{"id":12122,"date":"2025-12-27T18:55:03","date_gmt":"2025-12-27T15:55:03","guid":{"rendered":"https:\/\/vendor.energy\/articles\/vendor-energy-generator-verification-protocol\/"},"modified":"2026-01-05T11:05:29","modified_gmt":"2026-01-05T08:05:29","slug":"generator-vendor-energy-protocol-verificare","status":"publish","type":"post","link":"https:\/\/vendor.energy\/ro\/articles\/generator-vendor-energy-protocol-verificare\/","title":{"rendered":"Generatorul VENDOR.Energy: Arhitectur\u0103 electrodinamic\u0103, bilan\u021b energetic \u0219i protocol de verificare independent\u0103"},"content":{"rendered":"\t\t<div data-elementor-type=\"wp-post\" data-elementor-id=\"12122\" class=\"elementor elementor-12122 elementor-12094\" data-elementor-post-type=\"post\">\n\t\t\t\t<div class=\"elementor-element elementor-element-03295b9 e-flex e-con-boxed e-con e-parent\" data-id=\"03295b9\" data-element_type=\"container\" data-e-type=\"container\" data-settings=\"{&quot;background_background&quot;:&quot;classic&quot;}\">\n\t\t\t\t\t<div class=\"e-con-inner\">\n\t\t\t\t<div class=\"elementor-element elementor-element-2402ce3 elementor-widget elementor-widget-shortcode\" data-id=\"2402ce3\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"shortcode.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t<div class=\"elementor-shortcode\"><h2 class=\"custom-entry-title\">Generatorul VENDOR.Energy: Arhitectur\u0103 electrodinamic\u0103, bilan\u021b energetic \u0219i protocol de verificare independent\u0103<\/h2><\/div>\n\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-94a1029 elementor-widget elementor-widget-text-editor\" data-id=\"94a1029\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<p style=\"text-align: center;\">VENDOR este descris ca un sistem electrodinamic deschis, oper\u00e2nd strict \u00een cadrul legilor fizicii clasice.<br \/>Mediul gazos este tratat ca mediu de cuplare \u0219i condi\u021bie de frontier\u0103, nu ca surs\u0103 de energie.<br \/>Dezvoltarea urmeaz\u0103 o abordare bazat\u0103 pe TRL \u0219i validare prioritar\u0103; \u00een aceast\u0103 etap\u0103 nu sunt publicate afirma\u021bii de performan\u021b\u0103.<br \/>Dezv\u0103luirea detaliilor de implementare este condi\u021bionat\u0103 de verificarea independent\u0103 \u0219i de etapele de certificare (\u00een desf\u0103\u0219urare).<\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t<div class=\"elementor-element elementor-element-29f2f44 e-flex e-con-boxed e-con e-parent\" data-id=\"29f2f44\" data-element_type=\"container\" data-e-type=\"container\">\n\t\t\t\t\t<div class=\"e-con-inner\">\n\t\t\t\t<div class=\"elementor-element elementor-element-f2de26f elementor-widget elementor-widget-html\" data-id=\"f2de26f\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"html.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t<script>\nwindow.MathJax = {\n  tex: {\n    inlineMath: [['$', '$'], ['\\\\(', '\\\\)']],\n    displayMath: [['$$', '$$'], ['\\\\[', '\\\\]']]\n  },\n  svg: {\n    fontCache: 'global'\n  }\n};\n<\/script>\n<script src=\"https:\/\/cdnjs.cloudflare.com\/ajax\/libs\/mathjax\/3.2.2\/es5\/tex-mml-chtml.min.js\"><\/script>\n<script>\ndocument.addEventListener('DOMContentLoaded', function() {\n  setTimeout(function() {\n    if (window.MathJax && window.MathJax.typesetPromise) {\n      window.MathJax.typesetPromise().then(function() {\n        \/\/ \u041d\u0430\u0445\u043e\u0434\u0438\u043c \u0432\u0441\u0435 \u0444\u043e\u0440\u043c\u0443\u043b\u044b \u0438 \u043e\u0431\u043e\u0440\u0430\u0447\u0438\u0432\u0430\u0435\u043c \u0438\u0445 \u0432 \u0441\u043a\u0440\u043e\u043b\u043b-\u043a\u043e\u043d\u0442\u0435\u0439\u043d\u0435\u0440\u044b\n        const equations = document.querySelectorAll('mjx-container[display=\"true\"]');\n        equations.forEach(function(eq) {\n          if (!eq.closest('.math-scroll-wrapper')) {\n            const wrapper = document.createElement('div');\n            wrapper.className = 'math-scroll-wrapper';\n            eq.parentNode.insertBefore(wrapper, eq);\n            wrapper.appendChild(eq);\n          }\n        });\n      });\n    }\n  }, 1500);\n});\n<\/script>\n\n<style>\n\/* \u041e\u0431\u0435\u0440\u0442\u043a\u0430 \u0434\u043b\u044f \u0434\u043b\u0438\u043d\u043d\u044b\u0445 \u0444\u043e\u0440\u043c\u0443\u043b \u0441 \u043f\u0440\u043e\u043a\u0440\u0443\u0442\u043a\u043e\u0439 *\/\n.math-scroll-wrapper {\n  width: 100%;\n  overflow-x: auto;\n  overflow-y: hidden;\n  padding: 10px 0;\n  margin: 15px 0;\n  border: 1px solid #e0e0e0;\n  border-radius: 5px;\n  background: #fafafa;\n  -webkit-overflow-scrolling: touch;\n}\n\n.math-scroll-wrapper mjx-container {\n  min-width: max-content;\n  white-space: nowrap;\n  margin: 0 !important;\n}\n\n\/* \u041a\u0440\u0430\u0441\u0438\u0432\u044b\u0439 \u0441\u043a\u0440\u043e\u043b\u043b *\/\n.math-scroll-wrapper::-webkit-scrollbar {\n  height: 8px;\n}\n\n.math-scroll-wrapper::-webkit-scrollbar-track {\n  background: #f1f1f1;\n  border-radius: 10px;\n}\n\n.math-scroll-wrapper::-webkit-scrollbar-thumb {\n  background: #888;\n  border-radius: 10px;\n}\n\n.math-scroll-wrapper::-webkit-scrollbar-thumb:hover {\n  background: #555;\n}\n\n\/* \u0418\u043d\u0434\u0438\u043a\u0430\u0442\u043e\u0440 \u043f\u0440\u043e\u043a\u0440\u0443\u0442\u043a\u0438 *\/\n.math-scroll-wrapper::before {\n  content: \"\u2190 scroll to view full formula \u2192\";\n  display: block;\n  text-align: center;\n  font-size: 11px;\n  color: #666;\n  margin-bottom: 5px;\n  font-style: italic;\n}\n\n@media (min-width: 1200px) {\n  .math-scroll-wrapper::before {\n    display: none;\n  }\n  \n  .math-scroll-wrapper {\n    border: none;\n    background: transparent;\n    overflow: visible;\n  }\n}\n<\/style>\n<style>\n\/* \u0410\u0434\u0430\u043f\u0442\u0438\u0432\u043d\u044b\u0435 \u0442\u0430\u0431\u043b\u0438\u0446\u044b *\/\ntable {\n  width: 100% !important;\n  border-collapse: collapse !important;\n  margin: 20px 0 !important;\n  font-size: 14px !important;\n}\n\n\/* \u041e\u0431\u0435\u0440\u0442\u043a\u0430 \u0434\u043b\u044f \u0433\u043e\u0440\u0438\u0437\u043e\u043d\u0442\u0430\u043b\u044c\u043d\u043e\u0439 \u043f\u0440\u043e\u043a\u0440\u0443\u0442\u043a\u0438 \u0442\u0430\u0431\u043b\u0438\u0446 *\/\n.table-wrapper {\n  width: 100%;\n  overflow-x: auto;\n  -webkit-overflow-scrolling: touch;\n  margin: 20px 0;\n  border: 1px solid #ddd;\n  border-radius: 5px;\n}\n\n.table-wrapper table {\n  margin: 0 !important;\n  min-width: 600px; \/* \u041c\u0438\u043d\u0438\u043c\u0430\u043b\u044c\u043d\u0430\u044f \u0448\u0438\u0440\u0438\u043d\u0430 \u0442\u0430\u0431\u043b\u0438\u0446\u044b *\/\n}\n\n\/* \u0410\u0432\u0442\u043e\u043c\u0430\u0442\u0438\u0447\u0435\u0441\u043a\u043e\u0435 \u0441\u043e\u0437\u0434\u0430\u043d\u0438\u0435 \u043e\u0431\u0435\u0440\u0442\u043a\u0438 \u0447\u0435\u0440\u0435\u0437 CSS *\/\ntable {\n  display: block;\n  white-space: nowrap;\n  overflow-x: auto;\n  overflow-y: hidden;\n  max-width: 100%;\n}\n\ntable thead,\ntable tbody,\ntable tr {\n  display: table;\n  width: 100%;\n  table-layout: fixed;\n}\n\ntable thead {\n  width: calc(100% - 17px); \/* \u041a\u043e\u043c\u043f\u0435\u043d\u0441\u0430\u0446\u0438\u044f \u0441\u043a\u0440\u043e\u043b\u043b\u0431\u0430\u0440\u0430 *\/\n}\n\n\/* \u0421\u0442\u0438\u043b\u0438 \u0434\u043b\u044f \u044f\u0447\u0435\u0435\u043a \u0442\u0430\u0431\u043b\u0438\u0446\u044b *\/\ntable th,\ntable td {\n  padding: 8px 12px !important;\n  text-align: left !important;\n  border: 1px solid #ddd !important;\n  word-wrap: break-word !important;\n  display: table-cell !important;\n  white-space: normal !important;\n}\n\ntable th {\n  background-color: #f5f5f5 !important;\n  font-weight: bold !important;\n}\n\n\/* \u041c\u043e\u0431\u0438\u043b\u044c\u043d\u044b\u0435 \u0441\u0442\u0438\u043b\u0438 *\/\n@media (max-width: 768px) {\n  table {\n    font-size: 12px !important;\n  }\n  \n  table th,\n  table td {\n    padding: 6px 8px !important;\n  }\n  \n  \/* \u0410\u043b\u044c\u0442\u0435\u0440\u043d\u0430\u0442\u0438\u0432\u0430 - \u0432\u0435\u0440\u0442\u0438\u043a\u0430\u043b\u044c\u043d\u044b\u0439 \u043c\u0430\u043a\u0435\u0442 \u0434\u043b\u044f \u043e\u0447\u0435\u043d\u044c \u043c\u0430\u043b\u0435\u043d\u044c\u043a\u0438\u0445 \u044d\u043a\u0440\u0430\u043d\u043e\u0432 *\/\n  @media (max-width: 480px) {\n    .mobile-table-stack table,\n    .mobile-table-stack thead,\n    .mobile-table-stack tbody,\n    .mobile-table-stack th,\n    .mobile-table-stack td,\n    .mobile-table-stack tr {\n      display: block !important;\n    }\n    \n    .mobile-table-stack thead tr {\n      position: absolute !important;\n      top: -9999px !important;\n      left: -9999px !important;\n    }\n    \n    .mobile-table-stack tr {\n      border: 1px solid #ccc !important;\n      margin-bottom: 10px !important;\n      padding: 10px !important;\n    }\n    \n    .mobile-table-stack td {\n      border: none !important;\n      position: relative !important;\n      padding-left: 50% !important;\n      padding-top: 10px !important;\n      padding-bottom: 10px !important;\n    }\n    \n    .mobile-table-stack td:before {\n      content: attr(data-label) \": \" !important;\n      position: absolute !important;\n      left: 6px !important;\n      width: 45% !important;\n      text-align: left !important;\n      font-weight: bold !important;\n    }\n  }\n}\n\n\/* \u0421\u043a\u0440\u043e\u043b\u043b\u0431\u0430\u0440 \u0434\u043b\u044f \u0442\u0430\u0431\u043b\u0438\u0446 *\/\ntable::-webkit-scrollbar {\n  height: 10px;\n}\n\ntable::-webkit-scrollbar-track {\n  background: #f1f1f1;\n  border-radius: 5px;\n}\n\ntable::-webkit-scrollbar-thumb {\n  background: #888;\n  border-radius: 5px;\n}\n\ntable::-webkit-scrollbar-thumb:hover {\n  background: #555;\n}\n<\/style>\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-1e67cbb elementor-widget elementor-widget-text-editor\" data-id=\"1e67cbb\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<strong>Autori:<\/strong> O. Krishevich, V. Peretyachenko\n<h2>Interpretare \u0219i clarificare de scop<\/h2>\n<strong>Clasa sistemului:<\/strong> sistem electrodinamic deschis guvernat de legi clasice.\n\n<strong>Mediu:<\/strong> mediu de cuplaj \u0219i limit\u0103, nu o surs\u0103 consumabil\u0103.\n\n<strong>Validare \u00een prim-plan:<\/strong> lucru \u00een etap\u0103 TRL; nicio afirma\u021bie public\u0103 de performan\u021b\u0103 \u00een acest document.\n\n<strong>Declan\u0219are de divulgare:<\/strong> detaliile de implementare sunt dezv\u0103luite doar prin c\u0103i de verificare independent\u0103.\n\n<strong>Terminologie:<\/strong> dispozitivul este un sistem de conversie (transduc\u021bie) energetic\u0103; &#8222;generator&#8221; este folosit \u00een sens de denumire de brevet\/industrie \u0219i nu implic\u0103 crearea de energie.\n<\/ hr>\n<section>\n <div lang=\"ro\">\n    <h3>Clasificarea Dovezilor<\/h3>\n\n    <p>Acest document constituie <strong>dovezi de validare a regimului de func\u021bionare<\/strong>.<\/p>\n\n    <p>Procedurile, m\u0103sur\u0103torile \u0219i metodologiile descrise aici sunt destinate exclusiv:<\/p>\n\n    <ul>\n      <li>confirm\u0103rii existen\u021bei regimurilor de func\u021bionare repetabile,<\/li>\n      <li>evalu\u0103rii stabilit\u0103\u021bii regimului \u00een condi\u021bii de laborator controlate,<\/li>\n      <li>verific\u0103rii comportamentului limitat \u0219i excluderii interpret\u0103rilor liniare triviale.<\/li>\n    <\/ul>\n\n    <p>\n      Acest protocol nu reprezint\u0103 o validare a performan\u021bei \u0219i nu stabile\u0219te balan\u021ba energetic\u0103,\n      eficien\u021ba sau capacitatea de ie\u0219ire.\n    <\/p>\n\n    <p>\n      Toate concluziile legate de performan\u021b\u0103 sunt am\u00e2nate explicit pentru etapele ulterioare de validare\n      \u0219i sunt supuse unor protocoale independente de m\u0103surare integrat\u0103 a puterii \u0219i a parametrilor termici.\n    <\/p>\n  <\/div>\n<\/section>\n<\/ hr>\n\n<section class=\"vendor-non-claims-boundary\" aria-labelledby=\"non-claims-boundary-title-ro\">\n  <h3 id=\"non-claims-boundary-title-ro\">Limit\u0103 Explicit\u0103 a Afirma\u021biilor Neformulate<\/h3>\n\n  <p>Prezentul protocol exclude \u00een mod explicit urm\u0103toarele interpret\u0103ri \u0219i afirma\u021bii:<\/p>\n\n  <ul>\n    <li>ob\u021binerea unui c\u00e2\u0219tig energetic net sau amplificarea energiei;<\/li>\n    <li>func\u021bionare auto-sus\u021binut\u0103 sau generare autonom\u0103 de energie;<\/li>\n    <li>eficien\u021b\u0103 mai mare dec\u00e2t unitatea;<\/li>\n    <li>mediul sau mediul ambiant ca surs\u0103 de energie;<\/li>\n    <li>\u00eenlocuirea m\u0103sur\u0103torilor calorimetrice sau a m\u0103sur\u0103torilor integrate de putere;<\/li>\n    <li>concluzii derivate exclusiv din date de osciloscop sau analiz\u0103 spectral\u0103.<\/li>\n  <\/ul>\n\n  <p>\n    Orice interpretare care dep\u0103\u0219e\u0219te existen\u021ba, stabilitatea \u0219i repetabilitatea regimului\n    se afl\u0103 \u00een afara domeniului acestui document \u0219i este considerat\u0103 invalid\u0103\n    \u00een absen\u021ba unei verific\u0103ri dedicate \u0219i independente.\n  <\/p>\n<\/section>\n<\/ hr>\n\n<h3>De unde provine energia (f\u0103r\u0103 mituri)<\/h3>\nAcest sistem nu se bazeaz\u0103 pe combustibil, nu extrage energie &#8222;din aer&#8221;, nu pretinde func\u021bionare peste-unitate \u0219i nu pretinde crearea de energie. Nicio surs\u0103 de energie consumabil\u0103 nu este introdus\u0103 dincolo de interac\u021biunea sistemului cu mediul s\u0103u ca sistem electrodinamic deschis sub electrodinamica clasic\u0103.\n\n\u00cen termeni ingineri\u0219ti str\u00e2ns defini\u021bi, sistemul este o arhitectur\u0103 de conversie (transduc\u021bie) energetic\u0103 care livreaz\u0103 putere electric\u0103 prin \u00eenchiderea balan\u021bei de energie externe m\u0103surate a unui sistem electrodinamic deschis.\n\n\u00cen electrodinamica clasic\u0103, o &#8222;surs\u0103&#8221; nu este definit\u0103 ca un combustibil sau rezervor, ci ca balan\u021ba de energie extern\u0103 complet\u0103 a unui sistem deschis. Pentru sisteme care opereaz\u0103 \u00een regimuri rezonante neliniare cu circula\u021bie intern\u0103 \u0219i feedback, schimbul de energie trebuie contabilizat nu doar prin intr\u0103ri prin fire, ci \u0219i prin interac\u021biuni electromagnetice de limit\u0103.\n\n<strong>Portul (2)<\/strong> este introdus ca un <strong>termen de interfa\u021b\u0103 de limit\u0103 opera\u021bional\u0103<\/strong> folosit pentru a \u00eenchide balan\u021ba energetic\u0103. Reprezint\u0103 schimbul de energie mediat de limit\u0103 peste limita sistemului a\u0219a cum este descris de teorema Poynting \u0219i nu trebuie interpretat ca o surs\u0103 discret\u0103 de energie, o afirma\u021bie de generator sau o baterie secundar\u0103. Termenul &#8222;extern&#8221; se refer\u0103 la schimbul de energie care are loc peste limita sistemului (extern \u00een raport cu limita sistemului), nu la o surs\u0103 extern\u0103 identificat\u0103.\n\nModelele liniare intrare-ie\u0219ire e\u0219ueaz\u0103 \u00een acest context deoarece ignor\u0103 circula\u021bia intern\u0103 de energie \u0219i feedback-ul stabilizat \u00een faz\u0103. \u00cen astfel de regimuri, puterea de ie\u0219ire util\u0103 este sus\u021binut\u0103 prin men\u021binerea unei balan\u021be de energie stabile, nu prin intrare direct\u0103 continu\u0103 prin fire propor\u021bional\u0103 cu ie\u0219irea.\n\nDetaliile de implementare, parametrii interni \u0219i solu\u021biile constructive sunt tratate ca know-how protejat \u0219i sunt inten\u021bionat excluse din acest document. Verificarea este efectuat\u0103 folosind formate inginere\u0219ti standard: <strong>validare modul sigilat<\/strong> \u0219i <strong>divulgare controlat\u0103 sub NDA<\/strong>. \u00cen ambele formate, un laborator independent m\u0103soar\u0103 intr\u0103rile \u0219i ie\u0219irile externe cu propria sa instrumenta\u021bie \u0219i aplic\u0103 controale pentru a exclude c\u0103ile de cuplaj parazit. Divulgarea detaliilor specifice implement\u0103rii este condi\u021bionat\u0103 de finalizarea valid\u0103rii \u0219i jaloanelor de certificare.\n<h2>0. Statusul documentului, reproductibilitate \u0219i limite ale afirma\u021biilor<\/h2>\nAcest document este un raport de verificare inginereasc\u0103. Scopul s\u0103u este s\u0103 defineasc\u0103 comportamentul energetic verificabil, s\u0103 formalizeze balan\u021ba energetic\u0103 \u0219i s\u0103 specifice un protocol de testare metrologic\u0103 independent\u0103.\n\nDocumentul nu pretinde statutul unei publica\u021bii academice complete cu design deschis reproductibil: o parte din implementarea constructiv\u0103 constituie know-how \u0219i este protejat\u0103 de un portofoliu de brevete. Verificarea independent\u0103 este necesar\u0103 \u00een dou\u0103 formate acceptabile:\n<ul>\n \t<li><strong>Divulgare controlat\u0103 (sub NDA):<\/strong> un laborator independent prime\u0219te acces la noduri critice selectate strict \u00een scopuri de verificare.<\/li>\n \t<li><strong>Validare modul sigilat:<\/strong> un modul integrat (inclusiv elemente de interfa\u021b\u0103 (2), dac\u0103 sunt inseparabile tehnologic) este furnizat sigilat, iar toate m\u0103sur\u0103torile sunt efectuate de o parte independent\u0103 folosind propriul echipament.<\/li>\n<\/ul>\nAceste formate sunt standard pentru verificarea inginereasc\u0103 atunci c\u00e2nd detaliile de implementare sunt protejate. Sistemul nu este tratat ca o &#8222;cutie neagr\u0103&#8221; \u00een sens evaluativ: verificarea este metrologic\u0103 \u0219i se bazeaz\u0103 pe cantit\u0103\u021bi m\u0103surate, instrumente documentate, incertitudine \u0219i teste de control obligatorii care exclud c\u0103ile de energie parazit\u0103.\n<h3>Statusul metodologiei sub modul sigilat<\/h3>\nAcest document define\u0219te parametri m\u0103surabili, criterii de acceptare \u0219i condi\u021bii de testare.\n\nPentru configura\u021biile furnizate \u00een formatul modul sigilat, metoda de testare poate include elemente protejate ca know-how. \u00cen acest caz, raportul de testare con\u021bine o descriere a cantit\u0103\u021bilor m\u0103surate, instrumentelor de m\u0103surare utilizate, condi\u021biilor de testare \u0219i criteriilor de acceptare, dar nu con\u021bine o descriere complet\u0103 a designului intern sau implementarea interfe\u021bei de limit\u0103 asociate cu Portul (2).\n\nFocusul verific\u0103rii este strict metrologic: cantit\u0103\u021bi m\u0103surabile, incertitudine \u0219i teste de control \u2014 nu divulgarea construc\u021biei interne.\n\nAbsen\u021ba divulg\u0103rii complete a designului modulului sigilat nu afecteaz\u0103 validitatea rezultatelor testelor, cu condi\u021bia ca toate criteriile definite \u00een Sec\u021biunea 9 a acestui document s\u0103 fie \u00eendeplinite.\n<h2>0.1 Limite metodologice \u0219i limit\u0103ri interpretative<\/h2>\nAcest document este o specifica\u021bie inginereasc\u0103 pentru verificarea comportamentului energetic al sistemului \u0219i nu afirm\u0103 natura fizic\u0103 a schimbului de energie mediat de limit\u0103 contabilizat prin Portul (2) \u00een Modul B.\n\n\u00cen particular:\n<ul>\n \t<li>Documentul nu pretinde c\u0103 schimbul de energie mediat de limit\u0103 contabilizat prin portul (2) este cauzat de un c\u00e2mp fizic, interac\u021biune sau parametru de mediu specific (E, H, T, \u03c1, etc.).<\/li>\n \t<li>Documentul nu presupune existen\u021ba unei interac\u021biuni fundamentale noi sau a unei viol\u0103ri a legilor cunoscute ale fizicii.<\/li>\n \t<li>Documentul nu solicit\u0103 p\u0103r\u021bii verificatoare s\u0103 recunoasc\u0103 niciun mecanism de generare a energiei dincolo de balan\u021ba energetic\u0103 m\u0103surat\u0103 experimental.<\/li>\n<\/ul>\nPortul (2) este introdus exclusiv ca o desemnare inginereasc\u0103 opera\u021bional\u0103 a unei interfe\u021be de limit\u0103 prin care o contribu\u021bie energetic\u0103 reproductibil\u0103 este observat\u0103 \u00een condi\u021bii de testare controlate \u0219i este testat\u0103 \u00eempotriva \u2014 \u0219i nu trebuie s\u0103 fie atribuibil\u0103 \u2014 urm\u0103toarelor categorii:\n<ul>\n \t<li>intrare prin fire (portul (1)),<\/li>\n \t<li>elemente interne de stocare a energiei,<\/li>\n \t<li>recircularea pierderilor proprii ale sistemului,<\/li>\n \t<li>c\u0103i parazite cunoscute (conductive, bazate pe re\u021bea sau radiofrecven\u021b\u0103), inclusiv c\u0103i de returnare neurm\u0103rite, artefacte de ecranare\/\u00eemp\u0103m\u00e2ntare \u0219i erori de referin\u021b\u0103 de m\u0103surare.<\/li>\n<\/ul>\nDeterminarea naturii fizice a acestei contribu\u021bii este \u00een afara scopului acestei specifica\u021bii \u0219i apar\u021bine unei etape separate de cercetare fundamental\u0103, care nu este subiectul certific\u0103rii sau verific\u0103rii de investi\u021bii.\n<h2>1. Defini\u021bii \u0219i balan\u021b\u0103 energetic\u0103<\/h2>\n<h3>1.1 Defini\u021bii \u0219i balan\u021ba energetic\u0103 a sistemului<\/h3>\nSistemul VENDOR este descris prin teorema Poynting \u0219i analiza standard a energiei circuitului ca un sistem deschis cu schimb de energie extern\u0103 prin porturi \u0219i interfe\u021be de limit\u0103 definite.\n<h4>1.1.1 Portul (1): Interfa\u021b\u0103 energetic\u0103 prin fire<\/h4>\nPuterea activ\u0103 medie la portul (1) este m\u0103surat\u0103 ca:\n\n\\[\nP_{\\mathrm{elec,avg}} = \\frac{1}{T}\\int_{0}^{T} v_{\\mathrm{ext}}(t)\\, i_{\\mathrm{ext}}(t)\\, dt,\n\\]\n\nunde m\u0103surarea include toate c\u0103ile de curent de returnare, conductorii de referin\u021b\u0103, ecran\u0103rile \u0219i ansamblurile de cabluri asociate cu portul (1).\n<h4>1.1.2 Portul (2): Interfa\u021b\u0103 de cuplaj de limit\u0103 (interfa\u021b\u0103 de instalare)<\/h4>\n<strong>Not\u0103 de defini\u021bie:<\/strong> \u00cen acest document, &#8222;Portul (2)&#8221; denot\u0103 o clas\u0103 de limit\u0103\/interfa\u021b\u0103 pentru schimbul de energie peste limita sistemului (cuplaj dependent de instalare), nu o cerin\u021b\u0103 pentru un conector electric dedicat.\n\n<strong>Portul (2)<\/strong> este un <strong>termen de interfa\u021b\u0103 de limit\u0103 opera\u021bional\u0103<\/strong> introdus pentru a \u00eenchide balan\u021ba energetic\u0103 a unui sistem electrodinamic deschis. Nu reprezint\u0103 o afirma\u021bie de surs\u0103 de energie. \u00cen schimb, contabilizeaz\u0103 schimbul de energie mediat de limit\u0103 care are loc prin dispozitive de instalare \u0219i condi\u021bii electromagnetice de limit\u0103.\n\nReprezentarea formal\u0103 a schimbului mediat de limit\u0103 este exprimat\u0103 prin fluxul Poynting:\n\n\\[\nP_{\\mathrm{field,avg}} = \\oint_{\\partial V} \\langle \\mathbf{S} \\rangle \\cdot d\\mathbf{A},\n\\qquad \\mathbf{S} = \\mathbf{E} \\times \\mathbf{H}.\n\\]\n\n<strong>Not\u0103 metrologic\u0103:<\/strong> \u00een aceast\u0103 specifica\u021bie, contribu\u021bia de limit\u0103 asociat\u0103 cu Portul (2) este reprezentat\u0103 \u00een form\u0103 clasic\u0103 prin teorema Poynting; cu toate acestea, \u00een cadrul protocolului practic poate fi determinat\u0103 opera\u021bional ca reziduu al balan\u021bei energetice m\u0103surate, supus testelor de control obligatorii \u0219i limitelor de incertitudine (Sec\u021biunea 9.2.2). Aceasta este o abordare inginereasc\u0103 standard c\u00e2nd integrarea direct\u0103 a fluxului de c\u00e2mp apropiat nu este practic\u0103 pentru sistemele impulsive.\n\nNatura fizic\u0103 a schimbului de energie asociat cu Portul (2) este \u00een afara scopului acestui document \u0219i este abordat\u0103 exclusiv prin verificare metrologic\u0103. Nu se fac presupuneri a priori cu privire la purt\u0103torul s\u0103u fizic sau mecanismul de interac\u021biune subiacent.\n\n<strong>Not\u0103 important\u0103 de contabilizare:<\/strong> Portul (2) este o interfa\u021b\u0103 de contabilizare opera\u021bional\u0103, nu neap\u0103rat un conector fizic instrumentat direct. Reprezint\u0103 contribu\u021bia mediat\u0103 de limit\u0103 necesar\u0103 pentru a \u00eenchide balan\u021ba energetic\u0103 m\u0103surat\u0103 conform testelor de control specificate \u00een Sec\u021biunea 9.\n\nPortul (2) nu trebuie interpretat ca un artefact de contabilizare doar intern\u0103. \u00cen particular, termenul de limit\u0103 nu este redus la:\n<ul>\n \t<li>recirculare intern\u0103 de energie,<\/li>\n \t<li>reutilizarea pierderilor radiative sau reactive proprii ale sistemului,<\/li>\n \t<li>ie\u0219ire aparent\u0103 cauzat\u0103 exclusiv de deregulare sau desc\u0103rcare tranzitorie a energiei stocate,<\/li>\n \t<li>artefacte de m\u0103surare datorate c\u0103ilor de returnare neurm\u0103rite, \u00eemp\u0103m\u00e2nt\u0103rii, ecran\u0103rii sau conductorilor de referin\u021b\u0103.<\/li>\n<\/ul>\nModific\u0103rile capacit\u0103\u021bilor\/inductan\u021belor de limit\u0103 pot afecta regimul de operare \u0219i sunt tratate ca condi\u021bii de regim; ele nu sunt, prin ele \u00eensele, o afirma\u021bie de surs\u0103 extern\u0103 de energie.\n\nOrice energie care p\u0103r\u0103se\u0219te sistemul \u0219i nu este returnat\u0103 printr-o interfa\u021b\u0103 extern\u0103 explicit definit\u0103 este atribuit\u0103 lui \\(P_{\\mathrm{loss,avg}}\\).\n\nAstfel, Portul (2) reprezint\u0103 un termen de balan\u021b\u0103 energetic\u0103 extern\u0103 mediat de limit\u0103 definit exclusiv pe baz\u0103 experimental\u0103, f\u0103r\u0103 presupuneri cu privire la originea sa fizic\u0103, \u0219i introdus doar pentru a asigura o balan\u021b\u0103 energetic\u0103 complet\u0103 \u0219i necontradictorie a sistemului deschis.\n<h4>1.1.3 Cantit\u0103\u021bi interne<\/h4>\n<ul>\n \t<li>\\(P_{\\mathrm{load,avg}}\\) \u2014 putere util\u0103 livrat\u0103 la sarcin\u0103.<\/li>\n \t<li>\\(P_{\\mathrm{loss,avg}}\\) \u2014 pierderi totale (termice, dielectrice, radiative etc.).<\/li>\n \t<li>\\(E_{\\mathrm{buf}},\\; P_{\\mathrm{buf,avg}} = \\left\\langle \\frac{dE_{\\mathrm{buf}}}{dt} \\right\\rangle\\) \u2014 energia \u0219i puterea tamponului intern (dac\u0103 este prezent).<\/li>\n \t<li>\\(U_{\\mathrm{circ,max}}\\) \u2014 energia maxim\u0103 recuperabil\u0103 stocat\u0103 \u00een c\u00e2mpuri\/circuite circulante (limit\u0103 superioar\u0103 estimat\u0103 din \\(L,\\; C,\\; V_{\\mathrm{peak}},\\; I_{\\mathrm{peak}}\\)).<\/li>\n<\/ul>\n<h4>1.1.4 Balan\u021ba complet\u0103<\/h4>\nBalan\u021ba complet\u0103 a puterilor medii:\n\n\\[\nP_{\\mathrm{elec,avg}} + P_{\\mathrm{field,avg}}\n= P_{\\mathrm{loss,avg}} + P_{\\mathrm{load,avg}} + P_{\\mathrm{buf,avg}}.\n\\]\n\n\u00cen stare sta\u021bionar\u0103 cu privire la tampon:\n\n\\[\nP_{\\mathrm{elec,avg}} + P_{\\mathrm{field,avg}}\n= P_{\\mathrm{loss,avg}} + P_{\\mathrm{load,avg}}.\n\\]\n\nCriteriul &#8222;nu este o banc\u0103 de putere&#8221;: \u00een orice mod de operare autonom revendicat, trebuie s\u0103 se verifice:\n\n\\[\n\\int_{0}^{T} P_{\\mathrm{load}}\\, dt \\gg \\left|\\Delta E_{\\mathrm{buf}}\\right| + U_{\\mathrm{circ,max}}\n\\]\n\ncu control simultan al \\(P_{\\mathrm{elec,avg}} \\approx 0\\). \u00cen aceste condi\u021bii, energia livrat\u0103 sus\u021binut\u0103 trebuie atribuit\u0103 unui termen de limit\u0103 extern\u0103 conform clasific\u0103rii protocolului (Portul (2)), mai degrab\u0103 dec\u00e2t stoc\u0103rii interne, cu condi\u021bia ca toate controalele de excludere s\u0103 fie satisf\u0103cute.\n\n<em>Not\u0103:<\/em> \\(U_{\\mathrm{circ,max}}\\) reprezint\u0103 limita superioar\u0103 absolut\u0103 a energiei de c\u00e2mp intern recuperabile \u00een orice moment \u0219i, prin urmare, limiteaz\u0103 orice explica\u021bie posibil\u0103 bazat\u0103 pe stocare.\n<h3>1.2 De ce analiza liniar\u0103 duce la concluzii false<\/h3>\nUn argument tipic al criticilor:\n\n&#8222;C\u00e2t\u0103 putere poate fi extras\u0103 din c\u00e2mpul electrostatic al P\u0103m\u00e2ntului? Calculul arat\u0103\n\\(P \\sim 10^{-12}\\ \\mathrm{A\/m^2} \\times \\text{aria}\\), ceea ce este neglijabil. Prin urmare, sistemul este imposibil.&#8221;\n\nAceast\u0103 critic\u0103 r\u0103spunde la \u00eentrebarea:\n\n&#8222;Poate c\u00e2mpul atmosferic global s\u0103 alimenteze direct o sarcin\u0103 util\u0103 prin conductivitatea aerului?&#8221;\n\nDar sistemul pune o \u00eentrebare diferit\u0103:\n\n&#8222;Care este balan\u021ba extern\u0103 total\u0103 necesar\u0103 \\(P_{\\mathrm{in,avg}}\\) pentru a sus\u021bine un regim cu circula\u021bie intern\u0103 \u0219i pentru a livra putere la sarcin\u0103 \u00een condi\u021bii controlate?&#8221;\n\nAcestea sunt probleme diferite. Criticul modeleaz\u0103 implicit mediul ca o surs\u0103 direct\u0103 de putere, \u00een timp ce \u00een modelul corect fluxurile interne (inclusiv feedback-ul) sunt o redistribuire a energiei \u00een cadrul dispozitivului \u0219i nu formeaz\u0103 o intrare extern\u0103 suplimentar\u0103. Balan\u021ba extern\u0103 este definit\u0103 complet de:\n\n\\[\nP_{\\mathrm{in,avg}} = P_{\\mathrm{loss,avg}} + P_{\\mathrm{load,avg}} + P_{\\mathrm{buf,avg}}\n\\]\n\n(\u00een stare sta\u021bionar\u0103, ultimul termen \\(\\to 0\\)).\n<h2>2. Circuite rezonante LC: Energie \u0219i matematic\u0103<\/h2>\n<h3>2.1 Circuit LC ideal f\u0103r\u0103 pierderi<\/h3>\n\u00centr-un circuit LC ideal (f\u0103r\u0103 rezisten\u021b\u0103), sarcina \u0219i curentul oscileaz\u0103:\n\n\\[\n\\omega_{0}=\\frac{1}{\\sqrt{LC}}, \\qquad f_{0}=\\frac{1}{2\\pi\\sqrt{LC}}\n\\]\n\n\\[\nq(t)=q_{0}\\cos(\\omega_{0}t), \\qquad i(t)=\\frac{dq}{dt}=-q_{0}\\omega_{0}\\sin(\\omega_{0}t)\n\\]\n\nEnergia condensatorului \u0219i bobinei:\n\n\\[\nU_{C}(t)=\\frac{q(t)^{2}}{2C}, \\qquad U_{L}(t)=\\frac{1}{2}L\\,i(t)^{2}\n\\]\n\nEnergia total\u0103 stocat\u0103 r\u0103m\u00e2ne constant\u0103:\n\n\\[\nU_{\\mathrm{tot}}=U_{C}+U_{L}=\\frac{q_{0}^{2}}{2C}=\\mathrm{const}\n\\]\n\n<strong>Semnifica\u021bie fizic\u0103:<\/strong> energia se transfer\u0103 periodic \u00eentre c\u00e2mpul electric al condensatorului \u0219i c\u00e2mpul magnetic al bobinei la frecven\u021ba \\(f_{0}\\).\n\n<strong>Not\u0103 despre semn \u0219i faz\u0103:<\/strong> semnul \u00een expresia pentru \\(i(t)\\) depinde de direc\u021bia curentului aleas\u0103; relevant fizic sunt amplitudinea \u0219i defazajul de \\(\\pi\/2\\) \u00eentre \\(q(t)\\) \u0219i \\(i(t)\\).\n<h3>2.2 Circuit RLC real cu pierderi \u0219i tensiune extern\u0103<\/h3>\n\u00cen realitate, pierderile sunt prezente \u0219i sunt modelate printr-o rezisten\u021b\u0103 echivalent\u0103 \\(R\\):\n\n\\[\n\\frac{d^{2}q}{dt^{2}}+\\frac{R}{L}\\frac{dq}{dt}+\\frac{q}{LC}=\\frac{1}{L}v_{\\mathrm{drive}}(t)\n\\]\n\nunde \\(v_{\\mathrm{drive}}(t)\\) este tensiunea de excitare extern\u0103 (\u00eentr-un circuit practic, este format\u0103 de portul \\(v_{\\mathrm{ext}}(t)\\) prin topologia de conexiune corespunz\u0103toare).\n\nPentru un regim slab amortizat \\(\\left(R \\ll \\sqrt{\\frac{L}{C}}\\right)\\), energia se descompune aproximativ exponen\u021bial:\n\n\\[\nU(t)\\approx U_{0}\\exp\\!\\left(-\\frac{t}{\\tau}\\right), \\qquad \\tau \\approx \\frac{2L}{R}\n\\]\n\nFactorul de calitate (factorul Q) determin\u0103 rata de descompunere \u0219i eficien\u021ba energetic\u0103:\n\n\\[\nQ \\equiv 2\\pi \\times \\frac{\\text{energie stocat\u0103}}{\\text{pierderi pe ciclu}}=\\frac{\\omega_{0}L}{R}\\approx \\pi f_{0}\\tau\n\\]\n\nUn \\(Q\\) ridicat \u00eenseamn\u0103 descompunere lent\u0103: energia circul\u0103 de multe ori \u00eenainte de a fi complet disipat\u0103.\n<h3>2.3 Structura spectral\u0103 a puterii instantanee<\/h3>\n\u00centr-un circuit LC, curentul \u0219i tensiunea oscileaz\u0103 la frecven\u021ba rezonant\u0103 fundamental\u0103 \\(f_{0}\\):\n\n\\[\ni(t)=i_{0}\\cos(\\omega_{0}t), \\qquad v_{C}(t)=V_{0}\\sin(\\omega_{0}t)\n\\]\n\nEnergia la fiecare moment:\n\n\\[\nU_{C}(t)=\\frac{1}{2}C V_{0}^{2}\\sin^{2}(\\omega_{0}t)\n=\\frac{C V_{0}^{2}}{4}\\left[1-\\cos(2\\omega_{0}t)\\right]\n\\]\n\n\\[\nU_{L}(t)=\\frac{1}{2}L i_{0}^{2}\\cos^{2}(\\omega_{0}t)\n=\\frac{L i_{0}^{2}}{4}\\left[1+\\cos(2\\omega_{0}t)\\right]\n\\]\n\nCurentul \u0219i tensiunea au frecven\u021ba fundamental\u0103 \\(f_{0}\\), \u00een timp ce energia instantanee con\u021bine o component\u0103 DC \u0219i o component\u0103 la frecven\u021ba dublat\u0103 \\(2f_{0}\\).\n\n<strong>Semnifica\u021bie pentru circuite cuplate:<\/strong> \u00cen circuite cuplate, transferul de energie este determinat de puterea instantanee \\(p(t)=v(t)i(t)\\); pentru componente armonice \\(v \\sim \\sin(\\omega_{0}t)\\), \\(i \\sim \\cos(\\omega_{0}t)\\), produsul lor con\u021bine componente la \\(0\\) \u0219i \\(2\\omega_{0}\\). Prin urmare, c\u00e2nd se analizeaz\u0103 puterea \u0219i pierderile \u00eentr-un rezonator, este esen\u021bial s\u0103 se \u021bin\u0103 cont de componenta la \\(2f_{0}\\), chiar dac\u0103 curen\u021bii\/fluxurile sunt dominate de \\(f_{0}\\).\n<h3>2.4 Condi\u021bii pentru ini\u021bierea \u0219i sus\u021binerea oscila\u021biilor \u00eentr-un sistem cu feedback \u0219i canale disipative<\/h3>\nPentru a ini\u021bializa oscila\u021biile \u00eentr-un sistem cu feedback, energia livrat\u0103 circuitului prin portul (1) pe o perioad\u0103 \\(T\\) trebuie s\u0103 dep\u0103\u0219easc\u0103 pierderile:\n\n\\[\nE_{\\mathrm{ext,in}}(T) &gt; E_{\\mathrm{loss}}(T) + E_{\\mathrm{load}}(T)\n\\qquad \\text{(faz\u0103 de pornire)}\n\\]\n\nunde \\(E_{\\mathrm{ext,in}}(T)\\equiv \\int_{0}^{T} p_{\\mathrm{ext}}(t)\\, dt\\).\n\n\u00cen stare sta\u021bionar\u0103 (ciclu limit\u0103):\n\n\\[\nE_{\\mathrm{ext,in}}(T)=E_{\\mathrm{loss}}(T)+E_{\\mathrm{load}}(T)\n\\]\n\n\u00cen acest regim, amplitudinea se stabilizeaz\u0103 la un nivel determinat de neliniarit\u0103\u021bile sistemului (desc\u0103rc\u0103tor, satura\u021bie, diode de str\u0103pungere). Acest lucru este descris \u00een Sec\u021biunea 7.\n<h2>3. Arhitectura generatorului VENDOR<\/h2>\n<h3>3.1 Componentele sistemului<\/h3>\nConform brevetului WO2024209235A1:\n<ul>\n \t<li><strong>Interfa\u021b\u0103 energetic\u0103 bazat\u0103 pe port \/ nod de ini\u021biere mod (1)<\/strong> \u2014 un port bidirec\u021bional definit fizic prin care se efectueaz\u0103 schimbul de energie bazat pe port \u00een timpul pornirii \u0219i \u00een func\u021bionarea \u00een stare sta\u021bionar\u0103. \u00centr-o implementare practic\u0103, portul (1) poate fi conectat la un tampon de baterie prin BMS, permi\u021b\u00e2nd at\u00e2t livrarea de energie \u00een sistem, c\u00e2t \u0219i recep\u021bia energiei pentru re\u00eenc\u0103rcare c\u00e2nd exist\u0103 flux invers (recuperare).<\/li>\n \t<li><strong>Element de stocare nod de desc\u0103rcare (3)<\/strong> \u2014 un condensator \u00eenc\u0103rcat de la portul (1).<\/li>\n \t<li><strong>Desc\u0103rc\u0103toare multiple (14, 15, 16)<\/strong> \u2014 desc\u0103rc\u0103toare corona cu tensiuni de str\u0103pungere \u0219i caracteristici spectrale diferite.<\/li>\n \t<li><strong>\u00cenf\u0103\u0219urarea primar\u0103 (4)<\/strong> a transformatorului (5).<\/li>\n \t<li><strong>\u00cenf\u0103\u0219urarea secundar\u0103 (7) + condensator (8)<\/strong> \u2014 form\u00e2nd un circuit rezonant LC.<\/li>\n \t<li><strong>Cale de feedback (cale de cuplaj intern\u0103)<\/strong> \u2014 returneaz\u0103 o parte din energia din circuitul rezonant la elementul de stocare (3), permi\u021b\u00e2nd redistribuirea energiei \u0219i sus\u021binerea unui regim auto-oscilant.<\/li>\n \t<li><strong>Etapa de extrac\u021bie la ie\u0219ire (conform brevetului)<\/strong> \u2014 transfer\u0103 energie la sarcin\u0103 (13) printr-o topologie de extrac\u021bie izolat\u0103.<\/li>\n<\/ul>\n<h3>3.2 Secven\u021ba de operare<\/h3>\n<h4>Faza 1: \u00cenc\u0103rcarea elementului de stocare<\/h4>\nPrin portul (1), puterea extern\u0103 \\(P_{\\mathrm{ext}}\\) este livrat\u0103, \u00eenc\u0103rc\u00e2nd condensatorul (3) la o tensiune care dep\u0103\u0219e\u0219te tensiunea de str\u0103pungere a unuia sau mai multor desc\u0103rc\u0103toare.\n<h4>Faza 2: Desc\u0103rcarea \u0219i impulsul \u00een primar<\/h4>\nDesc\u0103rc\u0103torul se str\u0103punge; condensatorul (3) se descarc\u0103 rapid prin \u00eenf\u0103\u0219urarea primar\u0103 (4). Apare un impuls de curent cu un \\(di\/dt\\) ridicat, determinat de capacitatea \\(C_{3}\\), inductan\u021bele parazite \u0219i dinamica de desc\u0103rcare a desc\u0103rc\u0103torului. Acest impuls induce o tensiune pe \u00eenf\u0103\u0219urarea secundar\u0103 (7) prin cuplaj magnetic de transformator.\n<h4>Faza 3: Oscila\u021bia rezonant\u0103 a circuitului secundar<\/h4>\n\u00cenf\u0103\u0219urarea secundar\u0103 (7) \u00eempreun\u0103 cu condensatorul (8) formeaz\u0103 un circuit LC. Tensiunea indus\u0103 excit\u0103 acest circuit, iar cu un factor de calitate ridicat \\(Q\\), circuitul oscileaz\u0103 pentru multe cicluri. C\u00e2mpul magnetic al transformatorului poart\u0103 aceste oscila\u021bii.\n<h4>Faza 4: Feedback \u0219i dinamica regimului<\/h4>\nO parte din energia din circuitul secundar (prin calea de cuplaj intern\u0103) curge \u00een elementul de stocare (3). Acest feedback:\n<ul>\n \t<li>serve\u0219te ca un mecanism de feedback pozitiv pentru sus\u021binerea regimului,<\/li>\n \t<li>ofer\u0103 redistribuirea energiei \u00eentre elementul de stocare \u0219i rezonator,<\/li>\n \t<li>men\u021bine sistemul \u00eentr-un regim de ciclu limit\u0103 (vezi Sec\u021biunea 7).<\/li>\n<\/ul>\n\u00cen termeni baza\u021bi pe porturi, feedback-ul formeaz\u0103 o cale de transfer de energie intern\u0103 de la circuitul oscilant la elementul de stocare, modific\u00e2nd rela\u021biile de faz\u0103 \u0219i condi\u021biile de excitare, dar f\u0103r\u0103 a ad\u0103uga energie extern\u0103 dincolo de balan\u021ba extern\u0103 total\u0103 definit\u0103 de intr\u0103rile m\u0103surate \u0219i termenii de limit\u0103.\n\n\u00cen func\u021bionarea \u00een stare sta\u021bionar\u0103, balan\u021ba extern\u0103 total\u0103 compenseaz\u0103 pierderile \\(P_{\\mathrm{loss}}\\) \u0219i puterea de ie\u0219ire util\u0103 \\(P_{\\mathrm{load}}\\) \u00een conformitate cu formula de balan\u021b\u0103 dat\u0103 \u00een Sec\u021biunea 1.1.\n<h4>Faza 5: Extrac\u021bia puterii la sarcin\u0103<\/h4>\nEtapa de extrac\u021bie la ie\u0219ire transfer\u0103 energie la sarcin\u0103. Sarcina prime\u0219te putere \\(P_{\\mathrm{load}}\\), iar magnitudinea sa se reflect\u0103 \u00eentr-o reducere a factorului de calitate general \\(Q_{\\mathrm{tot}}\\) \u0219i o cre\u0219tere a influxului de energie extern\u0103 total\u0103 necesar \\(P_{\\mathrm{in,avg}}\\), a\u0219a cum este descris \u00een Sec\u021biunea 6.3.\n<h3>3.3 Rolul desc\u0103rc\u0103toarelor multiple \u0219i stabilitatea spectral\u0103<\/h3>\nDesc\u0103rc\u0103toarele au tensiuni de str\u0103pungere \u0219i caracteristici spectrale diferite, decalate \u00een frecven\u021b\u0103.\n\n<strong>Scop ingineresc:<\/strong>\n<ul>\n \t<li>C\u00e2nd condi\u021biile de operare se modific\u0103 (umiditate, temperatur\u0103, micro-goluri datorate eroziunii), un desc\u0103rc\u0103tor poate pierde caracteristicile optime.<\/li>\n \t<li>Alt desc\u0103rc\u0103tor cu o tensiune de str\u0103pungere vecin\u0103 se activeaz\u0103 apoi \u0219i sus\u021bine regimul.<\/li>\n \t<li>Ac\u021biunea colectiv\u0103 reduce sensibilitatea la deriva parametric\u0103.<\/li>\n \t<li>Aceasta este o redundan\u021b\u0103 inginereasc\u0103, nu un mecanism &#8222;magic&#8221;.<\/li>\n<\/ul>\n<strong>Stabilitatea regimului ca proprietate arhitectural\u0103:<\/strong>\n\nO structur\u0103 cu desc\u0103rc\u0103toare multiple cu praguri suprapuse \u0219i dinamic\u0103 de conductivitate implementeaz\u0103 &#8222;stabilitatea regimului&#8221;: sistemul p\u0103streaz\u0103 condi\u021biile de excitare ale rezonatorului sub deriva parametrilor de desc\u0103rcare (umiditate, eroziune, micro-geometrie) prin comutarea canalului de desc\u0103rcare activ, f\u0103r\u0103 a schimba principiul balan\u021bei externe\n\n\\[\nP_{\\mathrm{ext,avg}} = P_{\\mathrm{loss,avg}} + P_{\\mathrm{load,avg}} + P_{\\mathrm{buf,avg}}.\n\\]\n<h2>4. Desc\u0103rcarea corona ca element neliniar adaptiv<\/h2>\n<h3>4.1 Fizica desc\u0103rc\u0103rii corona<\/h3>\nDesc\u0103rcarea corona apare c\u00e2nd intensitatea c\u00e2mpului electric local \u00een apropierea unui electrod atinge valori suficiente pentru a ioniza gazul; pragul este determinat de geometrie (raza de curbur\u0103), presiune, compozi\u021bia gazului \u0219i regimul de operare (corona vs. streamer).\n\n<strong>Mecanism de ionizare:<\/strong>\n<ul>\n \t<li>Un gradient ridicat de c\u00e2mp electric ionizeaz\u0103 moleculele de aer \u00een vecin\u0103tatea v\u00e2rfului electrodului.<\/li>\n \t<li>Se formeaz\u0103 un nor de plasm\u0103 slab ionizat\u0103.<\/li>\n \t<li>Plasma prezint\u0103 o conductivitate efectiv\u0103 \\(\\sigma(t,E)\\), care depinde de intensitatea c\u00e2mpului electric \u0219i timp.<\/li>\n \t<li>Aceast\u0103 conductivitate este neliniar\u0103 \u0219i nestabil\u0103.<\/li>\n<\/ul>\nDesc\u0103rcarea corona genereaz\u0103 curen\u021bi impulsivi cu o densitate spectral\u0103 \u00een band\u0103 larg\u0103, \u00een func\u021bie de geometria electrodului, parametrii gazului \u0219i regimul de desc\u0103rcare (corona vs. streamer). Conductivitatea neliniar\u0103 afecteaz\u0103 zgomotul de faz\u0103, condi\u021biile de excitare a rezonatorului \u0219i stabilitatea regimului.\n<h3>4.2 Adaptivitatea regimului<\/h3>\nDesc\u0103rc\u0103toare corona multiple conectate \u00een paralel cu tensiuni de str\u0103pungere diferite formeaz\u0103 un sistem adaptiv:\n<ul>\n \t<li>La niveluri sc\u0103zute de c\u00e2mp, unele desc\u0103rc\u0103toare r\u0103m\u00e2n \u00een stare de ionizare slab\u0103.<\/li>\n \t<li>La niveluri mai ridicate de c\u00e2mp, alte desc\u0103rc\u0103toare se declan\u0219eaz\u0103 \u0219i atrag curentul.<\/li>\n \t<li>Regimul general r\u0103m\u00e2ne stabil pe o gam\u0103 larg\u0103 de condi\u021bii.<\/li>\n<\/ul>\n<h2>5. Mediul ambiental ca condi\u021bii de limit\u0103 \u0219i factor de reproductibilitate<\/h2>\n<h3>5.1 Influen\u021ba parametrilor de mediu<\/h3>\nParametrii electrici ai atmosferei (conductivitate \\(\\sigma\\), umiditate, presiune, temperatur\u0103) afecteaz\u0103:\n<ul>\n \t<li><strong>Praguri de str\u0103pungere \u0219i tranzi\u021bii de regim<\/strong> \u2014 pentru intervale uniforme, o dependen\u021b\u0103 de tip Paschen \\(U_{\\mathrm{br}} = f(pd)\\) serve\u0219te ca referin\u021b\u0103; cu toate acestea, pentru electrozi ascu\u021bi\u021bi, amplificarea c\u00e2mpului local \u0219i condi\u021biile de emisie devin decisive.<\/li>\n \t<li><strong>Stabilitatea desc\u0103rc\u0103rii corona<\/strong> \u2014 caracteristicile spectrale ale impulsului depind de presiune \u0219i compozi\u021bia gazului; umiditatea poate modifica semnificativ pragurile de str\u0103pungere \u0219i stabilitatea desc\u0103rc\u0103rii.<\/li>\n \t<li><strong>Pierderi parazite<\/strong> \u2014 pierderi dielectrice \u00een aer, scurgeri peste suprafe\u021be contaminate \u0219i curen\u021bi indu\u0219i.<\/li>\n<\/ul>\n<h3>5.2 Rol \u00een protocoalele de testare<\/h3>\n\u00cen VENDOR, atmosfera este considerat\u0103 exclusiv ca mediu de lucru \u0219i de limit\u0103 pentru procesele de desc\u0103rcare, nu ca surs\u0103 de energie.\n\nProtocoalele de verificare independent\u0103 trebuie:\n<ul>\n \t<li>S\u0103 \u00eenregistreze \u0219i s\u0103 controleze parametrii de mediu (\\(P, T, RH\\)).<\/li>\n \t<li>S\u0103 evalueze sensibilitatea regimului la varia\u021biile lor \u00een cadrul protocolului (Sec\u021biunea 9.5).<\/li>\n<\/ul>\n\u00cen scopuri de reproductibilitate, aceste influen\u021be sunt tratate ca sensibilit\u0103\u021bi de regim m\u0103surabile experimental, nu ca explica\u021bii a priori ale sursei de energie.\n<h2>6. Factorul de calitate \u0219i balan\u021ba energetic\u0103 \u00een sistemele rezonante cu sarcin\u0103<\/h2>\n<h3>6.1 Factorul Q \u0219i pierderile de putere \u00eentr-un rezonator<\/h3>\nPentru un rezonator cu energie stocat\u0103 \\(U\\) \u0219i frecven\u021b\u0103 unghiular\u0103 \\(\\omega_{0}\\), puterea disipat\u0103 \u00een pierderile interne este:\n\n\\[\nP_{0} = \\frac{\\omega_{0} U}{Q_{0}}\n\\]\n\nunde \\(Q_{0}\\) este factorul de calitate echivalent f\u0103r\u0103 sarcin\u0103, incluz\u00e2nd toate canalele disipative:\n\n\\[\n\\frac{1}{Q_{0}} = \\frac{1}{Q_{R}} + \\frac{1}{Q_{C}} + \\frac{1}{Q_{\\mathrm{rad}}}\n\\]\n\nAici, \\(Q_{R}\\) corespunde pierderilor ohmice, \\(Q_{C}\\) pierderilor dielectrice, iar \\(Q_{\\mathrm{rad}}\\) pierderilor radiative.\n<h3>6.2 Sarcina ca canal de disipare suplimentar<\/h3>\nC\u00e2nd o sarcin\u0103 este conectat\u0103 (etapa de extrac\u021bie), sarcina interac\u021bioneaz\u0103 cu c\u00e2mpul electromagnetic al rezonatorului \u0219i ac\u021bioneaz\u0103 ca un canal suplimentar pentru extrac\u021bia energiei din rezonator (cu energia fiind convertit\u0103 \u00een lucru util la sarcin\u0103). Aceasta este echivalent\u0103 cu introducerea unui factor de calitate al sarcinii:\n\n\\[\nQ_{L} = \\frac{\\omega_{0} U}{P_{\\mathrm{load}}}\n\\]\n\nFactorul de calitate total al sistemului este:\n\n\\[\n\\frac{1}{Q_{\\mathrm{tot}}} = \\frac{1}{Q_{0}} + \\frac{1}{Q_{L}}\n\\]\n<h3>6.3 Puterea extern\u0103 necesar\u0103 \u00een prezen\u021ba sarcinii<\/h3>\nPentru a men\u021bine un nivel specificat de energie stocat\u0103 \\(U\\) \u00een rezonator cu o sarcin\u0103 conectat\u0103, este necesar\u0103 compensarea pierderilor totale \u0219i extrac\u021bia energiei la sarcin\u0103. Puterea extern\u0103 medie total\u0103 corespunz\u0103toare este definit\u0103 ca:\n\n\\[\nP_{\\mathrm{in,avg}} = \\frac{\\omega_{0} U}{Q_{\\mathrm{tot}}},\n\\qquad\nP_{\\mathrm{in,avg}} \\equiv P_{\\mathrm{elec,avg}} + P_{\\mathrm{field,avg}}.\n\\]\n\nO cre\u0219tere a puterii de sarcin\u0103 util\u0103 \\(P_{\\mathrm{load}}\\) este echivalent\u0103 cu o reducere a factorului de calitate total \\(Q_{\\mathrm{tot}}\\) \u0219i necesit\u0103 o cre\u0219tere a influxului de energie extern\u0103 total\u0103 \\(P_{\\mathrm{in,avg}}\\). Contribu\u021bia la \\(P_{\\mathrm{in,avg}}\\) poate proveni fie din canalul bazat pe port prin fire, fie din termenul de limit\u0103 (c\u00e2mp), \u00een func\u021bie de regimul de operare \u0219i configura\u021bia cuplajului electrodinamic al sistemului cu mediul s\u0103u.\n\nAstfel, o cre\u0219tere a sarcinii nu necesit\u0103 neap\u0103rat o cre\u0219tere a puterii portului prin fire \\(P_{\\mathrm{elec}}\\); necesit\u0103 o cre\u0219tere a balan\u021bei externe totale, a\u0219a cum este determinat\u0103 de contabilitatea complet\u0103 a energiei sistemului.\n<h3>6.4 Nivelul energiei stocate ca parametru de design<\/h3>\nNivelul energiei stocate \\(U\\) \u00een rezonator este determinat de designul tehnic:\n\n\\[\nU = \\frac{1}{2} C_{8} V_{8}^{2} = \\frac{1}{2} L_{7} I_{7}^{2}\n\\]\n\nunde \\(C_{8}\\) \u0219i \\(L_{7}\\) sunt parametri de circuit. Cre\u0219terea \\(U\\) necesit\u0103 fie cre\u0219terea tensiunii \\(V_{8}\\) (cu cerin\u021be stricte de izola\u021bie), fie cre\u0219terea inductan\u021bei (mai multe spire, construc\u021bie fizic\u0103 mai mare).\n\nAcesta nu este un grad de libertate independent pentru cre\u0219terea puterii de ie\u0219ire. Nivelul \\(U\\) \u0219i puterea extern\u0103 necesar\u0103 \\(P_{\\mathrm{in,avg}}\\) sunt legate prin rela\u021bia dat\u0103 \u00een Sec\u021biunea 6.3.\n<h2>7. Dinamica neliniar\u0103 \u0219i regimul de ciclu limit\u0103<\/h2>\n<h3>7.1 Sisteme \u00eenchise cu feedback pozitiv<\/h3>\nEcua\u021bia pentru un sistem rezonant \u00eenchis cu feedback:\n\n\\[\n\\frac{dx}{dt} = f(x) + k \\cdot g(x)\n\\]\n\nunde:\n<ul>\n \t<li>\\(f(x)\\) \u2014 dinamica natural\u0103 (pierderi, amortizare),<\/li>\n \t<li>\\(g(x)\\) \u2014 semnal de feedback,<\/li>\n \t<li>\\(k\\) \u2014 coeficient de cuplaj.<\/li>\n<\/ul>\n<strong>Comportamentul sistemului:<\/strong>\n<ul>\n \t<li>\\(k = 0\\) (f\u0103r\u0103 feedback): traiectoria converge la echilibru (oscila\u021biile se descompun exponen\u021bial).<\/li>\n \t<li>\\(k\\) mic: amortizarea este \u00eencetinit\u0103.<\/li>\n \t<li>\\(k\\) critic: sistemul intr\u0103 \u00eentr-un ciclu limit\u0103 \u2014 un regim periodic cu amplitudine \u0219i frecven\u021b\u0103 fixe.<\/li>\n<\/ul>\n<strong>Semnifica\u021bia fizic\u0103 a vectorului de stare:<\/strong>\n\n\u00cen contextul VENDOR, vectorul de stare \\(x\\) poate include: tensiunea pe elementul de stocare \\(V_{3}\\), curen\u021bii \u00eenf\u0103\u0219ur\u0103rilor, faza \u0219i amplitudinea regimului rezonant \u00een circuitul secundar, parametrii efectivi de desc\u0103rcare (conductivitate echivalent\u0103 \\(\\sigma(t,E)\\)) \u0219i starea de \u00eenc\u0103rcare a tamponului (SoC).\n<h3>7.2 Ciclu limit\u0103 \u0219i balan\u021b\u0103 energetic\u0103<\/h3>\n\u00cen ciclul limit\u0103, sistemul \u00ee\u0219i auto-regleaz\u0103 amplitudinea astfel \u00eenc\u00e2t energia furnizat\u0103 prin portul (1) pe o perioad\u0103 \\(T\\) s\u0103 fie egal\u0103 cu energia pierdut\u0103 \u0219i livrat\u0103 la sarcin\u0103:\n\n\\[\nE_{\\mathrm{ext}}(T) = E_{\\mathrm{loss}}(T) + E_{\\mathrm{load}}(T)\n\\]\n\nunde\n\n\\[\nE_{\\mathrm{ext}}(T) \\equiv \\int_{0}^{T} v_{\\mathrm{ext}}(t)\\, i_{\\mathrm{ext}}(t)\\, dt.\n\\]\n\nC\u00e2nd un tampon de baterie este prezent prin BMS, cantitatea \\(E_{\\mathrm{ext}}(T)\\) este interpretat\u0103 ca fluxul total de energie prin portul (1), mai degrab\u0103 dec\u00e2t ca o desc\u0103rcare unidirec\u021bional\u0103 a bateriei. \u00cen stare sta\u021bionar\u0103 (\\(P_{\\mathrm{buf,avg}} \\approx 0\\)), intervalele de re\u00eenc\u0103rcare par\u021bial\u0103 a tamponului sunt posibile datorit\u0103 redistribuirii interne de energie \u0219i c\u0103ilor de recuperare, f\u0103r\u0103 a \u00eenc\u0103lca balan\u021ba energetic\u0103 general\u0103\n\n\\[\nP_{\\mathrm{ext,avg}} = P_{\\mathrm{loss,avg}} + P_{\\mathrm{load,avg}}.\n\\]\n\nAmplitudinea nici nu cre\u0219te, nici nu scade \u2014 sistemul rezid\u0103 la un punct de echilibru pe planul fazelor. Acest lucru nu \u00eencalc\u0103 legea conserv\u0103rii energiei; este pur \u0219i simplu un punct de operare stabil unde intrarea de energie este echilibrat\u0103 de cheltuirea energiei.\n<h3>7.3 Rolul neliniarit\u0103\u021bilor \u00een VENDOR<\/h3>\nElementele neliniare (desc\u0103rc\u0103toare, satura\u021bia transformatorului, diodele de str\u0103pungere) servesc la:\n<ul>\n \t<li>limitarea amplitudinii \u2014 prevenind cre\u0219terea exponen\u021bial\u0103 a tensiunilor,<\/li>\n \t<li>sincronizarea regimului \u2014 fixarea frecven\u021bei \u0219i fazei,<\/li>\n \t<li>adaptarea la sarcin\u0103 \u2014 modific\u0103rile \u00een \\(Q_{L}\\) duc la modific\u0103ri de amplitudine, \u00een timp ce regimul r\u0103m\u00e2ne stabil.<\/li>\n<\/ul>\n<h2>8. Balan\u021ba energetic\u0103 \u00een func\u021bionarea \u00een stare sta\u021bionar\u0103: Formulare strict\u0103<\/h2>\n<h3>8.1 Balan\u021ba complet\u0103 de putere<\/h3>\n\u00cen stare sta\u021bionar\u0103 (ciclu limit\u0103), pentru \u00eentregul sistem (mediat pe intervalul \\(T\\)):\n\n\\[\nP_{\\mathrm{ext,avg}} =\nP_{\\mathrm{Joule,avg}} +\nP_{\\mathrm{dielectric,avg}} +\nP_{\\mathrm{radiation,avg}} +\nP_{\\mathrm{erosion,avg}} +\nP_{\\mathrm{load,avg}} +\nP_{\\mathrm{buf,avg}}\n\\]\n\nsau, \u00een form\u0103 compact\u0103:\n\n\\[\nP_{\\mathrm{ext,avg}} = P_{\\mathrm{loss,avg}} + P_{\\mathrm{load,avg}} + P_{\\mathrm{buf,avg}}\n\\]\n\nunde\n\n\\[\nP_{\\mathrm{loss}} = P_{\\mathrm{Joule}} + P_{\\mathrm{diel}} + P_{\\mathrm{rad}} + P_{\\mathrm{erosion}} + \\ldots\n\\]\n\neste puterea total\u0103 de pierdere, \u0219i\n\n\\[\nP_{\\mathrm{buf,avg}} = \\left\\langle \\frac{dE_{\\mathrm{buf}}}{dt} \\right\\rangle\n\\]\n\neste puterea medie a tamponului.\n\n\u00cen stare sta\u021bionar\u0103 \u00een raport cu SoC, \\(P_{\\mathrm{buf,avg}} \\approx 0\\), deci:\n\n\\[\nP_{\\mathrm{ext,avg}} = P_{\\mathrm{loss,avg}} + P_{\\mathrm{load,avg}}.\n\\]\n\nPartea st\u00e2ng\u0103 reprezint\u0103 energia care intr\u0103 prin portul (1) \u0219i alte intr\u0103ri externe (inclusiv termenii de limit\u0103 defini\u021bi \u00een aceast\u0103 specifica\u021bie).\n\nPartea dreapt\u0103 reprezint\u0103 toate canalele de cheltuire a energiei \u0219i tamponare.\n<h3>8.2 Controlul intr\u0103rilor parazite \u00een protocolul de testare<\/h3>\nProtocolul de testare trebuie s\u0103 includ\u0103 m\u0103suri pentru controlul cuplajelor parazite (mecanice, termice, electromagnetice) \u0219i pentru evaluarea contribu\u021biilor lor. Obiectivul este de a demonstra c\u0103 balan\u021ba m\u0103surat\u0103\n\n\\[\nP_{\\mathrm{ext,avg}} \\approx P_{\\mathrm{load,avg}} + P_{\\mathrm{loss,avg}} + P_{\\mathrm{buf,avg}}\n\\]\n\neste p\u0103strat\u0103 sub varia\u021bia controlat\u0103 a condi\u021biilor externe \u0219i nu poate fi explicat\u0103 prin intr\u0103ri parazite. Un protocol detaliat este furnizat \u00een Sec\u021biunea 9.\n<h2>9. Protocol de verificare metrologic\u0103<\/h2>\nAnaliza teoretic\u0103 arat\u0103 c\u0103 arhitectura VENDOR este fizic consistent\u0103 \u00een cadrul electrodinamicii clasice. Verificarea final\u0103 necesit\u0103 validare de laborator independent\u0103.\n<h3>9.1 Clasificarea sitului de testare \u0219i criteriile low-EM<\/h3>\nPentru a exclude interpret\u0103rile legate de &#8222;recoltare 50\/60 Hz&#8221;, situl de testare trebuie caracterizat cantitativ.\n<h4>9.1.1 Metrica fondului de re\u021bea (50\/60 Hz)<\/h4>\nMetrica m\u0103surabil\u0103 \\(B_{50}\\) este definit\u0103 ca amplitudinea densit\u0103\u021bii fluxului magnetic la 50\/60 Hz (\u0219i \\(B_{150}\\) la a 3-a armonic\u0103) \u00eentr-un punct de control, m\u0103surat\u0103 folosind o bucl\u0103 de induc\u021bie calibrat\u0103 \u0219i un analizor de spectru \/ \u00eenregistrator FFT.\n\nEste stabilit un criteriu prag low-EM:\n<ul>\n \t<li>\\(B_{50}\\) \u0219i \\(B_{150}\\) la situl de testare nu trebuie s\u0103 dep\u0103\u0219easc\u0103 1% din nivelul &#8222;urban&#8221; de referin\u021b\u0103, m\u0103surat folosind acela\u0219i set de echipamente \u00eentr-un laborator urban tipic (sit de referin\u021b\u0103), la aceea\u0219i \u00een\u0103l\u021bime \u0219i cu aceea\u0219i orientare a buclei.<\/li>\n<\/ul>\n<em>Not\u0103:<\/em> valoarea de referin\u021b\u0103 poate fi \u00eenregistrat\u0103 \u00eenainte de testare, cu jurnalele de calibrare p\u0103strate.\n<h4>9.1.2 Calificarea sitului \u0219i \u00eenregistrarea infrastructurii de re\u021bea<\/h4>\nSitul de testare trebuie s\u0103 satisfac\u0103 simultan:\n<ul>\n \t<li>calificarea sitului bazat\u0103 pe fondul m\u0103surat \\(B_{50}\\) \/ \\(B_{150}\\) \u0219i cartografiere; distan\u021ba fa\u021b\u0103 de infrastructura de re\u021bea este \u00eenregistrat\u0103, dar acceptarea este determinat\u0103 de criteriile low-EM \u0219i scan\u0103rile de c\u00e2mp mai degrab\u0103 dec\u00e2t de o raz\u0103 fix\u0103;<\/li>\n \t<li>absen\u021ba cablurilor electrice subterane necontabilizate sau transformatoare \u00een raza identificat\u0103 prin scanarea preliminar\u0103 a \\(B_{50}\\), confirmat\u0103 prin cartografierea sitului \u0219i jurnalele de instrumenta\u021bie.<\/li>\n<\/ul>\n<h3>9.2 Testul principal: Balan\u021ba energetic\u0103<\/h3>\n<h4>9.2.1 Cantit\u0103\u021bi m\u0103surate<\/h4>\n\u00cen timpul test\u0103rii, urm\u0103toarele cantit\u0103\u021bi mediate \u00een timp sunt determinate:\n\n\\[\nP_{\\mathrm{elec,avg}} = \\frac{1}{T}\\int_{0}^{T} v_{\\mathrm{ext}}(t)\\, i_{\\mathrm{ext}}(t)\\, dt\n\\]\n\n\u2014 puterea electric\u0103 medie prin fire la portul (1), inclusiv toate c\u0103ile de returnare \u0219i referin\u021b\u0103.\n\n\\[\nP_{\\mathrm{buf,avg}} = \\left\\langle \\frac{dE_{\\mathrm{buf}}}{dt} \\right\\rangle\n\\]\n\n\u2014 rata medie de schimbare a energiei tamponului intern, determinat\u0103 prin audit energetic la bornele tamponului \u0219i\/sau estimare independent\u0103 a st\u0103rii de \u00eenc\u0103rcare (SoC).\n\n\\[\nP_{\\mathrm{load,avg}} = \\frac{1}{T}\\int_{0}^{T} v_{\\mathrm{out}}(t)\\, i_{\\mathrm{out}}(t)\\, dt\n\\]\n\n\u2014 puterea activ\u0103 medie livrat\u0103 la sarcin\u0103.\n\n\\[\nP_{\\mathrm{loss,avg}}\n\\]\n\n\u2014 puterea medie de pierdere, determinat\u0103 prin balan\u021b\u0103 termic\u0103 \u0219i\/sau calorimetric\u0103, inclusiv punctele fierbin\u021bi locale \u0219i disiparea total\u0103 de c\u0103ldur\u0103.\n<h4>9.2.1.1 Cerin\u021be pentru echipamentul de m\u0103surare \u0219i &#8222;metoda bornelor externe (cutie neagr\u0103)&#8221;<\/h4>\nDeoarece sistemul opereaz\u0103 cu forme de und\u0103 nesinusoidale, impulsive, m\u0103sur\u0103torile de putere trebuie efectuate folosind instrumenta\u021bie \u0219i metode demonstrabil potrivite pentru regimuri tranzitorii \u00een band\u0103 larg\u0103. Obiectivul este ob\u021binerea puterii active metrologic defensabile pe bornele externe f\u0103r\u0103 a necesita acces la noduri interne.\n\n<strong>(a) Abord\u0103ri de m\u0103surare permise (alege\u021bi una sau combina\u021bi):<\/strong>\n<ol>\n \t<li>Metoda analizorului de putere \u00een band\u0103 larg\u0103 (dac\u0103 capacitatea instrumentului este demonstrat\u0103 pentru clasa de forme de und\u0103 m\u0103surat\u0103), sau<\/li>\n \t<li>Metoda bazat\u0103 pe osciloscop folosind achizi\u021bie simultan\u0103 de tensiune \u0219i curent cu sonde calibrate \u0219i procesare documentat\u0103 a puterii instantanee \\(p(t)=v(t)\\cdot i(t)\\).<\/li>\n<\/ol>\n<strong>(b) Criterii de adecvare (obligatoriu):<\/strong>\n<ul>\n \t<li>Metoda selectat\u0103 trebuie s\u0103 demonstreze suficient\u0103 band\u0103 de trecere, e\u0219antionare \u0219i gam\u0103 dinamic\u0103 pentru a reprezenta formele de und\u0103 m\u0103surate f\u0103r\u0103 aliasing sau saturare front-end.<\/li>\n \t<li>Lan\u021bul de m\u0103surare trebuie s\u0103 includ\u0103 func\u021bii de transfer ale sondelor documentate (magnitudine \u0219i faz\u0103 unde este aplicabil) sau date de calibrare de la produc\u0103tor suficiente pentru a delimita erorile de amplitudine \u0219i faz\u0103 \u00een domeniul de frecven\u021b\u0103 care contribuie material la puterea activ\u0103.<\/li>\n \t<li>Deskew \/ alinierea \u00een timp \u00eentre canalele de tensiune \u0219i curent este obligatorie, cu o procedur\u0103 documentat\u0103 \u0219i incertitudine temporal\u0103 rezidual\u0103 rezultat\u0103.<\/li>\n \t<li>Laboratorul trebuie s\u0103 furnizeze un buget de incertitudine de m\u0103surare pentru \\(P_{\\mathrm{elec,avg}}\\) \u0219i \\(P_{\\mathrm{load,avg}}\\) consistent cu incertitudinea general\u0103 a balan\u021bei energetice definit\u0103 \u00een acest protocol.<\/li>\n<\/ul>\n<strong>(c) Constr\u00e2ngerea doar pe bornele externe (&#8222;cutie neagr\u0103&#8221;) (protec\u021bie IP):<\/strong>\n\nToate m\u0103sur\u0103torile electrice sunt efectuate exclusiv pe bornele externe:\n<ul>\n \t<li>Bornele portului (1), inclusiv toate c\u0103ile de returnare, ecran\u0103rile \u0219i conductorii de referin\u021b\u0103;<\/li>\n \t<li>Bornele de ie\u0219ire\/sarcin\u0103.<\/li>\n<\/ul>\nConectarea sondelor la noduri interne, trasee PCB, terminale de componente sau puncte de m\u0103surare interne nu este necesar\u0103 \u0219i nu este permis\u0103 conform regulilor de protec\u021bie IP ale acestui protocol.\n\n<strong>(d) Controale anti-artefact:<\/strong>\n\nPartea verificatoare trebuie s\u0103 documenteze m\u0103surile pentru a exclude c\u0103ile de returnare ascunse \u0219i erorile de referin\u021b\u0103 (\u00eemp\u0103m\u00e2nt\u0103ri, ecran\u0103ri, \u0219asiu, cabluri auxiliare, c\u0103i de \u00eemp\u0103m\u00e2ntare ale instrumenta\u021biei) \u0219i trebuie s\u0103 efectueze verific\u0103ri de control specificate \u00een Sec\u021biunea 9 pentru a demonstra integritatea m\u0103sur\u0103rii.\n\n<strong>(e) Cerin\u021be de calibrare \u0219i incertitudine:<\/strong>\n\nInstrumentele de m\u0103surare a puterii electrice trebuie calibrate cel pu\u021bin o dat\u0103 la 12 luni.\n\nM\u0103sur\u0103torile de temperatur\u0103 trebuie efectuate folosind senzori cu o precizie nu mai proast\u0103 de \u00b10.5\u00a0\u00b0C, calibra\u021bi cel pu\u021bin o dat\u0103 la 6 luni.\n\nIncertitudinea extins\u0103 a balan\u021bei energetice este luat\u0103 ca:\n\n\\[\n\\delta_{A} = 5\\% \\qquad (k = 2),\n\\]\n\ncorespunz\u0103toare incertitudinii combinate a m\u0103sur\u0103torilor electrice, termice \u0219i de energie stocat\u0103.\n\n<em>Not\u0103:<\/em> Pentru testele de putere redus\u0103 (\\(P_{\\mathrm{load,avg}} &lt; 50\\,\\mathrm{W}\\)), laboratorul poate specifica o limit\u0103 de incertitudine mai strict\u0103 sau justifica aplicabilitatea \\(\\delta_A\\).\n<h4>9.2.2 Ecua\u021bia balan\u021bei energetice<\/h4>\n\u00cen toate regimurile de operare, balan\u021ba energetic\u0103 mediat\u0103 trebuie s\u0103 se verifice:\n\n\\[\nP_{\\mathrm{elec,avg}} + P_{\\mathrm{field,avg}} \\approx\nP_{\\mathrm{loss,avg}} + P_{\\mathrm{load,avg}} + P_{\\mathrm{buf,avg}}.\n\\]\n\n<strong>Not\u0103 important\u0103 de contabilizare:<\/strong> Descompunerea \u00een \\(P_{\\mathrm{elec,avg}}\\) \u0219i \\(P_{\\mathrm{field,avg}}\\) este o descompunere de contabilizare a balan\u021bei externe totale, nu o afirma\u021bie a dou\u0103 surse independente sau aditive. Reprezint\u0103 o parti\u021bionare metrologic\u0103 a schimbului de energie peste diferite tipuri de interfa\u021b\u0103 (prin fire vs. mediat\u0103 de limit\u0103), ambele contribuind la balan\u021ba extern\u0103 total\u0103 a sistemului deschis.\n\nM\u0103surarea direct\u0103 a integralei fluxului vectorului Poynting\n\n\\[\n\\oint \\langle \\mathbf{S} \\rangle \\cdot d\\mathbf{A}\n\\]\n\n\u00eentr-un sistem impulsiv de c\u00e2mp apropiat este o sarcin\u0103 metrologic\u0103 complex\u0103. Prin urmare, \\(P_{\\mathrm{field,avg}}\\) poate fi determinat ca termenul rezidual al balan\u021bei energetice, supus testelor de control obligatorii listate \u00een Sec\u021biunile 9.2.3\u20139.2.7.\n<h4>9.2.3 Controlul stoc\u0103rii ascunse de energie (&#8222;testul de stres energetic + inspec\u021bie negativ\u0103&#8221;)<\/h4>\nDeoarece Solicitantul nu dezv\u0103luie topologia circuitului, nomenclatura componentelor (BOM) sau detaliile de implementare schematice (know-how protejat), verificarea c\u0103 dispozitivul nu con\u021bine surse ascunse de energie stocat\u0103 (baterii, celule primare, celule de combustibil, supercondensatoare sau echivalente) trebuie efectuat\u0103 folosind un protocol \u00een dou\u0103 etape:\n\n<strong>Etapa A \u2014 Testul de stres energetic (cerin\u021b\u0103 de durat\u0103)<\/strong>\n\nDispozitivul trebuie s\u0103 opereze continuu sub o sarcin\u0103 definit\u0103 cu ie\u0219ire stabil\u0103 astfel \u00eenc\u00e2t energia livrat\u0103 \\(E_{\\mathrm{out}}\\) s\u0103 dep\u0103\u0219easc\u0103 o limit\u0103 superioar\u0103 conservatoare asupra oric\u0103rei energii interne stocate plauzibile care ar putea \u00eenc\u0103pea fizic \u00een volumul dispozitivului.\n\n\\[\nE_{\\mathrm{out}}=\\int_{0}^{T_{\\mathrm{test}}} P_{\\mathrm{load}}(t)\\,dt\n\\]\n\nDurata minim\u0103 de testare \\(T_{\\mathrm{test}}\\) trebuie aleas\u0103 astfel \u00eenc\u00e2t:\n\n\\[\nE_{\\mathrm{out}} \\ge K_{\\mathrm{safety}}\\cdot E_{\\mathrm{max,storage}}\n\\]\n\nunde:\n<ul>\n \t<li>\\(E_{\\mathrm{max,storage}}\\) este o estimare superioar\u0103 conservatoare a energiei maxime stocate fizic plauzibile \u00een volumul sigilat, bazat\u0103 pe limite stabilite de densitate energetic\u0103 volumetric\u0103 a tehnologiilor de stocare cunoscute (celule primare, celule re\u00eenc\u0103rcabile, supercondensatoare, cartu\u0219e de combustibil etc.).<\/li>\n \t<li>\\(K_{\\mathrm{safety}}\\) este un factor de siguran\u021b\u0103 (recomandat \\(K_{\\mathrm{safety}}\\ge 2\\), cu excep\u021bia cazului \u00een care laboratorul justific\u0103 o valoare mai mare).<\/li>\n<\/ul>\n<strong>Discre\u021bia laboratorului (clauz\u0103 anti-disput\u0103):<\/strong>\n\nLaboratorul verificator define\u0219te \u0219i documenteaz\u0103 \\(E_{\\mathrm{max,storage}}\\) folosind limite industriale conservatoare \u0219i public\u0103 baza ca parte a raportului de testare. Protocolul nu impune o singur\u0103 valoare de chimie pentru a evita disputele asupra maximelor de pia\u021b\u0103.\n\n<strong>Criteriu de succes (Etapa A):<\/strong>\n\nDispozitivul completeaz\u0103 \\(T_{\\mathrm{test}}\\) f\u0103r\u0103 o sc\u0103dere sus\u021binut\u0103 a puterii de sarcin\u0103 livrate care ar fi consistent\u0103 cu epuizarea unei surse interne de stocare, \u0219i cu cerin\u021bele de neutralitate a tamponului din Sec\u021biunea 9.\n\n<strong>Defini\u021bie de stabilitate:<\/strong> Laboratorul trebuie s\u0103 predefineasc\u0103 \u0219i s\u0103 documenteze o metric\u0103 de stabilitate obiectiv\u0103 pentru &#8222;nicio sc\u0103dere sus\u021binut\u0103&#8221; (de ex. band\u0103 de deriv\u0103 permis\u0103 \u0219i fereastr\u0103 minim\u0103 de durat\u0103), adecvat\u0103 pentru sarcina \u0219i incertitudinea de m\u0103surare selectate, \u0219i s\u0103 o aplice consistent pe parcursul testului.\n\n<em>Not\u0103:<\/em> \\(T_{\\mathrm{test}}\\) nu trebuie s\u0103 fie mai mic\u0103 dec\u00e2t constantele de timp termice \u0219i de tampon caracteristice ale sistemului \u0219i, \u00een orice caz, nu mai pu\u021bin de c\u00e2teva ore pentru niveluri de putere peste \\(P_{\\mathrm{min}}\\), cu excep\u021bia cazului \u00een care se justific\u0103 altfel.\n\n<strong>Etapa B \u2014 Inspec\u021bie negativ\u0103 (verificare post-test f\u0103r\u0103 divulgare IP)<\/strong>\n\nImediat dup\u0103 Etapa A, dispozitivul trebuie s\u0103 fie supus inspec\u021biei negative pentru a confirma absen\u021ba surselor de energie stocat\u0103 interzise.\n\n<strong>Metode de inspec\u021bie permise (alege\u021bi una):<\/strong>\n<ol>\n \t<li>Deschiderea asistat\u0103 a carcasei \u00een condi\u021bii controlate, sau<\/li>\n \t<li>Inspec\u021bie cu raze X \/ CT unde deschiderea nu este posibil\u0103 (de ex. turnat complet).<\/li>\n<\/ol>\n<strong>Limitarea scopului de inspec\u021bie (protec\u021bie IP):<\/strong>\n<ul>\n \t<li>Inspectorul este autorizat doar s\u0103 caute incluziuni interzise: baterii\/celule primare, cartu\u0219e de combustibil, stive electrochimice, b\u0103nci de supercondensatoare, module ascunse de putere sau alte subsisteme de energie stocat\u0103.<\/li>\n \t<li>Solicitantul poate elimina marcajele componentelor, poate folosi turnare opac\u0103 \u0219i poate aplica capace de protec\u021bie ansamblurilor PCB.<\/li>\n<\/ul>\n<strong>Ac\u021biuni interzise (anti-spionaj):<\/strong>\n<ul>\n \t<li>Nicio inginerie invers\u0103: nicio urm\u0103rire sau documentare a topologiei PCB, nicio m\u0103surare a valorilor R\/L\/C, nicio \u00eencercare de a dizolva sau \u00eendep\u0103rta compu\u0219ii de protec\u021bie, nicio solicitare de BOM sau scheme.<\/li>\n \t<li>Foto\/video este limitat la unghiuri suficiente pentru a confirma absen\u021ba stoc\u0103rii interzise de energie (documentare de ansamblu). Fotografia macro sau imagistica destinat\u0103 s\u0103 capteze rutarea PCB, detalii de plasare a componentelor sau geometria \u00eenf\u0103\u0219ur\u0103rilor este interzis\u0103.<\/li>\n<\/ul>\n<strong>Limit\u0103ri X-ray\/CT:<\/strong>\n<ul>\n \t<li>Interpretarea imaginilor este limitat\u0103 la identificarea structurilor caracteristice dispozitivelor de energie stocat\u0103 (geometrii de celule, rulouri\/stive de electrozi, volume de electrolit, cutii de supercondensatoare etc.).<\/li>\n \t<li>Analiza pentru reconstruirea straturilor PCB, rutarea traseelor sau construc\u021biei interne dincolo de scopul inspec\u021biei negative nu este permis\u0103.<\/li>\n<\/ul>\n<strong>Regul\u0103 de verdict:<\/strong>\n\nDac\u0103 Etapa A este satisf\u0103cut\u0103 \u0219i Etapa B nu dezv\u0103luie surse de energie stocat\u0103 interzise, ipoteza &#8222;baterie\/stocare ascuns\u0103&#8221; este considerat\u0103 falsificat\u0103 f\u0103r\u0103 divulgarea schemei interne sau nomenclaturii componentelor.\n<h4>9.2.4 Excluderea intr\u0103rilor de energie prin fire \u0219i parazite<\/h4>\n\u00cen modul de testare autonom, urm\u0103toarele condi\u021bii trebuie \u00eendeplinite:\n<ul>\n \t<li>intrarea prin fire prin portul (1) este suprimat\u0103 \u0219i m\u0103surat\u0103:\n\\[\nP_{\\mathrm{elec,avg}} \\le \\varepsilon_{\\mathrm{elec}};\n\\]<\/li>\n \t<li>nicio cale ascuns\u0103 sau necontabilizat\u0103 prin fire, inclusiv \u00eemp\u0103m\u00e2nt\u0103ri, ecran\u0103ri, linii de semnal \u0219i referin\u021b\u0103;<\/li>\n \t<li>absen\u021ba injec\u021biei active de putere wireless confirmat\u0103 prin monitorizare spectral\u0103 independent\u0103 pe un interval definit de laborator adecvat sitului \u0219i clasei dispozitivului, cu rezultate incluse \u00een raportul de testare.<\/li>\n<\/ul>\n<h4>9.2.5 Statusul termenului rezidual de energie \\(P_{\\mathrm{field,avg}}\\)<\/h4>\nDeterminarea \\(P_{\\mathrm{field,avg}}\\) ca termen rezidual al balan\u021bei energetice nu constituie dovad\u0103 a unei interac\u021biuni fizice noi.\n\n\\(P_{\\mathrm{field,avg}}\\) trebuie interpretat ca o contribu\u021bie de limit\u0103 a c\u0103rei natur\u0103 fizic\u0103 este \u00een afara scopului acestei specifica\u021bii inginere\u0219ti \u0219i este subiect de cercetare fundamental\u0103 separat\u0103.\n\nOrice energie care p\u0103r\u0103se\u0219te sistemul \u0219i nu este returnat\u0103 printr-o interfa\u021b\u0103 extern\u0103 definit\u0103 este atribuit\u0103 lui \\(P_{\\mathrm{loss,avg}}\\) \u0219i nu poate fi inclus\u0103 \u00een \\(P_{\\mathrm{field,avg}}\\).\n<h4>9.2.6 Clasificarea modurilor de operare<\/h4>\n<strong>Modul A (intrare prin fire):<\/strong>\n\n\\[\n\\left| P_{\\mathrm{elec,avg}} &#8211; \\left(P_{\\mathrm{loss,avg}} + P_{\\mathrm{load,avg}} + P_{\\mathrm{buf,avg}}\\right) \\right| \\le \\delta_{A}.\n\\]\n\n<strong>Modul B (operare mediat\u0103 de limit\u0103 clasificat\u0103 prin Portul (2)):<\/strong>\n\nToate urm\u0103toarele condi\u021bii trebuie satisf\u0103cute simultan:\n<ul>\n \t<li>\\(P_{\\mathrm{elec,avg}} \\le \\varepsilon_{\\mathrm{elec}}\\);<\/li>\n \t<li>\\(\\left|P_{\\mathrm{buf,avg}}\\right| \\le \\varepsilon_{\\mathrm{buf}}\\);<\/li>\n \t<li>\\(P_{\\mathrm{load,avg}} \\ge P_{\\mathrm{min}}\\);<\/li>\n \t<li>testele de control din Sec\u021biunile 9.2.3\u20139.2.7 finalizate cu succes.<\/li>\n<\/ul>\n\u00cen acest caz:\n\n\\[\nP_{\\mathrm{field,avg}} \\approx P_{\\mathrm{loss,avg}} + P_{\\mathrm{load,avg}}.\n\\]\n<h4>9.2.7 Valori numerice ale toleran\u021belor<\/h4>\n<table>\n<thead>\n<tr>\n<th>Parametru<\/th>\n<th>Valoare<\/th>\n<\/tr>\n<\/thead>\n<tbody>\n<tr>\n<td>\\(\\delta_{A}\\)<\/td>\n<td>5\u00a0%<\/td>\n<\/tr>\n<tr>\n<td>\\(\\varepsilon_{\\mathrm{elec}}\\)<\/td>\n<td>\u2264 1\u00a0% din \\(P_{\\mathrm{load,avg}}\\)<\/td>\n<\/tr>\n<tr>\n<td>\\(\\varepsilon_{\\mathrm{buf}}\\)<\/td>\n<td>\u2264 0.5\u00a0% din \\(E_{\\mathrm{buf,max}}\\) pe \\(T_{\\mathrm{test}}\\)<\/td>\n<\/tr>\n<tr>\n<td>\\(P_{\\mathrm{min}}\\)<\/td>\n<td>10\u00a0W<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<h3>9.3 Caracteristici rezonante<\/h3>\n<strong>Frecven\u021b\u0103 rezonant\u0103:<\/strong>\n\n\\[\nf_{0}^{\\mathrm{meas}} = \\arg\\max_{f} \\left| \\mathrm{FFT}\\{i_{2}(t)\\} \\right|\n\\]\n\nA\u0219teptare:\n\n\\[\n\\left| f_{0}^{\\mathrm{meas}} &#8211; \\frac{1}{2\\pi\\sqrt{L_{7}C_{8}}} \\right| &lt; 10\\%.\n\\]\n\n<strong>Factor Q:<\/strong>\n\n\\[\nQ_{\\mathrm{meas}} = \\frac{f_{0}^{\\mathrm{meas}}}{\\Delta f_{3\\mathrm{dB}}},\n\\]\n\nunde \\(\\Delta f_{3\\mathrm{dB}}\\) este l\u0103\u021bimea de band\u0103 la nivelul \u22123\u00a0dB.\n<h3>9.4 Verificarea sarcinii prin factorul de calitate<\/h3>\n\\(Q_{\\mathrm{tot}}\\) este m\u0103surat pentru diferite valori de rezisten\u021b\u0103 de sarcin\u0103 \\(R_{L}\\):\n\n\\[\n\\frac{1}{Q_{\\mathrm{tot}}} = \\frac{1}{Q_{0}} + \\frac{1}{Q_{L}},\n\\qquad\nQ_{L} = \\frac{\\omega_{0}U}{P_{\\mathrm{load}}}.\n\\]\n\nA\u0219teptare: sarcina se manifest\u0103 ca un canal suplimentar de extrac\u021bie a energiei din rezonator (Q \u00eenc\u0103rcat), nu ca o surs\u0103 extern\u0103. Graficele \\(Q_{\\mathrm{tot}}(R_{L})\\) \u0219i puterea necesar\u0103 \\(P_{\\mathrm{in,avg}}(R_{L})\\) ar trebui s\u0103 urmeze teoria liniar.\n<h3>9.5 Controlul influen\u021bei de mediu<\/h3>\n<ul>\n \t<li>Varia\u021bia presiunii (\u00een intervalul camerei controlate disponibile, de ex. 500\u20131000 mbar): m\u0103surarea \\(\\Delta f_{0}\\), \\(\\Delta U_{\\mathrm{br}}\\), \\(\\Delta P_{\\mathrm{loss}}\\).<\/li>\n \t<li>Varia\u021bia umidit\u0103\u021bii (20\u201390% RH): verificarea derivei tensiunii de str\u0103pungere.<\/li>\n \t<li>Test pe termen lung (\u2265 24 h): stabilitatea regimului sub sarcin\u0103 fix\u0103 \u0219i monitorizarea SoC a tamponului.<\/li>\n \t<li>Izolare de c\u00e2mpurile parazite: ecranare Faraday, verificarea absen\u021bei induc\u021biei din c\u00e2mpurile de re\u021bea.<\/li>\n<\/ul>\n<h3>9.6 Excluderea intr\u0103rilor suplimentare de energie<\/h3>\n<ul>\n \t<li>Vibra\u021bii mecanice \u2014 sistem pe izola\u021bie de vibra\u021bii; m\u0103surarea accelera\u021biei.<\/li>\n \t<li>Gradien\u021bi termici \u2014 controlul temperaturii \u00een \u00b12\u00a0\u00b0C; excluderea efectelor Seebeck \u0219i Peltier.<\/li>\n \t<li>Induc\u021bie electromagnetic\u0103 \u2014 ecranare; verificarea c\u00e2mpurilor reziduale cu sursa (1) deconectat\u0103.<\/li>\n \t<li>Monitorizarea st\u0103rii de \u00eenc\u0103rcare a tamponului \u2014 confirmarea c\u0103 \u00een stare sta\u021bionar\u0103\n\\[\nP_{\\mathrm{buf,avg}} = \\left\\langle \\frac{dE_{\\mathrm{buf}}}{dt} \\right\\rangle \\approx 0\n\\]\npe parcursul testului, confirm\u00e2nd absen\u021ba surselor ascunse de energie.<\/li>\n<\/ul>\n<h3>9.7 Gestionarea datelor de test<\/h3>\n<h4>9.7.1 Datele primare sunt \u00eenregistrate continuu cu urm\u0103toarea periodicitate:<\/h4>\n<ul>\n \t<li>\\(P_{\\mathrm{elec}}, P_{\\mathrm{load}}\\): cel pu\u021bin o dat\u0103 pe minut;<\/li>\n \t<li>\\(B_{50}, B_{150}\\): cel pu\u021bin o dat\u0103 pe secund\u0103;<\/li>\n \t<li>SoC al tamponului \u0219i temperaturi: cel pu\u021bin o dat\u0103 la 5 minute.<\/li>\n<\/ul>\n<h4>9.7.2 Datele sunt stocate \u00een format CSV cu metadate incluz\u00e2nd data, ora, identificarea echipamentului \u0219i informa\u021bii de calibrare.<\/h4>\n<h4>9.7.3 Perioada minim\u0103 de re\u021binere pentru datele primare este de 5 ani dup\u0103 finalizarea test\u0103rii.<\/h4>\n<h4>9.7.4 Copia de siguran\u021b\u0103 a datelor se efectueaz\u0103 cel pu\u021bin o dat\u0103 pe zi pe un mediu de stocare independent.<\/h4>\n<h2>10. Cerin\u021be de siguran\u021b\u0103 \u0219i limit\u0103ri<\/h2>\n<h3>10.1 Clasificarea echipamentului<\/h3>\nEchipament clasa I (\u00eemp\u0103m\u00e2ntare de protec\u021bie).\n<h3>10.2 Tensiunea maxim\u0103 de operare<\/h3>\nSpecificat\u0103 \u00een fi\u0219a tehnic\u0103 a configura\u021biei particulare.\n<h3>10.3 Gradul de poluare<\/h3>\nGradul 2 (mediu atmosferic normal).\n<h3>10.4 Controlul ozonului<\/h3>\nMonitorizarea continu\u0103 a concentra\u021biei de ozon \\( \\mathrm{O_3} \\) cu oprirea automat\u0103 a sistemului dac\u0103 concentra\u021bia dep\u0103\u0219e\u0219te \\(0.05\\ \\mathrm{mg\/m^3}\\).\n<h3>10.5 Compatibilitate electromagnetic\u0103<\/h3>\nTestare \u00een conformitate cu EN 55011, Clasa A (echipament industrial).\n<h3>10.6 Limit\u0103ri de aplicare<\/h3>\nEchipamentul este destinat exclusiv pentru utilizare industrial\u0103 \u00een condi\u021bii controlate. Nu este destinat aplica\u021biilor domestice sau casnice.\n<h2>Concluzie<\/h2>\nGeneratorul VENDOR este un sistem electrodinamic deschis al c\u0103rui comportament este descris \u00een cadrul electrodinamicii clasice \u0219i al teoriei sistemelor rezonante neliniare. Contabilizarea complet\u0103 a energiei sistemului include at\u00e2t termeni de schimb de energie extern\u0103 baza\u021bi pe porturi (prin fire), c\u00e2t \u0219i termeni cupla\u021bi de limit\u0103, unde &#8222;extern&#8221; se refer\u0103 la schimbul de energie peste limita sistemului, nu la o surs\u0103 extern\u0103 identificat\u0103.\n\n\u00cen func\u021bionarea \u00een stare sta\u021bionar\u0103, balan\u021ba puterilor medii are forma:\n\n\\[\nP_{\\mathrm{elec,avg}} + P_{\\mathrm{field,avg}} = P_{\\mathrm{loss,avg}} + P_{\\mathrm{load,avg}} + P_{\\mathrm{buf,avg}},\n\\]\n\ncu \\(P_{\\mathrm{buf,avg}} \\approx 0\\).\n\nAstfel, puterea util\u0103 livrat\u0103 la sarcin\u0103 este sus\u021binut\u0103 de balan\u021ba energetic\u0103 extern\u0103 total\u0103 a unui sistem electrodinamic deschis. \u00cen clasificarea Mod B, contribu\u021bia cuplat\u0103 de limit\u0103 asociat\u0103 cu Portul (2) este tratat\u0103 ca un termen rezidual necesar pentru a \u00eenchide balan\u021ba m\u0103surat\u0103 conform testelor de control obligatorii din Sec\u021biunea 9. Aceasta nu constituie o afirma\u021bie de &#8222;surs\u0103&#8221; discret\u0103, \u0219i niciun purt\u0103tor fizic nu este afirmat \u00een cadrul acestei specifica\u021bii.\n\nClasa de putere (wa\u021bi \/ sute de wa\u021bi \/ kilowa\u021bi) \u00een scopul acestui document este un parametru supus verific\u0103rii conform Sec\u021biunii 9; orice valori numerice sunt considerate afirma\u021bii doar dup\u0103 un audit energetic independent \u00een Modurile A\/B cu finalizarea cu succes a testelor de control specificate \u00een Sec\u021biunea 9.2.\n<h2>Referin\u021be<\/h2>\n<ul>\n \t<li>Peretyachenko V. G., Krishevich O. K.\n<a href=\"https:\/\/patentscope.wipo.int\/search\/en\/detail.jsf?docId=WO2024209235\" target=\"_blank\" rel=\"noopener noreferrer\">\nGenerator for Electrical Energy Production\n<\/a>.\nPatent WO2024209235A1, depus apr. 2024.<\/li>\n \t<li>Dorf R. C., Bishop R. H.\n<a href=\"https:\/\/www.pearson.com\/en-us\/subject-catalog\/p\/modern-control-systems\/P200000003295\" target=\"_blank\" rel=\"noopener noreferrer\">\nModern Control Systems\n<\/a>.\nEd. 13. Pearson, 2017. \u2014 (dinamic\u0103 neliniar\u0103, feedback pozitiv, stabilitate)<\/li>\n \t<li>Khalil H. K.\n<a href=\"https:\/\/www.pearson.com\/en-us\/subject-catalog\/p\/nonlinear-control\/P200000003509\" target=\"_blank\" rel=\"noopener noreferrer\">\nNonlinear Control\n<\/a>.\nEd. 4. Pearson, 2021. \u2014 (cicluri limit\u0103, bifurca\u021bie, metode energetice)<\/li>\n \t<li>Lieberman M. A., Lichtenberg A. J.\n<a href=\"https:\/\/onlinelibrary.wiley.com\/doi\/book\/10.1002\/0471724254\" target=\"_blank\" rel=\"noopener noreferrer\">\nPrinciples of Plasma Discharges and Materials Processing\n<\/a>.\nEd. 2. Wiley, 2005. \u2014 (corona, arc, fizica plasmei)<\/li>\n \t<li>Raizer Y. P.\n<a href=\"https:\/\/link.springer.com\/book\/10.1007\/978-3-642-61247-3\" target=\"_blank\" rel=\"noopener noreferrer\">\nGas Discharge Physics\n<\/a>.\nSpringer, 1991. \u2014 (streamer, str\u0103pungere, desc\u0103rc\u0103ri auto-sus\u021binute)<\/li>\n \t<li>Pozar D. M.\n<a href=\"https:\/\/www.wiley.com\/en-us\/Microwave+Engineering%2C+4th+Edition-p-9780470631553\" target=\"_blank\" rel=\"noopener noreferrer\">\nMicrowave Engineering\n<\/a>.\nEd. 4. Wiley, 2012. \u2014 Capitolul 6 (rezonatoare, factor Q, l\u0103\u021bime de band\u0103, Q \u00eenc\u0103rcat)<\/li>\n \t<li>Jackson J. D.\n<a href=\"https:\/\/www.wiley.com\/en-us\/Classical+Electrodynamics%2C+3rd+Edition-p-9780471309321\" target=\"_blank\" rel=\"noopener noreferrer\">\nClassical Electrodynamics\n<\/a>.\nEd. 3. Wiley, 1998. \u2014 (ecua\u021bii Maxwell, energie, vector Poynting)<\/li>\n<\/ul>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t","protected":false},"excerpt":{"rendered":"<p>VENDOR este descris ca un sistem electrodinamic deschis, oper\u00e2nd strict \u00een cadrul legilor fizicii clasice.Mediul gazos este tratat ca mediu de cuplare \u0219i condi\u021bie de frontier\u0103, nu ca surs\u0103 de energie.Dezvoltarea urmeaz\u0103 o abordare bazat\u0103 pe TRL \u0219i validare prioritar\u0103; \u00een aceast\u0103 etap\u0103 nu sunt publicate afirma\u021bii de performan\u021b\u0103.Dezv\u0103luirea detaliilor de implementare este condi\u021bionat\u0103 de [&hellip;]<\/p>\n","protected":false},"author":1,"featured_media":18397,"comment_status":"closed","ping_status":"open","sticky":false,"template":"elementor_header_footer","format":"standard","meta":{"footnotes":""},"categories":[270,247,256,166,196],"tags":[945,848,946,968,976,975],"class_list":["post-12122","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-science-ro","category-science","category-science-zh-hans","category-technology-zh-hans","category-technology-ro","tag-bilant-energetic","tag-electrodinamica","tag-metrologie","tag-resonant-systems","tag-sisteme-rezonante","tag-verificare"],"_links":{"self":[{"href":"https:\/\/vendor.energy\/ro\/wp-json\/wp\/v2\/posts\/12122","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/vendor.energy\/ro\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/vendor.energy\/ro\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/vendor.energy\/ro\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/vendor.energy\/ro\/wp-json\/wp\/v2\/comments?post=12122"}],"version-history":[{"count":34,"href":"https:\/\/vendor.energy\/ro\/wp-json\/wp\/v2\/posts\/12122\/revisions"}],"predecessor-version":[{"id":15366,"href":"https:\/\/vendor.energy\/ro\/wp-json\/wp\/v2\/posts\/12122\/revisions\/15366"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/vendor.energy\/ro\/wp-json\/wp\/v2\/media\/18397"}],"wp:attachment":[{"href":"https:\/\/vendor.energy\/ro\/wp-json\/wp\/v2\/media?parent=12122"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/vendor.energy\/ro\/wp-json\/wp\/v2\/categories?post=12122"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/vendor.energy\/ro\/wp-json\/wp\/v2\/tags?post=12122"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}