{"id":6537,"date":"2023-08-30T15:03:20","date_gmt":"2023-08-30T07:03:20","guid":{"rendered":"https:\/\/zltechlaser.com\/?p=6537"},"modified":"2024-01-25T14:49:47","modified_gmt":"2024-01-25T06:49:47","slug":"derin-penetrasyon-lazer-kaynaginin-ana-islem-parametreleri","status":"publish","type":"post","link":"https:\/\/zltechlaser.com\/tr\/blog\/derin-penetrasyon-lazer-kaynaginin-ana-islem-parametreleri\/","title":{"rendered":"Derin Penetrasyon Lazer Kayna\u011f\u0131n\u0131n Ana Proses Parametreleri"},"content":{"rendered":"<h2>Giri\u015f:<\/h2>\n<p>Bir \u00f6nceki makalede Derin N\u00fcfuziyet Lazer Kayna\u011f\u0131n\u0131n prensiplerini ve \u00f6zelliklerini tart\u0131\u015ft\u0131k. Burada, ana i\u015flem parametrelerine odaklanaca\u011f\u0131z. Bu, bu kaynak tekni\u011fi hakk\u0131nda daha fazla bilgi edinmeniz i\u00e7in yararl\u0131d\u0131r.<\/p>\n<h2>Derin Penetrasyon Lazer Kayna\u011f\u0131n\u0131n Ana Proses Parametreleri<\/h2>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"alignnone wp-image-6496\" src=\"https:\/\/zltechlaser.com\/wp-content\/uploads\/2023\/08\/handheld_laser_welding_machine-2-300x225.webp\" alt=\"\" width=\"407\" height=\"305\" srcset=\"https:\/\/zltechlaser.com\/wp-content\/uploads\/2023\/08\/handheld_laser_welding_machine-2-300x225.webp 300w, https:\/\/zltechlaser.com\/wp-content\/uploads\/2023\/08\/handheld_laser_welding_machine-2-768x576.webp 768w, https:\/\/zltechlaser.com\/wp-content\/uploads\/2023\/08\/handheld_laser_welding_machine-2-800x600.webp 800w, https:\/\/zltechlaser.com\/wp-content\/uploads\/2023\/08\/handheld_laser_welding_machine-2.webp 1000w\" sizes=\"auto, (max-width: 407px) 100vw, 407px\" \/><\/p>\n<h3>1. Lazer g\u00fcc\u00fc<\/h3>\n<p>Lazer kayna\u011f\u0131nda lazer enerji yo\u011funlu\u011funun bir e\u015fik de\u011feri vard\u0131r. Bu de\u011ferin alt\u0131nda n\u00fcfuziyet derinli\u011fi \u00e7ok azd\u0131r. Bu de\u011fere ula\u015f\u0131ld\u0131\u011f\u0131nda veya bu de\u011fer a\u015f\u0131ld\u0131\u011f\u0131nda, n\u00fcfuziyet derinli\u011fi b\u00fcy\u00fck \u00f6l\u00e7\u00fcde artacakt\u0131r. Sadece i\u015f par\u00e7as\u0131 \u00fczerindeki lazer g\u00fc\u00e7 yo\u011funlu\u011fu bir e\u015fik de\u011ferini a\u015ft\u0131\u011f\u0131nda (malzemeye ba\u011fl\u0131 olarak) plazma \u00fcretilecektir. Bu, kararl\u0131 derin n\u00fcfuziyet kayna\u011f\u0131n\u0131n ilerlemesini i\u015faret eder.<\/p>\n<p>Lazer g\u00fcc\u00fc bu e\u015fi\u011fin alt\u0131ndaysa, i\u015f par\u00e7as\u0131nda sadece y\u00fczey erimesi meydana gelir. Bu kararl\u0131 \u0131s\u0131 iletim kayna\u011f\u0131d\u0131r. Bununla birlikte, lazer g\u00fc\u00e7 yo\u011funlu\u011fu k\u00fc\u00e7\u00fck deliklerin olu\u015fumu i\u00e7in kritik ko\u015fula yak\u0131n oldu\u011funda, derin n\u00fcfuziyet kayna\u011f\u0131 ve iletim kayna\u011f\u0131 d\u00f6n\u00fc\u015f\u00fcml\u00fc olarak ger\u00e7ekle\u015ftirilir. Bu, n\u00fcfuziyet derinli\u011finde b\u00fcy\u00fck dalgalanmalara neden olan karars\u0131z bir kaynak i\u015flemi haline gelir.<\/p>\n<p>Lazer derin n\u00fcfuziyet kayna\u011f\u0131 s\u0131ras\u0131nda lazer g\u00fcc\u00fc, n\u00fcfuziyet derinli\u011fini ve kaynak h\u0131z\u0131n\u0131 ayn\u0131 anda kontrol eder. Kaynak n\u00fcfuziyeti do\u011frudan \u0131\u015f\u0131n g\u00fcc\u00fc yo\u011funlu\u011fuyla ilgilidir ve gelen \u0131\u015f\u0131n g\u00fcc\u00fcn\u00fcn ve \u0131\u015f\u0131n odak noktas\u0131n\u0131n bir fonksiyonudur. Genel olarak, belirli bir \u00e7aptaki lazer \u0131\u015f\u0131n\u0131 i\u00e7in, \u0131\u015f\u0131n g\u00fcc\u00fc artt\u0131k\u00e7a n\u00fcfuziyet derinli\u011fi de artar.<\/p>\n<h3>2. I\u015f\u0131n odak noktas\u0131<\/h3>\n<p>I\u015f\u0131n noktas\u0131 boyutu, lazer kayna\u011f\u0131ndaki en \u00f6nemli de\u011fi\u015fkenlerden biridir. \u00c7\u00fcnk\u00fc g\u00fc\u00e7 yo\u011funlu\u011funu belirler. Ancak y\u00fcksek g\u00fc\u00e7l\u00fc lazerler i\u00e7in \u00f6l\u00e7\u00fcm\u00fc zordur. Bir\u00e7ok dolayl\u0131 \u00f6l\u00e7\u00fcm tekni\u011fi olmas\u0131na ra\u011fmen.<\/p>\n<p>I\u015f\u0131n oda\u011f\u0131n\u0131n k\u0131r\u0131n\u0131m s\u0131n\u0131rl\u0131 nokta boyutu, \u0131\u015f\u0131k k\u0131r\u0131n\u0131m teorisine g\u00f6re hesaplanabilir. Ancak odaklama merce\u011fi sapmas\u0131n\u0131n varl\u0131\u011f\u0131 nedeniyle, ger\u00e7ek nokta boyutu hesaplanan de\u011ferden daha b\u00fcy\u00fckt\u00fcr. En basit pratik y\u00f6ntem izotermal profilleme y\u00f6ntemidir. Bu, kal\u0131n ka\u011f\u0131tl\u0131 bir polipropilen plakay\u0131 k\u00f6m\u00fcrle\u015ftirdikten ve deldikten sonra odak noktas\u0131n\u0131 ve perforasyon \u00e7ap\u0131n\u0131 \u00f6l\u00e7mektir. Bu y\u00f6ntem, \u00f6l\u00e7\u00fcm prati\u011fi yoluyla lazer g\u00fcc\u00fcne ve \u0131\u015f\u0131n hareket s\u00fcresine hakim olmay\u0131 gerektirir.<\/p>\n<h3>3. Malzeme emilim de\u011feri<\/h3>\n<p>Lazer \u0131\u015f\u0131\u011f\u0131n\u0131n bir malzeme taraf\u0131ndan emilmesi, malzemenin baz\u0131 \u00f6nemli \u00f6zelliklerine ba\u011fl\u0131d\u0131r. \u00d6rne\u011fin emicilik, yans\u0131t\u0131c\u0131l\u0131k, termal iletkenlik, erime s\u0131cakl\u0131\u011f\u0131, buharla\u015fma s\u0131cakl\u0131\u011f\u0131 vb.<br \/>\nEn \u00f6nemli \u015fey emilim oran\u0131d\u0131r.<\/p>\n<p>Malzemenin lazer \u0131\u015f\u0131n\u0131n\u0131 so\u011furma oran\u0131n\u0131 etkileyen fakt\u00f6rler iki hususu i\u00e7erir:<\/p>\n<ul>\n<li>\u0130lk olarak, malzemenin parlat\u0131lm\u0131\u015f y\u00fczeyinin absorbans\u0131n\u0131 \u00f6l\u00e7\u00fcn. Malzemenin \u00f6zdirencinin, \u00f6zdiren\u00e7 katsay\u0131s\u0131n\u0131n karek\u00f6k\u00fc ile orant\u0131l\u0131 oldu\u011fu bulunmu\u015ftur. \u00d6zdiren\u00e7 katsay\u0131s\u0131 s\u0131cakl\u0131kla de\u011fi\u015fir.<\/li>\n<li>\u0130kinci olarak, malzemenin y\u00fczey durumu (veya fini\u015fi) \u0131\u015f\u0131n emme oran\u0131 \u00fczerinde daha \u00f6nemli bir etkiye sahiptir. Bu nedenle kaynak etkisi \u00fczerinde \u00f6nemli bir etkiye sahiptir.<\/li>\n<\/ul>\n<p>Seramik, cam, kau\u00e7uk ve plastik gibi metal olmayan malzemeler oda s\u0131cakl\u0131\u011f\u0131nda y\u00fcksek emilim oran\u0131na sahiptir. Bununla birlikte, metalik malzemeler oda s\u0131cakl\u0131\u011f\u0131nda zay\u0131f bir emilim oran\u0131na sahiptir. Malzeme eridi\u011finde veya hatta buharla\u015ft\u0131\u011f\u0131nda, bu oran keskin bir \u015fekilde artacakt\u0131r. Bir y\u00fczey kaplamas\u0131 veya y\u00fczey oksit filmi kullanmak, malzemenin \u0131\u015f\u0131k demeti emilimini etkili bir \u015fekilde iyile\u015ftirir.<\/p>\n<h3>4. Kaynak h\u0131z\u0131<\/h3>\n<p>Kaynak h\u0131z\u0131n\u0131n n\u00fcfuziyet derinli\u011fi \u00fczerinde b\u00fcy\u00fck bir etkisi vard\u0131r. H\u0131z\u0131 artt\u0131rmak n\u00fcfuziyeti daha s\u0131\u011f hale getirecektir. Ancak h\u0131z \u00e7ok d\u00fc\u015f\u00fckse, malzeme a\u015f\u0131r\u0131 eriyecek ve i\u015f par\u00e7as\u0131 kaynaklanacakt\u0131r. Bu nedenle, belirli bir lazer g\u00fcc\u00fcne ve kal\u0131nl\u0131\u011f\u0131na sahip belirli bir malzeme i\u00e7in uygun bir kaynak h\u0131z\u0131 aral\u0131\u011f\u0131 mevcuttur. Maksimum n\u00fcfuziyet derinli\u011fi, ilgili h\u0131z de\u011ferinde elde edilebilir.<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"alignnone wp-image-2975\" src=\"https:\/\/zltechlaser.com\/wp-content\/uploads\/2023\/04\/handheld_2000w_fiber_laser_welding_machine_price-300x225.webp\" alt=\"\" width=\"407\" height=\"305\" srcset=\"https:\/\/zltechlaser.com\/wp-content\/uploads\/2023\/04\/handheld_2000w_fiber_laser_welding_machine_price-300x225.webp 300w, https:\/\/zltechlaser.com\/wp-content\/uploads\/2023\/04\/handheld_2000w_fiber_laser_welding_machine_price-768x576.webp 768w, https:\/\/zltechlaser.com\/wp-content\/uploads\/2023\/04\/handheld_2000w_fiber_laser_welding_machine_price-800x600.webp 800w, https:\/\/zltechlaser.com\/wp-content\/uploads\/2023\/04\/handheld_2000w_fiber_laser_welding_machine_price.webp 1000w\" sizes=\"auto, (max-width: 407px) 100vw, 407px\" \/><\/p>\n<h3>5. Koruyucu gaz<\/h3>\n<p>Lazer kayna\u011f\u0131 s\u0131ras\u0131nda erimi\u015f havuzu korumak i\u00e7in genellikle inert gaz kullan\u0131l\u0131r. Baz\u0131 malzemeler y\u00fczey oksidasyonundan ba\u011f\u0131ms\u0131z olarak kaynaklan\u0131r ve koruma dikkate al\u0131nmayabilir. Ancak \u00e7o\u011fu uygulama i\u00e7in helyum, argon, nitrojen ve di\u011fer gazlar genellikle koruma olarak kullan\u0131l\u0131r.<\/p>\n<ul>\n<li>\n<h4>Helyum<\/h4>\n<\/li>\n<\/ul>\n<p>Helyum kolay iyonize olmaz (daha y\u00fcksek iyonizasyon enerjisi). Bu, lazerin sorunsuz bir \u015fekilde ge\u00e7mesine izin verir ve \u0131\u015f\u0131n enerjisi i\u015f par\u00e7as\u0131n\u0131n y\u00fczeyine engel olmadan ula\u015f\u0131r. Bu, lazer kayna\u011f\u0131nda kullan\u0131lan en etkili koruyucu gazd\u0131r. Ancak daha pahal\u0131d\u0131r.<\/p>\n<ul>\n<li>\n<h4>Argon gaz\u0131<\/h4>\n<\/li>\n<\/ul>\n<p>Argon gaz\u0131 daha ucuz ve yo\u011fundur, bu nedenle koruma etkisi daha iyidir. Ancak, y\u00fcksek s\u0131cakl\u0131kta metal plazma iyonizasyonuna kar\u015f\u0131 hassast\u0131r. Bu, \u0131\u015f\u0131n\u0131n bir k\u0131sm\u0131n\u0131n i\u015f par\u00e7as\u0131na \u00e7arpmas\u0131n\u0131 engelleyebilir, kaynak i\u00e7in etkili lazer g\u00fcc\u00fcn\u00fc azaltabilir ve kaynak h\u0131z\u0131na ve n\u00fcfuziyetine zarar verebilir. Argon ile korunan kaynak y\u00fczeyi, helyum ile korunana g\u00f6re daha p\u00fcr\u00fczs\u00fczd\u00fcr.<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"alignnone wp-image-6025\" src=\"https:\/\/zltechlaser.com\/wp-content\/uploads\/2023\/08\/assist_gas_selection-300x225.webp\" alt=\"\" width=\"407\" height=\"305\" srcset=\"https:\/\/zltechlaser.com\/wp-content\/uploads\/2023\/08\/assist_gas_selection-300x225.webp 300w, https:\/\/zltechlaser.com\/wp-content\/uploads\/2023\/08\/assist_gas_selection-768x576.webp 768w, https:\/\/zltechlaser.com\/wp-content\/uploads\/2023\/08\/assist_gas_selection-800x600.webp 800w, https:\/\/zltechlaser.com\/wp-content\/uploads\/2023\/08\/assist_gas_selection.webp 1000w\" sizes=\"auto, (max-width: 407px) 100vw, 407px\" \/><\/p>\n<ul>\n<li>\n<h4>Azot<\/h4>\n<\/li>\n<\/ul>\n<p>Azot en ucuz koruyucu gazd\u0131r. Ancak, emilim gibi metal\u00fcrjik sorunlar nedeniyle baz\u0131 paslanmaz \u00e7elik t\u00fcrlerinin kayna\u011f\u0131 i\u00e7in uygun de\u011fildir. Bazen bu, \u00fcst \u00fcste binen alanda g\u00f6zeneklilik olu\u015fturur.<\/p>\n<p>Koruyucu gaz kullan\u0131m\u0131 temel olarak a\u015fa\u011f\u0131daki \u00fc\u00e7 a\u00e7\u0131dan faydal\u0131d\u0131r:<\/p>\n<ul>\n<li>Lehimleme s\u0131ras\u0131nda i\u015f par\u00e7as\u0131n\u0131 oksidasyondan koruyun.<\/li>\n<li>Odaklama lensini, \u00f6zellikle y\u00fcksek g\u00fc\u00e7l\u00fc lazer kayna\u011f\u0131nda metal buhar\u0131 kontaminasyonundan ve s\u0131v\u0131 damlac\u0131klar\u0131n\u0131n p\u00fcsk\u00fcrt\u00fclmesinden koruyun. F\u0131rlatma g\u00fc\u00e7l\u00fc hale geldi\u011finden, lensi \u015fimdi korumak gerekir.<\/li>\n<li>Y\u00fcksek g\u00fc\u00e7l\u00fc lazer kayna\u011f\u0131 taraf\u0131ndan \u00fcretilen plazma kalkan\u0131n\u0131 da\u011f\u0131t\u0131n. Metal buhar\u0131 lazer \u0131\u015f\u0131n\u0131n\u0131 emer ve bir plazma bulutu halinde iyonize olur. Metal buhar\u0131 etraf\u0131ndaki koruyucu gaz da \u0131s\u0131 nedeniyle iyonize olur. \u00c7ok fazla plazma mevcutsa, lazer \u0131\u015f\u0131n\u0131 plazma taraf\u0131ndan bir \u015fekilde t\u00fcketilir. Plazma, \u00e7al\u0131\u015fma y\u00fczeyinde ikinci bir enerji olarak bulunur, bu da penetrasyonu s\u0131\u011fla\u015ft\u0131r\u0131r ve kaynak havuzunun y\u00fczeyini geni\u015fletir. Plazmadaki elektron yo\u011funlu\u011funu azaltmak i\u00e7in elektronlar\u0131n iyonlar ve n\u00f6tr atomlarla \u00fc\u00e7 cisim \u00e7arp\u0131\u015fmalar\u0131 art\u0131r\u0131larak elektronlar\u0131n rekombinasyon oran\u0131 art\u0131r\u0131l\u0131r. N\u00f6tr atomlar ne kadar hafif olursa \u00e7arp\u0131\u015fma frekans\u0131 ve rekombinasyon oran\u0131 da o kadar y\u00fcksek olur. \u00d6te yandan, sadece y\u00fcksek iyonla\u015fma enerjisine sahip koruyucu gaz, gaz\u0131n kendisinin iyonla\u015fmas\u0131 nedeniyle elektron yo\u011funlu\u011funu art\u0131rmayacakt\u0131r.<\/li>\n<\/ul>\n<h3>6. Lens odak uzakl\u0131\u011f\u0131<\/h3>\n<p>Odaklama y\u00f6ntemi genellikle kaynak s\u0131ras\u0131nda lazeri yo\u011funla\u015ft\u0131rmak i\u00e7in kullan\u0131l\u0131r ve genellikle 63~254 mm odak uzakl\u0131\u011f\u0131na sahip bir lens kullan\u0131l\u0131r. Odak noktas\u0131 boyutu odak uzakl\u0131\u011f\u0131 ile orant\u0131l\u0131d\u0131r. Odak uzakl\u0131\u011f\u0131 ne kadar k\u0131sa olursa, nokta o kadar k\u00fc\u00e7\u00fck olur. Bununla birlikte, odak uzakl\u0131\u011f\u0131 odak derinli\u011fini de etkiler. Yani, odak derinli\u011fi odak uzakl\u0131\u011f\u0131 ile e\u015fzamanl\u0131 olarak artar. Dolay\u0131s\u0131yla, k\u0131sa bir odak uzakl\u0131\u011f\u0131 g\u00fc\u00e7 yo\u011funlu\u011funu art\u0131rabilir. K\u00fc\u00e7\u00fck odak derinli\u011fi nedeniyle, lens ile i\u015f par\u00e7as\u0131 aras\u0131ndaki mesafe hassas bir \u015fekilde korunmal\u0131d\u0131r ve penetrasyon derinli\u011fi b\u00fcy\u00fck de\u011fildir.<\/p>\n<p>Kaynak i\u015fleminde olu\u015fan s\u0131\u00e7rama ve lazer modunun etkisi nedeniyle, ger\u00e7ek kaynakta kullan\u0131lan en k\u0131sa odak derinli\u011fi \u00e7o\u011funlukla 126mm (5\u2033) odak uzakl\u0131\u011f\u0131d\u0131r. Ba\u011flant\u0131 b\u00fcy\u00fck oldu\u011funda veya kaynak diki\u015finin nokta boyutunu art\u0131rarak b\u00fcy\u00fct\u00fclmesi gerekti\u011finde, 254 mm odak uzunlu\u011funa sahip bir lens se\u00e7ebilirsiniz. Bu durumda, derin penetrasyonlu i\u011fne deli\u011fi etkisini elde etmek i\u00e7in daha y\u00fcksek bir lazer \u00e7\u0131k\u0131\u015f g\u00fcc\u00fc (g\u00fc\u00e7 yo\u011funlu\u011fu) gerekir.<\/p>\n<p>Lazer g\u00fcc\u00fc 2kW'\u0131 a\u015ft\u0131\u011f\u0131nda (\u00f6zellikle 10.6\u03bcm CO2 lazer \u0131\u015f\u0131n\u0131 i\u00e7in), optik sistemi olu\u015fturmak i\u00e7in \u00f6zel optik malzemelerin kullan\u0131lmas\u0131 nedeniyle, odaklama merce\u011fine optik hasar riskini \u00f6nlemek i\u00e7in genellikle yans\u0131t\u0131c\u0131 odaklama y\u00f6ntemi kullan\u0131l\u0131r. Reflekt\u00f6r olarak genellikle cilal\u0131 bir bak\u0131r ayna kullan\u0131l\u0131r. Etkili so\u011futma nedeniyle genellikle y\u00fcksek g\u00fc\u00e7l\u00fc lazer \u0131\u015f\u0131nlar\u0131n\u0131n odaklanmas\u0131 i\u00e7in \u00f6nerilir.<\/p>\n<h3>7. Odak pozisyonu<\/h3>\n<p>Odak noktas\u0131 konumu, kaynak yaparken yeterli g\u00fc\u00e7 yo\u011funlu\u011funu korumak i\u00e7in kritik \u00f6neme sahiptir. Odak noktas\u0131n\u0131n i\u015f par\u00e7as\u0131 y\u00fczeyine g\u00f6re konumundaki de\u011fi\u015fiklikler, kaynak geni\u015fli\u011fini ve derinli\u011fini do\u011frudan etkiler.<br \/>\n\u00c7o\u011fu lazer kaynak uygulamas\u0131nda, odak noktas\u0131 tipik olarak i\u015f par\u00e7as\u0131 y\u00fczeyinin alt\u0131nda istenen f\u00fczyon derinli\u011finin yakla\u015f\u0131k 1\/4'\u00fc kadar bulunur.<\/p>\n<h3>8. Lazer \u0131\u015f\u0131n\u0131 konumu<\/h3>\n<p>Birbirine benzemeyen malzemelerin lazerle kayna\u011f\u0131nda lazer \u0131\u015f\u0131n\u0131 konumu, \u00f6zellikle bindirmeli ba\u011flant\u0131lardan ziyade al\u0131n ba\u011flant\u0131lar\u0131nda kayna\u011f\u0131n nihai kalitesini kontrol eder. \u00d6rne\u011fin, sertle\u015ftirilmi\u015f \u00e7elik bir di\u015fli yumu\u015fak \u00e7elik bir tambura kaynakland\u0131\u011f\u0131nda, lazer \u0131\u015f\u0131n\u0131 konumunun uygun \u015fekilde kontrol edilmesi, nispeten \u00e7atlamaya dayan\u0131kl\u0131 ve a\u011f\u0131rl\u0131kl\u0131 olarak d\u00fc\u015f\u00fck karbonlu bir bile\u015fene sahip bir kaynak \u00fcretilmesine yard\u0131mc\u0131 olacakt\u0131r. Baz\u0131 uygulamalarda, kaynak yap\u0131lacak i\u015f par\u00e7as\u0131n\u0131n geometrisi lazer \u0131\u015f\u0131n\u0131n\u0131n bir a\u00e7\u0131 ile sapt\u0131r\u0131lmas\u0131n\u0131 gerektirir. I\u015f\u0131n ekseni ile birle\u015ftirme d\u00fczlemi aras\u0131ndaki sapma a\u00e7\u0131s\u0131 100 derece i\u00e7inde oldu\u011funda, lazer enerjisinin i\u015f par\u00e7as\u0131 taraf\u0131ndan emilmesi etkilenmeyecektir.<\/p>\n<h3>9. Kayna\u011f\u0131n ba\u015flang\u0131\u00e7 ve biti\u015f noktalar\u0131nda lazer g\u00fcc\u00fcn\u00fcn kademeli olarak y\u00fckselme ve d\u00fc\u015fme kontrol\u00fc<\/h3>\n<p>Lazer derin n\u00fcfuziyet kayna\u011f\u0131 s\u0131ras\u0131nda, kaynak derinli\u011finden ba\u011f\u0131ms\u0131z olarak k\u00fc\u00e7\u00fck delikler her zaman mevcuttur. Kaynak i\u015flemi sonland\u0131r\u0131ld\u0131\u011f\u0131nda ve g\u00fc\u00e7 anahtar\u0131 kapat\u0131ld\u0131\u011f\u0131nda, kayna\u011f\u0131n sonunda bir \u00e7ukur g\u00f6r\u00fcnecektir. Ek olarak, lazer kaynak katman\u0131 orijinal kaynak diki\u015fini kaplad\u0131\u011f\u0131nda, lazer \u0131\u015f\u0131n\u0131n\u0131n a\u015f\u0131r\u0131 emilimi meydana gelecektir. Bu, kaynak par\u00e7as\u0131n\u0131n a\u015f\u0131r\u0131 \u0131s\u0131nmas\u0131na veya g\u00f6zeneklerin olu\u015fmas\u0131na neden olur.<\/p>\n<p>Yukar\u0131daki olaylar\u0131n meydana gelmesini \u00f6nlemek i\u00e7in, g\u00fc\u00e7 ba\u015flang\u0131\u00e7 ve biti\u015f zamanlar\u0131n\u0131 ayarlamak \u00fczere g\u00fc\u00e7 ba\u015flang\u0131\u00e7 ve biti\u015f noktalar\u0131 programlanabilir. Ba\u015flang\u0131\u00e7 g\u00fcc\u00fc elektronik olarak k\u0131sa bir s\u00fcre i\u00e7inde s\u0131f\u0131rdan ayarlanan g\u00fc\u00e7 de\u011ferine y\u00fckseltilir. Ve kaynak s\u00fcresi ayarlanabilir. Son olarak, kaynak sonland\u0131r\u0131ld\u0131\u011f\u0131nda g\u00fc\u00e7 kademeli olarak ayarlanan g\u00fc\u00e7ten s\u0131f\u0131ra d\u00fc\u015f\u00fcr\u00fcl\u00fcr.<\/p>","protected":false},"excerpt":{"rendered":"<p>Giri\u015f: Bir \u00f6nceki makalede Derin N\u00fcfuziyetli Lazer Kayna\u011f\u0131n\u0131n prensiplerini ve \u00f6zelliklerini tart\u0131\u015ft\u0131k. Burada, ana i\u015flem parametrelerine odaklanaca\u011f\u0131z. Bu, bu kaynak tekni\u011fi hakk\u0131nda daha fazla bilgi edinmeniz i\u00e7in yararl\u0131d\u0131r. Derin N\u00fcfuziyetli Lazer Kayna\u011f\u0131n\u0131n Ana Proses Parametreleri 1. Lazer g\u00fcc\u00fc Lazer g\u00fcc\u00fc Lazer g\u00fcc\u00fcn\u00fcn bir e\u015fik de\u011feri vard\u0131r...<\/p>","protected":false},"author":7,"featured_media":6544,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[1,57],"tags":[],"class_list":["post-6537","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-blog","category-laser-welding-machine-blog"],"yoast_head":"<!-- This site is optimized with the Yoast SEO plugin v28.3 - https:\/\/yoast.com\/product\/yoast-seo-wordpress\/ -->\n<title>The Main Process Parameters Of Deep Penetration Laser Welding<\/title>\n<meta name=\"description\" content=\"In today&#039;s article, we will discuss in depth the main process parameters of deep penetration laser welding.\" \/>\n<meta name=\"robots\" content=\"index, follow, max-snippet:-1, max-image-preview:large, max-video-preview:-1\" \/>\n<link rel=\"canonical\" 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