S\u00fcrt\u00fcnme kayna\u011f\u0131, bir bas\u0131n\u00e7l\u0131 kaynak y\u00f6nteminin g\u00fcvenilir bir ba\u011flant\u0131s\u0131n\u0131 elde etmek i\u00e7in malzemenin g\u00f6receli s\u00fcrt\u00fcnmesi taraf\u0131ndan \u00fcretilen \u0131s\u0131y\u0131 elde etmek i\u00e7in kayna\u011f\u0131n g\u00f6receli s\u00fcrt\u00fcnme hareketinin kullan\u0131lmas\u0131d\u0131r. Kaynak i\u015flemi bas\u0131n\u00e7 etkisi alt\u0131ndad\u0131r, s\u00fcrt\u00fcnme aras\u0131nda kaynak yap\u0131lacak malzemenin g\u00f6receli hareketi, b\u00f6ylece aray\u00fcz ve yak\u0131ndaki s\u0131cakl\u0131k y\u00fckselir ve termoplastik bir duruma ula\u015f\u0131r, \u00fcst d\u00f6vme kuvvetinin rol\u00fc ile aray\u00fczey oksidasyon filmi k\u0131r\u0131l\u0131r, malzeme plastik deformasyona u\u011frar ve metalurjik reaksiyonun dif\u00fczyonu ve yeniden kristalle\u015fmesi ve eklemlerin olu\u015fumu elemanlar\u0131n\u0131n aray\u00fcz\u00fc boyunca akar.<\/p>\n\n\n\n
Dairesel kesitli iki metal i\u015f par\u00e7as\u0131, s\u00fcrt\u00fcnme kayna\u011f\u0131ndan \u00f6nce d\u00f6nd\u00fcr\u00fclebilen bir aynaya ve ileri hareket ettirilebilen ve bas\u0131n\u00e7land\u0131r\u0131labilen bir aynaya s\u0131k\u0131\u015ft\u0131r\u0131l\u0131r. Kaynak ba\u015flang\u0131c\u0131nda, i\u015f par\u00e7as\u0131 1 y\u00fcksek h\u0131zda d\u00f6nd\u00fcr\u00fcl\u00fcr, i\u015f par\u00e7as\u0131 2 i\u015f par\u00e7as\u0131 1 y\u00f6n\u00fcnde hareket ettirilir ve temas ettirilir ve s\u00fcrt\u00fcnme \u0131s\u0131tma i\u015flemini ba\u015flatmak i\u00e7in yeterince b\u00fcy\u00fck s\u00fcrt\u00fcnme bas\u0131nc\u0131 uygulan\u0131r. Bir s\u00fcre s\u00fcrt\u00fcnmeden sonra, birle\u015ftirme metalinin s\u0131cakl\u0131\u011f\u0131 kaynak s\u0131cakl\u0131\u011f\u0131na ula\u015f\u0131r, i\u015f par\u00e7as\u0131 1'in d\u00f6n\u00fc\u015f\u00fcn\u00fc durdurur ve ayn\u0131 zamanda i\u015f par\u00e7as\u0131 2, \u00fcst d\u00f6vme bas\u0131nc\u0131n\u0131 uygulamak i\u00e7in h\u0131zla hareket eder, b\u00f6ylece \u00fcst d\u00f6vme deformasyonunu \u00fcretir ve kayna\u011f\u0131 tamamlar.<\/p>\n\n\n\n
S\u00fcrt\u00fcnme kayna\u011f\u0131n\u0131n bir\u00e7ok y\u00f6ntemi vard\u0131r, genellikle kaynak par\u00e7as\u0131n\u0131n g\u00f6receli hareketine ve i\u015flemin \u00f6zelliklerine g\u00f6re kategorize edilir, ana y\u00f6ntemler \u015funlard\u0131r:<\/p>\n\n\n\n
S\u00fcrt\u00fcnme bas\u0131nc\u0131n\u0131n etkisi alt\u0131nda, kaynakl\u0131 aray\u00fczler birbirleriyle temas eder, g\u00f6receli hareket yoluyla s\u00fcrt\u00fcnme, b\u00f6ylece mekanik enerji termal enerjiye d\u00f6n\u00fc\u015ft\u00fcr\u00fcl\u00fcr, s\u00fcrt\u00fcnme \u0131s\u0131s\u0131 aray\u00fczlerdeki oksitleri \u00e7\u0131karmak i\u00e7in kullan\u0131l\u0131r ve \u00fcst d\u00f6vme kuvvetinin etkisi alt\u0131nda g\u00fcvenilir bir ba\u011flant\u0131 olu\u015fturulur. Bu, yayg\u0131n bir s\u00fcrt\u00fcnme kayna\u011f\u0131 t\u00fcr\u00fcd\u00fcr, kaynak i\u015fleminde, i\u015f par\u00e7as\u0131, belirtilen s\u00fcrt\u00fcnme s\u00fcresine veya s\u00fcrt\u00fcnme deformasyonuna ula\u015fana kadar sabit bir h\u0131zda d\u00f6nen i\u015f mili motoru taraf\u0131ndan s\u00fcrekli olarak tahrik edilir, i\u015f par\u00e7as\u0131 hemen d\u00f6nmeyi durdurur ve \u00fcst d\u00f6vme kayna\u011f\u0131.<\/p>\n\n\n\n
\u0130\u015f par\u00e7as\u0131n\u0131n d\u00f6nen ucu volana s\u0131k\u0131\u015ft\u0131r\u0131l\u0131r ve kaynak i\u015flemi volan\u0131 ve i\u015f par\u00e7as\u0131n\u0131n d\u00f6nen ucunu belirli bir d\u00f6nme h\u0131z\u0131na h\u0131zland\u0131rarak ba\u015flar, ard\u0131ndan volan ana motordan ayr\u0131l\u0131r ve i\u015f par\u00e7as\u0131n\u0131n hareketli ucu s\u00fcrt\u00fcnme \u0131s\u0131tmas\u0131n\u0131 ba\u015flatmak i\u00e7in ileri do\u011fru hareket eder. Volan s\u00fcrt\u00fcnme torku taraf\u0131ndan frenlenir, h\u0131z kademeli olarak d\u00fc\u015f\u00fcr\u00fcl\u00fcr ve h\u0131z s\u0131f\u0131r oldu\u011funda kaynak i\u015flemi sona erer.<\/p>\n\n\n\n
faz s\u00fcrt\u00fcnme kayna\u011f\u0131<\/h3>\n\n\n\n
Esas olarak alt\u0131gen \u00e7elik, sekizgen \u00e7elik, otomotiv kumanda kollar\u0131 vb. gibi i\u015f par\u00e7as\u0131n\u0131n g\u00f6receli konum gereksinimleri i\u00e7in kullan\u0131l\u0131r, \u00e7atallar\u0131n kaynaktan sonra hizalanmas\u0131n\u0131, gereksinimleri kar\u015f\u0131lamak i\u00e7in sa\u011f veya faz y\u00f6n\u00fcn\u00fc gerektirir. Ana y\u00f6ntemler \u015funlard\u0131r:<\/p>\n\n\n\n
\n
Mekanik senkronize faz s\u00fcrt\u00fcnme kayna\u011f\u0131<\/li>\n\n\n\n
Kaynak yap\u0131lacak boru, borunun i\u00e7inde bir mandrel ile pahlan\u0131r, kaynak s\u0131ras\u0131nda iki boruya radyal s\u00fcrt\u00fcnme bas\u0131nc\u0131 uygulayan ve s\u00fcrt\u00fcnme \u0131s\u0131tmas\u0131n\u0131n sonunda \u00fcst d\u00f6vme bas\u0131nc\u0131 uygulanan, pahlanm\u0131\u015f bir y\u00fczeye sahip d\u00f6ner bir halka ile donat\u0131lm\u0131\u015ft\u0131r.<\/p>\n\n\n\n
S\u00fcrt\u00fcnme kaplamas\u0131<\/h3>\n\n\n\n
Kaplama metali yuvarlak \u00e7ubuk y\u00fcksek h\u0131zda d\u00f6ner ve ana metal \u00fczerinde s\u00fcrt\u00fcnme bas\u0131nc\u0131 uygular. Ana metalin b\u00fcy\u00fck hacmi nedeniyle, termal iletkenlik iyidir ve so\u011futma h\u0131z\u0131 h\u0131zl\u0131d\u0131r. B\u00f6ylece s\u00fcrt\u00fcnme y\u00fczeyi kaplama metali ve ana metal aray\u00fcz\u00fcnden kaplama metali taraf\u0131na ge\u00e7er. Ayn\u0131 zamanda, kaplama metali yo\u011funla\u015f\u0131r ve kaplama kaynak etini olu\u015fturmak i\u00e7in ana metale ge\u00e7er. Ana metal kaplama metal \u00e7ubu\u011funa g\u00f6re d\u00f6nd\u00fc\u011f\u00fcnde veya hareket etti\u011finde, ana metal \u00fczerinde bir y\u00fczey kayna\u011f\u0131 olu\u015fur.<\/p>\n\n\n\n
Kaynak yap\u0131lacak iki i\u015f par\u00e7as\u0131 sabit, di\u011feri ileri geri hareket i\u00e7in belirli bir h\u0131zda veya g\u00f6receli ileri geri hareket i\u00e7in iki i\u015f par\u00e7as\u0131, aray\u00fcz s\u00fcrt\u00fcnmesinin iki i\u015f par\u00e7as\u0131n\u0131n bas\u0131nc\u0131n\u0131n etkisi alt\u0131nda, kaynak elde etmek i\u00e7in \u0131s\u0131 \u00fcretir.<\/p>\n\n\n\n
B\u00fcy\u00fck miktarda s\u00fcrt\u00fcnme \u0131s\u0131s\u0131n\u0131n kenar\u0131na ba\u011fl\u0131 iki kayna\u011f\u0131n d\u00f6n\u00fc\u015f\u00fcn\u00fc ayarlamak i\u00e7in kar\u0131\u015ft\u0131rma kafas\u0131n\u0131n kenar\u0131na ba\u011fl\u0131 iki kaynakl\u0131 malzemenin derinliklerine d\u00f6nen kar\u0131\u015ft\u0131rma i\u011fnesinin belirli bir \u015feklinden yap\u0131lm\u0131\u015f y\u00fcksek s\u0131cakl\u0131\u011fa dayan\u0131kl\u0131 sert bir malzeme olacakt\u0131r, bu da metalin plastik yumu\u015famas\u0131n\u0131n ba\u011flant\u0131s\u0131nda \u00fcretilen metalin plastik yumu\u015famas\u0131n\u0131n plastik yumu\u015famas\u0131n\u0131n plastik yumu\u015famas\u0131n\u0131n kar\u0131\u015ft\u0131rma kafas\u0131ndaki alan\u0131n kar\u0131\u015ft\u0131rma etkisi alt\u0131nda, ekstr\u00fczyon ve kar\u0131\u015ft\u0131rma kafas\u0131 ile kaynak boyunca d\u00f6nerek plastik bir metal ak\u0131\u015f\u0131 olu\u015fturmak i\u00e7in geriye do\u011fru akar ve kafay\u0131 so\u011futma i\u015fleminden ve ekstr\u00fczyondan ve kat\u0131 faz kaynakl\u0131 ba\u011flant\u0131lar\u0131n olu\u015fumundan uzakla\u015ft\u0131r\u0131r. Plastik yumu\u015fat\u0131lm\u0131\u015f b\u00f6lge, kar\u0131\u015ft\u0131rma kafas\u0131n\u0131n etkisi alt\u0131nda kar\u0131\u015ft\u0131r\u0131l\u0131r ve s\u0131k\u0131\u015ft\u0131r\u0131l\u0131r ve kar\u0131\u015ft\u0131rma kafas\u0131n\u0131n d\u00f6n\u00fc\u015f\u00fc ile kaynak diki\u015fi boyunca geriye do\u011fru akar, plastik bir metal ak\u0131\u015f\u0131 olu\u015fturur ve kar\u0131\u015ft\u0131rma kafas\u0131n\u0131n ayr\u0131lmas\u0131ndan sonra so\u011futma i\u015fleminde, kat\u0131 faz kaynakl\u0131 bir ba\u011flant\u0131 olu\u015fturmak i\u00e7in s\u0131k\u0131\u015ft\u0131r\u0131l\u0131r.<\/p>\n\n\n\n
Orbital s\u00fcrt\u00fcnme kayna\u011f\u0131<\/h3>\n\n\n\n
Orbital s\u00fcrt\u00fcnme kayna\u011f\u0131, esas olarak dairesel olmayan kesitli i\u015f par\u00e7as\u0131n\u0131n kayna\u011f\u0131 i\u00e7in kullan\u0131lan yeni geli\u015ftirilmi\u015f bir kaynak y\u00f6ntemidir. Do\u011frusal y\u00f6r\u00fcnge s\u00fcrt\u00fcnme kayna\u011f\u0131 i\u015f par\u00e7as\u0131, titre\u015fim h\u0131z\u0131n\u0131n gerekli de\u011fere ula\u015fmas\u0131n\u0131 sa\u011flamak i\u00e7in belirli bir genlik ve frekans ile d\u00fcz bir yol boyunca, b\u00f6ylece kaynak y\u00fczeyinin g\u00f6receli tekrarlanan titre\u015fim s\u00fcrt\u00fcnmesi yapmas\u0131n\u0131 sa\u011flar. Kaynak y\u00fczeyinin s\u00fcrt\u00fcnmenin g\u00f6receli hareketini yapmas\u0131n\u0131 sa\u011flamak i\u00e7in dairesel y\u00f6r\u00fcnge boyunca ayn\u0131 yar\u0131\u00e7ap ve h\u0131za sahip her k\u00fctlenin dairesel y\u00f6r\u00fcnge s\u00fcrt\u00fcnme kayna\u011f\u0131 i\u015f par\u00e7as\u0131. Ek yeri kaynak s\u0131cakl\u0131\u011f\u0131na kadar \u0131s\u0131t\u0131ld\u0131\u011f\u0131nda, i\u015f par\u00e7as\u0131n\u0131n s\u00fcrt\u00fcnme hareketi durdurulur ve \u00fcst kaynak yap\u0131l\u0131r.<\/p>\n\n\n\n
S\u00fcrt\u00fcnme kaynak i\u015flemi<\/h2>\n\n\n\n
S\u00fcre\u00e7 \u00f6zellikleri<\/h3>\n\n\n\n
vantage<\/strong>:<\/p>\n\n\n\n\n
K\u0131sa kaynak yap\u0131m s\u00fcresi ve y\u00fcksek verimlilik.<\/li>\n\n\n\n
K\u00fc\u00e7\u00fck kaynak distorsiyonu, kaynak sonras\u0131 y\u00fcksek boyutsal do\u011fruluk.<\/li>\n\n\n\n
Y\u00fcksek derecede mekanizasyon ve otomasyon, istikrarl\u0131 kaynak kalitesi.<\/li>\n\n\n\n
Her t\u00fcrl\u00fc benzer olmayan malzemenin kayna\u011f\u0131 i\u00e7in uygundur ve geleneksel eritme alt\u0131nda kaynaklanamayan al\u00fcminyum-\u00e7elik, al\u00fcminyum-bak\u0131r, titanyum-bak\u0131r, metaller aras\u0131 bile\u015fikler-\u00e7elik vb.<\/li>\n\n\n\n
Ayn\u0131 ve farkl\u0131 \u00e7aplardaki \u00e7ubuk ve borular\u0131n kayna\u011f\u0131 m\u00fcmk\u00fcnd\u00fcr.<\/li>\n\n\n\n
Kaynak duman, ark \u0131\u015f\u0131\u011f\u0131 ve zararl\u0131 gazlar \u00fcretmez ve \u00e7evreyi kirletmez.<\/li>\n<\/ol>\n\n\n\n
Dezavantajlar.<\/strong><\/p>\n\n\n\n
1. Dairesel olmayan kesitlerin kaynaklanmas\u0131 daha zordur ve gerekli ekipman karma\u015f\u0131kt\u0131r; ayr\u0131ca disk \u015feklindeki ince par\u00e7alar\u0131n ve ince duvarl\u0131 boru ba\u011flant\u0131 par\u00e7alar\u0131n\u0131n kaynaklanmas\u0131 daha zordur \u00e7\u00fcnk\u00fc kelep\u00e7elenmeleri kolay de\u011fildir. 2. \u015eekli ve montaj konumu \u00f6nceden belirlenmi\u015f bile\u015fenler i\u00e7in s\u00fcrt\u00fcnme kayna\u011f\u0131 ger\u00e7ekle\u015ftirmek zordur. 3. Ba\u011flant\u0131lar a\u015f\u0131nmaya e\u011filimlidir ve kaynaktan sonra i\u015flenmelidir. 4. S\u0131k\u0131\u015ft\u0131rma par\u00e7as\u0131n\u0131n \u00e7izikler veya s\u0131k\u0131\u015ft\u0131rma izleri olu\u015fturmas\u0131 kolayd\u0131r<\/p>\n\n\n\n
S\u00fcrt\u00fcnme kaynak i\u015flemi<\/h2>\n\n\n\n
S\u00fcrt\u00fcnme kayna\u011f\u0131, s\u00fcrt\u00fcnme \u0131s\u0131s\u0131 ve mekanik kuvvetler kullan\u0131larak malzemelerin metal\u00fcrjik olarak birle\u015ftirilmesine dayanan olduk\u00e7a verimli bir kat\u0131 hal birle\u015ftirme tekni\u011fidir. S\u00fcre\u00e7, i\u015f par\u00e7as\u0131n\u0131n hassas bir \u015fekilde sabitlenmesiyle ba\u015flar - genellikle i\u015f par\u00e7as\u0131n\u0131n bir taraf\u0131 bir fikst\u00fcrde g\u00fcvenli bir \u015fekilde tutulurken, di\u011fer taraf\u0131 temas y\u00fczeylerinin temiz ve d\u00fcz olmas\u0131n\u0131 sa\u011flamak i\u00e7in bir d\u00f6ner s\u00fcr\u00fcc\u00fcye ba\u011flan\u0131r. Makine etkinle\u015ftirildi\u011finde, d\u00f6nen i\u015f par\u00e7as\u0131 eksenel bas\u0131n\u00e7 alt\u0131nda sabit par\u00e7a ile yak\u0131n temasa girer ve y\u00fcksek h\u0131zl\u0131 s\u00fcrt\u00fcnme, aray\u00fczde an\u0131nda y\u00fcksek s\u0131cakl\u0131klar \u00fcretir, bu da malzemeye h\u0131zla n\u00fcfuz eder ve onu plastik bir duruma getirir. Bu i\u015flem s\u0131ras\u0131nda s\u00fcrt\u00fcnme sadece y\u00fczeydeki oksit tabakas\u0131n\u0131 par\u00e7alamakla kalmaz, ayn\u0131 zamanda metal kafesin dinamik olarak yeniden kristalle\u015fmesini sa\u011flayarak akan yumu\u015fat\u0131lm\u0131\u015f bir tabaka olu\u015fturur. S\u0131cakl\u0131k kritik noktaya ula\u015ft\u0131\u011f\u0131nda, ekipman kararl\u0131 bir \u015fekilde d\u00f6nmeyi durdurur ve ard\u0131ndan \u00fcst d\u00f6vmeye daha fazla bas\u0131n\u00e7 uygular, bu s\u0131rada yumu\u015fat\u0131lm\u0131\u015f malzeme sanki ekstr\u00fczyon f\u00fczyonu gibi d\u00f6v\u00fclm\u00fc\u015f gibi, mikroskobik d\u00fczeyde atomik dif\u00fczyon ve tane s\u0131n\u0131r\u0131 g\u00f6\u00e7\u00fc, ba\u011flant\u0131 y\u00fczeyindeki kusurlar\u0131 tamamen ortadan kald\u0131r\u0131r, yo\u011fun ve kusursuz kaynakl\u0131 ba\u011flant\u0131lar\u0131n olu\u015fumu. So\u011futulduktan ve \u015fekillendirildikten sonra, kaynak neredeyse deformasyonsuzdur ve mukavemeti ana malzemenin mukavemetini bile a\u015fabilir.<\/p>\n\n\n\n
Geleneksel s\u00fcrt\u00fcnme kayna\u011f\u0131 ekipman\u0131<\/h3>\n\n\n\n
Geleneksel s\u00fcrt\u00fcnme kaynak ekipman\u0131, \u00e7ekirde\u011fi bir i\u015f mili g\u00fc\u00e7 mod\u00fcl\u00fc, bir hidrolik bas\u0131n\u00e7 cihaz\u0131 ve bir ak\u0131ll\u0131 kontrol sisteminden olu\u015fan mekanik bir tahrik sistemi arac\u0131l\u0131\u011f\u0131yla y\u00fcksek hassasiyetli bir bas\u0131n\u00e7 kontrol mekanizmas\u0131na sa\u011flam bir \u015fekilde ba\u011flan\u0131r. Ekipman, \u015faftlar\u0131n, borular\u0131n ve \u015fekilli i\u015f par\u00e7alar\u0131n\u0131n s\u0131k\u0131\u015ft\u0131rma gereksinimlerine esnek bir \u015fekilde uyarlanabilen, otomotiv \u00fcretim alan\u0131ndaki \u00f6nemli motor bile\u015fenlerinin verimli kayna\u011f\u0131n\u0131 ger\u00e7ekle\u015ftiren ve askeri alanda y\u00fcksek mukavemetli ala\u015f\u0131ml\u0131 malzemelerin g\u00fcvenilir ba\u011flant\u0131s\u0131n\u0131 tamamlamak i\u00e7in ger\u00e7ek zamanl\u0131 izleme sistemine dayanan mod\u00fcler tasar\u0131m\u0131 benimser. Geleneksel kaynak i\u015flemiyle kar\u015f\u0131la\u015ft\u0131r\u0131ld\u0131\u011f\u0131nda, ekipman enerji t\u00fcketimi kontrol\u00fc ve ba\u011flant\u0131 kalitesinde \u00f6nemli avantajlara sahiptir, \u00e7ok sens\u00f6rl\u00fc f\u00fczyon teknolojisi ile havac\u0131l\u0131k, demiryolu ta\u015f\u0131mac\u0131l\u0131\u011f\u0131 ve di\u011fer end\u00fcstrilerin hassas kaynak gereksinimlerini kar\u015f\u0131layabilir, seri end\u00fcstriyel \u00fcretim i\u00e7in temel ekipman haline gelebilir.<\/p>\n\n\n\n
S\u00fcrt\u00fcnme Kar\u0131\u015ft\u0131rma Kaynak Ekipmanlar\u0131<\/h3>\n\n\n\n
S\u00fcrt\u00fcnme Kar\u0131\u015ft\u0131rma Kayna\u011f\u0131 (FSW) ekipman\u0131, kat\u0131 hal birle\u015ftirme prensibine dayal\u0131 olarak geli\u015ftirilen geli\u015fmi\u015f bir kaynak ekipman\u0131d\u0131r ve temel yenili\u011fi, malzemelerin plastik ak\u0131\u015f\u0131n\u0131 ve metalurjik ba\u011flanmas\u0131n\u0131 sa\u011flamak i\u00e7in \u00f6zel kar\u0131\u015ft\u0131rma kafas\u0131n\u0131n kullan\u0131lmas\u0131nda yatmaktad\u0131r. Ekipman temel olarak y\u00fcksek sertlikte bir g\u00f6vde, bir d\u00f6ner tahrik sistemi, hassas bir s\u0131cakl\u0131k kontrol mod\u00fcl\u00fc ve \u00fc\u00e7 boyutlu bir kuvvet-pozisyon alg\u0131lama \u00fcnitesinden olu\u015fur. Kar\u0131\u015ft\u0131rma i\u011fnesi ve omuzun sinerjik etkisi sayesinde, al\u00fcminyum ala\u015f\u0131mlar\u0131 ve magnezyum ala\u015f\u0131mlar\u0131 gibi y\u00fcksek erime noktal\u0131 malzemelerin eritmeye gerek kalmadan sorunsuz bir \u015fekilde birle\u015ftirilmesi sa\u011flanabilir. Geleneksel s\u00fcrt\u00fcnme kayna\u011f\u0131 ile kar\u015f\u0131la\u015ft\u0131r\u0131ld\u0131\u011f\u0131nda, bu teknoloji ince levha kayna\u011f\u0131n\u0131n kalitesini \u00f6nemli \u00f6l\u00e7\u00fcde art\u0131r\u0131r, havac\u0131l\u0131k alan\u0131nda deri iskeletin entegre kal\u0131planmas\u0131n\u0131 ger\u00e7ekle\u015ftirir ve yeni enerji ara\u00e7lar\u0131 i\u00e7in pil tepsilerinin \u00fcretiminde yayg\u0131n olarak kullan\u0131l\u0131r ve kaynak diki\u015finin mukavemeti ana malzemenin 95%'sinden daha fazlas\u0131na ula\u015fabilir. En yeni ekipman, kaynak parametrelerini dinamik olarak ayarlayabilen ve benzer olmayan malzemeler (\u00f6rne\u011fin al\u00fcminyum \/ bak\u0131r, al\u00fcminyum \/ \u00e7elik) i\u00e7in birle\u015ftirme teknolojisinin darbo\u011faz\u0131n\u0131 ba\u015far\u0131yla a\u015fabilen g\u00f6rsel rehberlik ve uyarlanabilir kontrol algoritmalar\u0131n\u0131 entegre eder.<\/p>","protected":false},"excerpt":{"rendered":"
S\u00fcrt\u00fcnme kayna\u011f\u0131 tan\u0131m\u0131 S\u00fcrt\u00fcnme kayna\u011f\u0131, malzemelerin g\u00fcvenilir bir \u015fekilde ba\u011flanmas\u0131n\u0131 sa\u011flamak i\u00e7in \u0131s\u0131 \u00fcretmek i\u00e7in kaynak par\u00e7as\u0131n\u0131n g\u00f6receli s\u00fcrt\u00fcnme hareketinin kullan\u0131lmas\u0131d\u0131r, bir bas\u0131n\u00e7 kayna\u011f\u0131 y\u00f6ntemidir. Kaynak i\u015flemi bas\u0131n\u00e7 etkisi alt\u0131ndad\u0131r, s\u00fcrt\u00fcnme aras\u0131nda kaynak yap\u0131lacak malzemenin g\u00f6receli hareketi, b\u00f6ylece aray\u00fcz ve yak\u0131ndaki s\u0131cakl\u0131k y\u00fckselir ve termoplastik bir duruma ula\u015f\u0131r, \u00fcst d\u00f6vme kuvvetinin rol\u00fc ile aray\u00fczey oksidasyon filmi k\u0131r\u0131l\u0131r, malzeme plastik deformasyona u\u011frar ve aray\u00fcz eleman\u0131 dif\u00fczyonu ve metalurjik reaksiyonun yeniden kristalle\u015fmesi ve eklemlerin olu\u015fumu yoluyla akar. S\u00fcrt\u00fcnme kayna\u011f\u0131 prensibi S\u00fcrt\u00fcnme kayna\u011f\u0131nda metal i\u015f par\u00e7as\u0131n\u0131n iki yuvarlak b\u00f6l\u00fcm\u00fc s\u0131ras\u0131yla aynaya s\u0131k\u0131\u015ft\u0131r\u0131lmadan \u00f6nce d\u00f6nd\u00fcr\u00fclebilir ve aynay\u0131 bas\u0131n\u00e7land\u0131rmak i\u00e7in ileri do\u011fru hareket edebilir. Kaynak ba\u015flang\u0131c\u0131nda, i\u015f par\u00e7as\u0131 1 y\u00fcksek h\u0131zda d\u00f6ner, i\u015f par\u00e7as\u0131 2 i\u015f par\u00e7as\u0131 1 y\u00f6n\u00fcne do\u011fru hareket eder ve temas eder ve s\u00fcrt\u00fcnme \u0131s\u0131tma i\u015flemini ba\u015flatmak i\u00e7in yeterince b\u00fcy\u00fck bir s\u00fcrt\u00fcnme bas\u0131nc\u0131 uygulan\u0131r. Bir s\u00fcrt\u00fcnme s\u00fcresinden sonra ...<\/p>","protected":false},"author":1,"featured_media":2004,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":[],"categories":[21],"tags":[69],"class_list":["post-2003","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-about-news","tag-aluminum-alloy-manufacturing-process"],"_links":{"self":[{"href":"https:\/\/www.hexinmusu.com\/tr\/wp-json\/wp\/v2\/posts\/2003","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.hexinmusu.com\/tr\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.hexinmusu.com\/tr\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.hexinmusu.com\/tr\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/www.hexinmusu.com\/tr\/wp-json\/wp\/v2\/comments?post=2003"}],"version-history":[{"count":0,"href":"https:\/\/www.hexinmusu.com\/tr\/wp-json\/wp\/v2\/posts\/2003\/revisions"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/www.hexinmusu.com\/tr\/wp-json\/wp\/v2\/media\/2004"}],"wp:attachment":[{"href":"https:\/\/www.hexinmusu.com\/tr\/wp-json\/wp\/v2\/media?parent=2003"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.hexinmusu.com\/tr\/wp-json\/wp\/v2\/categories?post=2003"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.hexinmusu.com\/tr\/wp-json\/wp\/v2\/tags?post=2003"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}
![\"atalet](\"https:\/\/www.hexinmusu.com\/wp-content\/uploads\/2025\/03\/wz-39-Inertial-friction-welding.webp\")
<\/figure>\n\n\n\n![\"S\u00fcrt\u00fcnme](\"https:\/\/www.hexinmusu.com\/wp-content\/uploads\/2025\/03\/wz-39-Friction-welding-equipment-1024x926.jpg\")
<\/figure>\n\n\n\n