{"id":3632,"date":"2019-07-05T01:08:27","date_gmt":"2019-07-05T01:08:27","guid":{"rendered":"https:\/\/www.mcctcarbide.com\/?p=3632"},"modified":"2020-05-06T03:48:31","modified_gmt":"2020-05-06T03:48:31","slug":"why-turning-tools-corner-radius-or-edge-radius-so-critical","status":"publish","type":"post","link":"https:\/\/www.meetyoucarbide.com\/tr\/neden-torna-araclari-kose-yaricap-veya-kenar-yaricap-cok-kritik\/","title":{"rendered":"Neden Tak\u0131m\u0131n K\u00f6\u015fe Yar\u0131\u00e7ap\u0131 veya Kenar Yar\u0131\u00e7ap\u0131 bu kadar Kritik?"},"content":{"rendered":"
A\u015fa\u011f\u0131daki \u015fekilde g\u00f6sterildi\u011fi gibi, k\u00f6\u015fe yar\u0131\u00e7ap\u0131, \u00e7apraz \u00e7izgi ana kesme kenar\u0131 ve kenar kesme kenar\u0131 olarak da adland\u0131r\u0131lan yan kesme kenar\u0131 taraf\u0131ndan olu\u015fturulur.<\/p>\n\n\n\n \u015eekil 1'deki kar\u015f\u0131la\u015ft\u0131rma sayesinde, tak\u0131m ucu rady\u00fcs\u00fcn\u00fcn yar\u0131\u00e7ap\u0131n\u0131n ve d\u00f6nme ba\u015f\u0131na ilerlemenin, i\u015f par\u00e7as\u0131n\u0131n y\u00fczey p\u00fcr\u00fczl\u00fcl\u00fc\u011f\u00fc \u00fczerinde en b\u00fcy\u00fck etkiye sahip oldu\u011fu g\u00f6r\u00fclebilir. se\u00e7ilmelidir. A\u015fa\u011f\u0131daki \u015fekil, bu \u00fc\u00e7 \u00f6\u011fenin de\u011ferleri aras\u0131ndaki ili\u015fkinin bir referans tablosudur. Genellikle, tak\u0131m ucunun k\u00f6\u015fe yar\u0131\u00e7ap\u0131 besleme h\u0131z\u0131n\u0131n \u00fc\u00e7 ila d\u00f6rt kat\u0131 i\u00e7in uygundur.<\/p>\n\n\n\n r k\u00f6\u015fe yar\u0131\u00e7ap\u0131 mm<\/p>\n\n\n\n f Rot ba\u015f\u0131na maksimum ilerleme. mm<\/p>\n\n\n\n Ra P\u00fcr\u00fczl\u00fcl\u00fck \u03bcm<\/p>\n\n\n\n Tak\u0131m ucu rady\u00fcs\u00fcn\u00fcn yar\u0131\u00e7ap\u0131n\u0131 ve d\u00f6n\u00fc\u015f ba\u015f\u0131na ilerlemeyi se\u00e7mek i\u00e7in, teorik ampirik form\u00fcl (1) ile de belirlenebilir.<\/p>\n\n\n\n Ra = f2<\/sup>\/ R * 125<\/p>\n\n\n\n burada: <\/p>\n\n\n\n Ra (\u03bcm) - y\u00fczey p\u00fcr\u00fczl\u00fcl\u00fc\u011f\u00fc;<\/p>\n\n\n\n f (mm \/ devir) - devir ba\u015f\u0131na ilerleme;<\/p>\n\n\n\n r (mm) - alet ucu ark\u0131n\u0131n yar\u0131\u00e7ap\u0131;<\/p>\n\n\n\n 125 - sabit.<\/p>\n\n\n\n Tak\u0131m ucu rady\u00fcs\u00fcn\u00fcn yar\u0131\u00e7ap\u0131n\u0131n ayar de\u011ferini ve besleme miktar\u0131n\u0131 (1) de\u011fi\u015ftirerek, teorik y\u00fczey p\u00fcr\u00fczl\u00fcl\u00fc\u011f\u00fcn\u00fc ve y\u00fczey p\u00fcr\u00fczl\u00fcl\u00fc\u011f\u00fcn\u00fc de hesaplayabiliriz.<\/p>\n\n\n\n \u00d6rn: Tak\u0131m ucu ark\u0131n\u0131n yar\u0131\u00e7ap\u0131 0,8 mm'dir ve ilerleme h\u0131z\u0131<\/p>\n\n\n\n 0.2 mm \/ r, teorik y\u00fczey p\u00fcr\u00fczl\u00fcl\u00fc\u011f\u00fc i\u00e7in ikame form\u00fcl\u00fc (1).<\/p>\n\n\n\n Ra = 0.22<\/sup>\/0.8*125=6.25\u03bcm<\/p>\n\n\n\n Teorik y\u00fczey p\u00fcr\u00fczl\u00fcl\u00fc\u011f\u00fc: 6.25 \u03bcm<\/p>\n\n\n\n
Kesme i\u015fleminde, tak\u0131m ucu mukavemetini artt\u0131rmak ve makinenin y\u00fczey p\u00fcr\u00fczl\u00fcl\u00fc\u011f\u00fcn\u00fc azaltmak i\u00e7in, genellikle tak\u0131m burnunda dairesel bir ark ge\u00e7i\u015f kenar\u0131 bulunur. Ayr\u0131ca, genel yeniden ta\u015flamayan b\u0131\u00e7ak belli bir yar\u0131\u00e7apla ge\u00e7i\u015f olarak bir arka sahiptir. Sadece keskinle\u015ftirilmi\u015f d\u00f6nme ucu olmas\u0131na ra\u011fmen, hala belirli bir kemerli pah sahiptir. Herhangi bir d\u00f6n\u00fc\u015f ucunda mutlak k\u00f6\u015fe yoktur.<\/p>\n\n\n\nf<\/td> Ra<\/td> <\/td> <\/td> <\/td> <\/td> <\/td><\/tr> r<\/td> <\/td> 0.4<\/td> 0.8<\/td> 1.2<\/td> 1.6<\/td> 2.0<\/td><\/tr> <\/td> 1.6<\/td> 0.07<\/td> 0.1<\/td> 0.12<\/td> 0.14<\/td> 0.16<\/td><\/tr> <\/td> 3.2<\/td> 0.1<\/td> 0.14<\/td> 0.18<\/td> 0.2<\/td> 0.23<\/td><\/tr> <\/td> 6.3<\/td> 0.14<\/td> 0.2<\/td> 0.25<\/td> 0.28<\/td> 0.32<\/td><\/tr> <\/td> 12.5<\/td> 0.2<\/td> 0.28<\/td> 0.35<\/td> 0.4<\/td> 0.45<\/td><\/tr> <\/td> 25<\/td> 0.28<\/td> 0.4<\/td> 0.49<\/td> 0.56<\/td> 0.63<\/td><\/tr><\/tbody><\/table><\/figure>\n\n\n\n