{"id":15700,"date":"2026-01-07T01:23:57","date_gmt":"2026-01-06T22:23:57","guid":{"rendered":"https:\/\/vendor.energy\/articles\/regime-electrodynamics-vs-linear-models\/"},"modified":"2026-02-14T21:24:57","modified_gmt":"2026-02-14T18:24:57","slug":"regim-electrodinamic-vs-modele-liniare","status":"publish","type":"post","link":"https:\/\/vendor.energy\/ro\/articles\/regim-electrodinamic-vs-modele-liniare\/","title":{"rendered":"Sisteme electrodinamice bazate pe regim ca alternativ\u0103 la modelele energetice liniare: fundamentul \u0219tiin\u021bific al arhitecturii VENDOR.Energy\u2122"},"content":{"rendered":"\t\t<div data-elementor-type=\"wp-post\" data-elementor-id=\"15700\" class=\"elementor elementor-15700 elementor-15672\" 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\">Sisteme electrodinamice bazate pe regim ca alternativ\u0103 la modelele energetice liniare: fundamentul \u0219tiin\u021bific al arhitecturii VENDOR.Energy\u2122<\/h2><\/div>\n\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 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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\n<hr \/>\n\n<h2>Rezumat<\/h2>\nAcest articol prezint\u0103 un cadru riguros de bilan\u021b energetic pentru arhitectura VENDOR.Energy\u2122 \u2014 o clas\u0103 de sisteme electrodinamice neliniare cu separare func\u021bional\u0103 \u00eentre formarea regimului, compensarea pierderilor \u0219i extragerea puterii utile.\n\nObiectivul central este formalizarea rolului rut\u0103rii interne a puterii prin bucl\u0103 de feedback \u0219i al tampon\u0103rii \u00een men\u021binerea regimului de operare, \u00een cadrul unei contabiliz\u0103ri conforme cu primul principiu al termodinamicii, consistent\u0103 cu frontiera sistemului. Concret, clarific\u0103m modul \u00een care sistemul direc\u021bioneaz\u0103 o parte din puterea bus-ului DC intern al dispozitivului \u00eenapoi c\u0103tre nucleul activ (Circuitul\u00a0A). Bus-ul DC este un nod de distribu\u021bie intern alimentat de intrarea extern\u0103 \u0219i, unde este cazul, de putere intern\u0103 condi\u021bionat\u0103 din etapa de extrac\u021bie \u0219i\/sau din tampon; orice astfel de \u201eputere intern\u0103 condi\u021bionat\u0103&#8221; desemneaz\u0103 conversia \u0219i redistribuirea intern\u0103 a energiei deja contabilizate \u00een cadrul Frontierei Dispozitivului, nu un termen de intrare independent suplimentar. Prin urmare, calea de feedback este strict un mecanism intern de alocare a puterii \u00een cadrul Frontierei Dispozitivului. Demonstr\u0103m de ce aceast\u0103 arhitectur\u0103 \u00een bucl\u0103 \u00eenchis\u0103 este pe deplin compatibil\u0103 cu legile de conservare atunci c\u00e2nd frontiera sistemului este corect definit\u0103.\n\nLucrarea arat\u0103 c\u0103 concluziile aparente de \u201eeficien\u021b\u0103 &gt;\u00a0100%&#8221; apar exclusiv din erori de definire a frontierei sau incompletitudine a m\u0103sur\u0103torilor, nu din vreo \u00eenc\u0103lcare a fizicii.\n\n<strong>Cuvinte cheie:<\/strong> sisteme bazate pe regim, <a href=\"https:\/\/vendor.energy\/ro\/articles\/stabilizarea-regimurilor-electrodinamice\/\">electrodinamic\u0103 neliniar\u0103<\/a>, rezonan\u021b\u0103 pulsat\u0103, desc\u0103rcare \u00een gaz, bilan\u021b energetic, sisteme deschise, arhitectur\u0103 cu feedback.\n\n<hr \/>\n\n<h2>1. Problema: De unde vine puterea de sus\u021binere?<\/h2>\n<h3>1.1 De ce apare aceast\u0103 \u00eentrebare<\/h3>\n\u00cen arhitectura VENDOR, nucleul activ (Circuitul\u00a0A) func\u021bioneaz\u0103 \u00eentr-un regim electrodinamic neliniar cu circula\u021bie intern\u0103 ridicat\u0103 a energiei. Acest regim necesit\u0103 compensarea continu\u0103 a pierderilor ireversibile \u2014 ohmice, dielectrice, radiative \u0219i de desc\u0103rcare \u2014 pentru a r\u0103m\u00e2ne stabil.\n\nUn observator care examineaz\u0103 Circuitul\u00a0A izolat vede: o putere mic\u0103 de mentenan\u021b\u0103 care sus\u021bine un regim ce livreaz\u0103 o putere mult mai mare circuitului de extrac\u021bie. Reac\u021bia natural\u0103 este: <em>de unde vine energia lips\u0103?<\/em>\n\nAceast\u0103 confuzie are o origine precis\u0103: <strong>observatorul traseaz\u0103 frontiera sistemului \u00een jurul subsistemului gre\u0219it<\/strong>.\n<h3>1.2 R\u0103spunsul \u00eentr-un paragraf<\/h3>\nSistemul VENDOR func\u021bioneaz\u0103 ca o <strong>arhitectur\u0103 \u00een bucl\u0103 \u00eenchis\u0103<\/strong> cu dou\u0103 circuite separate func\u021bional:\n<ul>\n \t<li><strong>Circuitul A<\/strong> (Nucleul Activ) formeaz\u0103 \u0219i men\u021bine regimul electrodinamic neliniar.<\/li>\n \t<li><strong>Circuitul B<\/strong> (Extrac\u021bie Liniar\u0103) extrage putere din Circuitul\u00a0A prin induc\u021bie electromagnetic\u0103 clasic\u0103.<\/li>\n<\/ul>\nO frac\u021biune din puterea bus-ului DC intern al dispozitivului este alocat\u0103 \u00eenapoi prin bus-ul reglat c\u0103tre Circuitul\u00a0A ca putere de mentenan\u021b\u0103. Bus-ul DC este un nod de distribu\u021bie intern care poate fi alimentat de intrarea extern\u0103 \u0219i\/sau de c\u0103i interne de putere condi\u021bionat\u0103 (inclusiv etapa de extrac\u021bie \u0219i tamponul); aici, \u201eputere intern\u0103 condi\u021bionat\u0103&#8221; se refer\u0103 la redistribuirea intern\u0103 a energiei aflate deja \u00een cadrul Frontierei Dispozitivului, nu la o a doua surs\u0103 extern\u0103. Prin urmare, feedback-ul r\u0103m\u00e2ne o alocare intern\u0103 \u00een cadrul Frontierei Dispozitivului. \u00cen func\u021bionare sta\u021bionar\u0103, bus-ul DC este sus\u021binut \u00een cele din urm\u0103 de \\(P_{\\text{in,ext}}\\), cu abateri tranzitorii guvernate exclusiv de \\(\\Delta E_{\\text{stored}}\\). <strong>Bateria tampon cu BMS<\/strong> regleaz\u0103 aceast\u0103 alocare, netezind tranzitoriile \u0219i protej\u00e2nd stabilitatea regimului.\n\nEsen\u021bial: calea de feedback nu \u00eenlocuie\u0219te intrarea extern\u0103. La Frontiera Dispozitivului, orice func\u021bionare sus\u021binut\u0103 cu \\(P_{\\text{load}} \\neq 0\\) necesit\u0103 o intrare extern\u0103 medie \u00een timp \\(P_{\\text{in,ext}} \\neq 0\\), cu excep\u021bia intervalelor \u00een care energia stocat\u0103 se epuizeaz\u0103. Bucla de feedback este un mecanism de rutare a puterii care aloc\u0103 o parte din puterea bus-ului DC \u00eenapoi c\u0103tre nucleu; energia net\u0103 medie \u00een timp este contabilizat\u0103 prin \\(P_{\\text{in,ext}}\\) (cu abateri pe termen scurt guvernate de \\(\\Delta E_{\\text{stored}}\\)), \u00een timp ce alimentarea extern\u0103 acoper\u0103 bilan\u021bul net al sarcinii + pierderilor ireversibile + varia\u021biei stoc\u0103rii. \u00cen medie temporal\u0103, orice energie net\u0103 livrat\u0103 sarcinii \u0219i disipat\u0103 ca pierderi trebuie furnizat\u0103 de \\(P_{\\text{in,ext}}\\); recircularea intern\u0103 poate doar redistribui energia \u0219i temporar o \u00eemprumuta\/returna prin \\(\\Delta E_{\\text{stored}}\\).\n\nDin perspectiva <strong>frontierei complete a dispozitivului<\/strong>, puterea de feedback este o redistribuire intern\u0103 \u2014 nu o surs\u0103 nou\u0103 de energie. Singura intrare real\u0103 este puterea electric\u0103 extern\u0103 care traverseaz\u0103 frontiera dispozitivului. Singurele ie\u0219iri sunt puterea util\u0103 de sarcin\u0103 \u0219i pierderile ireversibile.\n\n<hr \/>\n\n<h2>2. Arhitectura sistemului \u0219i fluxul de energie<\/h2>\n<h3>2.1 Cele dou\u0103 circuite<\/h3>\n<strong>Circuitul A \u2014 Formarea regimului (Nucleul Activ)<\/strong>\n\nCircuitul\u00a0A este o structur\u0103 rezonant\u0103 neliniar\u0103 bazat\u0103 pe o combina\u021bie LC efectiv\u0103 cu desc\u0103rcare \u00een gaz ca element neliniar controlat. Frecven\u021ba de rezonan\u021b\u0103 efectiv\u0103 este:\n\n\\[\\omega_0 = \\frac{1}{\\sqrt{LC}}\\]\n\n\u00cen regimuri neliniare, \\(\\omega_0\\) poate depinde de amplitudine, conductivitate \u0219i parametrii de desc\u0103rcare; valoarea de mai sus este \u00een\u021beleas\u0103 ca frecven\u021ba de rezonan\u021b\u0103 echivalent\u0103 pentru punctul de operare ales.\n\nPentru un model echivalent de pierderi ales, un factor de calitate efectiv \\(Q_{\\text{eff}}\\) este definit experimental. Pentru o reprezentare RLC serie, \\(Q_{\\text{series}} = \\omega_0 L \/ R_s\\); pentru o reprezentare paralel\u0103, \\(Q_{\\text{parallel}} = \\omega_0 R_p C\\). \u00cen aceast\u0103 lucrare folosim \\(Q_{\\text{eff}}\\) ca factor de calitate al regimului m\u0103surat la frontiera aleas\u0103.\n\nDesc\u0103rcarea furnizeaz\u0103 conductivitate neliniar\u0103 dinamic\u0103 \\(\\sigma(E,t)\\), permi\u021b\u00e2nd sistemului s\u0103 ating\u0103 \u0219i s\u0103 sus\u021bin\u0103 un regim stabil de ciclu limit\u0103. Acest regim men\u021bine o circula\u021bie intern\u0103 ridicat\u0103 a energiei cu o putere de mentenan\u021b\u0103 comparativ mic\u0103 \u2014 o consecin\u021b\u0103 direct\u0103 a unui factor de calitate efectiv \\(Q_{\\text{eff}}\\) ridicat.\n\n<strong>Fizica esen\u021bial\u0103:<\/strong> Un \\(Q_{\\text{eff}}\\) ridicat \u00eenseamn\u0103 c\u0103 energia penduleaz\u0103 \u00eentre stocarea electric\u0103 \u0219i magnetic\u0103 de multe ori \u00eenainte de a fi disipat\u0103. Puterea de mentenan\u021b\u0103 trebuie s\u0103 compenseze doar frac\u021biunea pierdut\u0103 per ciclu, nu s\u0103 recreeze \u00eentreaga energie circulant\u0103.\n\n\u00cen aceast\u0103 lucrare, \u201ecircula\u021bia&#8221; denot\u0103 schimbul intern de energie \u0219i stocarea \u00een cadrul regimului (c\u00e2mpuri\/curen\u021bi), nu un aflux suplimentar de putere extern\u0103.\n\n<strong>Circuitul B \u2014 Extrac\u021bie liniar\u0103 a puterii<\/strong>\n\nCircuitul\u00a0B func\u021bioneaz\u0103 pe baza induc\u021biei clasice Faraday:\n\n\\[\\mathcal{E} = -\\frac{d\\Phi_B}{dt}\\]\n\nFluxul magnetic variabil \u00een timp generat de regimul Circuitului\u00a0A induce o FEM \u00eentr-o \u00eenf\u0103\u0219urare de extrac\u021bie. Aceast\u0103 FEM este redresat\u0103, filtrat\u0103 \u0219i convertit\u0103 \u00een putere util\u0103 DC sau AC.\n\n<strong>Legea lui Lenz se aplic\u0103 integral:<\/strong> extrac\u021bia reduce factorul de calitate sub sarcin\u0103:\n\n\\[\\frac{1}{Q_{\\text{eff,loaded}}} = \\frac{1}{Q_{\\text{core}}} + \\frac{1}{Q_L}\\]\n\nAceast\u0103 rela\u021bie aditiv\u0103 este utilizat\u0103 aici ca model echivalent de parti\u021bie a pierderilor la o defini\u021bie fix\u0103 a \\(E_{\\text{stored}}\\); \u00een practic\u0103, \\(Q_{\\text{eff,loaded}}\\) este identificat din m\u0103sur\u0103tori \u00een cadrul regimului de operare dat.\n\nExtrac\u021bie crescut\u0103 \u2192 pierderi efective crescute \u2192 cerin\u021b\u0103 crescut\u0103 de putere de mentenan\u021b\u0103.\n<h3>2.2 Bucla de feedback<\/h3>\nCaracteristica arhitectural\u0103 critic\u0103 este <strong>calea de feedback<\/strong>:\n<pre class=\"ascii-diagram\">\u250c\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2510\n\u2502          FRONTIERA DISPOZITIVULUI            \u2502\n\u2502                                              \u2502\nP_in,ext \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u25ba\u2502  \u250c\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2510    induc\u021bie       \u250c\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2510  \u2502\n(pornire +       \u2502  \u2502Circuitul \u2502 \u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u25ba   \u2502Circuitul \u2502  \u2502\n intrare ext.)   \u2502  \u2502    A     \u2502   legea Faraday   \u2502    B     \u2502  \u2502\n                 \u2502  \u2502(Nucleu   \u2502 \u25c4\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500   \u2502(Extrac\u021bie\u2502  \u2502\u2500\u2500\u25ba P_load\n                 \u2502  \u2502 Activ)   \u2502  feedback prin    \u2502 Liniar\u0103) \u2502  \u2502\n                 \u2502  \u2514\u2500\u2500\u2500\u2500\u252c\u2500\u2500\u2500\u2500\u2500\u2518  bus DC reglat    \u2514\u2500\u2500\u2500\u2500\u2500\u252c\u2500\u2500\u2500\u2500\u2518  \u2502\n                 \u2502       \u2502              \u25b2                \u2502       \u2502\n                 \u2502       \u2502              \u2502                \u2502       \u2502\n                 \u2502       \u2502         \u250c\u2500\u2500\u2500\u2500\u2534\u2500\u2500\u2500\u2500\u2500\u2510          \u2502       \u2502\n                 \u2502       \u2514\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u25ba\u2502  Tampon  \u2502\u25c4\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2518       \u2502\n                 \u2502                 \u2502  + BMS   \u2502                  \u2502\n                 \u2502                 \u2514\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2518                  \u2502\n\u2502                                             \u2502\n\u2514\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2518\n                          \u25bc\n                      B_total (c\u0103ldur\u0103,\n                      radia\u021bie etc.)\n<\/pre>\n<strong>Ce se \u00eent\u00e2mpl\u0103 pas cu pas:<\/strong>\n<ol>\n \t<li><strong>Pornire:<\/strong> Puterea extern\u0103 \\(P_{\\text{in,ext}}\\) aprinde regimul \u00een Circuitul\u00a0A \u0219i \u00eencarc\u0103 tamponul.<\/li>\n \t<li><strong>Formarea regimului:<\/strong> Circuitul\u00a0A atinge un regim neliniar stabil (ciclu limit\u0103) cu circula\u021bie intern\u0103 ridicat\u0103 a energiei.<\/li>\n \t<li><strong>Extrac\u021bie:<\/strong> Circuitul\u00a0B extrage putere din regimul Circuitului\u00a0A prin induc\u021bie.<\/li>\n \t<li><strong>Feedback:<\/strong> O parte din puterea intern\u0103 a dispozitivului disponibil\u0103 pe bus-ul DC reglat este alocat\u0103 \u00eenapoi ca putere de mentenan\u021b\u0103 c\u0103tre Circuitul\u00a0A. Bus-ul DC poate fi sus\u021binut de intrarea extern\u0103 \u0219i\/sau de c\u0103i interne condi\u021bionate (inclusiv etapa de extrac\u021bie \u0219i tamponul), astfel \u00eenc\u00e2t acest feedback r\u0103m\u00e2ne o alocare intern\u0103 \u00een cadrul Frontierei Dispozitivului; bilan\u021bul la nivel de dispozitiv r\u0103m\u00e2ne determinat de intrarea extern\u0103. \u00cen func\u021bionare sta\u021bionar\u0103, bus-ul DC este sus\u021binut \u00een cele din urm\u0103 de \\(P_{\\text{in,ext}}\\), cu abateri tranzitorii guvernate exclusiv de \\(\\Delta E_{\\text{stored}}\\).<\/li>\n \t<li><strong>Reglare:<\/strong> Tamponul + BMS neteze\u0219te acest feedback, compens\u00e2nd tranzitoriile \u0219i varia\u021biile de sarcin\u0103.<\/li>\n \t<li><strong>Func\u021bionare sta\u021bionar\u0103:<\/strong> Sistemul opereaz\u0103 ca o bucl\u0103 reglat\u0103 intern: calea intern\u0103 de feedback direc\u021bioneaz\u0103 o parte din puterea bus-ului DC pentru men\u021binerea regimului, \u00een timp ce intrarea extern\u0103 la Frontiera Dispozitivului furnizeaz\u0103 energia net\u0103 necesar\u0103 pentru (pierderi + putere livrat\u0103 sarcinii + varia\u021bia stoc\u0103rii). Feedback-ul este un mecanism de rutare a puterii, nu o surs\u0103 independent\u0103 de energie.<\/li>\n<\/ol>\n<h3>2.3 Rolul tamponului \u0219i al BMS<\/h3>\nBateria tampon <strong>nu este o surs\u0103 ascuns\u0103 de energie<\/strong>. Ea realizeaz\u0103:\n<ul>\n \t<li><strong>Netezirea tranzitoriilor:<\/strong> absoarbe v\u00e2rfurile de sarcin\u0103 \u0219i compenseaz\u0103 perturba\u021biile de regim<\/li>\n \t<li><strong>Stabilizarea bus-ului DC:<\/strong> previne sc\u0103derile de tensiune care ar putea provoca colapsul regimului neliniar<\/li>\n \t<li><strong>Stocarea energiei de pornire:<\/strong> furnizeaz\u0103 puterea ini\u021bial\u0103 de aprindere \u00eenainte ca bucla de feedback s\u0103 fie stabilit\u0103<\/li>\n \t<li><strong>Inteligen\u021ba BMS:<\/strong> gestioneaz\u0103 ciclurile de \u00eenc\u0103rcare\/desc\u0103rcare, protejeaz\u0103 \u00eempotriva supraextrac\u021biei \u0219i controleaz\u0103 secven\u021bele de pornire\/oprire lin\u0103<\/li>\n<\/ul>\n\u00cen stare sta\u021bionar\u0103, varia\u021bia net\u0103 a energiei tamponului se mediaz\u0103 la zero. Orice energie extras\u0103 \u00een timpul tranzitoriilor este re\u00eenc\u0103rcat\u0103 de pe bus-ul DC; energia net\u0103 medie \u00een timp este contabilizat\u0103 prin \\(P_{\\text{in,ext}}\\) (cu abateri pe termen scurt guvernate de \\(\\Delta E_{\\text{stored}}\\)).\n\n<hr \/>\n\n<h2>3. Bilan\u021bul energetic: Frontiere corecte vs. incorecte<\/h2>\n<h3>3.1 Frontiera complet\u0103 a dispozitivului (corect\u0103)<\/h3>\nPentru frontiera dispozitivului care cuprinde toate componentele (Circuitul\u00a0A + Circuitul\u00a0B + Tampon + Control), bilan\u021bul energetic conform primului principiu este:\n\n\\[\\frac{dE_{\\text{total}}}{dt} = P_{\\text{in,ext}} &#8211; B_{\\text{total}}(t) &#8211; P_{\\text{load}}\\]\n\nunde:\n<ul>\n \t<li>\\(P_{\\text{in,ext}}\\) \u2014 puterea electric\u0103 extern\u0103 total\u0103 care traverseaz\u0103 frontiera dispozitivului<\/li>\n \t<li>\\(B_{\\text{total}}(t)\\) \u2014 toate pierderile ireversibile (ohmice, dielectrice, radia\u021bie, chimie de desc\u0103rcare)<\/li>\n \t<li>\\(P_{\\text{load}}\\) \u2014 puterea util\u0103 de ie\u0219ire c\u0103tre sarcina extern\u0103<\/li>\n \t<li>\\(E_{\\text{total}}\\) \u2014 energia total\u0103 stocat\u0103 \u00een interiorul frontierei (c\u00e2mpuri + tampon + stocare intern\u0103)<\/li>\n<\/ul>\nAceast\u0103 ecua\u021bie presupune c\u0103 \\(P_{\\text{in,ext}}\\), \\(B_{\\text{total}}\\) \u0219i \\(P_{\\text{load}}\\) includ toate fluxurile de energie care traverseaz\u0103 Frontiera Dispozitivului (inclusiv orice transport de energie prin radia\u021bie EM, acustic\u0103 sau chimic\u0103).\n\n\u00cen stare sta\u021bionar\u0103 (\\(dE_{\\text{total}}\/dt = 0\\), medie temporal\u0103):\n\n\\[\\boxed{P_{\\text{in,ext}} = B_{\\text{total}} + P_{\\text{load}}}\\]\n\nTo\u021bi termenii sunt \u00een\u021bele\u0219i ca puteri mediate \u00een timp pe o fereastr\u0103 lung\u0103 comparativ cu perioada regimului. Pentru ferestre de mediere finite, se aplic\u0103 forma mai general\u0103 \\(P_{\\text{in,ext}} = \\langle B_{\\text{total}} \\rangle + P_{\\text{load}} + dE_{\\text{total}}\/dt\\); \u00een stare strict sta\u021bionar\u0103, \\(dE_{\\text{total}}\/dt = 0\\).\n\n\u00cen consecin\u021b\u0103, dac\u0103 \\(P_{\\text{in,ext}} = 0\\) pe o fereastr\u0103 de mediere finit\u0103, atunci o \\(P_{\\text{load}}\\) sus\u021binut\u0103 diferit\u0103 de zero este imposibil\u0103 f\u0103r\u0103 epuizarea energiei stocate; orice astfel de epuizare ar ap\u0103rea ca \\(\\Delta E_{\\text{stored}} &lt; 0\\).\n\nAici, \\(\\Delta E_{\\text{stored}}\\) se refer\u0103 la varia\u021bia net\u0103 a energiei stocate \u00een interiorul Frontierei Dispozitivului (c\u00e2mpuri + tampon + stocare intern\u0103), adic\u0103 \\(\\Delta E_{\\text{stored}} = E_{\\text{total}}(t_2) &#8211; E_{\\text{total}}(t_1)\\).\n\n<strong>Puterea de feedback nu apare \u00een aceast\u0103 ecua\u021bie<\/strong> deoarece este \u00een \u00eentregime intern\u0103 frontierei dispozitivului. Este energie redistribuit\u0103, nu energie creat\u0103.\n\nEficien\u021ba corect\u0103:\n\n\\[\\eta_{\\text{true}} = \\frac{P_{\\text{load}}}{P_{\\text{in,ext}}} \\leq 1\\]\n<h3>3.2 Frontiera doar pe nucleu (sursa confuziei)<\/h3>\nDac\u0103 frontiera este trasat\u0103 doar \u00een jurul Circuitului\u00a0A, atunci puterea de feedback din Circuitul\u00a0B apare ca o intrare \u00een nucleu:\n\n\\[P_{\\text{in,A}}(t) = P_{\\text{fb}}(t) + P_{\\text{aux}}(t)\\]\n\nunde \\(P_{\\text{aux}}(t)\\) reprezint\u0103 orice putere extern\u0103 sau auxiliar\u0103 livrat\u0103 Circuitului\u00a0A \u00een afara c\u0103ii de feedback (inclusiv aprinderea\/pornirea ca caz special; \\(P_{\\text{aux}}(t) = 0\\) pentru \\(t &gt; t_0\\) \u00een func\u021bionare sta\u021bionar\u0103).\n\nUn observator care m\u0103soar\u0103 doar \\(P_{\\text{fb}}\\) ca \u201eintrare&#8221; \u0219i o compar\u0103 cu \\(P_{\\text{load}}\\) calculeaz\u0103:\n\n\\[\\eta_{\\text{apparent}} = \\frac{P_{\\text{load}}}{P_{\\text{fb}}} \\gg 100\\%\\]\n\n<strong>Aceasta nu este o \u00eenc\u0103lcare a fizicii \u2014 este o eroare de frontier\u0103.<\/strong> Observatorul a:\n<ul>\n \t<li>Considerat doar canalul de mentenan\u021b\u0103 ca \u201eintrare&#8221;<\/li>\n \t<li>Ignorat faptul c\u0103 \\(P_{\\text{fb}}\\) provine din Circuitul\u00a0B, care extrage din acela\u0219i regim<\/li>\n \t<li>Ignorat varia\u021biile energiei stocate \u0219i pierderile totale ale sistemului<\/li>\n<\/ul>\n<h3>3.3 Exemplu numeric<\/h3>\n<strong>M\u0103sur\u0103tori la frontiera dispozitivului (stare sta\u021bionar\u0103, \\(dE_{\\text{stored}}\/dt = 0\\) medie temporal\u0103):<\/strong>\n<table>\n<thead>\n<tr>\n<th scope=\"col\">M\u0103rime<\/th>\n<th scope=\"col\">Valoare<\/th>\n<\/tr>\n<\/thead>\n<tbody>\n<tr>\n<td>Intrare extern\u0103 total\u0103 \\(P_{\\text{in,ext}}\\)<\/td>\n<td>2000 W<\/td>\n<\/tr>\n<tr>\n<td>Pierderi ireversibile totale \\(B_{\\text{total}}\\)<\/td>\n<td>1600 W<\/td>\n<\/tr>\n<tr>\n<td>Putere util\u0103 de ie\u0219ire \\(P_{\\text{load}}\\)<\/td>\n<td>400 W<\/td>\n<\/tr>\n<tr>\n<td>Varia\u021bia total\u0103 a energiei stocate \\(dE_{\\text{total}}\/dt\\)<\/td>\n<td>0 W<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<strong>Verificarea bilan\u021bului:<\/strong>\n\n\\[2000 = 400 + 1600 + 0 \\quad \\checkmark\\]\n\n<strong>Eficien\u021ba corect\u0103:<\/strong>\n\n\\[\\eta_{\\text{true}} = \\frac{400}{2000} = 20\\%\\]\n\n<strong>Eficien\u021ba \u201eaparent\u0103&#8221; incorect\u0103<\/strong> (m\u0103sur\u00e2nd doar canalul de feedback):\nDac\u0103 \\(P_{\\text{fb}} = 200\\) W:\n\n\\[\\eta_{\\text{apparent}} = \\frac{400}{200} = 200\\% \\quad \\text{\u2190 eroare de frontier\u0103, nu \u00eenc\u0103lcare a fizicii}\\]\n\n<hr \/>\n\n<h2>4. De ce un \\(Q_{\\text{eff}}\\) ridicat face arhitectura cu feedback viabil\u0103<\/h2>\n<h3>4.1 Factorul de calitate \u0219i puterea de mentenan\u021b\u0103<\/h3>\nFactorul de calitate efectiv \\(Q_{\\text{eff}}\\) determin\u0103 raportul dintre energia stocat\u0103 \u0219i energia pierdut\u0103 per ciclu:\n\n\\[Q_{\\text{eff}} \\equiv 2\\pi \\, \\frac{\\langle E_{\\text{stored}} \\rangle}{\\Delta E_{\\text{pierdere per ciclu}}}\\]\n\nPrefactorul numeric depinde de faptul dac\u0103 defini\u021bia este exprimat\u0103 \u00een termeni de dec\u0103dere a energiei sau a amplitudinii; \u00een aceast\u0103 lucrare, \\(Q_{\\text{eff}}\\) este tratat ca un parametru de regim identificat empiric, ob\u021binut din m\u0103sur\u0103tori de dec\u0103dere sau de l\u0103\u021bime de band\u0103 la frecven\u021ba dominant\u0103 a regimului.\n\nPentru \\(Q_{\\text{eff}}\\) ridicat: regimul re\u021bine cea mai mare parte a energiei sale circulante \u00een fiecare ciclu. Doar o frac\u021biune mic\u0103 trebuie re\u00eenc\u0103rcat\u0103.\n\n\\(\\langle P_{\\text{fb}} \\rangle\\) reprezint\u0103 alocarea intern\u0103 de mentenan\u021b\u0103 necesar\u0103 pentru a compensa pierderile de regim la un punct de operare dat (inclusiv efectele de cuplare cu sarcina capturate de \\(Q_{\\text{eff,loaded}}\\)). Prin urmare, \u00een func\u021bie de punctul de operare \u0219i arhitectura de cuplare, pot exista regimuri unde \\(\\langle P_{\\text{fb}} \\rangle &lt; \\langle P_{\\text{load}} \\rangle\\); aceasta nu modific\u0103 bilan\u021bul la frontiera dispozitivului, care r\u0103m\u00e2ne \\(\\langle P_{\\text{in,ext}} \\rangle = \\langle B_{\\text{total}} \\rangle + \\langle P_{\\text{load}} \\rangle + \\langle dE\/dt \\rangle\\).\n\nAnalogie: Un volant greu care se rote\u0219te la vitez\u0103 mare (energie stocat\u0103 ridicat\u0103) pierde energie lent prin frecare (rat\u0103 de pierderi sc\u0103zut\u0103). Un motor mic \u00eel poate men\u021bine \u00een rota\u021bie (mentenan\u021b\u0103), \u00een timp ce un generator cuplat la acela\u0219i volant poate extrage putere substan\u021bial\u0103 \u2014 dar doar p\u00e2n\u0103 la punctul \u00een care extrac\u021bia total\u0103 plus frecarea dep\u0103\u0219e\u0219te intrarea motorului.\n<h3>4.2 Desc\u0103rcarea \u00een gaz ca control neliniar al lui Q<\/h3>\nDesc\u0103rcarea \u00een gaz din Circuitul\u00a0A nu este o surs\u0103 de energie \u2014 este un <strong>element neliniar controlat<\/strong> care modeleaz\u0103 regimul:\n\n<strong>Avalan\u0219a Townsend<\/strong> (\u00een regimul de desc\u0103rcare Townsend) asigur\u0103 comutare rapid\u0103 a conductivit\u0103\u021bii:\n\n\\[n_e(x) = n_{e,0} \\exp(\\alpha x)\\]\n\nEnergia pentru ionizare provine din c\u00e2mpul electric al circuitului, nu din \u201eaer&#8221;.\n\n<strong>Desc\u0103rcarea corona<\/strong> furnizeaz\u0103:\n<ul>\n \t<li>Caracteristic\u0103 I\u2013V neliniar\u0103 care permite conductivitate adaptat\u0103 la regim<\/li>\n \t<li>Structur\u0103 pulsat\u0103 care se poate sincroniza cu modurile rezonante<\/li>\n \t<li>Interac\u021biune sensibil\u0103 la faz\u0103 cu regimul LC<\/li>\n<\/ul>\n<strong>Desc\u0103rcarea multi-canal<\/strong> ofer\u0103 redundan\u021b\u0103 \u0219i adaptare \u2014 dac\u0103 un canal de desc\u0103rcare se degradeaz\u0103, celelalte men\u021bin stabilitatea regimului.\n\nMediul (aer\/gaz) determin\u0103 caracteristicile regimului, dar nu furnizeaz\u0103 energie net\u0103. Este un mediu de lucru, precum apa \u00eentr-o turbin\u0103 \u2014 necesar pentru func\u021bionare, dar nu sursa de energie.\n\n<hr \/>\n\n<h2>5. Izolarea arhitectural\u0103: De ce extrac\u021bia nu distruge imediat regimul<\/h2>\n<h3>5.1 Problema la generatoarele clasice<\/h3>\nLa un generator clasic, sarcina creeaz\u0103 direct un cuplu de fr\u00e2nare pe arbore (legea lui Lenz). Sarcin\u0103 crescut\u0103 \u2192 fr\u00e2nare mecanic\u0103 imediat\u0103 \u2192 echilibru imediat.\n<h3>5.2 Abordarea VENDOR<\/h3>\n\u00cen VENDOR, legea lui Lenz se aplic\u0103 \u00een continuare \u2014 dar printr-un mecanism diferit:\n<ul>\n \t<li>Extrac\u021bia cre\u0219te amortizarea efectiv\u0103 (reduce \\(Q_L\\))<\/li>\n \t<li>Aceasta reduce \\(Q_{\\text{eff,loaded}}\\) total, necesit\u00e2nd mai mult\u0103 putere de mentenan\u021b\u0103<\/li>\n \t<li>Dar regimul neliniar se poate <strong>adapta \u00een cadrul regiunii sale de stabilitate<\/strong> \u00eenainte de a se pr\u0103bu\u0219i<\/li>\n \t<li>BMS-ul mediaz\u0103 aceasta prin ajustarea dinamic\u0103 a puterii de feedback<\/li>\n<\/ul>\nAceasta <strong>nu este o \u00eenc\u0103lcare a legii lui Lenz<\/strong> \u2014 reac\u021bia invers\u0103 r\u0103m\u00e2ne guvernat\u0103 de Maxwell\/Lenz; totu\u0219i, r\u0103spunsul la sarcin\u0103 observat extern este modelat de constantele de timp ale tamponului\/controlului \u0219i de bazinul de stabilitate al regimului, permi\u021b\u00e2nd un r\u0103spuns progresiv, nu instantaneu.\n<h3>5.3 Limitele de stabilitate<\/h3>\nFiecare regim are limite finite de extrac\u021bie. C\u00e2nd extrac\u021bia dep\u0103\u0219e\u0219te marja de stabilitate:\n<ul>\n \t<li>Reducerea treptat\u0103 a amplitudinii (\\(Q_{\\text{eff,loaded}}\\) scade prea mult)<\/li>\n \t<li>Tranzi\u021bie la un punct de operare de putere mai mic\u0103<\/li>\n \t<li>Colaps complet al regimului (dac\u0103 pierderile totale dep\u0103\u0219esc puterea de mentenan\u021b\u0103 disponibil\u0103 din intrarea extern\u0103)<\/li>\n<\/ul>\nAcesta este un comportament fizic a\u0219teptat \u0219i confirm\u0103 conformitatea cu legile de conservare.\n\n<hr \/>\n\n<h2>6. Sinteza: Imaginea complet\u0103<\/h2>\n<pre class=\"ascii-diagram\">\u250c\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2510\n\u2502  FRONTIERA DISPOZITIVULUI \u2014 Primul principiu se aplic\u0103 aici       \u2502\n\u2502                                                                   \u2502\n\u2502  P_in,ext \u2500\u2500\u25ba Circuitul A \u2500\u2500(induc\u021bie)\u2500\u2500\u25ba Circuitul B \u2500\u2500\u25ba P_load  \u2502\n\u2502                   \u25b2                            \u2502                  \u2502\n\u2502                   \u2502      P_fb (feedback)       \u2502                  \u2502\n\u2502                   \u2514\u2500\u2500\u2500\u2500\u2500\u2500 Tampon + BMS \u25c4\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2518                  \u2502\n\u2502                                                                   \u2502\n\u2502  Intern: P_fb este rutare de putere, nu creare de energie         \u2502\n\u2502  Extern: P_in,ext = B_total + P_load + dE\/dt                      \u2502\n\u2502  Eficien\u021b\u0103: \u03b7 = P_load \/ P_in,ext \u2264 1                             \u2502\n\u2514\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2500\u2518\n<\/pre>\n<strong>Concluzii cheie:<\/strong>\n<ol>\n \t<li><strong>Calea intern\u0103 de feedback din Circuitul\u00a0B furnizeaz\u0103 alocarea de putere de mentenan\u021b\u0103 pentru Circuitul\u00a0A.<\/strong> O frac\u021biune din puterea extras\u0103 este direc\u021bionat\u0103 prin bus-ul DC reglat pentru a compensa pierderile de regim ale nucleului; func\u021bionarea sus\u021binut\u0103 cu \\(P_{\\text{load}} \\neq 0\\) necesit\u0103 \\(P_{\\text{in,ext}} \\neq 0\\) mediat \u00een timp la Frontiera Dispozitivului.<\/li>\n \t<li><strong>Tamponul + BMS regleaz\u0103 aceast\u0103 rutare intern\u0103 a puterii<\/strong>, netezind tranzitoriile \u0219i protej\u00e2nd regimul neliniar de destabilizare.<\/li>\n \t<li><strong>Un factor de calitate efectiv \\(Q_{\\text{eff}}\\) ridicat<\/strong> permite regimului s\u0103 sus\u021bin\u0103 o circula\u021bie intern\u0103 mare a energiei cu o putere de mentenan\u021b\u0103 mic\u0103 \u2014 f\u0103c\u00e2nd arhitectura cu feedback viabil\u0103.<\/li>\n \t<li><strong>\u201e\u03b7 &gt; 100%&#8221; este \u00eentotdeauna o eroare de frontier\u0103 sau de incompletitudine a m\u0103sur\u0103torilor.<\/strong> C\u00e2nd se m\u0103soar\u0103 la frontiera corect\u0103 a dispozitivului cu instrumenta\u021bie complet\u0103, sistemul respect\u0103 legile de conservare.<\/li>\n \t<li><strong>Neliniaritatea modific\u0103 dinamica, nu conservarea.<\/strong> Arhitectura bazat\u0103 pe regim ofer\u0103 avantaje inginere\u0219ti (autostabilizare, adaptare la sarcin\u0103, reac\u021bie invers\u0103 progresiv\u0103), dar nu creeaz\u0103 energie.<\/li>\n<\/ol>\n\n<hr \/>\n\n<h3>Tabel de sintez\u0103: Fluxuri de energie \u0219i erori comune de contabilizare<\/h3>\n<table>\n<thead>\n<tr>\n<th scope=\"col\">M\u0103rime<\/th>\n<th scope=\"col\">Semnifica\u021bie<\/th>\n<th scope=\"col\">Unde apare<\/th>\n<th scope=\"col\">Eroare frecvent\u0103<\/th>\n<\/tr>\n<\/thead>\n<tbody>\n<tr>\n<td>\\(P_{\\text{in,ext}}\\)<\/td>\n<td>Intrare extern\u0103 total\u0103 la frontiera dispozitivului<\/td>\n<td>\\(\\frac{dE_{\\text{total}}}{dt} = P_{\\text{in,ext}} &#8211; B_{\\text{total}} &#8211; P_{\\text{load}}\\)<\/td>\n<td>Considerarea doar a \\(P_{\\text{fb}}\\) ca \u201eintrare&#8221;<\/td>\n<\/tr>\n<tr>\n<td>\\(P_{\\text{fb}}\\)<\/td>\n<td>Putere de feedback de la Circuitul\u00a0B la Circuitul\u00a0A (intern\u0103)<\/td>\n<td>Canal intern de redistribuire<\/td>\n<td>Tratarea ca singur\u0103 intrare \u0219i calcularea \u03b7 &gt; 100%<\/td>\n<\/tr>\n<tr>\n<td>\\(B_{\\text{total}}\\)<\/td>\n<td>Toate pierderile ireversibile la frontier\u0103<\/td>\n<td>Termen de pierderi \u00een bilan\u021b<\/td>\n<td>Ignorarea pierderilor induse de sarcin\u0103<\/td>\n<\/tr>\n<tr>\n<td>\\(P_{\\text{load}}\\)<\/td>\n<td>Putere util\u0103 de ie\u0219ire c\u0103tre sarcina extern\u0103<\/td>\n<td>M\u0103surat\u0103 la bornele de ie\u0219ire<\/td>\n<td>Presupunerea c\u0103 este \u201esus\u021binut\u0103&#8221; doar de \\(P_{\\text{fb}}\\)<\/td>\n<\/tr>\n<tr>\n<td>\\(dE_{\\text{stored}}\/dt\\)<\/td>\n<td>Varia\u021bia energiei stocate (tampon + c\u00e2mpuri)<\/td>\n<td>Ecua\u021bia de bilan\u021b<\/td>\n<td>Ignorarea \u00eenc\u0103rc\u0103rii\/desc\u0103rc\u0103rii tamponului<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n\n<hr \/>\n\n<h2>Anexa A: Simboluri \u0219i nota\u021bii<\/h2>\n<table>\n<thead>\n<tr>\n<th scope=\"col\">Simbol<\/th>\n<th scope=\"col\">Semnifica\u021bie<\/th>\n<th scope=\"col\">Unitate<\/th>\n<\/tr>\n<\/thead>\n<tbody>\n<tr>\n<td>\\(P_{\\text{in,ext}}\\)<\/td>\n<td>Putere de intrare extern\u0103 total\u0103<\/td>\n<td>W<\/td>\n<\/tr>\n<tr>\n<td>\\(P_{\\text{load}}\\)<\/td>\n<td>Putere util\u0103 de ie\u0219ire<\/td>\n<td>W<\/td>\n<\/tr>\n<tr>\n<td>\\(P_{\\text{fb}}\\)<\/td>\n<td>Putere de feedback (intern\u0103)<\/td>\n<td>W<\/td>\n<\/tr>\n<tr>\n<td>\\(P_{\\text{aux}}\\)<\/td>\n<td>Putere auxiliar\u0103\/extern\u0103 c\u0103tre Circuitul A (incl. pornire)<\/td>\n<td>W<\/td>\n<\/tr>\n<tr>\n<td>\\(B_{\\text{total}}\\)<\/td>\n<td>Pierderi ireversibile totale<\/td>\n<td>W<\/td>\n<\/tr>\n<tr>\n<td>\\(E_{\\text{total}}\\)<\/td>\n<td>Energia total\u0103 stocat\u0103 a sistemului<\/td>\n<td>J<\/td>\n<\/tr>\n<tr>\n<td>\\(\\eta\\)<\/td>\n<td>Eficien\u021b\u0103<\/td>\n<td>\u2014<\/td>\n<\/tr>\n<tr>\n<td>\\(Q_{\\text{eff}}\\)<\/td>\n<td>Factor de calitate efectiv al regimului<\/td>\n<td>\u2014<\/td>\n<\/tr>\n<tr>\n<td>\\(\\omega_0\\)<\/td>\n<td>Frecven\u021ba unghiular\u0103 de rezonan\u021b\u0103<\/td>\n<td>rad\/s<\/td>\n<\/tr>\n<tr>\n<td>\\(L\\), \\(C\\)<\/td>\n<td>Inductan\u021b\u0103, capacitate<\/td>\n<td>H, F<\/td>\n<\/tr>\n<tr>\n<td>\\(\\alpha\\)<\/td>\n<td>Primul coeficient Townsend<\/td>\n<td>m\u207b\u00b9<\/td>\n<\/tr>\n<tr>\n<td>\\(\\sigma\\)<\/td>\n<td>Conductivitatea mediului<\/td>\n<td>S\/m<\/td>\n<\/tr>\n<tr>\n<td>\\(\\Phi_B\\)<\/td>\n<td>Flux magnetic<\/td>\n<td>Wb<\/td>\n<\/tr>\n<tr>\n<td>\\(\\mathcal{E}\\)<\/td>\n<td>For\u021b\u0103 electromotoare<\/td>\n<td>V<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n\n<hr \/>\n\n<h2>Anexa B: Not\u0103 de transparen\u021b\u0103<\/h2>\nAcest articol prezint\u0103 o <strong>formulare matematic\u0103 \u0219i corect\u0103 din punct de vedere al frontierei<\/strong> a bilan\u021bului energetic pentru arhitectura VENDOR.Energy\u2122. Scopul s\u0103u este eliminarea erorilor de interpretare \u2014 \u00een special a paradoxului \u201e\u03b7 &gt; 100%&#8221; \u2014 nu divulgarea detaliilor complete de implementare.\n\nExemplele numerice sunt <strong>ilustra\u021bii conservative la nivel de model<\/strong>. Capacitatea de putere este o func\u021bie de configura\u021bie (arhitectur\u0103, marje de stabilitate, design de extrac\u021bie, constr\u00e2ngeri termice), iar parametrii de implementare sunt divulga\u021bi doar prin documenta\u021bie controlat\u0103 c\u0103tre p\u0103r\u021bi calificate prin <a href=\"https:\/\/vendor.energy\/investor-room\/\" target=\"_blank\" rel=\"noopener\">Silent Pitch Room<\/a>.\n\n<hr \/>\n\n<h2>Bibliografie<\/h2>\n<ol>\n \t<li>Documenta\u021bie de brevet: <a href=\"https:\/\/patentscope.wipo.int\/search\/en\/detail.jsf?docId=WO2024209235\" target=\"_blank\" rel=\"noopener\">WO2024209235<\/a> (PCT); ES2950176 (Spania); EUIPO Nr. 019220462<\/li>\n \t<li>Maxwell, J. C. <em>A Treatise on Electricity and Magnetism<\/em> \u2014 fundamentul induc\u021biei electromagnetice (Circuitul B)<\/li>\n \t<li>Griffiths, D. J. <em>Introduction to Electrodynamics<\/em> (ed. a 4-a) \u2014 pierderi ohmice, dielectrice \u0219i radiative<\/li>\n \t<li>Khalil, H. K. <em>Nonlinear Systems<\/em> (ed. a 3-a) \u2014 analiz\u0103 de stabilitate \u0219i cicluri limit\u0103<\/li>\n \t<li>Factor de calitate: <a href=\"https:\/\/en.wikipedia.org\/wiki\/Q_factor\" target=\"_blank\" rel=\"noopener\">Wikipedia<\/a>; <a href=\"https:\/\/www.zhinst.com\/en\/blogs\/resonance-engineering-quality-factor-q-control-method\" target=\"_blank\" rel=\"noopener\">Zurich Instruments<\/a><\/li>\n \t<li>Desc\u0103rcarea Townsend: <a href=\"https:\/\/en.wikipedia.org\/wiki\/Townsend_discharge\" target=\"_blank\" rel=\"noopener\">Wikipedia<\/a><\/li>\n \t<li>Rezonan\u021b\u0103 parametric\u0103: Caldwell (2016), <a href=\"https:\/\/open.clemson.edu\/all_theses\/3041\/\" target=\"_blank\" rel=\"noopener\">Clemson Thesis<\/a><\/li>\n \t<li>Sisteme termodinamice deschise: <a href=\"https:\/\/www.britannica.com\/science\/thermodynamics\/Open-systems\" target=\"_blank\" rel=\"noopener\">Britannica<\/a><\/li>\n \t<li>Cicluri limit\u0103: <a href=\"https:\/\/en.wikipedia.org\/wiki\/Limit_cycle\" target=\"_blank\" rel=\"noopener\">Wikipedia<\/a><\/li>\n \t<li>Documenta\u021bie VENDOR: <a href=\"https:\/\/vendor.energy\" target=\"_blank\" rel=\"noopener\">vendor.energy<\/a><\/li>\n<\/ol>\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>Autori: O. Krishevich, V. Peretyachenko Rezumat Acest articol prezint\u0103 un cadru riguros de bilan\u021b energetic pentru arhitectura VENDOR.Energy\u2122 \u2014 o clas\u0103 de sisteme electrodinamice neliniare cu separare func\u021bional\u0103 \u00eentre formarea regimului, compensarea pierderilor \u0219i extragerea puterii utile. Obiectivul central este formalizarea rolului rut\u0103rii interne a puterii prin bucl\u0103 de feedback \u0219i al tampon\u0103rii \u00een men\u021binerea [&hellip;]<\/p>\n","protected":false},"author":1,"featured_media":15691,"comment_status":"open","ping_status":"open","sticky":false,"template":"elementor_header_footer","format":"standard","meta":{"footnotes":""},"categories":[270,196],"tags":[945,1006,942,1017,1020,999,1016,1018,1000,915,1001,1019,918],"class_list":["post-15700","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-science-ro","category-technology-ro","tag-bilant-energetic","tag-bucla-de-control","tag-energy-balance","tag-extractie-inductiva","tag-fizica-descarcarilor-gazoase","tag-inductive-extraction","tag-inginerie-rezonanta","tag-lectrodinamica-neliniara","tag-nonlinear-electrodynamics","tag-open-systems","tag-resonant-engineering","tag-sisteme-de-regim","tag-sisteme-deschise"],"_links":{"self":[{"href":"https:\/\/vendor.energy\/ro\/wp-json\/wp\/v2\/posts\/15700","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=15700"}],"version-history":[{"count":13,"href":"https:\/\/vendor.energy\/ro\/wp-json\/wp\/v2\/posts\/15700\/revisions"}],"predecessor-version":[{"id":16493,"href":"https:\/\/vendor.energy\/ro\/wp-json\/wp\/v2\/posts\/15700\/revisions\/16493"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/vendor.energy\/ro\/wp-json\/wp\/v2\/media\/15691"}],"wp:attachment":[{"href":"https:\/\/vendor.energy\/ro\/wp-json\/wp\/v2\/media?parent=15700"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/vendor.energy\/ro\/wp-json\/wp\/v2\/categories?post=15700"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/vendor.energy\/ro\/wp-json\/wp\/v2\/tags?post=15700"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}