{"id":3955,"date":"2026-08-06T08:22:11","date_gmt":"2026-08-06T08:22:11","guid":{"rendered":"https:\/\/nbaem.com\/?p=3955"},"modified":"2026-07-23T08:28:30","modified_gmt":"2026-07-23T08:28:30","slug":"what-is-magnetic-coupling-in-transformer","status":"publish","type":"post","link":"https:\/\/nbaem.com\/tr\/what-is-magnetic-coupling-in-transformer\/","title":{"rendered":"Transformat\u00f6rlerde Manyetik T\u0131mba\/Birle\u015fim Nedir ve Nas\u0131l A\u00e7\u0131klar?"},"content":{"rendered":"<p>Bir transformat\u00f6r\u00fcn bir devreden di\u011ferine megavatlarca g\u00fcc\u00fc tek bir fiziksel kablo ba\u011flant\u0131s\u0131 olmadan nas\u0131l aktarabildi\u011fini hi\u00e7 merak ettiniz mi? Cevap, <strong>transformat\u00f6rdeki manyetik kavrulama<\/strong> tasar\u0131mlar\u0131nda yatmaktad\u0131r\u2014tam galvanik izolasyon e\u015fli\u011finde verimli g\u00fc\u00e7 aktar\u0131m\u0131n\u0131 sa\u011flayan temel bir elektromanyetkin s\u00fcre\u00e7.<\/p>\n<p>\u0130\u015fte elektrik enerjisini g\u00fcvenilir bir \u015fekilde aktarmak i\u00e7in manyetik kavray\u0131\u015ftan nas\u0131l yararland\u0131\u011f\u0131m\u0131za dair kesin ad\u0131m ad\u0131m fiziksel s\u00fcre\u00e7.<\/p>\n<hr \/>\n<h2>Manyetik Kavraman\u0131n Nas\u0131l \u00c7al\u0131\u015ft\u0131\u011f\u0131: Ad\u0131m Ad\u0131m Fizik<\/h2>\n<h3>Ad\u0131m 1: AC Ak\u0131m Giri\u015fi ve Dinamik Manyetik Alan \u00dcretimi<\/h3>\n<p>Her manyetik kavrama s\u00fcreci <strong>birincil sarg\u0131<\/strong>ile ba\u015flar. Bu giri\u015f bobu\u011fundan alternatif ak\u0131m (AC) ge\u00e7ti\u011finde sal\u0131n\u0131ml\u0131 bir manyetik alan yarat\u0131r. AC y\u00f6n\u00fcn\u00fc ve b\u00fcy\u00fckl\u00fc\u011f\u00fcn\u00fc s\u00fcrekli de\u011fi\u015ftirdi\u011fi i\u00e7in olu\u015fan manyetik alan dinamik olup, giri\u015f dalgas\u0131 ile birlikte geni\u015fler ve \u00e7\u00f6ker.<\/p>\n<ul>\n<li style=\"list-style-type: none;\">\n<ul>\n<li><strong>Anahtar Mekanizma:<\/strong> Ak\u0131m de\u011fi\u015fim h\u0131z\u0131 do\u011frudan manyetik alan\u0131n g\u00fcc\u00fcn\u00fc ve frekans\u0131n\u0131 belirler.<\/li>\n<li><strong>Ana Gereklilik:<\/strong> Enerji iletimi bu s\u00fcrekli alan varyasyonuna ba\u011fl\u0131d\u0131r; sabit bir DC ak\u0131m\u0131 dinamik kavramay\u0131 s\u00fcrd\u00fcremez.<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<h3>Ad\u0131m 2: Y\u00fcksek Doyum Ba\u015fl\u0131kl\u0131 \u00c7ekirdek ile Ak\u0131 Yo\u011funla\u015ft\u0131rma<\/h3>\n<p>A\u00e7\u0131k havada manyetik alanlar her y\u00f6ne da\u011f\u0131l\u0131r, \u015fiddetli enerji kayb\u0131na neden olur. Manyetik ba\u011fla\u015f\u0131m\u0131 en \u00fcst d\u00fczeye \u00e7\u0131karmak i\u00e7in bu enerjiyi bir <strong>y\u00fcksek manyetik ge\u00e7irgenlikli g\u00f6vde<\/strong> (lamine edilmi\u015f silikon \u00e7eli\u011fi veya geli\u015fmi\u015f yumu\u015fak manyetik ala\u015f\u0131mlar gibi).<\/p>\n<ul>\n<li style=\"list-style-type: none;\">\n<ul>\n<li><strong>Flux Kanalizasyonu:<\/strong> \u00c7ekirdek d\u00fc\u015f\u00fck-ge\u00e7irgenlikli bir yol sa\u011flar, <strong>manyetik ak\u0131 ba\u011flant\u0131s\u0131n\u0131 hapseder ve yo\u011funla\u015ft\u0131r\u0131r<\/strong>.<\/li>\n<li><strong>S\u0131zd\u0131rmazl\u0131k Kontrol\u00fc:<\/strong> G\u00fc\u00e7 hatlar\u0131n\u0131 s\u0131n\u0131rland\u0131rmak, ak\u0131 s\u0131zd\u0131rmas\u0131n\u0131 \u00f6nler ve \u00fcretilen enerjinin b\u00fcy\u00fck \u00e7o\u011funlu\u011funun do\u011frudan \u00e7\u0131k\u0131\u015f sarmal\u0131na gitmesini sa\u011flar.<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<h3>Ad\u0131m 3: Sekonder Sarmalda Gerilim End\u00fcksiyonu<\/h3>\n<p>Dinamik manyetik ak\u0131 \u00e7ekirde\u011fin \u00fczerinden hareket ederken do\u011frudan <strong>sekonder sarmayla<\/strong>ba\u011flant\u0131l\u0131d\u0131r. Bu de\u011fi\u015fen manyetik ortam <strong>Faraday'\u0131n Elektromanyetik \u0130nd\u00fcksiyon Yasas\u0131'n\u0131<\/strong>.<\/p>\n<ul>\n<li style=\"list-style-type: none;\">\n<ul>\n<li><strong>EMF \u00dcretimi:<\/strong> Zamanla de\u011fi\u015fen manyetik ak\u0131, ikincil sarg\u0131 sarmalar\u0131n\u0131 keser, elektromotor kuvveti (EMF) ind\u00fckler ve kesin bir \u00e7\u0131kt\u0131 gerilimi \u00fcretir.<\/li>\n<li><strong>Galvanik \u0130zolasyon:<\/strong> G\u00fc\u00e7 yaln\u0131zca manyetik ak\u0131 \u00fczerinden hareket eder, birincil ve ikincil devreleri elektriksel olarak tamamen izole eder.<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<h2>Manyetik E\u015fle\u015fmeyi Y\u00f6neten Temel Parametreler<\/h2>\n<p>Y\u00fcksek verimli trafolar tasarlarken, ba\u015fl\u0131ca elektriksel parametreler manyetik enerjinin sarg\u0131lar aras\u0131nda ne kadar etkili hareket etti\u011fini tan\u0131mlar. Bu de\u011fi\u015fkenleri kontrol etmek, istenmeyen kay\u0131plar\u0131 en aza indirirken enerji transferini maksimize etmemizi sa\u011flar.<\/p>\n<h3>Kendili\u011finden End\u00fcksiyon (Self-Inductance) &amp; Kar\u015f\u0131l\u0131kl\u0131 End\u00fcksiyon (Mutual Inductance)<\/h3>\n<ul>\n<li style=\"list-style-type: none;\">\n<ul>\n<li><strong>Kendili\u011finden End\u00fcksiyon (L1, L2):<\/strong> De\u011fi\u015fken AC ak\u0131m\u0131 ile hareket ettirildi\u011finde tek ba\u015f\u0131na birincil veya ikincil sarg\u0131n\u0131n kendi i\u00e7inde gerilim ind\u00fckleme yetene\u011fi.<\/li>\n<li><strong>Kar\u015f\u0131l\u0131kl\u0131 End\u00fcksiyon (M):<\/strong> Birincil sarg\u0131da ak\u0131m de\u011fi\u015fikliklerinin ikincil sarg\u0131 \u00fczerinde gerilim ind\u00fckleme etme g\u00fcc\u00fcn\u00fcn \u00f6l\u00e7\u00fcs\u00fcd\u00fcr. Y\u00fcksek kar\u015f\u0131l\u0131kl\u0131 end\u00fcksiyon etkili bir tasla\u011f\u0131n belkemi\u011fini olu\u015fturur. <a href=\"https:\/\/nbaem.com\/tr\/magnetic-coupling\/\">manyetik ba\u011flant\u0131<\/a> Tasar\u0131m.<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<h3>Ba\u011flant\u0131 Katsay\u0131s\u0131 (k)<\/h3>\n<p>Ba\u011flant\u0131 katsay\u0131s\u0131 (<strong>k<\/strong>) birincil manyetik ak\u0131 toplam\u0131n\u0131n ikincil sarg\u0131ya ula\u015fma oran\u0131n\u0131 nicelle\u015ftirir. De\u011feri strictly aras\u0131nda <strong>0<\/strong> (tam izolasyon) ve <strong>1<\/strong> (m\u00fckemmel ak\u0131\u015f transferi).<\/p>\n<p>Matematiksel ili\u015fki \u015fu \u015fekilde hesaplan\u0131r: <strong>M = k * sqrt(L1 * L2)<\/strong><\/p>\n<h3>\u0130deal ile Ger\u00e7ek D\u00fcnya E\u015fle\u015fmesi (k De\u011feri Da\u011f\u0131l\u0131m\u0131)<\/h3>\n<table>\n<thead>\n<tr>\n<th style=\"text-align: left;\">E\u015fle\u015fme S\u0131n\u0131f\u0131<\/th>\n<th style=\"text-align: left;\">k Fakt\u00f6r\u00fc Aral\u0131\u011f\u0131<\/th>\n<th style=\"text-align: left;\">Fiziksel Davran\u0131\u015f<\/th>\n<th style=\"text-align: left;\">Birincil Uygulamalar<\/th>\n<\/tr>\n<\/thead>\n<tbody>\n<tr>\n<td style=\"text-align: left;\"><strong>\u0130deal E\u015fle\u015fme<\/strong><\/td>\n<td style=\"text-align: left;\">k = 1.0<\/td>\n<td style=\"text-align: left;\">100% ak\u0131\u015f ba\u011flant\u0131s\u0131; s\u0131f\u0131r s\u0131z\u0131nt\u0131 ak\u0131\u015f\u0131.<\/td>\n<td style=\"text-align: left;\">Sadece kuramsal modeller.<\/td>\n<\/tr>\n<tr>\n<td style=\"text-align: left;\"><strong>S\u0131k\u0131 E\u015fle\u015fme<\/strong><\/td>\n<td style=\"text-align: left;\">0.95 &lt;= k &lt; 1.0<\/td>\n<td style=\"text-align: left;\">Y\u00fcksek ge\u00e7irgenlikli n\u00fcve; minimum s\u0131z\u0131nt\u0131 ak\u0131m\u0131.<\/td>\n<td style=\"text-align: left;\">\u015eebeke g\u00fc\u00e7 tranformat\u00f6rleri, y\u00fckseltme\/al\u00e7altma \u00fcniteleri.<\/td>\n<\/tr>\n<tr>\n<td style=\"text-align: left;\"><strong>Gev\u015fek Ba\u011flant\u0131<\/strong><\/td>\n<td style=\"text-align: left;\">k &lt; 0,5<\/td>\n<td style=\"text-align: left;\">B\u00fcy\u00fck hava bo\u015fluklar\u0131; d\u00fc\u015f\u00fck manyetik ba\u011flant\u0131.<\/td>\n<td style=\"text-align: left;\">Kablosuz \u015farj, rezonans d\u00f6n\u00fc\u015ft\u00fcr\u00fcc\u00fcler.<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<h3>Transformat\u00f6r Polenli\u011fi: Nokta Kural\u0131<\/h3>\n<p>Winding y\u00f6n\u00fc, giri\u015f ve \u00e7\u0131k\u0131\u015f terminalleri aras\u0131ndaki gerilim faz ili\u015fkilerini belirler. Biz g\u00fcveniyoruz <strong>nokta kural\u0131na<\/strong> do\u011fru devre polaritesini korumak i\u00e7in:<\/p>\n<ul>\n<li style=\"list-style-type: none;\">\n<ul>\n<li><strong>Ayn\u0131 Faz Ko\u015fulu:<\/strong> Ak\u0131m i\u015faretli birincil terminale d\u00fc\u015ft\u00fc\u011f\u00fcnde, i\u015faretli ikincil terminal an\u0131nda pozitiftir.<\/li>\n<li><strong>Faz Terslemesi:<\/strong> Ak\u0131m i\u015faretli olmayan birincil terminale girdi\u011finde, i\u015faretli ikincil terminal g\u00f6receli negatif gerilim \u00fcretir.<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<p>Do\u011fru polarite e\u015fle\u015fmesi sinyalin yok olmas\u0131n\u0131 engeller ve paralel transformat\u00f6r konfig\u00fcrasyonlar\u0131nda y\u0131k\u0131c\u0131 dola\u015f\u0131m ak\u0131mlar\u0131n\u0131 durdurur.<\/p>\n<h2>Ba\u011flant\u0131 Verimlilik Kayb\u0131 ve \u00c7ekirde\u011fi Etkileyen Tasar\u0131m Fakt\u00f6rleri<\/h2>\n<p>Y\u00fcksek manyetik ge\u00e7irgenlik malzemelerle bile, ger\u00e7ek d\u00fcnyadaki hi\u00e7bir sistem m\u00fckemmel performans elde edemez <strong>transformat\u00f6rdeki manyetik kavrulama<\/strong> y\u00fcksek verimli tranformat\u00f6rler in\u015fa ederken ve optimize ederken, bir dizi fiziksel tasar\u0131m fakt\u00f6r\u00fc birincil ile ikincil sarg\u0131 aras\u0131nda tam ak\u0131 transferini engeller. Bu kay\u0131p mekanizmalar\u0131n\u0131 anlamak, enerji transferini maksimize etmeyi ve y\u00fcksek kapsama katsay\u0131s\u0131n\u0131 korumay\u0131 sa\u011flar (<strong>k<\/strong>).<\/p>\n<h3>S\u0131zd\u0131rma Ak\u0131m\u0131 ve S\u0131zd\u0131rma End\u00fcktans\u0131<\/h3>\n<p>Birincil sarg\u0131 taraf\u0131ndan \u00fcretilen t\u00fcm manyetik ak\u0131, \u00e7ekirde\u011fin \u00fczerinden ikincil sarg\u0131ya ba\u011flanacak \u015fekilde hareket etmez. Baz\u0131 ak\u0131lar \u00e7evreleyen havaya ka\u00e7ar\u2014bu durum <strong>s\u0131zd\u0131rma ak\u0131s\u0131<\/strong>.<\/p>\n<ul>\n<li style=\"list-style-type: none;\">\n<ul>\n<li><strong>Sistem Etkisi:<\/strong> S\u0131zd\u0131rma ak\u0131s\u0131 <strong>s\u0131zd\u0131rma end\u00fcktans\u0131n\u0131 olu\u015fturur<\/strong>, tranformat\u00f6r sarg\u0131lar\u0131 ile seri olarak istenmeyen bir end\u00fcktif empedans gibi davran\u0131r.<\/li>\n<li><strong>Verimlilik Kayb\u0131:<\/strong> Artan s\u0131zd\u0131rma ak\u0131s\u0131 toplam manyetik ak\u0131 ba\u011flant\u0131s\u0131n\u0131 d\u00fc\u015f\u00fcr\u00fcr (<strong>\u03a6<\/strong>), do\u011frudan ideal seviyelerin alt\u0131na kapsama katsay\u0131s\u0131n\u0131 d\u00fc\u015f\u00fcr\u00fcr.<\/li>\n<li><strong>Tasar\u0131m Kontrol\u00fc:<\/strong> S\u0131k\u0131 sarg\u0131 geometrileri, konik sarg\u0131 d\u00fczenlemeleri ve y\u00fcksek ge\u00e7irgenli\u011fe sahip \u00e7ekirdek tasar\u0131mlar\u0131yla s\u0131zd\u0131rma end\u00fcktans\u0131n\u0131 minimize ederiz.<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<h3>K\u0131sa Davalar Sistemlerinde \u00c7ekirdek Kay\u0131plar\u0131<\/h3>\n<p>Manyetik \u00e7evrim s\u0131ras\u0131nda \u00e7ekirdek malzemesinin kendisi i\u00e7inde olu\u015fan kay\u0131plar, enerjiyi \u0131s\u0131 olarak da\u011f\u0131t\u0131r ve toplam sistem verimlili\u011fini d\u00fc\u015f\u00fcr\u00fcr.<\/p>\n<table>\n<thead>\n<tr>\n<th style=\"text-align: left;\">Kay\u0131p Mekanizmas\u0131<\/th>\n<th style=\"text-align: left;\">Neden<\/th>\n<th style=\"text-align: left;\">M\u00fchendislik \u00c7\u00f6z\u00fcm\u00fc<\/th>\n<\/tr>\n<\/thead>\n<tbody>\n<tr>\n<td style=\"text-align: left;\"><strong>\u00c7evresel Ak\u0131m Kayb\u0131<\/strong><\/td>\n<td style=\"text-align: left;\">De\u011fi\u015fen manyetik alanlar nedeniyle iletken \u00e7ekirdek malzemesi i\u00e7inde ind\u00fcklenen dolayl\u0131 ak\u0131mlar.<\/td>\n<td style=\"text-align: left;\">Kullan <strong>yap\u0131sal olarak lamine edilmi\u015f silikon \u00e7elik \u00e7ekirdek<\/strong> veya elektriksel yollar\u0131 kesintiye u\u011fratmak i\u00e7in y\u00fcksek diren\u00e7li ferrit malzemeler<\/td>\n<\/tr>\n<tr>\n<td style=\"text-align: left;\"><strong>Histerezis Kayb\u0131<\/strong><\/td>\n<td style=\"text-align: left;\">her alternatif ak\u0131m (AC) d\u00f6ng\u00fcs\u00fc s\u0131ras\u0131nda manyetik alanlar\u0131 y\u00f6nlendirmek i\u00e7in gereken enerji.<\/td>\n<td style=\"text-align: left;\">\u00d6zel olarak se\u00e7 <strong>yumu\u015fak manyetik malzemeler<\/strong> dar hysteresis d\u00f6ng\u00fclerine ve d\u00fc\u015f\u00fck koersiviteye sahip<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<p>\u00c7ekirdek kay\u0131plar\u0131n\u0131 kontrol etmek, y\u00fcksek frekansl\u0131 transformat\u00f6r \u00e7ekirdeklerinde kritiktir; burada y\u00fckselen \u00e7al\u0131\u015fma frekanslar\u0131 s\u0131cakl\u0131k art\u0131\u015f\u0131n\u0131 ve enerji dissipas\u0131n\u0131 h\u0131zland\u0131r\u0131r.<\/p>\n<h3>Manyetik \u00c7ekirdek Doymas\u0131<\/h3>\n<p>Her manyetik \u00e7ekirdek malzemesinin maksimum manyetik ak\u0131 yo\u011funlu\u011fu s\u0131n\u0131r\u0131 vard\u0131r. Manyetik alan g\u00fcc\u00fc bu e\u015fikten daha fazla artt\u0131\u011f\u0131nda, \u00e7ekirdek <strong>manyetik \u00e7ekirdek doygunlu\u011fu<\/strong>.<\/p>\n<ul>\n<li style=\"list-style-type: none;\">\n<ul>\n<li><strong>E\u015fle\u015fme Bozulmas\u0131:<\/strong> Doygunlukta \u00e7ekirde\u011fin g\u00f6receli manyetik ge\u00e7irgenli\u011fi 1\u2019e (havayla ayn\u0131 ge\u00e7irgenlik) do\u011fru keskin bir \u015fekilde d\u00fc\u015fer. Bu, manyetik e\u015fle\u015fme performans\u0131nda dramatik bir d\u00fc\u015f\u00fc\u015fe yol a\u00e7ar.<\/li>\n<li><strong>Termal ve Elektrik Riski:<\/strong> Doygunluk, \u015fiddetli ak\u0131m y\u00fckselmelerine, \u00e7\u0131kt\u0131 dalga bi\u00e7imi bozulmas\u0131na ve sar\u0131mlara kar\u015f\u0131 a\u015f\u0131r\u0131 termal strese yol a\u00e7ar.<\/li>\n<li><strong>Gev\u015fetme \u00d6nlemi:<\/strong> Yeterli ak\u0131 kapasitesine sahip kesit alanlar\u0131na sahip bir transformat\u00f6r \u00e7ekirde\u011fi tasarl\u0131yor ve y\u00fcksek doygunluk ak\u0131 yo\u011funlu\u011fu i\u00e7in tasarlanm\u0131\u015f yumu\u015fak manyetik ala\u015f\u0131mlar\u0131 se\u00e7iyoruz.<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<h2>Maksimum E\u015fle\u015fme Verimlili\u011fi \u0130\u00e7in Yumu\u015fak Manyetik Malzemelerin Se\u00e7imi<\/h2>\n<p>Bir transformat\u00f6rde maksimum manyetik e\u015fle\u015fme verimlili\u011fini elde etmek i\u00e7in \u00e7ekirdek malzemesi se\u00e7imi kritiktir. \u00c7ekirdek, birincil sarg\u0131dan ikincil sarg\u0131ya manyetik ak\u0131 ba\u011flant\u0131s\u0131n\u0131 y\u00f6nlendirir ve do\u011frudan e\u015fle\u015fme katsay\u0131s\u0131n\u0131 (k) ideal performansa yakla\u015ft\u0131r\u0131r.<\/p>\n<h3>\u0130deal Transformat\u00f6r \u00c7ekirde\u011fi Malzemelerinin \u00d6zellikleri<\/h3>\n<p>Y\u00fcksek verimlilikli transformat\u00f6r \u00e7ekirdekleri tasarlarken belirli fiziksel ve manyetik \u00f6zellikleri ar\u0131yoruz:<\/p>\n<ul>\n<li style=\"list-style-type: none;\">\n<ul>\n<li><strong>Y\u00fcksek Manyetik Permeabilite (\u00b5):<\/strong> Manyetik ak\u0131y\u0131 y\u00f6nlendirir ve yo\u011funla\u015ft\u0131r\u0131r, s\u0131z\u0131nt\u0131 end\u00fcktans\u0131n\u0131 azalt\u0131r.<\/li>\n<li><strong>Y\u00fcksek Doygunluk Ak\u0131 Yo\u011funlu\u011fu (Bs):<\/strong> Yo\u011fun y\u00fck ak\u0131mlar\u0131 alt\u0131nda \u00e7ekirdek doygunlu\u011funu \u00f6nler.<\/li>\n<li><strong>D\u00fc\u015f\u00fck Histerezis Kayb\u0131:<\/strong> S\u00fcrekli AC d\u00f6ng\u00fcs\u00fc s\u0131ras\u0131nda termal enerji kay\u0131plar\u0131n\u0131 en aza indirir.<\/li>\n<li><strong>Y\u00fcksek Elektrik Direnci:<\/strong> Manyetik \u00e7ekirdekteki kay\u0131plar\u0131 d\u00fc\u015f\u00fck tutmak i\u00e7in eddy ak\u0131mlar\u0131n\u0131 bast\u0131r\u0131r.<\/li>\n<li><strong>Yap\u0131sal Kararl\u0131l\u0131k:<\/strong> \u00c7al\u0131\u015fma gerilimi alt\u0131nda mekanik g\u00fcvenilirlik sa\u011flar; kal\u0131c\u0131 manyetik malzeme k\u0131r\u0131lganl\u0131\u011f\u0131 olan sert manyetik sistemlerin aksine <a href=\"https:\/\/nbaem.com\/tr\/permanent-magnetic-material-brittleness\/\">k\u0131r\u0131lganl\u0131k<\/a> i\u015fleme zorluklar\u0131<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<h3>Yumu\u015fak Manyetik Malzeme Se\u00e7eneklerinin Kar\u015f\u0131la\u015ft\u0131r\u0131lmas\u0131<\/h3>\n<p>Farkl\u0131 \u00e7al\u0131\u015fma frekanslar\u0131, performans\u0131 optimize etmek ve enerji kayb\u0131n\u0131 \u00f6nlemek i\u00e7in \u00f6zel olarak uyarlanm\u0131\u015f yumu\u015fak manyetik malzemeler gerektirir:<\/p>\n<table>\n<thead>\n<tr>\n<th style=\"text-align: left;\">Malzeme T\u00fcr\u00fc<\/th>\n<th style=\"text-align: left;\">Manyetik Ge\u00e7irgenlik (\u00b5)<\/th>\n<th style=\"text-align: left;\">Doygunluk Ak\u0131 Yo\u011funlu\u011fu (Bs)<\/th>\n<th style=\"text-align: left;\">Optimal Frekans Aral\u0131\u011f\u0131<\/th>\n<th style=\"text-align: left;\">\u00c7ekirdek Dayan\u0131kl\u0131l\u0131\u011f\u0131<\/th>\n<\/tr>\n<\/thead>\n<tbody>\n<tr>\n<td style=\"text-align: left;\"><strong>Kaplamal\u0131 Silikon \u00c7eli\u011fi<\/strong><\/td>\n<td style=\"text-align: left;\">Y\u00fcksek<\/td>\n<td style=\"text-align: left;\">\u00c7ok Y\u00fcksek (~2.0 T)<\/td>\n<td style=\"text-align: left;\">50 Hz \u2013 400 Hz<\/td>\n<td style=\"text-align: left;\">K hatlar\u0131na i\u00e7in maksimum g\u00fc\u00e7 i\u015fleme<\/td>\n<\/tr>\n<tr>\n<td style=\"text-align: left;\"><strong>MnZn \/ NiZn Florit<\/strong><\/td>\n<td style=\"text-align: left;\">Orta ile Y\u00fcksek<\/td>\n<td style=\"text-align: left;\">D\u00fc\u015f\u00fck (~0.4 \u2013 0.5 T)<\/td>\n<td style=\"text-align: left;\">20 kHz \u2013 1 MHz+<\/td>\n<td style=\"text-align: left;\">Y\u00fcksek diren\u00e7lilik, neredeyse s\u0131f\u0131r eddy current kay\u0131plar\u0131<\/td>\n<\/tr>\n<tr>\n<td style=\"text-align: left;\"><strong>Amorf Ala\u015f\u0131m<\/strong><\/td>\n<td style=\"text-align: left;\">\u00c7ok Y\u00fcksek<\/td>\n<td style=\"text-align: left;\">Orta (~1.5 T)<\/td>\n<td style=\"text-align: left;\">50 Hz \u2013 10 kHz<\/td>\n<td style=\"text-align: left;\">Y\u00fcksek verimli da\u011f\u0131t\u0131m i\u00e7in ultra-d\u00fc\u015f\u00fck \u00e7ekirdek kayb\u0131<\/td>\n<\/tr>\n<tr>\n<td style=\"text-align: left;\"><strong>Nanokristalin<\/strong><\/td>\n<td style=\"text-align: left;\">En y\u00fcksek<\/td>\n<td style=\"text-align: left;\">Orta-Y\u00fcksek (~1.2 T)<\/td>\n<td style=\"text-align: left;\">10 kHz \u2013 100 kHz+<\/td>\n<td style=\"text-align: left;\">Minimal termal da\u011f\u0131lma ile \u00fcst d\u00fczey ge\u00e7irgenlik<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<p>\u00c7er\u00e7eve malzeme \u00f6zelliklerini do\u011frudan \u00e7al\u0131\u015fma frekanslar\u0131na e\u015fle\u015ftirerek manyetik stray ak\u0131m\u0131 ortadan kald\u0131r\u0131r ve \u00f6zel tranform\u00f6r tasar\u0131mlar\u0131 aras\u0131nda ba\u011flanma performans\u0131n\u0131 maksimize eder.<\/p>\n<h2>NBAEM taraf\u0131ndan Y\u00fcksek Performansl\u0131 Transformat\u00f6r Laminasyon \u00c7\u00f6z\u00fcmleri<\/h2>\n<p>NBAEM'de, maksimuma \u00e7\u0131karmak i\u00e7in hassas \u00e7ekirdek laminasyonlar\u0131 tasarl\u0131yor ve \u00fcretiyoruz <strong>transformat\u00f6rdeki manyetik kavrulama<\/strong> ayn\u0131 anda u\u011fra\u015f\u0131rken rastgele enerji kay\u0131plar\u0131n\u0131 minimize etmek. Geli\u015fmi\u015f \u00fcretim yeteneklerimiz, g\u00fc\u00e7 elektroni\u011fi m\u00fchendislerinin y\u00fcksek performansl\u0131 g\u00fc\u00e7 transformat\u00f6rleri \u00fczerinde s\u0131k manyetik ak\u0131 ba\u011flant\u0131s\u0131, azalt\u0131lm\u0131\u015f s\u0131z\u0131nt\u0131 end\u00fcktans\u0131 ve \u00fcst\u00fcn termal verimlilik elde etmelerine yard\u0131mc\u0131 olur.<\/p>\n<h3>\u00d6zel Laminasyon \u00c7ekirde\u011fi \u0130stifleri<\/h3>\n<p>Her tranformat\u00f6r topolojisi kendine \u00f6zg\u00fc fiziksel ve elektriksel s\u0131n\u0131rlamalara sahiptir. Tam performans spesifikasyonlar\u0131n\u0131za g\u00f6re \u00f6zel olarak tasarlanm\u0131\u015f laminasyon y\u0131\u011f\u0131nlar\u0131 \u00fcretiminde uzman\u0131z:<\/p>\n<ul>\n<li style=\"list-style-type: none;\">\n<ul>\n<li><strong>\u00d6zel \u0130\u00e7 Taban Geometrileri:<\/strong> EI, UI, EFD, PQ ve \u00f6zel damgal\u0131 konfig\u00fcrasyonlar, y\u00fcksek yuva-doldurma oran\u0131 ve kompakt ayak izi i\u00e7in optimize edilmi\u015ftir.<\/li>\n<li><strong>Tasnif ve Yap\u0131\u015ft\u0131rma Hassasiyeti<\/strong> Sesli g\u00fcr\u00fclt\u00fcy\u00fc ve mekanik titre\u015fimi ortadan kald\u0131rmak i\u00e7in tasarlanm\u0131\u015f kilitleme, lazerle kaynak ve \u00f6zel epoxy yap\u0131\u015f\u0131m teknikleri.<\/li>\n<li><strong>Azalt\u0131lm\u0131\u015f Daire D\u0131\u015f\u0131nda Kay\u0131p:<\/strong> \u0130nce ultra ince lamination kesimleri, eddy ak\u0131m\u0131 devrelerini k\u0131saltmak ve y\u00fcksek ba\u011flan\u0131m katsay\u0131lar\u0131n\u0131 korumak i\u00e7in \u00f6zel olarak tasarlanm\u0131\u015ft\u0131r.<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<h3>Geni\u015f Yumu\u015fak Magneatik Malzeme Portf\u00f6y\u00fc<\/h3>\n<p>Geni\u015f bir \u00fcr\u00fcn yelpazesi s\u00fcrd\u00fcrd\u00fc\u011f\u00fcm\u00fcz <strong>yumu\u015fak manyetik malzemeler<\/strong> \u00e7e\u015fitli \u00e7al\u0131\u015fma frekanslar\u0131n\u0131, ak\u0131\u015f yo\u011funluklar\u0131n\u0131 ve termal profilleri desteklemek i\u00e7in:<\/p>\n<ul>\n<li style=\"list-style-type: none;\">\n<ul>\n<li><strong>Grain-Oriented Silicon Steel (CRGO):<\/strong> \u00c7izgisel ak\u0131m frekansl\u0131 g\u00fc\u00e7 trafolar\u0131 i\u00e7in en iyi, yuvarlama y\u00f6n\u00fcnde maksimum manyetik ge\u00e7irgenlik talep edenler i\u00e7indir.<\/li>\n<li><strong>Non-Oriented Silicon Steel (CRNGO):<\/strong> \u00c7ok eksenli manyetik ak\u0131mlar boyunca dengeli manyetik \u00f6zellikler i\u00e7in \u00e7ok y\u00f6nl\u00fc bir se\u00e7enek.<\/li>\n<li><strong>Nikel-\u0130ron Ala\u015f\u0131mlar\u0131 (Permalloy):<\/strong> ultra hassas, y\u00fcksek do\u011fruluklu sinyal ve ak\u0131m transformat\u00f6rleri i\u00e7in son derece y\u00fcksek ba\u015flang\u0131\u00e7 ge\u00e7irgenli\u011fi.<\/li>\n<li><strong>Malzeme Se\u00e7imi Deste\u011fi:<\/strong> Kutu tasar\u0131mlar\u0131n\u0131 de\u011ferlendiren m\u00fchendisler \u00e7o\u011funlukla \u015fu soruyu sorar <a href=\"https:\/\/nbaem.com\/tr\/is-aluminum-a-magnetic-material\/\">Al\u00fcminyum manyetik bir malzeme midir<\/a>, ekipman\u0131n\u0131z i\u00e7in manyetik olmayan yap\u0131sal \u00e7er\u00e7evelere y\u00f6nlendiriyoruz; \u00e7ekirdek y\u0131\u011f\u0131n\u0131 ise premium yumu\u015fak manyetik ala\u015f\u0131mlar kullan\u0131r.<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<h3>\u00dcretim Standartlar\u0131 ve Kalite Kontrol\u00fc<\/h3>\n<p>K\u00fctlesel mekanik toleranslar\u0131 s\u0131k\u0131 tutmak, \u00e7ekirdek montajlar\u0131n\u0131n b\u00fct\u00fcnl\u00fc\u011f\u00fcn\u00fc do\u011frudan korur. <strong>transformat\u00f6rdeki manyetik kavrulama<\/strong> Her \u00fcretim a\u015famas\u0131nda kat\u0131 kalite kontrol sa\u011flar\u0131m:<\/p>\n<table>\n<thead>\n<tr>\n<th style=\"text-align: left;\">Kontrol Parametresi<\/th>\n<th style=\"text-align: left;\">NBAEM \u00dcretim Standard\u0131<\/th>\n<th style=\"text-align: left;\">M\u00fchendislik Yararlar\u0131<\/th>\n<\/tr>\n<\/thead>\n<tbody>\n<tr>\n<td style=\"text-align: left;\"><strong>K\u00fcrkme Y\u00fcksekli\u011fi<\/strong><\/td>\n<td style=\"text-align: left;\">0.02 mm'nin Alt\u0131nda<\/td>\n<td style=\"text-align: left;\">\u0130\u00e7 katmanlar aras\u0131 elektriksel k\u0131sa devreleri \u00f6nler ve eddy ak\u0131m\u0131 kay\u0131plar\u0131n\u0131 azalt\u0131r<\/td>\n<\/tr>\n<tr>\n<td style=\"text-align: left;\"><strong>\u0130stifleme Fakt\u00f6r\u00fc<\/strong><\/td>\n<td style=\"text-align: left;\">96%'ye kadar<\/td>\n<td style=\"text-align: left;\">Etkin \u00e7ekirdek kesit alan\u0131n\u0131 ve manyetik ak\u0131 kapasitesini maksimize eder<\/td>\n<\/tr>\n<tr>\n<td style=\"text-align: left;\"><strong>Boyutsal Tolerans<\/strong><\/td>\n<td style=\"text-align: left;\">ISO 2768-m Hassasiyet<\/td>\n<td style=\"text-align: left;\">E\u015fit aral\u0131klar ve tutarl\u0131 kar\u015f\u0131 ind\u00fcktans sa\u011flar<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<p>ISO sertifikal\u0131 \u00fcretimimiz, her laminasyon tak\u0131m\u0131n\u0131n \u00f6ng\u00f6r\u00fclebilir ind\u00fcktans, ultra-d\u00fc\u015f\u00fck \u00e7ekirdek kayb\u0131 ve k\u00fcpe\u015ftelenmi\u015f manyetik performans sunmas\u0131n\u0131 k\u00fcresel enerji sistemleri i\u00e7in garanti eder.<\/p>\n<h2>S\u0131k\u00e7a Sorulan Sorular (SSS)<\/h2>\n<p>Ald\u0131\u011f\u0131m\u0131z en yayg\u0131n m\u00fchendislik sorunlar\u0131na do\u011frudan yan\u0131tlar \u015funlard\u0131r <strong>transformatorlerdeki manyetik e\u015fle\u015fmede g\u00f6r\u00fclen enerji verimlili\u011fi ilkelerine benzer<\/strong>.<\/p>\n<hr \/>\n<h3>Do\u011frudan elektriksel ba\u011flant\u0131 ile manyetik ba\u011flama aras\u0131ndaki ana fark nedir?<\/h3>\n<p>Do\u011frudan elektriksel ba\u011flant\u0131, elektrik sinyallerini iletmek i\u00e7in s\u00fcrekli fiziksel bir iletken kullan\u0131r; hem AC hem de DC ge\u00e7ebilir. <strong>Transformat\u00f6rlerde manyetik ba\u011flama<\/strong> ba\u011f\u0131ms\u0131z bir \u00e7ekirdek \u00fczerinden payla\u015f\u0131lan manyetik alan arac\u0131l\u0131\u011f\u0131yla enerji iletir; do\u011frudan metal ba\u011flant\u0131 yoktur. Bu, tamamen <strong>galvanik izolasyon<\/strong>, a\u015fa\u011f\u0131 ak\u0131m ekipman\u0131n\u0131 tehlikeli DC kaymalar\u0131ndan ve y\u00fcksek voltaj dalgalanmalar\u0131ndan korur.<\/p>\n<table>\n<thead>\n<tr>\n<th style=\"text-align: left;\">\u00d6zellik<\/th>\n<th style=\"text-align: left;\">Do\u011frudan Elektriksel Ba\u011flant\u0131<\/th>\n<th style=\"text-align: left;\">Transformat\u00f6rde Manyetik Ba\u011flant\u0131<\/th>\n<\/tr>\n<\/thead>\n<tbody>\n<tr>\n<td style=\"text-align: left;\"><strong>Fiziksel Yol<\/strong><\/td>\n<td style=\"text-align: left;\">Do\u011frudan iletken ba\u011flant\u0131<\/td>\n<td style=\"text-align: left;\">\u0130leti\u015fimsiz manyetik ak\u0131\u015f yolu<\/td>\n<\/tr>\n<tr>\n<td style=\"text-align: left;\"><strong>Galvanik \u0130zolasyon<\/strong><\/td>\n<td style=\"text-align: left;\">Yok (ortak toprak potansiyeli)<\/td>\n<td style=\"text-align: left;\">Tam fiziksel ve elektriksel izolasyon<\/td>\n<\/tr>\n<tr>\n<td style=\"text-align: left;\"><strong>DC Sinyal Transferi<\/strong><\/td>\n<td style=\"text-align: left;\">Destekleniyor<\/td>\n<td style=\"text-align: left;\">Engellendi (yaln\u0131zca AC transferleri)<\/td>\n<\/tr>\n<tr>\n<td style=\"text-align: left;\"><strong>G\u00fcr\u00fclt\u00fc ve G\u00fcvenlik<\/strong><\/td>\n<td style=\"text-align: left;\">Toprak d\u00f6ng\u00fclerine e\u011filimli ve y\u00fcksek g\u00fcr\u00fclt\u00fc<\/td>\n<td style=\"text-align: left;\">\u00dcst\u00fcn g\u00fcr\u00fclt\u00fc bast\u0131rma ve g\u00fcvenlik<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<hr \/>\n<h3>Ger\u00e7ek trafolar\u0131n nedensel \u00e7al\u0131\u015fmas\u0131nda ba\u011flama katsay\u0131s\u0131 (k) neden hi\u00e7bir zaman 1'den k\u00fc\u00e7\u00fck olur?<\/h3>\n<p>Bir teorik ideal transf\u00f6rde, birincil sarg\u0131n\u0131n olu\u015fturdu\u011fu manyetik ak\u0131 hatt\u0131n\u0131n t\u00fcm\u00fc ikincil sarg\u0131 \u00fczerinden ge\u00e7er ve sonu\u00e7 olarak ba\u011flama katsay\u0131s\u0131 <strong>k = 1<\/strong>.<\/p>\n<p>Ger\u00e7ek d\u00fcnyadaki trafolarda, <strong>k her zaman 1'den k\u00fc\u00e7\u00fckt\u00fcr<\/strong> \u00e7evresindeki havaya veya \u00e7ekirdek izolasyonuna baz\u0131 manyetik hatlar ka\u00e7t\u0131\u011f\u0131 i\u00e7in. Bu ba\u011flant\u0131s\u0131z alana <strong>s\u0131zd\u0131rma ak\u0131s\u0131<\/strong>. k'n\u0131n 1'in alt\u0131na inmesine neden olan fakt\u00f6rler \u015funlard\u0131r:<\/p>\n<ul>\n<li style=\"list-style-type: none;\">\n<ul>\n<li>Fiziksel sarg\u0131 ayr\u0131m\u0131 ve \u00e7ekirdek geometrisi<\/li>\n<li>\u00c7ekirdek malzemesinin s\u0131n\u0131rl\u0131 manyetik ge\u00e7irgenli\u011fi<\/li>\n<li>Ak\u0131\u015fkanl\u0131k k\u0131rpmalar\u0131n\u0131n neden oldu\u011fu y\u00fcksek \u00e7al\u0131\u015fma frekanslar\u0131 flux sa\u00e7\u0131lmas\u0131na neden olur<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<hr \/>\n<h3>\u00c7ekirdek laminasyonlar\u0131 transformat\u00f6rlerde manyetik e\u015fle\u015fmeyi nas\u0131l geli\u015ftirir?<\/h3>\n<p>Alternatif manyetik alanlar dola\u015fan elektrik ak\u0131mlar\u0131\u2014bilinen ad\u0131yla <strong>eddy ak\u0131mlar\u0131<\/strong>\u2014kat\u0131 iletken \u00e7ekirdekler i\u00e7inde. Bu ak\u0131mlar, b\u00fcy\u00fck enerji kayb\u0131 ve a\u011f\u0131r a\u015f\u0131r\u0131 \u0131s\u0131nma olu\u015fturur.<\/p>\n<p>\u00c7ekirde\u011fin laminasyonu, ince, elektrik olarak izole edilmi\u015f silikon \u00e7elik levhalar\u0131n \u00fcst \u00fcste getirilmesiyle yap\u0131l\u0131r. Manyetik alanlar\u0131n kay\u0131ps\u0131z y\u00f6nlendirilmesini anlamak i\u00e7in incelemek <a href=\"https:\/\/nbaem.com\/tr\/how-is-the-magnetic-rod-works\/\">manyetik \u00e7ubuk yap\u0131lar\u0131n nas\u0131l \u00e7al\u0131\u015ft\u0131\u011f\u0131<\/a> flux y\u00f6n\u00fc hakk\u0131nda b\u00fcy\u00fck i\u00e7g\u00f6r\u00fc sa\u011flar. Transformat\u00f6r \u00e7ekirdeklerinde laminasyonlar eddy ak\u0131m yolunu par\u00e7alayarak maksimum manyetik ak\u0131y\u0131 ikincil sarg\u0131ya odaklar ve sistem verimlili\u011fini korur.<\/p>\n<hr \/>\n<h3>Y\u00fcksek frekansl\u0131 transformat\u00f6r e\u015fle\u015fmesi i\u00e7in en uygun yumu\u015fak manyetik malzeme hangisidir?<\/h3>\n<p>Standart silikon \u00e7elik \u00e7ekirdekler 50\/60 Hz \u015febeke frekanslar\u0131nda iyi \u00e7al\u0131\u015f\u0131r, ancak y\u00fcksek frekansl\u0131 e\u015fle\u015fme (kHz ile MHz aral\u0131\u011f\u0131) ciddi \u00e7ekirdek kayb\u0131n\u0131 \u00f6nlemek i\u00e7in daha y\u00fcksek elektrik direncine sahip malzemeler gerektirir:<\/p>\n<ul>\n<li style=\"list-style-type: none;\">\n<ul>\n<li><strong>MnZn &amp; NiZn Yumu\u015fak Ferritler:<\/strong> D\u00fc\u015f\u00fck maliyetli, y\u00fcksek frekansl\u0131 g\u00fc\u00e7 kaynaklar\u0131 ve RF transformat\u00f6rleri i\u00e7in neredeyse yal\u0131tkan elektrik direnci nedeniyle en uygun olanlar.<\/li>\n<li><strong>Nanokristalin Ala\u015f\u0131mlar:<\/strong> Yo\u011fun s\u0131k\u0131\u015ft\u0131rmal\u0131, ultra y\u00fcksek verimli tasar\u0131mlar i\u00e7in y\u00fcksek doyum ak\u0131 yo\u011funlu\u011fu ve \u00fcst\u00fcn manyetik ge\u00e7irgenlik gerektirenler i\u00e7in idealdir.<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<div id=\"references\">\n<h2>\u0130lgili Kaynaklar<\/h2>\n<ul>\n<li><a href=\"https:\/\/thesis.caltech.edu\/928\/3\/Zhang_Z_1987.pdf\" target=\"_blank\" rel=\"noopener noreferrer\">https:\/\/thesis.caltech.edu\/928\/3\/Zhang_Z_1987.pdf<\/a><\/li>\n<li><a href=\"https:\/\/www.mdpi.com\/2072-666X\/13\/3\/418\" target=\"_blank\" rel=\"noopener noreferrer\">https:\/\/www.mdpi.com\/2072-666X\/13\/3\/418<\/a><\/li>\n<\/ul>\n<\/div>","protected":false},"excerpt":{"rendered":"<p>Transformatorde Manyetik E\u015fle\u015fme nedir? Kar\u015f\u0131l\u0131kl\u0131 ind\u00fcksiyon ba\u011flant\u0131 katsay\u0131s\u0131, \u00e7ekirdek tasar\u0131m\u0131 ve ger\u00e7ek d\u00fcnya uygulamalar\u0131<\/p>","protected":false},"author":1,"featured_media":3954,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"om_disable_all_campaigns":false,"_monsterinsights_skip_tracking":false,"_jetpack_newsletter_access":"","_jetpack_dont_email_post_to_subs":false,"_jetpack_newsletter_tier_id":0,"_jetpack_memberships_contains_paywalled_content":false,"_jetpack_memberships_contains_paid_content":false,"footnotes":""},"categories":[1],"tags":[],"class_list":["post-3955","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-uncategorized"],"jetpack_sharing_enabled":true,"jetpack_featured_media_url":"https:\/\/nbaem.com\/wp-content\/uploads\/2026\/07\/Transformer_magnetic_flux_coupling_Wwz.webp","_links":{"self":[{"href":"https:\/\/nbaem.com\/tr\/wp-json\/wp\/v2\/posts\/3955","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/nbaem.com\/tr\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/nbaem.com\/tr\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/nbaem.com\/tr\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/nbaem.com\/tr\/wp-json\/wp\/v2\/comments?post=3955"}],"version-history":[{"count":2,"href":"https:\/\/nbaem.com\/tr\/wp-json\/wp\/v2\/posts\/3955\/revisions"}],"predecessor-version":[{"id":3958,"href":"https:\/\/nbaem.com\/tr\/wp-json\/wp\/v2\/posts\/3955\/revisions\/3958"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/nbaem.com\/tr\/wp-json\/wp\/v2\/media\/3954"}],"wp:attachment":[{"href":"https:\/\/nbaem.com\/tr\/wp-json\/wp\/v2\/media?parent=3955"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/nbaem.com\/tr\/wp-json\/wp\/v2\/categories?post=3955"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/nbaem.com\/tr\/wp-json\/wp\/v2\/tags?post=3955"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}