{"id":43210,"date":"2019-10-08T13:04:57","date_gmt":"2019-10-08T12:04:57","guid":{"rendered":"https:\/\/www.thermal-engineering.org\/quest-ce-que-lebullition-de-transition-lebullition-partielle-du-film-definition\/"},"modified":"2020-02-06T19:39:37","modified_gmt":"2020-02-06T18:39:37","slug":"quest-ce-que-lebullition-de-transition-lebullition-partielle-du-film-definition","status":"publish","type":"post","link":"https:\/\/www.thermal-engineering.org\/fr\/quest-ce-que-lebullition-de-transition-lebullition-partielle-du-film-definition\/","title":{"rendered":"Qu&#8217;est-ce que l&#8217;\u00e9bullition de transition &#8211; l&#8217;\u00e9bullition partielle du film &#8211; D\u00e9finition"},"content":{"rendered":"<div class=\"su-quote su-quote-style-default\">\n<div class=\"su-quote-inner su-clearfix\">\u00c9bullition de transition &#8211; \u00e9bullition partielle du film.\u00a0Imm\u00e9diatement apr\u00e8s que le flux de chaleur critique a \u00e9t\u00e9 atteint, l&#8217;\u00e9bullition devient instable et une \u00e9bullition de transition se produit.\u00a0G\u00e9nie thermique<\/div>\n<\/div>\n<div class=\"su-divider su-divider-style-dotted\"><\/div>\n<div class=\"lgc-column lgc-grid-parent lgc-grid-100 lgc-tablet-grid-100 lgc-mobile-grid-100 lgc-equal-heights lgc-first lgc-last\">\n<div class=\"inside-grid-column\">\n<div class=\"su-spacer\"><\/div>\n<h2>\u00c9bullition de transition &#8211; \u00e9bullition partielle<\/h2>\n<p><strong>Cat\u00e9gorisation par la temp\u00e9rature de surchauffe des murs, \u0394T\u00a0<\/strong><strong><sub>sat<\/sub><\/strong><strong>\u00a0:<\/strong><\/p>\n<p><a href=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Boiling-Curve-Boiling-Modes.png\"><img loading=\"lazy\" class=\"alignright size-medium wp-image-20779 lazy-loaded\" src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Boiling-Curve-Boiling-Modes-208x300.png\" alt=\"Courbe d'\u00e9bullition - Modes d'\u00e9bullition\" width=\"208\" height=\"300\" data-lazy-type=\"image\" data-src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Boiling-Curve-Boiling-Modes-208x300.png\" \/><\/a>Le travail de pionnier en mati\u00e8re d&#8217;\u00e9bullition a \u00e9t\u00e9 effectu\u00e9 en 1934 par\u00a0\u00a0<strong>S. Nukiyama<\/strong>\u00a0, qui a utilis\u00e9 des fils de nichrome et de platine chauff\u00e9s \u00e9lectriquement immerg\u00e9s dans des liquides dans ses exp\u00e9riences.\u00a0Nukiyama fut le premier \u00e0 identifier\u00a0\u00a0<strong>diff\u00e9rents r\u00e9gimes de piscine en \u00e9bullition<\/strong>\u00a0\u00a0\u00e0\u00a0<strong>l&#8217;<\/strong>\u00a0aide de son appareil.\u00a0Il a\u00a0remarqu\u00e9 que l&#8217;\u00a0\u00e9bullition prend des formes diff\u00e9rentes, en\u00a0fonction de la valeur de la temp\u00e9rature de surchauffe de la\u00a0paroi\u00a0\u00a0<strong>AT\u00a0<\/strong><strong><sub>sat<\/sub><\/strong>\u00a0\u00a0(\u00e9galement connu comme l&#8217;exc\u00e8s de\u00a0temp\u00e9rature)\u00a0<strong>,\u00a0<\/strong>\u00a0qui est d\u00e9finie comme la diff\u00e9rence entre la temp\u00e9rature de paroi,\u00a0\u00a0<strong>T\u00a0<sub>paroi<\/sub><\/strong>\u00a0\u00a0et la temp\u00e9rature de saturation,\u00a0<strong>\u00a0T\u00a0<sub>sat<\/sub><\/strong>\u00a0.<\/p>\n<p>On observe quatre r\u00e9gimes diff\u00e9rents d\u2019\u00e9bullition en piscine (bas\u00e9s sur l\u2019exc\u00e8s de temp\u00e9rature):<\/p>\n<ul>\n<li><strong>Point d&#8217;\u00e9bullition par convection naturelle\u00a0<\/strong>\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0 \u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0 \u00a0<strong>\u0394T\u00a0<\/strong><strong><sub>sat<\/sub><\/strong>\u00a0\u00a0&lt;5 \u00b0 C<\/li>\n<li><strong>Nucl\u00e9ate en \u00e9bullition<\/strong>\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0 \u00a0\u00a0\u00a05 \u00b0 C &lt;\u00a0\u00a0<strong>\u0394T\u00a0<\/strong><strong><sub>sat<\/sub><\/strong>\u00a0\u00a0&lt;30 \u00b0 C<\/li>\n<li><strong>Transition d&#8217;\u00e9bullition<\/strong>\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0 \u00a0\u00a030 \u00b0 C &lt;\u00a0\u00a0<strong>\u0394T\u00a0<\/strong><strong><sub>sat<\/sub><\/strong>\u00a0\u00a0&lt;200 \u00b0 C<\/li>\n<li><strong>Film en \u00e9bullition<\/strong>\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0 200 \u00b0 C &lt;\u00a0\u00a0<strong>\u0394T\u00a0<\/strong><strong><sub>sat<\/sub><\/strong><\/li>\n<\/ul>\n<h2>\u00c9bullition de transition<\/h2>\n<p><a href=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Transition-Boiling-Partial-Film-Boiling-schema.png\"><img loading=\"lazy\" class=\"alignright size-medium wp-image-20777 lazy-loaded\" src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Transition-Boiling-Partial-Film-Boiling-schema-300x225.png\" alt=\"\u00c9bullition de transition - \u00e9bullition partielle\" width=\"300\" height=\"225\" data-lazy-type=\"image\" data-src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Transition-Boiling-Partial-Film-Boiling-schema-300x225.png\" \/><\/a>Le flux de chaleur d&#8217;\u00e9bullition nucl\u00e9\u00e9e ne peut pas \u00eatre augment\u00e9 ind\u00e9finiment.\u00a0Nous appelons cela un \u00ab\u00a0<strong>flux de chaleur critique<\/strong>\u00a0\u00bb (\u00a0<strong>CHF<\/strong>\u00a0), la vapeur produite peut former une couche isolante sur la surface, ce qui d\u00e9t\u00e9riore le coefficient de transfert de chaleur.\u00a0En effet, une grande partie de la surface est recouverte d\u2019un film de vapeur qui joue le r\u00f4le d\u2019isolant thermique en raison de la faible conductivit\u00e9 thermique de la vapeur par rapport \u00e0 celle du liquide.\u00a0Imm\u00e9diatement apr\u00e8s que le flux de chaleur critique a \u00e9t\u00e9 atteint, l&#8217;\u00e9bullition devient instable et une \u00e9bullition de transition se produit.\u00a0La transition de l&#8217;\u00e9bullition nucl\u00e9\u00e9e \u00e0 l&#8217;\u00e9bullition pelliculaire est appel\u00e9e \u00ab\u00a0<strong>crise d&#8217;\u00e9bullition<\/strong>\u00a0\u00bb.\u00a0Au-del\u00e0 du point CHF, le coefficient de transfert de chaleur diminue, le passage \u00e0 l&#8217;\u00e9bullition du film est g\u00e9n\u00e9ralement in\u00e9vitable.<\/p>\n<\/div>\n<\/div>\n<div class=\"lgc-column lgc-grid-parent lgc-grid-100 lgc-tablet-grid-100 lgc-mobile-grid-100 lgc-equal-heights lgc-first lgc-last\">\n<div class=\"inside-grid-column\">\n<div class=\"su-spacer\"><\/div>\n<div class=\"lgc-column lgc-grid-parent lgc-grid-100 lgc-tablet-grid-100 lgc-mobile-grid-100 lgc-equal-heights  lgc-first lgc-last\">\n<div class=\"inside-grid-column\">\n<h2><span>Flux thermique critique<\/span><\/h2>\n<p><a href=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Dryout-DNB-min.png\"><img loading=\"lazy\" class=\"alignright size-medium wp-image-14862 lazy-loaded\" src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Dryout-DNB-min-225x300.png\" alt=\"S\u00e9cher vs DNB\" width=\"225\" height=\"300\" data-lazy-type=\"image\" data-src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Dryout-DNB-min-225x300.png\" \/><\/a><span>Comme cela a \u00e9t\u00e9 \u00e9crit, dans\u00a0\u00a0<\/span><a href=\"https:\/\/www.nuclear-power.com\/nuclear-power-plant\/nuclear-reactor\/\"><span>les r\u00e9acteurs nucl\u00e9aires<\/span><\/a><span>\u00a0, les limitations du\u00a0\u00a0<\/span><strong><span>flux de chaleur local<\/span><\/strong><span>\u00a0\u00a0sont de la plus haute importance pour la s\u00fbret\u00e9 des r\u00e9acteurs.\u00a0Pour les\u00a0\u00a0<\/span><a href=\"https:\/\/www.nuclear-power.com\/pwr-pressurized-water-reactor\/\"><span>r\u00e9acteurs \u00e0 eau sous pression<\/span><\/a><span>\u00a0\u00a0et \u00e9galement pour les\u00a0\u00a0<\/span><a href=\"https:\/\/www.nuclear-power.com\/bwr-boiling-water-reactor\/\"><span>r\u00e9acteurs \u00e0 eau bouillante<\/span><\/a><span>\u00a0, il existe des ph\u00e9nom\u00e8nes thermohydrauliques qui provoquent une baisse brutale de l&#8217;\u00a0\u00a0<\/span><strong><span>efficacit\u00e9 du transfert de chaleur<\/span><\/strong><span>\u00a0\u00a0(plus pr\u00e9cis\u00e9ment du\u00a0\u00a0<\/span><strong><span>coefficient de transfert de chaleur<\/span><\/strong><span>\u00a0).\u00a0Ces ph\u00e9nom\u00e8nes se produisent \u00e0 une certaine valeur du flux de chaleur, connue sous le nom de \u00ab\u00a0<\/span><strong><span>flux de chaleur critique<\/span><\/strong><span>\u00a0\u00bb.\u00a0Les ph\u00e9nom\u00e8nes qui provoquent la d\u00e9t\u00e9rioration du transfert de chaleur sont diff\u00e9rents pour les REP et pour les REB.<\/span><\/p>\n<p><span>Dans les deux types de r\u00e9acteurs, le probl\u00e8me est plus ou moins associ\u00e9 au d\u00e9part de l&#8217;\u00e9bullition nucl\u00e9\u00e9e.\u00a0Le flux de chaleur d&#8217;\u00e9bullition nucl\u00e9\u00e9e ne peut pas \u00eatre augment\u00e9 ind\u00e9finiment.\u00a0\u00c0 une certaine valeur, nous l&#8217;appelons le \u00ab\u00a0<\/span><strong><span>flux de chaleur critique<\/span><\/strong><span>\u00a0\u00bb (\u00a0<\/span><strong><span>CHF<\/span><\/strong><span>\u00a0), la vapeur produite peut former une couche isolante sur la surface, qui \u00e0 son tour d\u00e9t\u00e9riore le coefficient de transfert de chaleur.\u00a0Imm\u00e9diatement apr\u00e8s que le flux de chaleur critique a \u00e9t\u00e9 atteint, l&#8217;\u00e9bullition devient instable et l&#8217;\u00e9bullition en film se produit.\u00a0La transition de l&#8217;\u00e9bullition nucl\u00e9\u00e9e \u00e0 l&#8217;\u00e9bullition pelliculaire est connue sous le nom de \u00ab\u00a0<\/span><strong><span>crise d&#8217;\u00e9bullition<\/span><\/strong><span>\u00a0\u00bb.\u00a0Comme cela a \u00e9t\u00e9 \u00e9crit, les ph\u00e9nom\u00e8nes qui provoquent la d\u00e9t\u00e9rioration du transfert de chaleur sont diff\u00e9rents pour les REP et pour les REB.<\/span><\/p>\n<\/div>\n<\/div>\n<div class=\"lgc-column lgc-grid-parent lgc-grid-100 lgc-tablet-grid-100 lgc-mobile-grid-100 lgc-equal-heights  lgc-first lgc-last\">\n<div class=\"inside-grid-column\">\n<div class=\"su-spacer\"><\/div>\n<h2><span>Flux thermique minimal &#8211; Leidenfrost Point<\/span><\/h2>\n<p><a href=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Leidenfrost-Point-Boiling-Curve.png\"><img loading=\"lazy\" class=\"alignright size-medium wp-image-20772 lazy-loaded\" src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Leidenfrost-Point-Boiling-Curve-283x300.png\" alt=\"Leidenfrost Point\" width=\"283\" height=\"300\" data-lazy-type=\"image\" data-src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Leidenfrost-Point-Boiling-Curve-283x300.png\" \/><\/a><span>Le\u00a0<\/span><strong><span>point Leidenfrost<\/span><\/strong><span>\u00a0, qui correspond au\u00a0<\/span><strong><span>flux de chaleur minimal<\/span><\/strong><span>\u00a0, pr\u00e9sente un int\u00e9r\u00eat pratique car il repr\u00e9sente la limite inf\u00e9rieure du flux de chaleur dans le r\u00e9gime d&#8217;\u00e9bullition du film.\u00a0Si le flux de chaleur tombe en dessous de ce minimum, le film s&#8217;effondrera, provoquant le refroidissement de la surface et le r\u00e9tablissement de l&#8217;\u00e9bullition nucl\u00e9\u00e9e.\u00a0Par cons\u00e9quent, \u00e0 ce stade, le\u00a0<\/span><strong><span>retour \u00e0 l&#8217;\u00e9bullition nucl\u00e9\u00e9e<\/span><\/strong><span>\u00a0(RNB) se produit.\u00a0Les termes trempe, flux de chaleur minimum, retour \u00e0 l&#8217;\u00e9bullition nucl\u00e9\u00e9e, d\u00e9part de l&#8217;\u00e9bullition du film, effondrement de l&#8217;\u00e9bullition du film et point Leidenfrost ont \u00e9t\u00e9 utilis\u00e9s de mani\u00e8re interchangeable pour d\u00e9signer diverses formes de remouillage, mais ils ne sont pas exactement synonymes.<\/span><\/p>\n<p><span>En utilisant la th\u00e9orie de la stabilit\u00e9, Zuber a d\u00e9riv\u00e9 l&#8217;expression suivante pour le flux de chaleur minimum (et le\u00a0<\/span><strong><span>point Leidenfrost<\/span><\/strong><span>\u00a0correspondant\u00a0) pour une grande plaque horizontale:<\/span><\/p>\n<p><a href=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/leidenfrost-point-equation.png\"><img loading=\"lazy\" class=\"aligncenter size-full wp-image-20788 lazy-loaded\" src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/leidenfrost-point-equation.png\" alt=\"leidenfrost point - \u00e9quation\" width=\"413\" height=\"83\" data-lazy-type=\"image\" data-src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/leidenfrost-point-equation.png\" \/><\/a><\/p>\n<p><span>o\u00f9<\/span><\/p>\n<ul>\n<li><span>q\u00a0<\/span><sub><span>min<\/span><\/sub><span>\u00a0&#8211; flux thermique minimal [W \/ m\u00a0<\/span><sup><span>2<\/span><\/sup><span>\u00a0]<\/span><\/li>\n<li><span>h\u00a0<\/span><sub><span>fg<\/span><\/sub><span>\u00a0\u00a0&#8211; enthalpie de vaporisation, J \/ kg<\/span><\/li>\n<li><span>g &#8211; acc\u00e9l\u00e9ration gravitationnelle m \/ s\u00a0<\/span><sup><span>2<\/span><\/sup><\/li>\n<li><span>\u03c1\u00a0<\/span><sub><span>l<\/span><\/sub><span>\u00a0&#8211; densit\u00e9 du liquide kg \/ m\u00a0<\/span><sup><span>3<\/span><\/sup><\/li>\n<li><span>\u03c1\u00a0<\/span><sub><span>v<\/span><\/sub><span>\u00a0&#8211; densit\u00e9 de vapeur kg \/ m\u00a0<\/span><sup><span>3<\/span><\/sup><\/li>\n<li><span>\u03c3 &#8211; interface tension liquide-vapeur de surface N \/ m<\/span><\/li>\n<\/ul>\n<\/div>\n<\/div>\n<div class=\"lgc-column lgc-grid-parent lgc-grid-100 lgc-tablet-grid-100 lgc-mobile-grid-100 lgc-equal-heights  lgc-first lgc-last\">\n<div class=\"inside-grid-column\">\n<div class=\"su-spacer\"><\/div>\n<h2><span>Effet Leidenfrost<\/span><\/h2>\n<p><span>L&#8217;\u00a0<\/span><strong><span>effet Leidenfrost<\/span><\/strong><span>\u00a0est un ph\u00e9nom\u00e8ne physique dans lequel un liquide, au contact proche d&#8217;une masse significativement plus chaude (par exemple une goutte d&#8217;eau dans une casserole chaude) que le point d&#8217;\u00e9bullition du liquide, produit une couche de vapeur isolante emp\u00eachant ce liquide de bouillir rapidement.\u00a0Le fait qu&#8217;une goutte d&#8217;eau dure longtemps lorsqu&#8217;elle est d\u00e9pos\u00e9e sur un m\u00e9tal beaucoup plus chaud que la temp\u00e9rature d&#8217;\u00e9bullition de l&#8217;eau a \u00e9t\u00e9 signal\u00e9 pour la premi\u00e8re fois par Hermann Boerhaave en 1732. Elle n&#8217;a \u00e9t\u00e9 \u00e9tudi\u00e9e en profondeur qu&#8217;en 1756 lorsqu&#8217;un m\u00e9decin allemand Johann Gottlob Leidenfrost a publi\u00e9 &#8221; A Traitez de certaines qualit\u00e9s de l&#8217;eau courante. &#8221;<\/span><\/p>\n<p><span>Cet effet peut \u00eatre couramment d\u00e9montr\u00e9 pendant la cuisson lorsque l&#8217;on asperge des gouttes d&#8217;eau dans une casserole pour mesurer sa temp\u00e9rature: si la temp\u00e9rature de la casserole est au niveau ou au-dessus du\u00a0<\/span><strong><span>point de<\/span><\/strong><span>\u00a0d\u00e9givrage de Leiden, l&#8217;eau skitte \u00e0 travers la casserole et prend plus de temps \u00e0 s&#8217;\u00e9vaporer que dans une casserole en dessous de la temp\u00e9rature du point Leidenfrost (mais toujours au-dessus de la temp\u00e9rature d&#8217;\u00e9bullition).\u00a0Le point Leidenfrost, qui correspond au flux de chaleur minimal, pr\u00e9sente un int\u00e9r\u00eat pratique car il repr\u00e9sente la limite inf\u00e9rieure du flux de chaleur dans le r\u00e9gime d&#8217;\u00e9bullition du film.\u00a0Si le flux de chaleur tombe en dessous de ce minimum, le film s&#8217;effondrera, provoquant le refroidissement de la surface et le r\u00e9tablissement de l&#8217;\u00e9bullition nucl\u00e9\u00e9e.\u00a0L&#8217;effet Leidenfrost est \u00e9galement responsable de la capacit\u00e9 de l&#8217;azote liquide \u00e0 skitter \u00e0 travers les planchers.<\/span><\/p>\n<p><a href=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Leidenfrost-Effect-Water-Drop.png\"><img loading=\"lazy\" class=\"aligncenter size-full wp-image-20771 lazy-loaded\" src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Leidenfrost-Effect-Water-Drop.png\" alt=\"Effet Leidenfrost - Goutte d'eau\" width=\"1148\" height=\"681\" data-lazy-type=\"image\" data-src=\"https:\/\/thermal-engineering.org\/wp-content\/uploads\/2019\/05\/Leidenfrost-Effect-Water-Drop.png\" \/><\/a><\/p>\n<\/div>\n<\/div>\n<div class=\"lgc-column lgc-grid-parent lgc-grid-100 lgc-tablet-grid-100 lgc-mobile-grid-100 lgc-equal-heights  lgc-first lgc-last\">\n<div class=\"inside-grid-column\"><\/div>\n<\/div>\n<\/div>\n<\/div>\n<p>&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;&#8230;.<\/p>\n<p>Cet article est bas\u00e9 sur la traduction automatique de l&#8217;article original en anglais. Pour plus d&#8217;informations, voir l&#8217;article en anglais. Pouvez vous nous aider Si vous souhaitez corriger la traduction, envoyez-la \u00e0 l&#8217;adresse: translations@nuclear-power.com ou remplissez le formulaire de traduction en ligne. Nous appr\u00e9cions votre aide, nous mettrons \u00e0 jour la traduction le plus rapidement possible. Merci<\/p>\n","protected":false},"excerpt":{"rendered":"<p>\u00c9bullition de transition &#8211; \u00e9bullition partielle du film.\u00a0Imm\u00e9diatement apr\u00e8s que le flux de chaleur critique a \u00e9t\u00e9 atteint, l&#8217;\u00e9bullition devient instable et une \u00e9bullition de transition se produit.\u00a0G\u00e9nie thermique \u00c9bullition de transition &#8211; \u00e9bullition partielle Cat\u00e9gorisation par la temp\u00e9rature de surchauffe des murs, \u0394T\u00a0sat\u00a0: Le travail de pionnier en mati\u00e8re d&#8217;\u00e9bullition a \u00e9t\u00e9 effectu\u00e9 en &#8230; <a title=\"Qu&#8217;est-ce que l&#8217;\u00e9bullition de transition &#8211; l&#8217;\u00e9bullition partielle du film &#8211; D\u00e9finition\" class=\"read-more\" href=\"https:\/\/www.thermal-engineering.org\/fr\/quest-ce-que-lebullition-de-transition-lebullition-partielle-du-film-definition\/\" aria-label=\"En savoir plus sur Qu&#8217;est-ce que l&#8217;\u00e9bullition de transition &#8211; l&#8217;\u00e9bullition partielle du film &#8211; D\u00e9finition\">Lire la suite<\/a><\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":[],"categories":[8],"tags":[],"yoast_head":"<!-- This site is optimized with the Yoast SEO plugin v15.4 - https:\/\/yoast.com\/wordpress\/plugins\/seo\/ -->\n<title>Qu&#039;est-ce que l&#039;\u00e9bullition de transition - l&#039;\u00e9bullition partielle du film - D\u00e9finition<\/title>\n<meta name=\"description\" content=\"\u00c9bullition de transition - \u00e9bullition partielle du film. 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