, \u03b2 = 20\u00b0, z = 15 i\u00e7in: ek dairedeki u\u00e7 kal\u0131nl\u0131\u011f\u0131 s_a, invol\u00fct geometrisinden hesaplanabilir \u2014 sivrilmeden \u00f6nceki maksimum x, z = 15 i\u00e7in yakla\u015f\u0131k x_max \u2248 0,55\u20130,65'tir. z = 24 i\u00e7in: x_max \u2248 0,70\u20130,80. x_max'\u0131n \u00f6tesinde, minimum u\u00e7 kal\u0131nl\u0131\u011f\u0131n\u0131 korumak i\u00e7in di\u015f ucu k\u0131salt\u0131lmal\u0131d\u0131r (ek daire k\u00fc\u00e7\u00fcltme), bu da aktif profil uzunlu\u011funu ve dolay\u0131s\u0131yla temas oran\u0131n\u0131 azalt\u0131r. Korea Ever-Power, profil kaymas\u0131 olan her di\u015f i\u00e7in u\u00e7 kal\u0131nl\u0131\u011f\u0131 kontrol\u00fcn\u00fc ger\u00e7ekle\u015ftirir. helisel di\u015fli<\/strong>.<\/p>\n<\/div>\n

Mevcut bir di\u015fli \u00e7ark\u0131n profil kaymas\u0131, tak\u0131m tezgah\u0131nda de\u011fi\u015fiklik yap\u0131lmadan yeniden tasarlanabilir mi?<\/strong><\/p>\n

Evet \u2014 standart x = 0 di\u015fli i\u00e7in kullan\u0131lan ayn\u0131 freze b\u0131\u00e7a\u011f\u0131, radyal ilerleme derinli\u011fini (kesim s\u0131ras\u0131nda freze b\u0131\u00e7a\u011f\u0131 ekseni ile di\u015fli ekseni aras\u0131ndaki merkez mesafesi) ayarlayarak yakla\u015f\u0131k x = \u22120,5 ile x = +0,8 aras\u0131nda herhangi bir profil kaymas\u0131n\u0131 \u00fcretebilir. Yeni bir freze b\u0131\u00e7a\u011f\u0131na gerek yoktur. Profil kaymas\u0131 i\u00e7in helisel di\u015fli<\/strong> CNC ta\u015flama makinesi, benzer \u015fekilde yaz\u0131l\u0131m profil ayar\u0131 arac\u0131l\u0131\u011f\u0131yla kaymay\u0131 uygulamak i\u00e7in ta\u015flama d\u00f6ng\u00fcs\u00fcn\u00fc ayarlar; |x| \u2264 0,7 pratik aral\u0131\u011f\u0131nda ta\u015flama tekerle\u011fi bilemesinde herhangi bir de\u011fi\u015fiklik gerekmez. Korea Ever-Power, belirtilen herhangi bir profil kaymas\u0131n\u0131 herhangi bir i\u015fleme uygular. helisel di\u015fli<\/strong> Standart mod\u00fcl freze ve ta\u015flama ta\u015f\u0131 kombinasyonlar\u0131n\u0131 kullanarak, tak\u0131m de\u011fi\u015fikli\u011fi veya teslim s\u00fcresinde herhangi bir aksama olmadan.<\/p>\n<\/div>\n

Di\u015fli analiz\u00f6r\u00fc, helisel di\u015flinin do\u011fru profil kaymas\u0131na sahip olup olmad\u0131\u011f\u0131n\u0131 nas\u0131l belirler?<\/strong><\/p>\n

Di\u015fli analiz\u00f6r\u00fc, di\u015f kal\u0131nl\u0131\u011f\u0131 de\u011ferlendirmesinin bir par\u00e7as\u0131 olarak taban te\u011fet uzunlu\u011funu (a\u00e7\u0131kl\u0131k \u00f6l\u00e7\u00fcm\u00fc W_k'ye e\u015fde\u011fer) \u00f6l\u00e7er. Profil kaymas\u0131 durumunda helisel di\u015fli<\/strong>\u00d6l\u00e7\u00fclen W_k, x = 0 nominal de\u011ferini \u015fu kadar a\u015fmaktad\u0131r: \u0394W_k = 2 \u00d7 x \u00d7 Mn \u00d7 sin \u03b1_n \u00d7 cos \u03b1_n (profil kaymas\u0131n\u0131n a\u00e7\u0131kl\u0131k \u00f6l\u00e7\u00fcm\u00fcne katk\u0131s\u0131). Korea Ever-Power'\u0131n analiz\u00f6r raporlar\u0131, belirtilen x de\u011feri i\u00e7in nominal W_k de\u011ferini i\u00e7ermektedir, bu nedenle \u00f6l\u00e7\u00fclen W_k do\u011frudan kar\u015f\u0131la\u015ft\u0131r\u0131labilir \u2014 profil kaymas\u0131 d\u00fczeltilmi\u015f nominal de\u011ferin \u00fcst\u00fcnde veya alt\u0131nda \u00f6l\u00e7\u00fclen bir W_k, kesim s\u0131ras\u0131nda yanl\u0131\u015f kayman\u0131n uyguland\u0131\u011f\u0131n\u0131 g\u00f6sterir. Bu, standart di\u015f kal\u0131nl\u0131\u011f\u0131 \u00f6l\u00e7\u00fcm\u00fcn\u00fcn \u00f6tesinde herhangi bir \u00f6zel analiz\u00f6r kurulumuna gerek kalmadan profil kaymas\u0131 uyumlulu\u011funun basit bir say\u0131sal kontrol\u00fcn\u00fc sa\u011flar.<\/p>\n<\/div>\n

\n

Helisel Di\u015fli Uygulaman\u0131z \u0130\u00e7in Profil Kayd\u0131rma Tasar\u0131m\u0131<\/h2>\n

Di\u015f say\u0131n\u0131z\u0131, mod\u00fcl\u00fcn\u00fcz\u00fc, helis a\u00e7\u0131n\u0131z\u0131, ger\u00e7ek g\u00f6vde merkez mesafesini ve di\u015fli oran\u0131n\u0131z\u0131 belirtin. Korea Ever-Power, amac\u0131n\u0131za (alt kesme \u00f6nleme, merkez mesafesi d\u00fczeltme veya dengeli b\u00fckme) uygun do\u011fru x\u2081 ve x\u2082 de\u011ferlerini hesaplar ve \u00fcretim \u00f6ncesinde u\u00e7 kal\u0131nl\u0131\u011f\u0131n\u0131 ve temas oran\u0131n\u0131 do\u011frular.<\/p>\n

Profil Kayd\u0131rma Hesaplamas\u0131 Talebi<\/a>
\nHelisel Di\u015fli \u00dcr\u00fcn Yelpazesi<\/a><\/div>\n

x katsay\u0131s\u0131 tasar\u0131m\u0131 \u00b7 Alt kesme kontrol\u00fc \u00b7 U\u00e7 kal\u0131nl\u0131\u011f\u0131 do\u011frulamas\u0131 \u00b7 Temas oran\u0131 kontrol\u00fc \u00b7 Muayene i\u00e7in W_k aral\u0131\u011f\u0131 \u00b7 Tak\u0131m de\u011fi\u015fikli\u011fi yok<\/p>\n<\/div>\n

Edit\u00f6r: Cxm<\/p>\n<\/div>","protected":false},"excerpt":{"rendered":"

Profil Kayd\u0131rmal\u0131 Helisel Di\u015fliler \u2014 Ek De\u011fi\u015fiklik, Alt Kesme \u00d6nleme ve Merkez Mesafesi D\u00fczeltmesi Helisel di\u015flilerde profil kayd\u0131rma \u2014 frezeleme s\u0131ras\u0131nda kesici tak\u0131m\u0131n di\u015fli bo\u015flu\u011funa g\u00f6re kas\u0131tl\u0131 olarak yer de\u011fi\u015ftirmesi \u2014 helisel di\u015fli spesifikasyonunda en g\u00fc\u00e7l\u00fc ancak en az anla\u015f\u0131lan tasar\u0131m ara\u00e7lar\u0131ndan biridir. Do\u011fru uygulanan bir profil kayd\u0131rma [\u2026]<\/p>","protected":false},"author":1,"featured_media":0,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"_et_pb_use_builder":"","_et_pb_old_content":"","_et_gb_content_width":"","footnotes":""},"categories":[3082],"tags":[],"class_list":["post-2381","post","type-post","status-publish","format-standard","hentry","category-helical-gears"],"_links":{"self":[{"href":"https:\/\/helicalcutgears.top\/tr\/wp-json\/wp\/v2\/posts\/2381","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/helicalcutgears.top\/tr\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/helicalcutgears.top\/tr\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/helicalcutgears.top\/tr\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/helicalcutgears.top\/tr\/wp-json\/wp\/v2\/comments?post=2381"}],"version-history":[{"count":1,"href":"https:\/\/helicalcutgears.top\/tr\/wp-json\/wp\/v2\/posts\/2381\/revisions"}],"predecessor-version":[{"id":2382,"href":"https:\/\/helicalcutgears.top\/tr\/wp-json\/wp\/v2\/posts\/2381\/revisions\/2382"}],"wp:attachment":[{"href":"https:\/\/helicalcutgears.top\/tr\/wp-json\/wp\/v2\/media?parent=2381"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/helicalcutgears.top\/tr\/wp-json\/wp\/v2\/categories?post=2381"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/helicalcutgears.top\/tr\/wp-json\/wp\/v2\/tags?post=2381"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}