{"id":1,"date":"2026-01-22T10:52:40","date_gmt":"2026-01-22T10:52:40","guid":{"rendered":"http:\/\/sciences-physiques.org\/?p=1"},"modified":"2026-04-29T15:40:51","modified_gmt":"2026-04-29T15:40:51","slug":"cours-metrologie","status":"publish","type":"post","link":"https:\/\/sciences-physiques.org\/index.php\/2026\/01\/22\/cours-metrologie\/","title":{"rendered":"Cours de m\u00e9trologie"},"content":{"rendered":"\n<p class=\"is-style-default has-medium-font-size\" style=\"margin-right:var(--wp--preset--spacing--50);margin-left:var(--wp--preset--spacing--50)\">La m\u00e9trologie est la science de la mesure. Elle s'int\u00e9resse aux grandeurs physiques, chimique ou biologiques, \u00e0 leurs unit\u00e9s et aux incertitudes de mesure. Ces domaines d\u2019application concernent la recherche et le d\u00e9veloppement, le contr\u00f4le de la qualit\u00e9 et l\u2019assurance qualit\u00e9 dans les industries, la certification des entreprises qui r\u00e9alisent des prestations de contr\u00f4le, la v\u00e9rification de la conformit\u00e9 aux r\u00e8gles l\u00e9gales, la v\u00e9rification de l\u2019utilisation d\u2019une m\u00e9thode agr\u00e9\u00e9e, l\u2019\u00e9talonnage des \u00e9talons et de l\u2019appareillage et la v\u00e9rification des appareils de mesure.<\/p>\n\n\n\n\n\n\n\n<h2 class=\"wp-block-heading is-style-default\" style=\"margin-right:var(--wp--preset--spacing--50);margin-left:var(--wp--preset--spacing--50)\">Les grandeurs<\/h2>\n\n\n\n<h3 class=\"wp-block-heading\" style=\"margin-right:var(--wp--preset--spacing--50);margin-left:var(--wp--preset--spacing--50)\">D\u00e9finitions<\/h3>\n\n\n<div style=\"border: 3px solid #004780; border-radius: 25px; background-color: #e3f7f7; \" class=\"ub-styled-box ub-bordered-box wp-block-ub-styled-box\" id=\"ub-styled-box-76167e75-c0a6-4b8a-9c56-b60d9d897b86\">\n<p class=\"has-medium-font-size\" id=\"ub-styled-box-bordered-content-\">Propri\u00e9t\u00e9 d'un ph\u00e9nom\u00e8ne, d'un corps ou d'une substance, que l'on peut exprimer quantitativement sous forme d'un nombre et d'une r\u00e9f\u00e9rence. La r\u00e9f\u00e9rence peut \u00eatre une unit\u00e9 de mesure, une proc\u00e9dure de mesure, un mat\u00e9riau de r\u00e9f\u00e9rence, ou une de leurs combinaisons. Les symboles des grandeurs doivent toujours \u00eatre \u00e9crits en italique (ISO 80000)<span class=\"zp-InText-zp-ID--20404111-GTVNKYYL--wp1 zp-InText-Citation loading\" rel=\"{ 'pages': 'np', 'items': '{20404111:GTVNKYYL}', 'format': '(%a%, %d%, %p%)', 'brackets': '', 'etal': '', 'separator': '', 'and': '' }\"><\/span>.<\/p>\n\n\n<\/div>\n\n\n<div class=\"wp-block-group is-layout-constrained wp-block-group-is-layout-constrained\">\n<div class=\"wp-block-group is-layout-constrained wp-block-group-is-layout-constrained\">\n<div class=\"wp-block-group is-layout-constrained wp-block-group-is-layout-constrained\"><div style=\"border: 3px outset #fab300; border-radius: 26px; background-color: #fff6e2; \" class=\"ub-styled-box ub-bordered-box wp-block-ub-styled-box\" id=\"ub-styled-box-a09da862-d8d0-460a-ad76-7975c728af40\">\n<p class=\"has-small-font-size\" id=\"ub-styled-box-bordered-content-\">Exemples :<\/p>\n\n\n\n<ul class=\"wp-block-list\">\n<li class=\"has-small-font-size\">Une masse <em>m <\/em>= 2,5 kg (la grandeur est la masse et la r\u00e9f\u00e9rence est le kilogramme).<\/li>\n\n\n\n<li class=\"has-small-font-size\">Une r\u00e9sistance \u00e9lectrique  <em>R<\/em> = 50 <math data-latex=\"\\Omega\"><semantics><mrow><mi mathvariant=\"normal\">\u03a9<\/mi><\/mrow><annotation encoding=\"application\/x-tex\">\\Omega<\/annotation><\/semantics><\/math> (la grandeur est la r\u00e9sistance \u00e9lectrique  et la r\u00e9f\u00e9rence est l'ohm).<\/li>\n\n\n\n<li class=\"has-small-font-size\">Un acier de duret\u00e9 de Rockwell <em>C<\/em> =  60 HRC. (la grandeur est la duret\u00e9 et la r\u00e9f\u00e9rence est l'\u00e9chelle de Rockwell HRC qui correspond \u00e0 la profondeur r\u00e9manente de p\u00e9n\u00e9tration d'un c\u00f4ne de diamant).<\/li>\n<\/ul>\n\n\n<\/div>\n\n\n<p class=\"has-medium-font-size\">Dans son trait\u00e9 d'\u00e9lectricit\u00e9 et de mag\u00e9tisme, James Clerk Maxwell (1831-1879) <span class=\"zp-InText-zp-ID--20404111-4EFUZV59--wp1 zp-InText-Citation loading\" rel=\"{ 'pages': 'np', 'items': '{20404111:4EFUZV59}', 'format': '(%a%, %d%, %p%)', 'brackets': '', 'etal': '', 'separator': '', 'and': '' }\"><\/span> d\u00e9fini les grandeurs physiques de la fa\u00e7on suivante :<\/p>\n\n\n\n<p class=\"has-medium-font-size\"><em>Toute expression d\u2019une grandeur physique est form\u00e9e de deux facteurs. L\u2019un d\u2019entre eux est le nom d\u2019une grandeur connue de m\u00eame nature que la quantit\u00e9 \u00e0 exprimer qui est pris comme \u00e9talon ou r\u00e9f\u00e9rence. L\u2019autre composante est le nombre de fois qu\u2019il faut reporter l\u2019\u00e9talon pour reproduire la grandeur consid\u00e9r\u00e9e. Techniquement, la grandeur \u00e9talon est appel\u00e9e unit\u00e9 et le nombre de reports est appel\u00e9e la valeur num\u00e9rique de la grandeur.<\/em><\/p>\n\n\n\n<p class=\"has-medium-font-size\">Les grandeurs pour lesquelles on ne peut d\u00e9finir d'\u00e9talon ne sont pas des grandeurs physiques. Pour les autres grandeurs, des \u00e9chelles permettent de les \u00e9valuer. L'\u00e9chelle visuelle analogique EVA permet de mesurer la douleur, l'\u00e9chelle Rockwell mesure la duret\u00e9 des aciers, l\u2019\u00e9chelle de Mohs mesure la duret\u00e9 des min\u00e9raux, l'\u00e9chelle de Mercalli mesure de l'intensit\u00e9 des s\u00e9ismes d'apr\u00e8s l'observation de leurs effets en un lieu donn\u00e9.<\/p>\n\n\n\n<p class=\"has-medium-font-size\" style=\"margin-right:var(--wp--preset--spacing--50);margin-left:var(--wp--preset--spacing--50)\">Les grandeurs sont de m\u00eame nature si elles sont  mutuellement comparables. La chaleur, le travail, l'\u00e9nergie cin\u00e9tique sont des grandeurs de m\u00eame nature \u00e0  savoir la nature de l'\u00e9nergie mais la grandeur moment d'une force et la grandeur \u00e9nergie ne sont pas consid\u00e9r\u00e9es comme des grandeurs de m\u00eame nature bien qu'elles aient la m\u00eame dimension.<\/p>\n\n\n\n<h3 class=\"wp-block-heading\">Syst\u00e8me de grandeurs<\/h3>\n\n\n<div style=\"border: 3px solid #004780; border-radius: 25px; background-color: #e3f7f7; \" class=\"ub-styled-box ub-bordered-box wp-block-ub-styled-box\" id=\"ub-styled-box-fbf09d21-1979-41a2-88ba-8ee263529a6d\">\n<p class=\"has-medium-font-size\" id=\"ub-styled-box-bordered-content-\">Un syst\u00e8me de grandeurs est un ensemble de grandeurs associ\u00e9es \u00e0 un ensemble de relations non contradictoires entre ces grandeurs. Les grandeurs de base forment un sous-ensemble choisi par convention dans un syst\u00e8me de grandeurs donn\u00e9 de fa\u00e7on \u00e0 ce qu'aucune grandeur du sous-ensemble ne puisse \u00eatre exprim\u00e9e en fonction des autres.<\/p>\n\n\n<\/div><\/div>\n\n\n<div style=\"border: 3px outset #fab300; border-radius: 26px; background-color: #fff6e2; \" class=\"ub-styled-box ub-bordered-box wp-block-ub-styled-box\" id=\"ub-styled-box-af3dc9fa-ac9d-4276-9941-6fef5e40eb97\">\n<p class=\"has-small-font-size\" id=\"ub-styled-box-bordered-content-\">Exemples :<\/p>\n\n\n\n<ul class=\"wp-block-list\">\n<li class=\"has-small-font-size\">la masse, la longueur et  le temps forment le syst\u00e8me des grandeurs de la m\u00e9canique. La vitesse, la force, l\u2019acc\u00e9l\u00e9ration, l\u2019\u00e9nergie, etc.  sont li\u00e9es \u00e0 ces grandeurs de base<\/li>\n\n\n\n<li class=\"has-small-font-size\">la quantit\u00e9 de mati\u00e8re, le volume, la pression et la temp\u00e9rature caract\u00e9rise un syst\u00e8me chimique.<\/li>\n\n\n\n<li class=\"has-small-font-size\">La duret\u00e9 de Rockwell  n'est pas consid\u00e9r\u00e9e comme faisant partie d'un syst\u00e8me de grandeurs, parce qu'elle n'est  reli\u00e9e \u00e0 d'autres grandeurs que par des relations empiriques..<\/li>\n<\/ul>\n\n\n<\/div><\/div>\n\n\n\n<p class=\"has-medium-font-size\">Une grandeur d\u00e9riv\u00e9e est une grandeu<strong>r <\/strong>d\u00e9finie, dans un syst\u00e8me de grandeurs, en fonction des grandeurs de base de ce syst\u00e8me.<\/p>\n\n\n\n<p class=\"has-medium-font-size\">Dans le syst\u00e8me masse, longueur et temps, les grandeurs suivantes sont des grandeurs d\u00e9riv\u00e9es :<\/p>\n\n\n\n<ul class=\"wp-block-list\">\n<li class=\"has-medium-font-size\" style=\"margin-top:0;margin-right:var(--wp--preset--spacing--50);margin-bottom:0;margin-left:var(--wp--preset--spacing--50)\">vitesse : <math data-latex=\"v=\\frac{\\ell}{t}\"><semantics><mrow><mi>v<\/mi><mo>=<\/mo><mfrac><mi>\u2113<\/mi><mi>t<\/mi><\/mfrac><\/mrow><annotation encoding=\"application\/x-tex\">v=\\frac{\\ell}{t}<\/annotation><\/semantics><\/math>  est d\u00e9finie \u00e0 partir de la longueur et du temps ;<\/li>\n\n\n\n<li class=\"has-medium-font-size\" style=\"margin-right:var(--wp--preset--spacing--50);margin-left:var(--wp--preset--spacing--50)\">l'acc\u00e9l\u00e9ration :  <math data-latex=\"a=\\frac{v}{t}=\\frac{\\ell}{t^2}\"><semantics><mrow><mi>a<\/mi><mo>=<\/mo><mfrac><mi>v<\/mi><mi>t<\/mi><\/mfrac><mo>=<\/mo><mfrac><mi>\u2113<\/mi><msup><mi>t<\/mi><mn>2<\/mn><\/msup><\/mfrac><\/mrow><annotation encoding=\"application\/x-tex\">a=\\frac{v}{t}=\\frac{\\ell}{t^2}<\/annotation><\/semantics><\/math>  est d\u00e9finie \u00e0 partir de la longueur et du temps ;<\/li>\n\n\n\n<li class=\"has-medium-font-size\" style=\"margin-right:var(--wp--preset--spacing--50);margin-left:var(--wp--preset--spacing--50)\">la force : <math data-latex=\"F =ma=m\\frac{\\ell}{t^2}\"><semantics><mrow><mi>F<\/mi><mo>=<\/mo><mi>m<\/mi><mi>a<\/mi><mo>=<\/mo><mi>m<\/mi><mfrac><mi>\u2113<\/mi><msup><mi>t<\/mi><mn>2<\/mn><\/msup><\/mfrac><\/mrow><annotation encoding=\"application\/x-tex\">F =ma=m\\frac{\\ell}{t^2}<\/annotation><\/semantics><\/math>  est d\u00e9finie \u00e0 partir de la masse, de la longueur et du temps <\/li>\n<\/ul>\n<\/div>\n\n\n\n<h3 class=\"wp-block-heading\">Dimension d'une grandeur<\/h3>\n\n\n<div style=\"border: 3px solid #004780; border-radius: 25px; background-color: #e3f7f7; \" class=\"ub-styled-box ub-bordered-box wp-block-ub-styled-box\" id=\"ub-styled-box-586aaa7a-54e7-4d93-9d54-50aecff873c8\">\n<p class=\"has-medium-font-size\" id=\"ub-styled-box-bordered-content-\">La dimension d'une grandeur exprime la d\u00e9pendance d'une grandeur par rapport aux grandeurs de base d'un syst\u00e8me de grandeurs sous la forme d'un produit de puissances de facteurs correspondant aux grandeurs de base, en omettant tout facteur num\u00e9rique. Par convention, la repr\u00e9sentation symbolique de la dimension d'une grandeur de base est une lettre majuscule unique en caract\u00e8re romain (droit) sans empattement. Par convention, la repr\u00e9sentation symbolique de la dimension d'une grandeur d\u00e9riv\u00e9e est le produit de puissances des dimensions des grandeurs de base conform\u00e9ment \u00e0 la d\u00e9finition de la grandeur d\u00e9riv\u00e9e. La dimension de la grandeur <em>Q <\/em> est not\u00e9e dim <em>Q<\/em>.<\/p>\n\n\n\n<p class=\"has-medium-font-size\">Les grandeurs de m\u00eame nature ont la m\u00eame dimension mais les grandeurs de m\u00eame dimension ne sont toutes de m\u00eame nature. Les grandeurs de dimensions diff\u00e9rentes ne sont pas de m\u00eame nature.<\/p>\n\n\n<\/div>\n\n<div style=\"border: 3px outset #fab300; border-radius: 26px; background-color: #fff6e2; \" class=\"ub-styled-box ub-bordered-box wp-block-ub-styled-box\" id=\"ub-styled-box-8761c26c-ca99-4765-b231-3d02df3087ea\">\n<p class=\"has-small-font-size\" id=\"ub-styled-box-bordered-content-\">Exemples :<\/p>\n\n\n\n<p class=\"has-small-font-size\">si on note <strong>M<\/strong>, <strong>L<\/strong>, <strong>T<\/strong>, les dimensions des grandeurs masse, longueur et temps alors :<\/p>\n\n\n\n<ul class=\"wp-block-list\">\n<li class=\"has-small-font-size\">dim <em>F<\/em>  = <strong>M.L.T<\/strong><sup>-2<\/sup> . Les exposants dimensionnels sont respectivement 1, 1 et -2.<\/li>\n\n\n\n<li class=\"has-small-font-size\">dim <em>E <\/em>= <strong>M.L<\/strong><sup>2<\/sup><strong>.T<\/strong><sup>-2<\/sup> . Les exposants dimensionnels sont respectivement 1, 2 et -2 (l'\u00e9nergie est de m\u00eame nature que le travail <code><span class=\"katex-eq\" data-katex-display=\"false\">W = F.\\ell<\/span><\/code>).<\/li>\n<\/ul>\n\n\n<\/div>\n\n\n<p class=\"has-medium-font-size\" style=\"margin-right:var(--wp--preset--spacing--50);margin-left:var(--wp--preset--spacing--50)\">Dans le syst\u00e8me international des grandeurs (International System of Quantities ISQ) \n<div id='zp-InTextBib-zotpress-8a78ea4e1e507fd0bdb1671e5f30fd77' class='zp-Zotpress zp-Zotpress-InTextBib wp-block-group zp-Post-1'>\r\n\t\t<span class=\"ZP_ITEM_KEY ZP_ATTR\">{20404111:GTVNKYYL};{20404111:4EFUZV59}<\/span>\r\n\t\t<span class=\"ZP_STYLE ZP_ATTR\">S9UGB9TQ<\/span>\r\n\t\t<span class=\"ZP_SORTBY ZP_ATTR\">default<\/span>\r\n\t\t<span class=\"ZP_ORDER ZP_ATTR\"><\/span>\r\n\t\t<span class=\"ZP_TITLE ZP_ATTR\"><\/span>\r\n\t\t<span class=\"ZP_SHOWIMAGE ZP_ATTR\"><\/span>\r\n\t\t<span class=\"ZP_SHOWTAGS ZP_ATTR\"><\/span>\r\n\t\t<span class=\"ZP_DOWNLOADABLE ZP_ATTR\"><\/span>\r\n\t\t<span class=\"ZP_NOTES ZP_ATTR\"><\/span>\r\n\t\t<span class=\"ZP_ABSTRACT ZP_ATTR\"><\/span>\r\n\t\t<span class=\"ZP_CITEABLE ZP_ATTR\"><\/span>\r\n\t\t<span class=\"ZP_TARGET ZP_ATTR\"><\/span>\r\n\t\t<span class=\"ZP_URLWRAP ZP_ATTR\"><\/span>\r\n\t\t<span class=\"ZP_FORCENUM ZP_ATTR\">0<\/span>\r\n\t\t<span class=\"ZP_HIGHLIGHT ZP_ATTR\"><\/span>\r\n\t\t<span class=\"ZP_POSTID ZP_ATTR\">1<\/span><div class='zp-List loading'>\n<div class=\"zp-SEO-Content\"><\/div><!-- .zp-zp-SEO-Content -->\n<\/div><!-- .zp-List --><\/div><!--.zp-Zotpress-->\n\nform\u00e9 de sept grandeurs de base longueur, masse, temps, intensit\u00e9 du courant \u00e9lectrique, temp\u00e9rature, quantit\u00e9 de mati\u00e8re et intensit\u00e9 lumineuse. Les symboles correspondant aux dimensions des grandeurs de base sont :<\/p>\n\n\n\n<figure class=\"wp-block-table aligncenter has-medium-font-size\"><table class=\"has-background\" style=\"background-color:#edecec;border-width:2px\"><tbody><tr><td><strong>Grandeur<\/strong><\/td><td class=\"has-text-align-center\" data-align=\"center\"><strong>Symbole<\/strong><\/td><td class=\"has-text-align-center\" data-align=\"center\"><strong>Dimension<\/strong><\/td><\/tr><tr><td>longueur<\/td><td class=\"has-text-align-center\" data-align=\"center\"><math data-latex=\"x, \\ell\"><semantics><mrow><mi>x<\/mi><mo separator=\"true\">,<\/mo><mi>\u2113<\/mi><\/mrow><annotation encoding=\"application\/x-tex\">x, \\ell<\/annotation><\/semantics><\/math><\/td><td class=\"has-text-align-center\" data-align=\"center\"><strong>L<\/strong><\/td><\/tr><tr><td>masse<\/td><td class=\"has-text-align-center\" data-align=\"center\"><math data-latex=\"m\"><semantics><mi>m<\/mi><annotation encoding=\"application\/x-tex\">m<\/annotation><\/semantics><\/math><\/td><td class=\"has-text-align-center\" data-align=\"center\"><strong>M<\/strong><\/td><\/tr><tr><td>temps<\/td><td class=\"has-text-align-center\" data-align=\"center\"><math data-latex=\"t\"><semantics><mi>t<\/mi><annotation encoding=\"application\/x-tex\">t<\/annotation><\/semantics><\/math><\/td><td class=\"has-text-align-center\" data-align=\"center\"><strong>T<\/strong><\/td><\/tr><tr><td>Intensit\u00e9 du courant \u00e9lectrique<\/td><td class=\"has-text-align-center\" data-align=\"center\"><math data-latex=\"i, I\"><semantics><mrow><mi>i<\/mi><mo separator=\"true\">,<\/mo><mi>I<\/mi><\/mrow><annotation encoding=\"application\/x-tex\">i, I<\/annotation><\/semantics><\/math><\/td><td class=\"has-text-align-center\" data-align=\"center\"><strong>I<\/strong><\/td><\/tr><tr><td>temp\u00e9rature<\/td><td class=\"has-text-align-center\" data-align=\"center\">T<\/td><td class=\"has-text-align-center\" data-align=\"center\"><code><span class=\"katex-eq\" data-katex-display=\"false\">\\Theta<\/span><\/code><\/td><\/tr><tr><td>quantit\u00e9 de mati\u00e8re<\/td><td class=\"has-text-align-center\" data-align=\"center\"><math data-latex=\"n\"><semantics><mi>n<\/mi><annotation encoding=\"application\/x-tex\">n<\/annotation><\/semantics><\/math><\/td><td class=\"has-text-align-center\" data-align=\"center\"><strong>N<\/strong><\/td><\/tr><tr><td>Intensit\u00e9 lumineuse<\/td><td class=\"has-text-align-center\" data-align=\"center\"><math data-latex=\"I_\\nu\"><semantics><msub><mi>I<\/mi><mi>\u03bd<\/mi><\/msub><annotation encoding=\"application\/x-tex\">I_\\nu<\/annotation><\/semantics><\/math><\/td><td class=\"has-text-align-center\" data-align=\"center\"><strong>J<\/strong><\/td><\/tr><\/tbody><\/table><\/figure>\n\n\n\n<p class=\"has-medium-font-size\">Dans le syst\u00e8me de grandeurs ISQ, la dimension d'une grandeur <em>Q <\/em> s'\u00e9crit : <\/p>\n\n\n\n<div class=\"wp-block-katex-display-block katex-eq\" data-katex-display=\"true\"><pre>\\mathrm{dim} \\,Q =\\mathrm{L}^\\alpha \\mathrm{M}^\\beta \\mathrm{T}^\\gamma \\mathrm{I}^\\delta \\mathrm{\\Theta}^\\epsilon \\mathrm{N}^\\zeta \\mathrm{J}^\\eta <\/pre><\/div>\n\n\n\n<p class=\"has-medium-font-size\"><code><span class=\"katex-eq\" data-katex-display=\"false\">\\alpha, \\beta, \\gamma,\\delta,\\epsilon,\\zeta,\\eta<\/span><\/code> sont les exposants dimensionnels qui sont entiers, rationnels ou nuls.<\/p>\n\n\n\n<p class=\"has-medium-font-size\" style=\"margin-right:var(--wp--preset--spacing--50);margin-left:var(--wp--preset--spacing--50)\">Si tous les exposants dimensionnels sont nuls, la grandeur est de dimension <strong>1<\/strong>. Dans le langage courant, on parle de grandeurs sans dimension. L'angle plan, l'angle solide, l'indice de r\u00e9fraction, la perm\u00e9abilit\u00e9 relative, la fraction massique, le facteur de frottement, le nombre de Mach sont des grandeurs de dimension <strong>1<\/strong> de m\u00eame que le nombre d'entit\u00e9s comme le nombre de tours dans une bobine, le nombre de mol\u00e9cules dans un sp\u00e9cimen donn\u00e9, la d\u00e9g\u00e9n\u00e9rescence des niveaux d'\u00e9nergie d'un syst\u00e8me quantique. <\/p>\n\n\n\n<h2 class=\"wp-block-heading\">Unit\u00e9s de mesure<\/h2>\n\n\n\n<h3 class=\"wp-block-heading\">D\u00e9finitions<\/h3>\n\n\n<div style=\"border: 3px solid #004780; border-radius: 25px; background-color: #e3f7f7; \" class=\"ub-styled-box ub-bordered-box wp-block-ub-styled-box\" id=\"ub-styled-box-59b5dced-6241-4dd8-852c-323e8f463c67\">\n<p class=\"has-medium-font-size\" id=\"ub-styled-box-bordered-content-\">Une unit\u00e9 de mesure est une grandeur scalaire r\u00e9elle, d\u00e9finie et adopt\u00e9e par convention, \u00e0 laquelle on peut comparer toute autre grandeur de m\u00eame nature pour exprimer le rapport des deux grandeurs sous forme d'un nombre.<\/p>\n\n\n\n<p class=\"has-medium-font-size\">Les noms unit\u00e9s sont imprim\u00e9s en caract\u00e8res droits sans majuscule sauf en d\u00e9but de phrase.<\/p>\n\n\n\n<p class=\"has-medium-font-size\">Les unit\u00e9s des grandeurs sans dimension sont des nombres, g\u00e9n\u00e9ralement 1. Dans certains cas, on leur donne des noms sp\u00e9ciaux, par exemple radian, st\u00e9radian et d\u00e9cibel, ou on les exprime par des quotients comme le milligramme par kilogramme \u00e9gal \u00e0 10<sup>\u20136<\/sup>.<\/p>\n\n\n<\/div>\n\n<div style=\"border: 3px outset #fab300; border-radius: 26px; background-color: #fff6e2; \" class=\"ub-styled-box ub-bordered-box wp-block-ub-styled-box\" id=\"ub-styled-box-490ae8f2-53de-482e-b54a-4c9808e02e83\">\n<p class=\"has-small-font-size\" id=\"ub-styled-box-bordered-content-\">Exemples :<\/p>\n\n\n\n<ul class=\"wp-block-list\">\n<li class=\"has-small-font-size\">Le newton m\u00e8tre et le joule sont les unit\u00e9s du moment d'une force et de l'\u00e9nergie qui sont des grandeurs de m\u00eame dimension mais de nature diff\u00e9rente.<\/li>\n\n\n\n<li class=\"has-small-font-size\">l'unit\u00e9 seconde \u00e0 la puissance -1 (1\/s) est  appel\u00e9e hertz (Hz) pour les fr\u00e9quences et becquerel (Bq) pour les activit\u00e9s de radionucl\u00e9ides.<\/li>\n\n\n\n<li class=\"has-small-font-size\">l'\u00e9criture correcte de l'unit\u00e9 de temp\u00e9rature dont le symbole est \u00b0C est degr\u00e9 Celsius. l'unit\u00e9 degr\u00e9 commence par la lettre minuscule d et Celsius comme par la lettre majuscule C car Celsius est un nom propre.<\/li>\n<\/ul>\n\n\n<\/div>\n\n\n<h3 class=\"wp-block-heading\">Le syst\u00e8me international d'unit\u00e9s<\/h3>\n\n\n<div style=\"border: 3px solid #004780; border-radius: 25px; background-color: #e3f7f7; \" class=\"ub-styled-box ub-bordered-box wp-block-ub-styled-box\" id=\"ub-styled-box-b1c4ecce-9ba7-41c3-81b4-8cf53c4a3ccf\">\n<p class=\"has-medium-font-size\" id=\"ub-styled-box-bordered-content-\">Le syst\u00e8me d'unit\u00e9s, fond\u00e9 sur le Syst\u00e8me international de grandeurs (ISQ), comportant les noms et symboles des unit\u00e9s, une s\u00e9rie de pr\u00e9fixes avec leurs noms et symboles, ainsi que des r\u00e8gles pour leur emploi, adopt\u00e9 par la Conf\u00e9rence g\u00e9n\u00e9rale des poids et mesures (CGPM).<\/p>\n\n\n<\/div>\n\n<div style=\"border: 3px outset #fab300; border-radius: 26px; background-color: #fff6e2; \" class=\"ub-styled-box ub-bordered-box wp-block-ub-styled-box\" id=\"ub-styled-box-de10e9b7-0afc-4f75-a4cd-d0539fb1772f\">\n<p class=\"has-small-font-size\" id=\"ub-styled-box-bordered-content-\">Autres syst\u00e8me d'unit\u00e9s :<\/p>\n\n\n\n<ul class=\"wp-block-list\">\n<li class=\"has-small-font-size\">le syst\u00e8me CGS : centim\u00e8tre, gramme, seconde. Dans ce syst\u00e8me, l'unit\u00e9 d\u2019\u00e9nergie est le erg. L'unit\u00e9 de pression est la barye (ba) : 10<sup>6<\/sup> ba = 1 bar.<\/li>\n\n\n\n<li class=\"has-small-font-size\">Les syst\u00e8mes imp\u00e9riaux et am\u00e9ricain. Ils sont bas\u00e9s sur le pied (unit\u00e9 de longueur) divis\u00e9 en 12 pouces, la livre  (unit\u00e9 de longueur) divis\u00e9e en 16 onces et la seconde (unit\u00e9 de temps). L'unit\u00e9 de pression est le psi (pound per square inch). A not\u00e9 que la num\u00e9ration dans ces syst\u00e8mes peut \u00eatre duod\u00e9cimal ou hexad\u00e9cimal : 1 pied = 12 pouces = 144 lignes = 1728 points.<\/li>\n<\/ul>\n\n\n<\/div>\n\n\n<p class=\"has-medium-font-size\">Les noms et les symboles des sept <strong>unit\u00e9s de base <\/strong>sont donn\u00e9s dans le tableau suivant.<\/p>\n\n\n\n<figure class=\"wp-block-table aligncenter has-medium-font-size\"><table class=\"has-background\" style=\"background-color:#edecec;border-width:2px\"><tbody><tr><td><strong>Grandeur<\/strong><\/td><td class=\"has-text-align-center\" data-align=\"center\"><strong>nom<\/strong><\/td><td class=\"has-text-align-center\" data-align=\"center\"><strong>Symbole<\/strong><\/td><\/tr><tr><td>longueur<\/td><td class=\"has-text-align-center\" data-align=\"center\">m\u00e8tre<\/td><td class=\"has-text-align-center\" data-align=\"center\">m<\/td><\/tr><tr><td>masse<\/td><td class=\"has-text-align-center\" data-align=\"center\">kilogramme<\/td><td class=\"has-text-align-center\" data-align=\"center\">kg<\/td><\/tr><tr><td>temps<\/td><td class=\"has-text-align-center\" data-align=\"center\">seconde<\/td><td class=\"has-text-align-center\" data-align=\"center\">s<\/td><\/tr><tr><td>Intensit\u00e9 du courant \u00e9lectrique<\/td><td class=\"has-text-align-center\" data-align=\"center\">amp\u00e8re<\/td><td class=\"has-text-align-center\" data-align=\"center\">A<\/td><\/tr><tr><td>temp\u00e9rature<\/td><td class=\"has-text-align-center\" data-align=\"center\">kelvin<\/td><td class=\"has-text-align-center\" data-align=\"center\">K<\/td><\/tr><tr><td>quantit\u00e9 de mati\u00e8re<\/td><td class=\"has-text-align-center\" data-align=\"center\">mole<\/td><td class=\"has-text-align-center\" data-align=\"center\">mol<\/td><\/tr><tr><td>Intensit\u00e9 lumineuse<\/td><td class=\"has-text-align-center\" data-align=\"center\">candela<\/td><td class=\"has-text-align-center\" data-align=\"center\">cd<\/td><\/tr><\/tbody><\/table><\/figure>\n\n\n\n<p class=\"has-medium-font-size\">Les d\u00e9finitions des unit\u00e9s de base su Syst\u00e8me International <strong>SI<\/strong> ont \u00e9t\u00e9 r\u00e9vis\u00e9es la CGPM (Conf\u00e9rence G\u00e9n\u00e9rale des Poids et Mesures) en novembre 2018 et les nouvelles d\u00e9finitions ont pris effet le 20 mai 2019,sont bas\u00e9s sur 7 constantes fondamentales de la nature :<\/p>\n\n\n\n<ul class=\"wp-block-list\">\n<li class=\"has-medium-font-size\">la fr\u00e9quence de la transition hyperfine de l\u2019\u00e9tat fondamental de l\u2019atome de c\u00e9sium 133 non perturb\u00e9, <math data-latex=\"\\Delta \\nu_{Cs}\"><semantics><mrow><mrow><mi mathvariant=\"normal\">\u0394<\/mi><\/mrow><msub><mi>\u03bd<\/mi><mrow><mi>C<\/mi><mi>s<\/mi><\/mrow><\/msub><\/mrow><annotation encoding=\"application\/x-tex\">\\Delta \\nu_{Cs}<\/annotation><\/semantics><\/math>, est \u00e9gale \u00e0 9 192 631 770 Hz,<\/li>\n\n\n\n<li class=\"has-medium-font-size\">la vitesse de la lumi\u00e8re dans le vide, <em>c<\/em>, est \u00e9gale \u00e0 299 792 458 m\/s,<\/li>\n\n\n\n<li class=\"has-medium-font-size\">la constante de Planck, <math data-latex=\"h\"><semantics><mi>h<\/mi><annotation encoding=\"application\/x-tex\">h<\/annotation><\/semantics><\/math>, est \u00e9gale \u00e0 6,626 070 15 \u00d7 10<sup>\u221234<\/sup> J s,<\/li>\n\n\n\n<li class=\"has-medium-font-size\">la charge \u00e9l\u00e9mentaire, <math data-latex=\"e\"><semantics><mi>e<\/mi><annotation encoding=\"application\/x-tex\">e<\/annotation><\/semantics><\/math>, est \u00e9gale \u00e0 1,602 176 634 \u00d7 10<sup>\u221219<\/sup> C,<\/li>\n\n\n\n<li class=\"has-medium-font-size\">la constante de Boltzmann, <math data-latex=\"k\"><semantics><mi>k<\/mi><annotation encoding=\"application\/x-tex\">k<\/annotation><\/semantics><\/math>, est \u00e9gale \u00e0 1,380 649 \u00d7 10<sup>\u221223<\/sup> J\/K,<\/li>\n\n\n\n<li class=\"has-medium-font-size\">la constante d\u2019Avogadro, <math data-latex=\"N_A\"><semantics><msub><mi>N<\/mi><mi>A<\/mi><\/msub><annotation encoding=\"application\/x-tex\">N_A<\/annotation><\/semantics><\/math>, est \u00e9gale \u00e0 6,022 140 76 \u00d7 10<sup>23 <\/sup>mol<sup>\u22121<\/sup>,<\/li>\n\n\n\n<li class=\"has-medium-font-size\">l\u2019efficacit\u00e9 lumineuse d\u2019un rayonnement monochromatique de fr\u00e9quence 540 <math data-latex=\"\\times\"><semantics><mo lspace=\"0em\" rspace=\"0em\">\u00d7<\/mo><annotation encoding=\"application\/x-tex\">\\times<\/annotation><\/semantics><\/math> 10<sup>12<\/sup> Hz, <math data-latex=\"K_{cd}\"><semantics><msub><mi>K<\/mi><mrow><mi>c<\/mi><mi>d<\/mi><\/mrow><\/msub><annotation encoding=\"application\/x-tex\">K_{cd}<\/annotation><\/semantics><\/math>, est \u00e9gale \u00e0 683 lm\/W.<\/li>\n<\/ul>\n\n\n\n<p class=\"has-medium-font-size\">On retrouvera les d\u00e9finitions des 7 unit\u00e9s de base sur la brochure du SI \u00e9dit\u00e9e par le <a href=\"http:\/\/www.bipm.org\">Bureau International des Poids et Mesures<\/a> o\u00f9 elle est disponible en ligne.<\/p>\n\n\n\n<h3 class=\"wp-block-heading\">Unit\u00e9s d\u00e9riv\u00e9es<\/h3>\n\n\n\n<p class=\"has-medium-font-size\">Les unit\u00e9s d\u00e9riv\u00e9es sont d\u00e9finies comme des produits de puissances des unit\u00e9s de base. Lorsque le facteur num\u00e9rique de ce produit est un, les unit\u00e9s d\u00e9riv\u00e9es sont appel\u00e9es <em>unit\u00e9s d\u00e9riv\u00e9es coh\u00e9rentes<\/em>. Certaines unit\u00e9s d\u00e9riv\u00e9es coh\u00e9rentes du SI ont re\u00e7u un nom sp\u00e9cial. Elles sont au nombre de 22 : radian, st\u00e9radian, hertz, newton, pascal, joule, watt, coulomb, volt, farad, ohm, siemens, weber,  tesla, henry, degr\u00e9 Celsius, lumen, lux, becquerel, gray, sievert et katal. Les sept unit\u00e9s de base et les unit\u00e9s d\u00e9riv\u00e9es coh\u00e9rentes constituent la partie centrale de l\u2019ensemble des unit\u00e9s du SI : toutes les autres unit\u00e9s du SI sont des combinaisons de certaines de ces 29 unit\u00e9s.<\/p>\n\n\n\n<p class=\"has-medium-font-size\">On trouvera dans la brochure <a href=\"https:\/\/doi.org\/10.59161\/AUEZ1291\">Le Syst\u00e8me international d'unit\u00e9s<\/a> \u00e9dit\u00e9 par le BIPM la d\u00e9finition de l'ensemble de ces unit\u00e9s d\u00e9riv\u00e9es.<\/p>\n\n\n\n<p class=\"has-medium-font-size\">Exemples :<\/p>\n\n\n\n<ul class=\"wp-block-list has-medium-font-size\">\n<li>vitesse : <math data-latex=\"v =\"><semantics><mrow><mi>v<\/mi><mo>=<\/mo><\/mrow><annotation encoding=\"application\/x-tex\">v =<\/annotation><\/semantics><\/math>3,6 m s<sup>-1<\/sup>,<\/li>\n\n\n\n<li>concentration de quantit\u00e9 de mati\u00e8re : <math data-latex=\"c\"><semantics><mi>c<\/mi><annotation encoding=\"application\/x-tex\">c<\/annotation><\/semantics><\/math> = 1,22 mol m<sup>-3<\/sup>,<\/li>\n\n\n\n<li>Camp magn\u00e9tique : <math data-latex=\"H\"><semantics><mi>H<\/mi><annotation encoding=\"application\/x-tex\">H<\/annotation><\/semantics><\/math> = 4,2 A m<sup>-1<\/sup>,<\/li>\n\n\n\n<li>Induction magn\u00e9tique : <math data-latex=\"B \"><semantics><mi>B<\/mi><annotation encoding=\"application\/x-tex\">B <\/annotation><\/semantics><\/math> = 0,2 T,<\/li>\n\n\n\n<li>conductivit\u00e9 thermique : <math data-latex=\"\\lambda \"><semantics><mi>\u03bb<\/mi><annotation encoding=\"application\/x-tex\">\\lambda <\/annotation><\/semantics><\/math> = 0,056 W m<sup>-1<\/sup> K<sup>-1<\/sup>,<\/li>\n\n\n\n<li>permittivit\u00e9 : <math data-latex=\"\\epsilon_0 \"><semantics><msub><mi>\u03f5<\/mi><mn>0<\/mn><\/msub><annotation encoding=\"application\/x-tex\">\\epsilon_0 <\/annotation><\/semantics><\/math> =8,854&nbsp;187&nbsp;82&nbsp;<math data-latex=\"\\times \"><semantics><mo lspace=\"0em\" rspace=\"0em\">\u00d7<\/mo><annotation encoding=\"application\/x-tex\">\\times <\/annotation><\/semantics><\/math>\u202f10<sup>\u221212<\/sup> &nbsp;F&nbsp;m<sup>\u22121<\/sup> <\/li>\n<\/ul>\n\n\n\n<h3 class=\"wp-block-heading\">\u00c9criture des unit\u00e9s<\/h3>\n\n\n\n<p class=\"has-medium-font-size\">Les pr\u00e9fixes SI qui repr\u00e9sentent strictement des puissances de 10 pour les multiples et sous- multiples des unit\u00e9s<strong> <\/strong>sont donn\u00e9s dans le tableau ci-dessous :<\/p>\n\n\n\n<figure class=\"wp-block-table aligncenter has-medium-font-size\"><table class=\"has-background\" style=\"background-color:#edecec;border-width:2px\"><tbody><tr><td><strong>facteur<\/strong><\/td><td class=\"has-text-align-center\" data-align=\"center\"><strong>nom<\/strong><\/td><td class=\"has-text-align-center\" data-align=\"center\"><strong>Symbole<\/strong><\/td><\/tr><tr><td>10<sup>30<\/sup><\/td><td class=\"has-text-align-center\" data-align=\"center\">quetta<\/td><td class=\"has-text-align-center\" data-align=\"center\">Q<\/td><\/tr><tr><td>10<sup>27<\/sup><\/td><td class=\"has-text-align-center\" data-align=\"center\">ronna<\/td><td class=\"has-text-align-center\" data-align=\"center\">R<\/td><\/tr><tr><td>10<sup>24<\/sup><\/td><td class=\"has-text-align-center\" data-align=\"center\">yotta<\/td><td class=\"has-text-align-center\" data-align=\"center\">Y<\/td><\/tr><tr><td>10<sup>21<\/sup><\/td><td class=\"has-text-align-center\" data-align=\"center\">zetta<\/td><td class=\"has-text-align-center\" data-align=\"center\">Z<\/td><\/tr><tr><td>10<sup>18<\/sup><\/td><td class=\"has-text-align-center\" data-align=\"center\">exa<\/td><td class=\"has-text-align-center\" data-align=\"center\">E<\/td><\/tr><tr><td>10<sup>15<\/sup><\/td><td class=\"has-text-align-center\" data-align=\"center\">p\u00e9ta<\/td><td class=\"has-text-align-center\" data-align=\"center\">P<\/td><\/tr><tr><td>10<sup>12<\/sup><\/td><td class=\"has-text-align-center\" data-align=\"center\">t\u00e9ra<\/td><td class=\"has-text-align-center\" data-align=\"center\">T<\/td><\/tr><tr><td>10<sup>9<\/sup><\/td><td class=\"has-text-align-center\" data-align=\"center\">giga<\/td><td class=\"has-text-align-center\" data-align=\"center\">G<\/td><\/tr><tr><td>10<sup>6<\/sup><\/td><td class=\"has-text-align-center\" data-align=\"center\">m\u00e9ga<\/td><td class=\"has-text-align-center\" data-align=\"center\">M<\/td><\/tr><tr><td>10<sup>3<\/sup><\/td><td class=\"has-text-align-center\" data-align=\"center\">kilo<\/td><td class=\"has-text-align-center\" data-align=\"center\">k<\/td><\/tr><tr><td>10<sup>2<\/sup><\/td><td class=\"has-text-align-center\" data-align=\"center\">hecto<\/td><td class=\"has-text-align-center\" data-align=\"center\">h<\/td><\/tr><tr><td>10<sup>1<\/sup><\/td><td class=\"has-text-align-center\" data-align=\"center\">d\u00e9ca<\/td><td class=\"has-text-align-center\" data-align=\"center\">da<\/td><\/tr><tr><td>10<sup>-1<\/sup><\/td><td class=\"has-text-align-center\" data-align=\"center\">d\u00e9ci<\/td><td class=\"has-text-align-center\" data-align=\"center\">d<\/td><\/tr><tr><td>10<sup>-2<\/sup><\/td><td class=\"has-text-align-center\" data-align=\"center\">centi<\/td><td class=\"has-text-align-center\" data-align=\"center\">c<\/td><\/tr><tr><td>10<sup>-3<\/sup><\/td><td class=\"has-text-align-center\" data-align=\"center\">milli<\/td><td class=\"has-text-align-center\" data-align=\"center\">m<\/td><\/tr><tr><td>10<sup>-6<\/sup><\/td><td class=\"has-text-align-center\" data-align=\"center\">micro<\/td><td class=\"has-text-align-center\" data-align=\"center\"><math data-latex=\"\\mathrm{\\mu}\"><semantics><mrow><mi mathvariant=\"normal\">\u03bc<\/mi><\/mrow><annotation encoding=\"application\/x-tex\">\\mathrm{\\mu}<\/annotation><\/semantics><\/math><\/td><\/tr><tr><td>10<sup>-9<\/sup><\/td><td class=\"has-text-align-center\" data-align=\"center\">nano<\/td><td class=\"has-text-align-center\" data-align=\"center\">n<\/td><\/tr><tr><td>10<sup>-12<\/sup><\/td><td class=\"has-text-align-center\" data-align=\"center\">pico<\/td><td class=\"has-text-align-center\" data-align=\"center\">p<\/td><\/tr><tr><td>10<sup>-15<\/sup><\/td><td class=\"has-text-align-center\" data-align=\"center\">femto<\/td><td class=\"has-text-align-center\" data-align=\"center\">f<\/td><\/tr><tr><td>10<sup>-18<\/sup><\/td><td class=\"has-text-align-center\" data-align=\"center\">atto<\/td><td class=\"has-text-align-center\" data-align=\"center\">a<\/td><\/tr><tr><td>10<sup>-21<\/sup><\/td><td class=\"has-text-align-center\" data-align=\"center\">zepto<\/td><td class=\"has-text-align-center\" data-align=\"center\">z<\/td><\/tr><tr><td>10<sup>-24<\/sup><\/td><td class=\"has-text-align-center\" data-align=\"center\">yocto<\/td><td class=\"has-text-align-center\" data-align=\"center\">y<\/td><\/tr><tr><td>10<sup>-27<\/sup><\/td><td class=\"has-text-align-center\" data-align=\"center\">ronto<\/td><td class=\"has-text-align-center\" data-align=\"center\">r<\/td><\/tr><tr><td>10<sup>-30<\/sup><\/td><td class=\"has-text-align-center\" data-align=\"center\">quecto<\/td><td class=\"has-text-align-center\" data-align=\"center\">q<\/td><\/tr><\/tbody><\/table><\/figure>\n\n\n\n<p class=\"has-medium-font-size\">On ne doit pas  utiliser les pr\u00e9fixes SI pour des puissances de 2. Par exemple, il convient de ne pas utiliser 1 kilobit pour repr\u00e9senter 1 024 bits (210 bits), qui est 1 kibibit. De m\u00eame la capacit\u00e9 d'un disque dur de 2 To doit \u00eatre nomm\u00e9e 2 Tio (2 t\u00e9bioctets).<\/p>\n\n\n\n<p class=\"has-medium-font-size\">Les r\u00e8gles classiques de multiplication ou de division alg\u00e9briques s\u2019appliquent pour former les produits et quotients de symboles d\u2019unit\u00e9s. La multiplication doit \u00eatre indiqu\u00e9e par une espace ou un point \u00e0 mi-hauteur centr\u00e9 (<math data-latex=\"\\cdot\"><semantics><mo lspace=\"0em\" rspace=\"0em\">\u22c5<\/mo><annotation encoding=\"application\/x-tex\">\\cdot<\/annotation><\/semantics><\/math>) pour \u00e9viter que certains pr\u00e9fixes soient interpr\u00e9t\u00e9s \u00e0 tort comme un symbole d\u2019unit\u00e9. La division est indiqu\u00e9e par une ligne horizontale, par une barre oblique (\/) ou par des exposants n\u00e9gatifs. Lorsque l\u2019on combine plusieurs symboles d\u2019unit\u00e9s, il faut prendre soin d\u2019\u00e9viter toute ambigu\u00eft\u00e9 en utilisant par exemple des crochets, des parenth\u00e8ses ou des exposants n\u00e9gatifs. Il ne faut pas utiliser plus d\u2019une barre oblique dans une expression donn\u00e9e s\u2019il n\u2019y a pas de parenth\u00e8ses pour lever toute ambigu\u00eft\u00e9.<\/p>\n\n\n\n<p class=\"has-medium-font-size\">Il y a toujours un espace entre le nombre et l'unit\u00e9 sauf pour le degr\u00e9 de l'angle plan. Les nombres comportant un grand nombre de chiffres peuvent \u00eatre partag\u00e9s en tranches de trois chiffres, s\u00e9par\u00e9es par une espace, afin de faciliter la lecture. Ces tranches ne sont jamais s\u00e9par\u00e9es par des points, ni par des virgules. Pour les nombres entre +1 et -1, le s\u00e9parateur d\u00e9cimal est pr\u00e9c\u00e9d\u00e9 d'un z\u00e9ro.<\/p>\n\n\n\n<p>Exemples :<\/p>\n\n\n\n<ul class=\"wp-block-list has-medium-font-size\">\n<li>longueur : <math data-latex=\"\\ell\"><semantics><mi>\u2113<\/mi><annotation encoding=\"application\/x-tex\">\\ell<\/annotation><\/semantics><\/math> = 1,54 cm = 154 cm , <math data-latex=\"x = -0,678\\,943\\,2\\;\\mathrm{m}\"><semantics><mrow><mi>x<\/mi><mo>=<\/mo><mo form=\"prefix\" stretchy=\"false\">\u2212<\/mo><mn>0,678<\/mn><mspace width=\"0.1667em\"><\/mspace><mn>943<\/mn><mspace width=\"0.1667em\"><\/mspace><mn>2<\/mn><mspace width=\"0.2778em\"><\/mspace><mrow><mi mathvariant=\"normal\">m<\/mi><\/mrow><\/mrow><annotation encoding=\"application\/x-tex\">x = -0,678\\,943\\,2\\;\\mathrm{m}<\/annotation><\/semantics><\/math><\/li>\n\n\n\n<li>masse : <math data-latex=\"m\"><semantics><mi>m<\/mi><annotation encoding=\"application\/x-tex\">m<\/annotation><\/semantics><\/math> = 1,54 g = 1,54<math data-latex=\"\\times 10^{-3}\"><semantics><mrow><mo>\u00d7<\/mo><msup><mn>10<\/mn><mrow><mo lspace=\"0em\" rspace=\"0em\">\u2212<\/mo><mn>3<\/mn><\/mrow><\/msup><\/mrow><annotation encoding=\"application\/x-tex\">\\times 10^{-3}<\/annotation><\/semantics><\/math> kg , on ne doit pas employer <math data-latex=\"m\"><semantics><mi>m<\/mi><annotation encoding=\"application\/x-tex\">m<\/annotation><\/semantics><\/math> = 1,54 mkg  (2 pr\u00e9fixes),<\/li>\n\n\n\n<li>imp\u00e9dance complexe : <math data-latex=\"\\underline Z = (5+3\\mathrm{j}) \\;\\Omega\"><semantics><mrow><menclose notation=\"bottom\" class=\"tml-underline\"><mi>Z<\/mi><\/menclose><mo>=<\/mo><mo form=\"prefix\" stretchy=\"false\">(<\/mo><mn>5<\/mn><mo>+<\/mo><mn>3<\/mn><mrow><mi mathvariant=\"normal\">j<\/mi><\/mrow><mo form=\"postfix\" stretchy=\"false\">)<\/mo><mspace width=\"0.2778em\"><\/mspace><mrow><mi mathvariant=\"normal\">\u03a9<\/mi><\/mrow><\/mrow><annotation encoding=\"application\/x-tex\">\\underline Z = (5+3\\mathrm{j}) \\;\\Omega<\/annotation><\/semantics><\/math>,<\/li>\n\n\n\n<li>indice de r\u00e9fraction : <math data-latex=\"n\"><semantics><mi>n<\/mi><annotation encoding=\"application\/x-tex\">n<\/annotation><\/semantics><\/math>=1,32<\/li>\n\n\n\n<li>angle : <math data-latex=\"\\alpha = 12,3^\\circ\"><semantics><mrow><mi>\u03b1<\/mi><mo>=<\/mo><mn>12<\/mn><mo separator=\"true\">,<\/mo><msup><mn>3<\/mn><mo form=\"prefix\" stretchy=\"false\">\u2218<\/mo><\/msup><\/mrow><annotation encoding=\"application\/x-tex\">\\alpha = 12,3^\\circ<\/annotation><\/semantics><\/math> (pas d'espace entre le nombre et l'unit\u00e9)<\/li>\n\n\n\n<li>temp\u00e9rature : <math data-latex=\"T\"><semantics><mi>T<\/mi><annotation encoding=\"application\/x-tex\">T<\/annotation><\/semantics><\/math> = -15 \u00b0C (un espace entre la valeur et le symbole \u00b0C),<\/li>\n\n\n\n<li>molalit\u00e9 d'un ion  dans un sp\u00e9cimen donn\u00e9 d'eau : <math data-latex=\"c\"><semantics><mi>c<\/mi><annotation encoding=\"application\/x-tex\">c<\/annotation><\/semantics><\/math> = 1,76 \u03bcmol\/kg,<\/li>\n\n\n\n<li>composante d'une force : <math data-latex=\"(F_x;F_y;F_z) = (12,2; 56,7;31,4) \\;\\mathrm{N}\"><semantics><mrow><mo form=\"prefix\" stretchy=\"false\">(<\/mo><msub><mi>F<\/mi><mi>x<\/mi><\/msub><mo separator=\"true\">;<\/mo><msub><mi>F<\/mi><mi>y<\/mi><\/msub><mo separator=\"true\">;<\/mo><msub><mi>F<\/mi><mi>z<\/mi><\/msub><mo form=\"postfix\" stretchy=\"false\">)<\/mo><mo>=<\/mo><mo form=\"prefix\" stretchy=\"false\">(<\/mo><mn>12,2<\/mn><mo separator=\"true\">;<\/mo><mn>56,7<\/mn><mo separator=\"true\">;<\/mo><mn>31,4<\/mn><mo form=\"postfix\" stretchy=\"false\">)<\/mo><mspace width=\"0.2778em\"><\/mspace><mrow><mi mathvariant=\"normal\">N<\/mi><\/mrow><\/mrow><annotation encoding=\"application\/x-tex\">(F_x;F_y;F_z) = (12,2; 56,7;31,4) \\;\\mathrm{N}<\/annotation><\/semantics><\/math>,<\/li>\n\n\n\n<li>\u00e9nergie : <math data-latex=\"W\"><semantics><mi>W<\/mi><annotation encoding=\"application\/x-tex\">W<\/annotation><\/semantics><\/math> = 43 279,168 29(54) J. Le nombre entre parenth\u00e8se indique la valeur num\u00e9rique de l'incertitude-type sur les deux derniers chiffres de la valeur estim\u00e9e.<\/li>\n<\/ul>\n\n\n\n<h3 class=\"wp-block-heading\"><strong>Unit\u00e9s en dehors du SI dont l\u2019usage est accept\u00e9 avec le SI<\/strong><\/h3>\n\n\n\n<p class=\"has-medium-font-size\">Certaines unit\u00e9s en dehors du SI sont tr\u00e8s utilis\u00e9es et continueront selon toute vraisemblance \u00e0 l\u2019\u00eatre pendant de nombreuses ann\u00e9es. C\u2019est la raison pour laquelle le CIPM a accept\u00e9 que certaines unit\u00e9s en dehors du SI soient utilis\u00e9es avec le SI. Elles figurent dans le tableau ci-dessous :<\/p>\n\n\n\n<figure class=\"wp-block-table aligncenter has-medium-font-size\"><table class=\"has-background\" style=\"background-color:#edecec;border-width:2px\"><tbody><tr><td><strong>Grandeur<\/strong><\/td><td class=\"has-text-align-left\" data-align=\"left\"><strong>nom<\/strong><\/td><td class=\"has-text-align-center\" data-align=\"center\"><strong>Symbole<\/strong><\/td><td class=\"has-text-align-center\" data-align=\"center\"><strong>Valeur en unit\u00e9 SI<\/strong><\/td><\/tr><tr><td>temps<\/td><td class=\"has-text-align-left\" data-align=\"left\">minute<br>heure<br>jour<\/td><td class=\"has-text-align-center\" data-align=\"center\">min<br>h<br>d<\/td><td class=\"has-text-align-center\" data-align=\"center\">1 min = 60s<br>1 h = 60 min = 3600 s<br>1 d = 24 h = 86 400 s<\/td><\/tr><tr><td>longueur<\/td><td class=\"has-text-align-left\" data-align=\"left\">unit\u00e9 astronomique<\/td><td class=\"has-text-align-center\" data-align=\"center\">au<\/td><td class=\"has-text-align-center\" data-align=\"center\">1 au = 149 597 870 700 m<\/td><\/tr><tr><td>angle plan et de phase<\/td><td class=\"has-text-align-left\" data-align=\"left\">degr\u00e9<br>minute<br>seconde<\/td><td class=\"has-text-align-center\" data-align=\"center\">\u00b0<br><math data-latex=\"'\"><semantics><msup><mrow><\/mrow><mo lspace=\"0em\" rspace=\"0em\" class=\"tml-prime\">\u2032<\/mo><\/msup><annotation encoding=\"application\/x-tex\">'<\/annotation><\/semantics><\/math><br><math data-latex=\"''\"><semantics><msup><mrow><\/mrow><mrow><mo lspace=\"0em\" rspace=\"0em\" class=\"tml-prime\">\u2032<\/mo><mo lspace=\"0em\" rspace=\"0em\" class=\"tml-prime\">\u2032<\/mo><\/mrow><\/msup><annotation encoding=\"application\/x-tex\">''<\/annotation><\/semantics><\/math><\/td><td class=\"has-text-align-center\" data-align=\"center\">1\u00b0 = <math data-latex=\"\\left({\\pi}\/{180}\\right)\"><semantics><mrow><mo fence=\"true\" form=\"prefix\">(<\/mo><mi>\u03c0<\/mi><mi>\/<\/mi><mn>180<\/mn><mo fence=\"true\" form=\"postfix\">)<\/mo><\/mrow><annotation encoding=\"application\/x-tex\">\\left({\\pi}\/{180}\\right)<\/annotation><\/semantics><\/math> rad<br>1<math data-latex=\"'\"><semantics><msup><mrow><\/mrow><mo lspace=\"0em\" rspace=\"0em\" class=\"tml-prime\">\u2032<\/mo><\/msup><annotation encoding=\"application\/x-tex\">'<\/annotation><\/semantics><\/math>= <math data-latex=\"\\left({\\pi}\/{10\\,800}\\right)\"><semantics><mrow><mo fence=\"true\" form=\"prefix\">(<\/mo><mi>\u03c0<\/mi><mi>\/<\/mi><mrow><mn>10<\/mn><mspace width=\"0.1667em\"><\/mspace><mn>800<\/mn><\/mrow><mo fence=\"true\" form=\"postfix\">)<\/mo><\/mrow><annotation encoding=\"application\/x-tex\">\\left({\\pi}\/{10\\,800}\\right)<\/annotation><\/semantics><\/math> rad<br>1<math data-latex=\"''\"><semantics><msup><mrow><\/mrow><mrow><mo lspace=\"0em\" rspace=\"0em\" class=\"tml-prime\">\u2032<\/mo><mo lspace=\"0em\" rspace=\"0em\" class=\"tml-prime\">\u2032<\/mo><\/mrow><\/msup><annotation encoding=\"application\/x-tex\">''<\/annotation><\/semantics><\/math> = <math data-latex=\"\\left({\\pi}\/{648\\,000}\\right)\"><semantics><mrow><mo fence=\"true\" form=\"prefix\">(<\/mo><mi>\u03c0<\/mi><mi>\/<\/mi><mrow><mn>648<\/mn><mspace width=\"0.1667em\"><\/mspace><mn>000<\/mn><\/mrow><mo fence=\"true\" form=\"postfix\">)<\/mo><\/mrow><annotation encoding=\"application\/x-tex\">\\left({\\pi}\/{648\\,000}\\right)<\/annotation><\/semantics><\/math> rad<\/td><\/tr><tr><td>volume<\/td><td class=\"has-text-align-left\" data-align=\"left\">litre<\/td><td class=\"has-text-align-center\" data-align=\"center\">L<\/td><td class=\"has-text-align-center\" data-align=\"center\">1 L = 10<sup>-3<\/sup> m<sup>3<\/sup><\/td><\/tr><tr><td>masse<\/td><td class=\"has-text-align-left\" data-align=\"left\">tonne<br>dalton<\/td><td class=\"has-text-align-center\" data-align=\"center\">t<br>Da<\/td><td class=\"has-text-align-center\" data-align=\"center\">1 t = 1000 kg<br>1 Da = 1,660 539 068 92(52) \u00d7 10<sup>\u221227<\/sup> kg<\/td><\/tr><tr><td>\u00e9nergie<\/td><td class=\"has-text-align-left\" data-align=\"left\">\u00e9lectronvolt<\/td><td class=\"has-text-align-center\" data-align=\"center\">eV<\/td><td class=\"has-text-align-center\" data-align=\"center\">1 eV = 1,602 176 634 <math data-latex=\"\\times\"><semantics><mo lspace=\"0em\" rspace=\"0em\">\u00d7<\/mo><annotation encoding=\"application\/x-tex\">\\times<\/annotation><\/semantics><\/math> 10<sup>\u221219<\/sup>  J<\/td><\/tr><tr><td>logarithme <br>d'un rapport<\/td><td class=\"has-text-align-left\" data-align=\"left\">n\u00e9per<br>bel<br>d\u00e9cibel<\/td><td class=\"has-text-align-center\" data-align=\"center\">Np<br>B<br>dB<\/td><td class=\"has-text-align-center\" data-align=\"center\">log<sub>e<\/sub> du rapport de deux grandeurs<br>log<sub>10<\/sub> du rapport de deux grandeurs<br>1 dB = 1\/10 B<\/td><\/tr><\/tbody><\/table><\/figure>\n\n\n\n<p class=\"has-medium-font-size\">Le d\u00e9cret n\u00b0 2020-709 du 11 juin 2020 fixe les unit\u00e9s de mesure l\u00e9gales en France. En plus des unit\u00e9s pr\u00e9cit\u00e9es, sont autoris\u00e9es pour l'\u00e9nergie le wattheure : 1Wh = 3600 J, pour la puissance apparente le voltamp\u00e8re (VA) et le var (var) pour la puissance \u00e9lectrique r\u00e9active en courant alternatif conform\u00e9ment aux normes internationales IEC (International Electrotechnical Commission).<\/p>\n\n\n\n<h2 class=\"wp-block-heading\">Les incertitudes de mesure<\/h2>\n\n\n\n<h3 class=\"wp-block-heading\">Mesurage<\/h3>\n\n\n<div style=\"border: 3px solid #004780; border-radius: 25px; background-color: #e3f7f7; \" class=\"ub-styled-box ub-bordered-box wp-block-ub-styled-box\" id=\"ub-styled-box-060f8bab-993e-4e35-9fba-1be6a2ccedab\">\n<p class=\"has-medium-font-size\" id=\"ub-styled-box-bordered-content-\">Le mesurage est le processus consistant \u00e0 obtenir exp\u00e9rimentalement une ou plusieurs valeurs que l'on peut raisonnablement attribuer \u00e0 une grandeur. Le mesurande est la grandeur que l'on veut mesurer. Le principe de mesure est le ph\u00e9nom\u00e8ne servant de base \u00e0 un mesurage. La m\u00e9thode de mesure, est la description g\u00e9n\u00e9rique de l'organisation logique des op\u00e9rations mises en \u0153uvre dans un mesurage.<\/p>\n\n\n\n<p class=\"has-medium-font-size\">La proc\u00e9dure de mesure, est la description d\u00e9taill\u00e9e d'un mesurage conform\u00e9ment \u00e0 un ou plusieurs principes de mesureet \u00e0 une m\u00e9thode de mesure donn\u00e9e, fond\u00e9e sur un mod\u00e8le de mesure et incluant tout calcul destin\u00e9 \u00e0 obtenir un r\u00e9sultat de mesure.<\/p>\n\n\n\n<p class=\"has-medium-font-size\">Le r\u00e9sultat d'un mesurage est ensemble de valeurs attribu\u00e9es \u00e0 un mesurande, compl\u00e9t\u00e9 par toute autre information pertinente disponible. Le r\u00e9sultat de mesure est g\u00e9n\u00e9ralement exprim\u00e9 par une valeur mesur\u00e9e unique et une incertitude de mesure.<\/p>\n\n\n<\/div>\n\n<div style=\"border: 3px outset #fab300; border-radius: 26px; background-color: #fff6e2; \" class=\"ub-styled-box ub-bordered-box wp-block-ub-styled-box\" id=\"ub-styled-box-466c7b26-9b8e-49b0-9160-98564073d84b\">\n<p class=\"has-small-font-size\" id=\"ub-styled-box-bordered-content-\">Exemple : Pr\u00e9paration d'une solution \u00e9talon de cadmium<\/p>\n\n\n\n<ul class=\"wp-block-list\">\n<li class=\"has-small-font-size\">Proc\u00e9dure de mesure  : nettoyage de la surface du m\u00e9tal de grande puret\u00e9 pour retirer toute contamination par les oxydes m\u00e9talliques, pesage du m\u00e9tal et dissolution dans le l'acide nitrique dans une fiole volum\u00e9trique.<\/li>\n\n\n\n<li class=\"has-small-font-size\">Mesurande : le mesurande est la concentration de cadmium en mg L<sup>-1<\/sup> : <math data-latex=\"c_{Cd} = \\frac{1000 \\cdot m\\cdot P}{V}\"><semantics><mrow><msub><mi>c<\/mi><mrow><mi>C<\/mi><mi>d<\/mi><\/mrow><\/msub><mo>=<\/mo><mfrac><mrow><mn>1000<\/mn><mo>\u22c5<\/mo><mi>m<\/mi><mo>\u22c5<\/mo><mi>P<\/mi><\/mrow><mi>V<\/mi><\/mfrac><\/mrow><annotation encoding=\"application\/x-tex\">c_{Cd} = \\frac{1000 \\cdot m\\cdot P}{V}<\/annotation><\/semantics><\/math>. 1000 est le facteur de conversion de mL en L, <math data-latex=\"m\"><semantics><mi>m<\/mi><annotation encoding=\"application\/x-tex\">m<\/annotation><\/semantics><\/math> la masse de m\u00e9tal en mg, <math data-latex=\"P\"><semantics><mi>P<\/mi><annotation encoding=\"application\/x-tex\">P<\/annotation><\/semantics><\/math> la puret\u00e9 du m\u00e9tal exprim\u00e9e sous forme de fraction de masse (unit\u00e9 1), <math data-latex=\"V\"><semantics><mi>V<\/mi><annotation encoding=\"application\/x-tex\">V<\/annotation><\/semantics><\/math> le volume de la fiole volum\u00e9trique en mL.<\/li>\n\n\n\n<li class=\"has-small-font-size\">R\u00e9sultat du mesurage : <math data-latex=\"c_{Cd} = 1002,5 \\pm 1,8 \"><semantics><mrow><msub><mi>c<\/mi><mrow><mi>C<\/mi><mi>d<\/mi><\/mrow><\/msub><mo>=<\/mo><mn>1002,5<\/mn><mo>\u00b1<\/mo><mn>1,8<\/mn><\/mrow><annotation encoding=\"application\/x-tex\">c_{Cd} = 1002,5 \\pm 1,8 <\/annotation><\/semantics><\/math> mg L<sup>-1<\/sup>.<\/li>\n<\/ul>\n\n\n<\/div>\n\n\n<h3 class=\"wp-block-heading\">Erreur de mesure<\/h3>\n\n\n<div style=\"border: 3px solid #004780; border-radius: 25px; background-color: #e3f7f7; \" class=\"ub-styled-box ub-bordered-box wp-block-ub-styled-box\" id=\"ub-styled-box-74c49859-a08f-416e-8195-52f179daefbf\">\n<p class=\"has-medium-font-size\" id=\"ub-styled-box-bordered-content-\">Un mesurage pr\u00e9sente, en g\u00e9n\u00e9ral, des imperfections qui occasionnent une erreur pour le r\u00e9sultat de mesure. On envisage traditionnellement qu'une erreur poss\u00e8de deux composantes, \u00e0 savoir une composante al\u00e9atoire et une composante syst\u00e9matique.<\/p>\n\n\n<\/div>\n\n\n<p class=\"has-medium-font-size\">L'erreur al\u00e9atoire provient probablement de variations temporelles et spatiales non pr\u00e9visibles ou stochastiques de grandeurs d'influence. Les effets de telles variations, appel\u00e9s ci-apr\u00e8s effets al\u00e9atoires, entra\u00eenent des variations pour les observations r\u00e9p\u00e9t\u00e9es du mesurande. Bien qu'il ne soit pas possible de compenser l'erreur al\u00e9atoire d'un r\u00e9sultat de mesure, elle peut g\u00e9n\u00e9ralement \u00eatre r\u00e9duite en augmentant le nombre d'observations. Son esp\u00e9rance math\u00e9matique ou valeur esp\u00e9r\u00e9e est \u00e9gale \u00e0 z\u00e9ro.<br>L'erreur syst\u00e9matique, comme l'erreur al\u00e9atoire, ne peut pas \u00eatre \u00e9limin\u00e9e mais, elle aussi, peut souvent \u00eatre r\u00e9duite. Si une erreur syst\u00e9matique se produit sur un r\u00e9sultat de mesure \u00e0 partir d'un effet reconnu d'une grandeur d'influence, effet appel\u00e9 ci-apr\u00e8s effet syst\u00e9matique, l'effet peut \u00eatre quantifi\u00e9 et, s'il est significatif par rapport \u00e0 l'exactitude requise du mesurage, une correction ou un facteur de correction peut \u00eatre appliqu\u00e9 pour compenser l'effet. On suppose qu'apr\u00e8s correction l'esp\u00e9rance math\u00e9matique de l'erreur qui provient d'un effet syst\u00e9matique est \u00e9gale \u00e0 z\u00e9ro.<\/p>\n\n\n\n<figure class=\"wp-block-image aligncenter size-full\"><img loading=\"lazy\" decoding=\"async\" width=\"640\" height=\"480\" src=\"https:\/\/sciences-physiques.org\/wp-content\/uploads\/2026\/01\/gauss.png\" alt=\"\" class=\"wp-image-103\" srcset=\"https:\/\/sciences-physiques.org\/wp-content\/uploads\/2026\/01\/gauss.png 640w, https:\/\/sciences-physiques.org\/wp-content\/uploads\/2026\/01\/gauss-300x225.png 300w\" sizes=\"auto, (max-width: 640px) 100vw, 640px\" \/><\/figure>\n\n\n\n<p class=\"has-medium-font-size\">Si <math data-latex=\"\\mu\"><semantics><mi>\u03bc<\/mi><annotation encoding=\"application\/x-tex\">\\mu<\/annotation><\/semantics><\/math> est la valeur vraie de la grandeur <math data-latex=\"X\"><semantics><mi>X<\/mi><annotation encoding=\"application\/x-tex\">X<\/annotation><\/semantics><\/math>, la valeur observ\u00e9e peut se mod\u00e9liser par :<\/p>\n\n\n\n<div class=\"wp-block-katex-display-block katex-eq\" data-katex-display=\"true\"><pre>X_k = \\mu + e_{sys} + e_k<\/pre><\/div>\n\n\n\n<p class=\"has-medium-font-size\">o\u00f9 <math data-latex=\"e_{sys}\"><semantics><msub><mi>e<\/mi><mrow><mi>s<\/mi><mi>y<\/mi><mi>s<\/mi><\/mrow><\/msub><annotation encoding=\"application\/x-tex\">e_{sys}<\/annotation><\/semantics><\/math> d\u00e9signe l'erreur syst\u00e9matique (de m\u00eame valeur non nulle quelque soit l'observation <math data-latex=\"k\"><semantics><mi>k<\/mi><annotation encoding=\"application\/x-tex\">k<\/annotation><\/semantics><\/math>) et <math data-latex=\"e_k\"><semantics><msub><mi>e<\/mi><mi>k<\/mi><\/msub><annotation encoding=\"application\/x-tex\">e_k<\/annotation><\/semantics><\/math>, l'erreur al\u00e9atoire dont l'esp\u00e9rance math\u00e9matique est nulle. Le nombre d\u2019erreurs al\u00e9atoires est fonction du nombre de sources d'incertitude.<\/p>\n\n\n\n<h3 class=\"wp-block-heading has-medium-font-size\">Incertitude<\/h3>\n\n\n<div style=\"border: 3px solid #004780; border-radius: 25px; background-color: #e3f7f7; \" class=\"ub-styled-box ub-bordered-box wp-block-ub-styled-box\" id=\"ub-styled-box-d4f732da-c8e9-4c33-87f9-3d7e071570d7\">\n<p class=\"has-medium-font-size\" id=\"ub-styled-box-bordered-content-\">L'incertitude de mesure est un  param\u00e8tre non n\u00e9gatif qui caract\u00e9rise la dispersion des valeurs attribu\u00e9es \u00e0 un mesurande, \u00e0 partir des informations utilis\u00e9es.<br>L'incertitude de mesure comprend des composantes provenant d'effets syst\u00e9matiques, telles que les composantes associ\u00e9es aux corrections et aux valeurs assign\u00e9es des \u00e9talons, ainsi que l'incertitude d\u00e9finitionnelle. Parfois, on ne corrige pas des effets syst\u00e9matiques estim\u00e9s, mais on ins\u00e8re plut\u00f4t des composantes associ\u00e9es de l'incertitude.<br>Le param\u00e8tre peut \u00eatre, par exemple, un \u00e9cart-type appel\u00e9 incertitude-type (ou un de ses multiples) ou la demi-\u00e9tendue d'un intervalle ayant une probabilit\u00e9 de couverture d\u00e9termin\u00e9e.<\/p>\n\n\n<\/div>\n\n\n<p class=\"has-medium-font-size\">Les sources d'incertitudes peuvent \u00eatre :<\/p>\n\n\n\n<ul class=\"wp-block-list\">\n<li class=\"has-medium-font-size\">la d\u00e9finition incompl\u00e8te du mesurande ;<\/li>\n\n\n\n<li class=\"has-medium-font-size\">la r\u00e9alisation imparfaite de la d\u00e9finition du mesurande ;<\/li>\n\n\n\n<li class=\"has-medium-font-size\">l'\u00e9chantillonnage non repr\u00e9sentatif. L'\u00e9chantillon mesur\u00e9 peut ne pas repr\u00e9senter le mesurande d\u00e9fini ;<\/li>\n\n\n\n<li class=\"has-medium-font-size\">la connaissance insuffisante des effets des conditions d'environnement sur le mesurage ou mesurage imparfait des conditions d'environnement ;<\/li>\n\n\n\n<li class=\"has-medium-font-size\">le biais d\u00fb \u00e0 l'observateur pour la lecture des instruments analogiques ;<\/li>\n\n\n\n<li class=\"has-medium-font-size\">la r\u00e9solution finie de l'instrument ou le  seuil de mobilit\u00e9 ;<\/li>\n\n\n\n<li class=\"has-medium-font-size\">les  valeurs inexactes des \u00e9talons et mat\u00e9riaux de r\u00e9f\u00e9rence ;<\/li>\n\n\n\n<li class=\"has-medium-font-size\">les valeurs inexactes des constantes et autres param\u00e8tres obtenus de sources ext\u00e9rieures et utilis\u00e9s dans l'algorithme de traitement des donn\u00e9es ;<\/li>\n\n\n\n<li class=\"has-medium-font-size\">les approximations et hypoth\u00e8ses introduites dans la m\u00e9thode et dans la proc\u00e9dure de mesure ;<\/li>\n\n\n\n<li class=\"has-medium-font-size\">les variations entre les observations r\u00e9p\u00e9t\u00e9es du mesurande dans des conditions apparemment identiques.<\/li>\n<\/ul>\n\n\n\n<p class=\"has-medium-font-size\">Ces sources ne sont pas n\u00e9cessairement ind\u00e9pendantes. Elles peuvent \u00eatre r\u00e9sum\u00e9es par un graphique appel\u00e9 arbre d'Ishikawa ou diagramme des 5M :<\/p>\n\n\n\n<figure class=\"wp-block-image aligncenter size-full\"><img loading=\"lazy\" decoding=\"async\" width=\"572\" height=\"211\" src=\"https:\/\/sciences-physiques.org\/wp-content\/uploads\/2026\/01\/5M.png\" alt=\"\" class=\"wp-image-102\" srcset=\"https:\/\/sciences-physiques.org\/wp-content\/uploads\/2026\/01\/5M.png 572w, https:\/\/sciences-physiques.org\/wp-content\/uploads\/2026\/01\/5M-300x111.png 300w\" sizes=\"auto, (max-width: 572px) 100vw, 572px\" \/><\/figure>\n\n\n\n<ul class=\"wp-block-list\">\n<li class=\"has-medium-font-size\">milieu : environnement (temp\u00e9rature, humidit\u00e9, vibrations, ...) ;<\/li>\n\n\n\n<li class=\"has-medium-font-size\">moyen : instrument de mesure, \u00e9talonnage , logiciels ;<\/li>\n\n\n\n<li class=\"has-medium-font-size\">mati\u00e8re : \u00e9chantillonnage, puret\u00e9 ;<\/li>\n\n\n\n<li class=\"has-medium-font-size\">main d\u2019\u0153uvre : observateur, lecture, manipulation ;<\/li>\n\n\n\n<li class=\"has-medium-font-size\"> m\u00e9thode : mode op\u00e9ratoire.<\/li>\n<\/ul>\n\n\n\n<h3 class=\"wp-block-heading\">Mod\u00e9lisation du mesurage<\/h3>\n\n\n\n<p class=\"is-style-text-display has-medium-font-size\" style=\"border-style:none;border-width:0px;margin-right:0;margin-left:0\">Dans la plupart des cas, un mesurande <math data-latex=\"Y\"><semantics><mi>Y<\/mi><annotation encoding=\"application\/x-tex\">Y<\/annotation><\/semantics><\/math> n'est pas mesur\u00e9 directement mais il est d\u00e9termin\u00e9 \u00e0 partir de <math data-latex=\"N \"><semantics><mi>N<\/mi><annotation encoding=\"application\/x-tex\">N <\/annotation><\/semantics><\/math> grandeurs d'entr\u00e9e <math data-latex=\"X_1, X_2, \\cdots, X_N\"><semantics><mrow><msub><mi>X<\/mi><mn>1<\/mn><\/msub><mo separator=\"true\">,<\/mo><msub><mi>X<\/mi><mn>2<\/mn><\/msub><mo separator=\"true\">,<\/mo><mo>\u22ef<\/mo><mspace width=\"0.1667em\"><\/mspace><mo separator=\"true\">,<\/mo><msub><mi>X<\/mi><mi>N<\/mi><\/msub><\/mrow><annotation encoding=\"application\/x-tex\">X_1, X_2, \\cdots, X_N<\/annotation><\/semantics><\/math> par une relation fonctionnelle <math data-latex=\"f\"><semantics><mi>f<\/mi><annotation encoding=\"application\/x-tex\">f<\/annotation><\/semantics><\/math> : <math data-latex=\"Y = f\\left(X_1, X_2, \\cdots, X_N\\right)\"><semantics><mrow><mi>Y<\/mi><mo>=<\/mo><mi>f<\/mi><mrow><mo fence=\"true\" form=\"prefix\">(<\/mo><msub><mi>X<\/mi><mn>1<\/mn><\/msub><mo separator=\"true\">,<\/mo><msub><mi>X<\/mi><mn>2<\/mn><\/msub><mo separator=\"true\">,<\/mo><mo>\u22ef<\/mo><mspace width=\"0.1667em\"><\/mspace><mo separator=\"true\">,<\/mo><msub><mi>X<\/mi><mi>N<\/mi><\/msub><mo fence=\"true\" form=\"postfix\">)<\/mo><\/mrow><\/mrow><annotation encoding=\"application\/x-tex\">Y = f\\left(X_1, X_2, \\cdots, X_N\\right)<\/annotation><\/semantics><\/math>. L'estimation du mesurande <math data-latex=\"y\"><semantics><mi>y<\/mi><annotation encoding=\"application\/x-tex\">y<\/annotation><\/semantics><\/math> est obtenue \u00e0 partir de la fonction <math data-latex=\"f\"><semantics><mi>f<\/mi><annotation encoding=\"application\/x-tex\">f<\/annotation><\/semantics><\/math> en utilisant les estimations<math data-latex=\"x_1, x_2, \\cdots, x_N\"><semantics><mrow><msub><mi>x<\/mi><mn>1<\/mn><\/msub><mo separator=\"true\">,<\/mo><msub><mi>x<\/mi><mn>2<\/mn><\/msub><mo separator=\"true\">,<\/mo><mo>\u22ef<\/mo><mspace width=\"0.1667em\"><\/mspace><mo separator=\"true\">,<\/mo><msub><mi>x<\/mi><mi>N<\/mi><\/msub><\/mrow><annotation encoding=\"application\/x-tex\">x_1, x_2, \\cdots, x_N<\/annotation><\/semantics><\/math> (\u00e0 proprement parl\u00e9 l'esp\u00e9rance math\u00e9matique d'une s\u00e9rie d'observations <math data-latex=\"X_{i,k}\"><semantics><msub><mi>X<\/mi><mrow><mi>i<\/mi><mo separator=\"true\">,<\/mo><mi>k<\/mi><\/mrow><\/msub><annotation encoding=\"application\/x-tex\">X_{i,k}<\/annotation><\/semantics><\/math> de la valeur observ\u00e9e de Dans la plupart des cas, un mesurande <math data-latex=\"Y\"><semantics><mi>Y<\/mi><annotation encoding=\"application\/x-tex\">Y<\/annotation><\/semantics><\/math> n'est pas mesur\u00e9 directement mais il est d\u00e9termin\u00e9 \u00e0 partir de <math data-latex=\"N \"><semantics><mi>N<\/mi><annotation encoding=\"application\/x-tex\">N <\/annotation><\/semantics><\/math> grandeurs d'entr\u00e9e <math data-latex=\"X_1, X_2, \\cdots, X_N\"><semantics><mrow><msub><mi>X<\/mi><mn>1<\/mn><\/msub><mo separator=\"true\">,<\/mo><msub><mi>X<\/mi><mn>2<\/mn><\/msub><mo separator=\"true\">,<\/mo><mo>\u22ef<\/mo><mspace width=\"0.1667em\"><\/mspace><mo separator=\"true\">,<\/mo><msub><mi>X<\/mi><mi>N<\/mi><\/msub><\/mrow><annotation encoding=\"application\/x-tex\">X_1, X_2, \\cdots, X_N<\/annotation><\/semantics><\/math> par une relation fonctionnelle <math data-latex=\"f\"><semantics><mi>f<\/mi><annotation encoding=\"application\/x-tex\">f<\/annotation><\/semantics><\/math> : <math data-latex=\"Y = f\\left(X_1, X_2, \\cdots, X_N\\right)\"><semantics><mrow><mi>Y<\/mi><mo>=<\/mo><mi>f<\/mi><mrow><mo fence=\"true\" form=\"prefix\">(<\/mo><msub><mi>X<\/mi><mn>1<\/mn><\/msub><mo separator=\"true\">,<\/mo><msub><mi>X<\/mi><mn>2<\/mn><\/msub><mo separator=\"true\">,<\/mo><mo>\u22ef<\/mo><mspace width=\"0.1667em\"><\/mspace><mo separator=\"true\">,<\/mo><msub><mi>X<\/mi><mi>N<\/mi><\/msub><mo fence=\"true\" form=\"postfix\">)<\/mo><\/mrow><\/mrow><annotation encoding=\"application\/x-tex\">Y = f\\left(X_1, X_2, \\cdots, X_N\\right)<\/annotation><\/semantics><\/math>. L'estimation du mesurande <math data-latex=\"y\"><semantics><mi>y<\/mi><annotation encoding=\"application\/x-tex\">y<\/annotation><\/semantics><\/math> est obtenue \u00e0 partir de la fonction <math data-latex=\"f\"><semantics><mi>f<\/mi><annotation encoding=\"application\/x-tex\">f<\/annotation><\/semantics><\/math> en utilisant les estimations<math data-latex=\"x_1, x_2, \\cdots, x_N\"><semantics><mrow><msub><mi>x<\/mi><mn>1<\/mn><\/msub><mo separator=\"true\">,<\/mo><msub><mi>x<\/mi><mn>2<\/mn><\/msub><mo separator=\"true\">,<\/mo><mo>\u22ef<\/mo><mspace width=\"0.1667em\"><\/mspace><mo separator=\"true\">,<\/mo><msub><mi>x<\/mi><mi>N<\/mi><\/msub><\/mrow><annotation encoding=\"application\/x-tex\">x_1, x_2, \\cdots, x_N<\/annotation><\/semantics><\/math> (\u00e0 proprement parl\u00e9 l'esp\u00e9rance math\u00e9matique d'une s\u00e9rie d'observations de la valeur observ\u00e9e de <math data-latex=\"X_{i}\"><semantics><msub><mi>X<\/mi><mi>i<\/mi><\/msub><annotation encoding=\"application\/x-tex\">X_{i}<\/annotation><\/semantics><\/math> ) pour les <math data-latex=\"N\"><semantics><mi>N<\/mi><annotation encoding=\"application\/x-tex\">N<\/annotation><\/semantics><\/math> valeurs <math data-latex=\"X_1, X_2, \\cdots, X_N\"><semantics><mrow><msub><mi>X<\/mi><mn>1<\/mn><\/msub><mo separator=\"true\">,<\/mo><msub><mi>X<\/mi><mn>2<\/mn><\/msub><mo separator=\"true\">,<\/mo><mo>\u22ef<\/mo><mspace width=\"0.1667em\"><\/mspace><mo separator=\"true\">,<\/mo><msub><mi>X<\/mi><mi>N<\/mi><\/msub><\/mrow><annotation encoding=\"application\/x-tex\">X_1, X_2, \\cdots, X_N<\/annotation><\/semantics><\/math> : <math data-latex=\"y = f\\left(x_1,x_2, \\cdots, x_N\\right)\"><semantics><mrow><mi>y<\/mi><mo>=<\/mo><mi>f<\/mi><mrow><mo fence=\"true\" form=\"prefix\">(<\/mo><msub><mi>x<\/mi><mn>1<\/mn><\/msub><mo separator=\"true\">,<\/mo><msub><mi>x<\/mi><mn>2<\/mn><\/msub><mo separator=\"true\">,<\/mo><mo>\u22ef<\/mo><mspace width=\"0.1667em\"><\/mspace><mo separator=\"true\">,<\/mo><msub><mi>x<\/mi><mi>N<\/mi><\/msub><mo fence=\"true\" form=\"postfix\">)<\/mo><\/mrow><\/mrow><annotation encoding=\"application\/x-tex\">y = f\\left(x_1,x_2, \\cdots, x_N\\right)<\/annotation><\/semantics><\/math>.<\/p>\n\n\n\n<p class=\"has-medium-font-size\">On pr\u00e9f\u00e9ra utiliser pour l'estimation du r\u00e9sultat <math data-latex=\"y\"><semantics><mi>y<\/mi><annotation encoding=\"application\/x-tex\">y<\/annotation><\/semantics><\/math> du mesurande obtenue apr\u00e8s <math data-latex=\"n\"><semantics><mi>n<\/mi><annotation encoding=\"application\/x-tex\">n<\/annotation><\/semantics><\/math> observations ind\u00e9pendantes <math data-latex=\"Y_k\"><semantics><msub><mi>Y<\/mi><mi>k<\/mi><\/msub><annotation encoding=\"application\/x-tex\">Y_k<\/annotation><\/semantics><\/math> de <math data-latex=\"Y\"><semantics><mi>Y<\/mi><annotation encoding=\"application\/x-tex\">Y<\/annotation><\/semantics><\/math>:<\/p>\n\n\n\n<div class=\"wp-block-katex-display-block katex-eq\" data-katex-display=\"true\"><pre>y = \\overline{Y}=\\frac{1}{n}\\sum_{k=1}^n\\overline{Y_k}=\\frac{1}{n}\\sum_{k=1}^n f\\left(X_{1k},X_{2k},\\cdots,X_{N,k}\\right)<\/pre><\/div>\n\n\n\n<p class=\"has-medium-font-size\">plut\u00f4t que de faire :<\/p>\n\n\n\n<div class=\"wp-block-katex-display-block katex-eq\" data-katex-display=\"true\"><pre>y =  f\\left(\\overline{X}_{1},\\overline{X}_{2},\\cdots,\\overline{X}_{N}\\right)<\/pre><\/div>\n\n\n\n<p class=\"has-medium-font-size\">car la fonction <math data-latex=\"f\"><semantics><mi>f<\/mi><annotation encoding=\"application\/x-tex\">f<\/annotation><\/semantics><\/math> peut-\u00eatre non lin\u00e9aire.<\/p>\n\n\n\n<h3 class=\"wp-block-heading\">\u00c9valuation de type A de l'incertitude-type<\/h3>\n\n\n\n<p class=\"has-medium-font-size\">Dans certains cas, la meilleure estimation <math data-latex=\"x\"><semantics><mi>x<\/mi><annotation encoding=\"application\/x-tex\">x<\/annotation><\/semantics><\/math> disponible de esp\u00e9rance math\u00e9matique d'une grandeur d'entr\u00e9e <math data-latex=\"X\"><semantics><mi>X<\/mi><annotation encoding=\"application\/x-tex\">X<\/annotation><\/semantics><\/math> qui varie au hasard (c'est \u00e0 dire d'une variable al\u00e9atoire) pour la quelle on a obtenu <math data-latex=\"n\"><semantics><mi>n<\/mi><annotation encoding=\"application\/x-tex\">n<\/annotation><\/semantics><\/math> observations ind\u00e9pendantes <math data-latex=\"X_k\"><semantics><msub><mi>X<\/mi><mi>k<\/mi><\/msub><annotation encoding=\"application\/x-tex\">X_k<\/annotation><\/semantics><\/math> est la moyenne arithm\u00e9tique : <math data-latex=\"\\overline{X} = \\frac{1}{n} \\sum\\limits_{k=1}^{n}X_k\"><semantics><mrow><menclose notation=\"top\" class=\"tml-overline\"><mi>X<\/mi><\/menclose><mo>=<\/mo><mfrac><mn>1<\/mn><mi>n<\/mi><\/mfrac><mrow><munderover><mo movablelimits=\"false\">\u2211<\/mo><mrow><mi>k<\/mi><mo>=<\/mo><mn>1<\/mn><\/mrow><mi>n<\/mi><\/munderover><\/mrow><msub><mi>X<\/mi><mi>k<\/mi><\/msub><\/mrow><annotation encoding=\"application\/x-tex\">\\overline{X} = \\frac{1}{n} \\sum\\limits_{k=1}^{n}X_k<\/annotation><\/semantics><\/math>.<\/p>\n\n\n\n<p class=\"has-medium-font-size\">L\u2019\u00e9cart-type exp\u00e9rimental de la moyenne <math data-latex=\"\\overline{X}\"><semantics><menclose notation=\"top\" class=\"tml-overline\"><mi>X<\/mi><\/menclose><annotation encoding=\"application\/x-tex\">\\overline{X}<\/annotation><\/semantics><\/math>peut \u00eatre utilis\u00e9 comme mesure de l'incertitude <math data-latex=\"u(x)\"><semantics><mrow><mi>u<\/mi><mo form=\"prefix\" stretchy=\"false\">(<\/mo><mi>x<\/mi><mo form=\"postfix\" stretchy=\"false\">)<\/mo><\/mrow><annotation encoding=\"application\/x-tex\">u(x)<\/annotation><\/semantics><\/math> : <\/p>\n\n\n\n<div class=\"wp-block-katex-display-block katex-eq\" data-katex-display=\"true\"><pre>u(x) = s(\\overline{X}) =\\frac{s(X_k)}{\\sqrt{n}} = \\sqrt{\\frac{\\frac{1}{n-1}\\sum\\limits_{j=1}^{n}\\left(X_j-\\overline{X}\\right)^2}{n}}<\/pre><\/div>\n\n\n\n<p class=\"has-medium-font-size\"><math data-latex=\"u(x)\"><semantics><mrow><mi>u<\/mi><mo form=\"prefix\" stretchy=\"false\">(<\/mo><mi>x<\/mi><mo form=\"postfix\" stretchy=\"false\">)<\/mo><\/mrow><annotation encoding=\"application\/x-tex\">u(x)<\/annotation><\/semantics><\/math> est appel\u00e9 incertitude-type de Type A.<\/p>\n\n\n\n<p class=\"has-medium-font-size\">Exemple :<\/p>\n\n\n\n<p class=\"has-medium-font-size\">Vingt observations r\u00e9p\u00e9t\u00e9es de la temp\u00e9rature d'une \u00e9tuve  <math data-latex=\"T\"><semantics><mi>T<\/mi><annotation encoding=\"application\/x-tex\">T<\/annotation><\/semantics><\/math> en \u00b0C  ont donn\u00e9 les r\u00e9sultats suivants :<\/p>\n\n\n\n<figure class=\"wp-block-table has-small-font-size\"><table class=\"has-background\" style=\"background-color:#edecec\"><tbody><tr><td class=\"has-text-align-center\" data-align=\"center\">1<\/td><td>2<\/td><td>3<\/td><td>4<\/td><td>5<\/td><td>6<\/td><td>7<\/td><td>8<\/td><td>9<\/td><td>10<\/td><td>11<\/td><td>12<\/td><td>13<\/td><td>14<\/td><td>15<\/td><td>16<\/td><td>17<\/td><td>18<\/td><td>19<\/td><td class=\"has-text-align-center\" data-align=\"center\">20<\/td><\/tr><tr><td class=\"has-text-align-center\" data-align=\"center\">36,9           <\/td><td>37,7<\/td><td>36,1<\/td><td>35,5<\/td><td>37,3<\/td><td>37,8<\/td><td>36,3<\/td><td>36,3<\/td><td>36,6<\/td><td>35,7<\/td><td>36,7<\/td><td>37,6<\/td><td>36,4 <\/td><td>36,6<\/td><td><br>36,9 <br><\/td><td>37,1 <\/td><td>37,2  <\/td><td>37,5<\/td><td>36,9<\/td><td class=\"has-text-align-center\" data-align=\"center\">37,2<\/td><\/tr><\/tbody><\/table><\/figure>\n\n\n\n<p class=\"has-medium-font-size\">La moyenne est <math data-latex=\"\\overline{T} = 36,675\\;\\mathrm{\u00b0C}\"><semantics><mrow><menclose notation=\"top\" class=\"tml-overline\"><mi>T<\/mi><\/menclose><mo>=<\/mo><mn>36,675<\/mn><mspace width=\"0.2778em\"><\/mspace><mrow><mi>\u00b0<\/mi><mrow><mi mathvariant=\"normal\">C<\/mi><\/mrow><\/mrow><\/mrow><annotation encoding=\"application\/x-tex\">\\overline{T} = 36,675\\;\\mathrm{\u00b0C}<\/annotation><\/semantics><\/math>, l'\u00e9cart-type <math data-latex=\"s(T_k) = 0,747\\;\\mathrm{\u00b0C}\"><semantics><mrow><mi>s<\/mi><mo form=\"prefix\" stretchy=\"false\">(<\/mo><msub><mi>T<\/mi><mi>k<\/mi><\/msub><mo form=\"postfix\" stretchy=\"false\">)<\/mo><mo>=<\/mo><mn>0,747<\/mn><mspace width=\"0.2778em\"><\/mspace><mrow><mi>\u00b0<\/mi><mrow><mi mathvariant=\"normal\">C<\/mi><\/mrow><\/mrow><\/mrow><annotation encoding=\"application\/x-tex\">s(T_k) = 0,747\\;\\mathrm{\u00b0C}<\/annotation><\/semantics><\/math>, l'\u00e9cart-type de la moyenne  <math data-latex=\"s(\\overline{T}) = \\frac{0,747}{\\sqrt{20}} =0,167 \\;\\mathrm{^{\\circ}C} \\simeq 0,17 \\;\\mathrm{^{\\circ}C}\"><semantics><mrow><mi>s<\/mi><mo form=\"prefix\" stretchy=\"false\">(<\/mo><menclose notation=\"top\" class=\"tml-overline\"><mi>T<\/mi><\/menclose><mo form=\"postfix\" stretchy=\"false\">)<\/mo><mo>=<\/mo><mfrac><mn>0,747<\/mn><msqrt><mn>20<\/mn><\/msqrt><\/mfrac><mo>=<\/mo><mn>0,167<\/mn><mspace width=\"0.2778em\"><\/mspace><mrow><msup><mrow><\/mrow><mo lspace=\"0em\" rspace=\"0em\">\u2218<\/mo><\/msup><mrow><mi mathvariant=\"normal\">C<\/mi><\/mrow><\/mrow><mo>\u2243<\/mo><mn>0,17<\/mn><mspace width=\"0.2778em\"><\/mspace><mrow><msup><mrow><\/mrow><mo lspace=\"0em\" rspace=\"0em\">\u2218<\/mo><\/msup><mrow><mi mathvariant=\"normal\">C<\/mi><\/mrow><\/mrow><\/mrow><annotation encoding=\"application\/x-tex\">s(\\overline{T}) = \\frac{0,747}{\\sqrt{20}} =0,167 \\;\\mathrm{^{\\circ}C} \\simeq 0,17 \\;\\mathrm{^{\\circ}C}<\/annotation><\/semantics><\/math>. On peut estimer l'incertitude-type de type A : <math data-latex=\"u(T) = 0,17\\;\\mathrm{^{\\circ}C}\"><semantics><mrow><mi>u<\/mi><mo form=\"prefix\" stretchy=\"false\">(<\/mo><mi>T<\/mi><mo form=\"postfix\" stretchy=\"false\">)<\/mo><mo>=<\/mo><mn>0,17<\/mn><mspace width=\"0.2778em\"><\/mspace><mrow><msup><mrow><\/mrow><mo lspace=\"0em\" rspace=\"0em\">\u2218<\/mo><\/msup><mrow><mi mathvariant=\"normal\">C<\/mi><\/mrow><\/mrow><\/mrow><annotation encoding=\"application\/x-tex\">u(T) = 0,17\\;\\mathrm{^{\\circ}C}<\/annotation><\/semantics><\/math> si l'on consid\u00e8re que la distribution des observations ob\u00e9it \u00e0 une loi de probabilit\u00e9 normale.<\/p>\n\n\n\n<h3 class=\"wp-block-heading\">\u00c9valuation de Type B de l'incertitude-type<\/h3>\n\n\n\n<p class=\"has-medium-font-size\">Pour une estimation <math data-latex=\"x_i\"><semantics><msub><mi>x<\/mi><mi>i<\/mi><\/msub><annotation encoding=\"application\/x-tex\">x_i<\/annotation><\/semantics><\/math> d'une grandeur d'entr\u00e9e <math data-latex=\"X_i\"><semantics><msub><mi>X<\/mi><mi>i<\/mi><\/msub><annotation encoding=\"application\/x-tex\">X_i<\/annotation><\/semantics><\/math> qui n'a pas \u00e9t\u00e9 obtenue \u00e0 partir d'observations r\u00e9p\u00e9t\u00e9es, l'incertitude-type est \u00e9valu\u00e9e par un jugement scientifique fond\u00e9 sur toutes les informations disponibles concernant les causes de variabilit\u00e9 possible de <math data-latex=\"X_i\"><semantics><msub><mi>X<\/mi><mi>i<\/mi><\/msub><annotation encoding=\"application\/x-tex\">X_i<\/annotation><\/semantics><\/math>. L'ensemble des informations peut comprendre :<\/p>\n\n\n\n<ul class=\"wp-block-list\">\n<li class=\"has-medium-font-size\">des r\u00e9sultats de mesures ant\u00e9rieures ;<\/li>\n\n\n\n<li class=\"has-medium-font-size\">l'exp\u00e9rience ou la connaissance du comportement et des propri\u00e9t\u00e9s des mat\u00e9riaux et instruments de mesure utilis\u00e9s ;<\/li>\n\n\n\n<li class=\"has-medium-font-size\">les sp\u00e9cifications du fabricant ;<\/li>\n\n\n\n<li class=\"has-medium-font-size\">les donn\u00e9es fournies par les certificats d'\u00e9talonnage ou d'autres certificats ;<\/li>\n\n\n\n<li class=\"has-medium-font-size\">l'incertitude assign\u00e9e \u00e0 des valeurs de r\u00e9f\u00e9rence provenant d'ouvrage et manuels.<\/li>\n<\/ul>\n\n\n\n<p class=\"has-medium-font-size\"><math data-latex=\"u(x_i)\"><semantics><mrow><mi>u<\/mi><mo form=\"prefix\" stretchy=\"false\">(<\/mo><msub><mi>x<\/mi><mi>i<\/mi><\/msub><mo form=\"postfix\" stretchy=\"false\">)<\/mo><\/mrow><annotation encoding=\"application\/x-tex\">u(x_i)<\/annotation><\/semantics><\/math> \u00e9valu\u00e9 de cette fa\u00e7on porte le nom d'incertitude de type B.<\/p>\n\n\n\n<p class=\"has-medium-font-size\">Exemple :<\/p>\n\n\n\n<p class=\"has-medium-font-size\">Le certificat d'\u00e9talonnage d'une masse \u00e9talon de classe E1 de valeur nominale 100 g indique que la masse \u00e9talon en acier inoxydable est <math data-latex=\"m = 100,000\\, 032\\, 5\\; \\mathrm{g}\"><semantics><mrow><mi>m<\/mi><mo>=<\/mo><mn>100,000<\/mn><mspace width=\"0.1667em\"><\/mspace><mn>032<\/mn><mspace width=\"0.1667em\"><\/mspace><mn>5<\/mn><mspace width=\"0.2778em\"><\/mspace><mrow><mi mathvariant=\"normal\">g<\/mi><\/mrow><\/mrow><annotation encoding=\"application\/x-tex\">m = 100,000\\, 032\\, 5\\; \\mathrm{g}<\/annotation><\/semantics><\/math>. Pour les \u00e9talons de masse de classe E1, l'erreur maximale tol\u00e9r\u00e9e est <math data-latex=\"\\delta m =0,05\\;\\mathrm{mg}\"><semantics><mrow><mi>\u03b4<\/mi><mi>m<\/mi><mo>=<\/mo><mn>0,05<\/mn><mspace width=\"0.2778em\"><\/mspace><mrow><mtext><\/mtext><mi>mg<\/mi><\/mrow><\/mrow><annotation encoding=\"application\/x-tex\">\\delta m =0,05\\;\\mathrm{mg}<\/annotation><\/semantics><\/math>. L'incertitude \u00e9largie (<math data-latex=\"k=2\"><semantics><mrow><mi>k<\/mi><mo>=<\/mo><mn>2<\/mn><\/mrow><annotation encoding=\"application\/x-tex\">k=2<\/annotation><\/semantics><\/math>) est donn\u00e9e par la recommandation internationale OIML R 111-1 : <math data-latex=\"U(m) \\leq 1\/3\\, \\delta m\"><semantics><mrow><mi>U<\/mi><mo form=\"prefix\" stretchy=\"false\">(<\/mo><mi>m<\/mi><mo form=\"postfix\" stretchy=\"false\">)<\/mo><mo>\u2264<\/mo><mn>1<\/mn><mi>\/<\/mi><mn>3<\/mn><mspace width=\"0.1667em\"><\/mspace><mi>\u03b4<\/mi><mi>m<\/mi><\/mrow><annotation encoding=\"application\/x-tex\">U(m) \\leq 1\/3\\, \\delta m<\/annotation><\/semantics><\/math>. On a donc <math data-latex=\"U(m) =2\\times u(m) =\\frac{0,05}{3} = 0,017\\;\\mathrm{mg}\"><semantics><mrow><mi>U<\/mi><mo form=\"prefix\" stretchy=\"false\">(<\/mo><mi>m<\/mi><mo form=\"postfix\" stretchy=\"false\">)<\/mo><mo>=<\/mo><mn>2<\/mn><mo>\u00d7<\/mo><mi>u<\/mi><mo form=\"prefix\" stretchy=\"false\">(<\/mo><mi>m<\/mi><mo form=\"postfix\" stretchy=\"false\">)<\/mo><mo>=<\/mo><mfrac><mn>0,05<\/mn><mn>3<\/mn><\/mfrac><mo>=<\/mo><mn>0,017<\/mn><mspace width=\"0.2778em\"><\/mspace><mrow><mtext><\/mtext><mi>mg<\/mi><\/mrow><\/mrow><annotation encoding=\"application\/x-tex\">U(m) =2\\times u(m) =\\frac{0,05}{3} = 0,017\\;\\mathrm{mg}<\/annotation><\/semantics><\/math> et <math data-latex=\"u(m) = \\frac{0,017}{2} =0,0083\\;\\mathrm{mg}\"><semantics><mrow><mi>u<\/mi><mo form=\"prefix\" stretchy=\"false\">(<\/mo><mi>m<\/mi><mo form=\"postfix\" stretchy=\"false\">)<\/mo><mo>=<\/mo><mfrac><mn>0,017<\/mn><mn>2<\/mn><\/mfrac><mo>=<\/mo><mn>0,0083<\/mn><mspace width=\"0.2778em\"><\/mspace><mrow><mtext><\/mtext><mi>mg<\/mi><\/mrow><\/mrow><annotation encoding=\"application\/x-tex\">u(m) = \\frac{0,017}{2} =0,0083\\;\\mathrm{mg}<\/annotation><\/semantics><\/math>. On \u00e9crira donc :<math data-latex=\"m = 100,000\\,032\\,5(83) \\;\\mathrm{g}\"><semantics><mrow><mi>m<\/mi><mo>=<\/mo><mn>100,000<\/mn><mspace width=\"0.1667em\"><\/mspace><mn>032<\/mn><mspace width=\"0.1667em\"><\/mspace><mn>5<\/mn><mo form=\"prefix\" stretchy=\"false\">(<\/mo><mn>83<\/mn><mo form=\"postfix\" stretchy=\"false\">)<\/mo><mspace width=\"0.2778em\"><\/mspace><mrow><mi mathvariant=\"normal\">g<\/mi><\/mrow><\/mrow><annotation encoding=\"application\/x-tex\">m = 100,000\\,032\\,5(83) \\;\\mathrm{g}<\/annotation><\/semantics><\/math>.<\/p>\n\n\n\n<h3 class=\"wp-block-heading\">Demi-intervalle et incertitude-type<\/h3>\n\n\n\n<p class=\"has-medium-font-size\">L\u2019incertitude fournie pour une grandeur d'entr\u00e9e <math data-latex=\"x_i\"><semantics><msub><mi>x<\/mi><mi>i<\/mi><\/msub><annotation encoding=\"application\/x-tex\">x_i<\/annotation><\/semantics><\/math> n'est pas n\u00e9cessairement une incertitude-type c'est \u00e0 dire un \u00e9cart-type mais peut-\u00eatre un multiple de l'\u00e9cart-type ou un demi-intervalle. Dans le cas o\u00f9 l'incertitude fournie est un intervalle correspondant \u00e0 un niveau de confiance de 90, 95 ou 99%, l'incertitude-type est obtenue en divisant l'intervalle par les facteurs 1,64; 1,96 et 2,58 correspondant aux trois niveaux de confiances ci-dessus et en supposant qu'une loi normale a \u00e9t\u00e9 utilis\u00e9 pour d\u00e9terminer l'intervalle au niveau de confiance donn\u00e9.<\/p>\n\n\n\n<p class=\"has-medium-font-size\">Dans le cas o\u00f9 seules les limites inf\u00e9rieures et sup\u00e9rieures pour une grandeur <math data-latex=\"X_i\"><semantics><msub><mi>X<\/mi><mi>i<\/mi><\/msub><annotation encoding=\"application\/x-tex\">X_i<\/annotation><\/semantics><\/math> sont connues, on peut juste conclure que la probabilit\u00e9 que la valeur <math data-latex=\"x_i\"><semantics><msub><mi>x<\/mi><mi>i<\/mi><\/msub><annotation encoding=\"application\/x-tex\">x_i<\/annotation><\/semantics><\/math> de <math data-latex=\"X_i\"><semantics><msub><mi>X<\/mi><mi>i<\/mi><\/msub><annotation encoding=\"application\/x-tex\">X_i<\/annotation><\/semantics><\/math> soient comprise entre les valeurs des limites <math data-latex=\"a_-\"><semantics><msub><mi>a<\/mi><mo>\u2212<\/mo><\/msub><annotation encoding=\"application\/x-tex\">a_-<\/annotation><\/semantics><\/math> et <math data-latex=\"a_+\"><semantics><msub><mi>a<\/mi><mo>+<\/mo><\/msub><annotation encoding=\"application\/x-tex\">a_+<\/annotation><\/semantics><\/math> est \u00e9gale \u00e0 1 et  \u00e0 0 en dehors de l'intervalle. La valeur de l'incertitude-type <math data-latex=\"u(x_i)\"><semantics><mrow><mi>u<\/mi><mo form=\"prefix\" stretchy=\"false\">(<\/mo><msub><mi>x<\/mi><mi>i<\/mi><\/msub><mo form=\"postfix\" stretchy=\"false\">)<\/mo><\/mrow><annotation encoding=\"application\/x-tex\">u(x_i)<\/annotation><\/semantics><\/math> d\u00e9pend alors des connaissances sur les valeurs possibles de <math data-latex=\"X_i\"><semantics><msub><mi>X<\/mi><mi>i<\/mi><\/msub><annotation encoding=\"application\/x-tex\">X_i<\/annotation><\/semantics><\/math> \u00e0 l\u2019int\u00e9rieur de l'intervalle <math data-latex=\"2a = a_+-a_-\"><semantics><mrow><mn>2<\/mn><mi>a<\/mi><mo>=<\/mo><msub><mi>a<\/mi><mo form=\"prefix\" stretchy=\"false\">+<\/mo><\/msub><mo>\u2212<\/mo><msub><mi>a<\/mi><mo form=\"prefix\" stretchy=\"false\">\u2212<\/mo><\/msub><\/mrow><annotation encoding=\"application\/x-tex\">2a = a_+-a_-<\/annotation><\/semantics><\/math> (<math data-latex=\"a\"><semantics><mi>a<\/mi><annotation encoding=\"application\/x-tex\">a<\/annotation><\/semantics><\/math> est le demi-intervalle).<\/p>\n\n\n\n<figure class=\"wp-block-table aligncenter has-medium-font-size\"><table class=\"has-background\" style=\"background-color:#edecec\"><tbody><tr><td class=\"has-text-align-center\" data-align=\"center\">Connaissance<\/td><td class=\"has-text-align-center\" data-align=\"center\">distribution<\/td><td class=\"has-text-align-center\" data-align=\"center\">incertitude-type<\/td><td><\/td><\/tr><tr><td class=\"has-text-align-center\" data-align=\"center\">aucune<\/td><td class=\"has-text-align-center\" data-align=\"center\">rectangulaire<\/td><td class=\"has-text-align-center\" data-align=\"center\"><math data-latex=\"\\frac{a}{\\sqrt{3}}\"><semantics><mfrac><mi>a<\/mi><msqrt><mn>3<\/mn><\/msqrt><\/mfrac><annotation encoding=\"application\/x-tex\">\\frac{a}{\\sqrt{3}}<\/annotation><\/semantics><\/math><\/td><td><img loading=\"lazy\" decoding=\"async\" width=\"150\" height=\"122\" class=\"wp-image-117\" style=\"width: 150px;\" src=\"https:\/\/sciences-physiques.org\/wp-content\/uploads\/2026\/04\/rectangulaire.png\" alt=\"\" srcset=\"https:\/\/sciences-physiques.org\/wp-content\/uploads\/2026\/04\/rectangulaire.png 677w, https:\/\/sciences-physiques.org\/wp-content\/uploads\/2026\/04\/rectangulaire-300x244.png 300w\" sizes=\"auto, (max-width: 150px) 100vw, 150px\" \/><\/td><\/tr><tr><td class=\"has-text-align-center\" data-align=\"center\">Valeurs autour des limites<br> moins probables<\/td><td class=\"has-text-align-center\" data-align=\"center\">trap\u00e9zo\u00efdale de base <math data-latex=\"2a\"><semantics><mrow><mn>2<\/mn><mi>a<\/mi><\/mrow><annotation encoding=\"application\/x-tex\">2a<\/annotation><\/semantics><\/math> <br>et de sommet <math data-latex=\"2 a\\beta\"><semantics><mrow><mn>2<\/mn><mi>a<\/mi><mi>\u03b2<\/mi><\/mrow><annotation encoding=\"application\/x-tex\">2 a\\beta<\/annotation><\/semantics><\/math> <br>(<math data-latex=\"0\\leq \\beta \\leq 1\"><semantics><mrow><mn>0<\/mn><mo>\u2264<\/mo><mi>\u03b2<\/mi><mo>\u2264<\/mo><mn>1<\/mn><\/mrow><annotation encoding=\"application\/x-tex\">0\\leq \\beta \\leq 1<\/annotation><\/semantics><\/math>)<\/td><td class=\"has-text-align-center\" data-align=\"center\"><math data-latex=\"\\frac{a\\sqrt{1+\\beta^2}}{\\sqrt{6}}\"><semantics><mfrac><mrow><mi>a<\/mi><msqrt><mrow><mn>1<\/mn><mo>+<\/mo><msup><mi>\u03b2<\/mi><mn>2<\/mn><\/msup><\/mrow><\/msqrt><\/mrow><msqrt><mn>6<\/mn><\/msqrt><\/mfrac><annotation encoding=\"application\/x-tex\">\\frac{a\\sqrt{1+\\beta^2}}{\\sqrt{6}}<\/annotation><\/semantics><\/math><\/td><td><img loading=\"lazy\" decoding=\"async\" width=\"150\" height=\"125\" class=\"wp-image-116\" style=\"width: 150px;\" src=\"https:\/\/sciences-physiques.org\/wp-content\/uploads\/2026\/04\/trapezoidale.png\" alt=\"\" srcset=\"https:\/\/sciences-physiques.org\/wp-content\/uploads\/2026\/04\/trapezoidale.png 649w, https:\/\/sciences-physiques.org\/wp-content\/uploads\/2026\/04\/trapezoidale-300x249.png 300w\" sizes=\"auto, (max-width: 150px) 100vw, 150px\" \/><\/td><\/tr><tr><td class=\"has-text-align-center\" data-align=\"center\">Valeurs autour des limites<br> moins probables<\/td><td class=\"has-text-align-center\" data-align=\"center\">Triangulaire de base <br> (<math data-latex=\"2a\"><semantics><mrow><mn>2<\/mn><mi>a<\/mi><\/mrow><annotation encoding=\"application\/x-tex\">2a<\/annotation><\/semantics><\/math><math data-latex=\"\\beta = 0)\"><semantics><mrow><mi>\u03b2<\/mi><mo>=<\/mo><mn>0<\/mn><mo form=\"postfix\" stretchy=\"false\">)<\/mo><\/mrow><annotation encoding=\"application\/x-tex\">\\beta = 0)<\/annotation><\/semantics><\/math><\/td><td class=\"has-text-align-center\" data-align=\"center\"><math data-latex=\"\\frac{a}{\\sqrt{6}}\"><semantics><mfrac><mi>a<\/mi><msqrt><mn>6<\/mn><\/msqrt><\/mfrac><annotation encoding=\"application\/x-tex\">\\frac{a}{\\sqrt{6}}<\/annotation><\/semantics><\/math><\/td><td><img loading=\"lazy\" decoding=\"async\" width=\"150\" height=\"127\" class=\"wp-image-115\" style=\"width: 150px;\" src=\"https:\/\/sciences-physiques.org\/wp-content\/uploads\/2026\/04\/triangulaire.png\" alt=\"\" srcset=\"https:\/\/sciences-physiques.org\/wp-content\/uploads\/2026\/04\/triangulaire.png 655w, https:\/\/sciences-physiques.org\/wp-content\/uploads\/2026\/04\/triangulaire-300x254.png 300w\" sizes=\"auto, (max-width: 150px) 100vw, 150px\" \/><\/td><\/tr><tr><td class=\"has-text-align-center\" data-align=\"center\">Valeurs autour des limites<br> plus probables<\/td><td class=\"has-text-align-center\" data-align=\"center\">Arcsinus<\/td><td class=\"has-text-align-center\" data-align=\"center\"><math data-latex=\"\\frac{a}{\\sqrt{2}}\"><semantics><mfrac><mi>a<\/mi><msqrt><mn>2<\/mn><\/msqrt><\/mfrac><annotation encoding=\"application\/x-tex\">\\frac{a}{\\sqrt{2}}<\/annotation><\/semantics><\/math><\/td><td><img loading=\"lazy\" decoding=\"async\" width=\"150\" height=\"135\" class=\"wp-image-114\" style=\"width: 150px;\" src=\"https:\/\/sciences-physiques.org\/wp-content\/uploads\/2026\/04\/arcsinus.png\" alt=\"\" srcset=\"https:\/\/sciences-physiques.org\/wp-content\/uploads\/2026\/04\/arcsinus.png 661w, https:\/\/sciences-physiques.org\/wp-content\/uploads\/2026\/04\/arcsinus-300x270.png 300w\" sizes=\"auto, (max-width: 150px) 100vw, 150px\" \/><\/td><\/tr><\/tbody><\/table><\/figure>\n\n\n<div style=\"border: 3px outset #fab300; border-radius: 26px; background-color: #fff6e2; \" class=\"ub-styled-box ub-bordered-box wp-block-ub-styled-box\" id=\"ub-styled-box-1ed14b6c-44eb-422d-8c58-af83cdf3c6c1\">\n<p class=\"has-small-font-size\" id=\"ub-styled-box-bordered-content-\">Exemple : <\/p>\n\n\n\n<ul class=\"wp-block-list\">\n<li class=\"has-small-font-size\">La r\u00e9solution d''un appareil de mesure num\u00e9rique est \u00e9gale  au 1\/2 digit avec une distribution rectangulaire : <math data-latex=\"\\frac{digit}{2\\sqrt{3}}\"><semantics><mfrac><mrow><mi>d<\/mi><mi>i<\/mi><mi>g<\/mi><mi>i<\/mi><mi>t<\/mi><\/mrow><mrow><mn>2<\/mn><msqrt><mn>3<\/mn><\/msqrt><\/mrow><\/mfrac><annotation encoding=\"application\/x-tex\">\\frac{digit}{2\\sqrt{3}}<\/annotation><\/semantics><\/math><\/li>\n\n\n\n<li class=\"has-small-font-size\">La r\u00e9solution d'un appareil de mesure analogique est \u00e9gale  \u00e0 la 1\/2 graduation avec une distribution rectangulaire : <math data-latex=\"\\frac{graduation}{2\\sqrt{3}}\"><semantics><mfrac><mrow><mi>g<\/mi><mi>r<\/mi><mi>a<\/mi><mi>d<\/mi><mi>u<\/mi><mi>a<\/mi><mi>t<\/mi><mi>i<\/mi><mi>o<\/mi><mi>n<\/mi><\/mrow><mrow><mn>2<\/mn><msqrt><mn>3<\/mn><\/msqrt><\/mrow><\/mfrac><annotation encoding=\"application\/x-tex\">\\frac{graduation}{2\\sqrt{3}}<\/annotation><\/semantics><\/math><\/li>\n\n\n\n<li class=\"has-small-font-size\">L'erreur maximale tol\u00e9r\u00e9e d'une fiole jaug\u00e9e de classe A de capacit\u00e9 nominale 100 mL est selon l'ISO 1042 : <math data-latex=\"EMT = \\pm 0,100\\; \\mathrm{mL}\"><semantics><mrow><mi>E<\/mi><mi>M<\/mi><mi>T<\/mi><mo>=<\/mo><mo form=\"prefix\" stretchy=\"false\">\u00b1<\/mo><mn>0,100<\/mn><mspace width=\"0.2778em\"><\/mspace><mrow><mtext><\/mtext><mi>mL<\/mi><\/mrow><\/mrow><annotation encoding=\"application\/x-tex\">EMT = \\pm 0,100\\; \\mathrm{mL}<\/annotation><\/semantics><\/math>. L'instrument volum\u00e9trique \u00e9tant \u00e9talonn\u00e9 individuellement, il raisonnable de penser que la valeur la plus probable est plus proche de la valeur nominale que des valeurs limites (distribution triangulaire). L'incertitude de tol\u00e9rance de la verrerie de classe A sera donc prise \u00e9gale \u00e0 : <math data-latex=\"\\frac{EMT}{\\sqrt{6}}\"><semantics><mfrac><mrow><mi>E<\/mi><mi>M<\/mi><mi>T<\/mi><\/mrow><msqrt><mn>6<\/mn><\/msqrt><\/mfrac><annotation encoding=\"application\/x-tex\">\\frac{EMT}{\\sqrt{6}}<\/annotation><\/semantics><\/math><\/li>\n\n\n\n<li class=\"has-small-font-size\">Si la temp\u00e9rature d'une pi\u00e8ce est r\u00e9gul\u00e9e \u00e0 <math data-latex=\"T = 20\\pm 4 \\mathrm{\u00b0C}\"><semantics><mrow><mi>T<\/mi><mo>=<\/mo><mn>20<\/mn><mo>\u00b1<\/mo><mn>4<\/mn><mrow><mi>\u00b0<\/mi><mrow><mi mathvariant=\"normal\">C<\/mi><\/mrow><\/mrow><\/mrow><annotation encoding=\"application\/x-tex\">T = 20\\pm 4 \\mathrm{\u00b0C}<\/annotation><\/semantics><\/math>, elle va osciller entre deux valeurs limites 16 et 24 \u00b0C. On peut consid\u00e9rer que cette variation est sinuso\u00efdale. L'incertitude-type de la temp\u00e9rature de la pi\u00e8ce sera <math data-latex=\"u(T)=\\frac{4}{\\sqrt{2}} = 2,8\u00b0\\mathrm{C}\"><semantics><mrow><mi>u<\/mi><mo form=\"prefix\" stretchy=\"false\">(<\/mo><mi>T<\/mi><mo form=\"postfix\" stretchy=\"false\">)<\/mo><mo>=<\/mo><mfrac><mn>4<\/mn><msqrt><mn>2<\/mn><\/msqrt><\/mfrac><mo>=<\/mo><mn>2,8<\/mn><mi>\u00b0<\/mi><mrow><mi mathvariant=\"normal\">C<\/mi><\/mrow><\/mrow><annotation encoding=\"application\/x-tex\">u(T)=\\frac{4}{\\sqrt{2}} = 2,8\u00b0\\mathrm{C}<\/annotation><\/semantics><\/math> (distribution arcsinus).<\/li>\n<\/ul>\n\n\n<\/div>\n\n\n<h3 class=\"wp-block-heading\">\u00c9valuation de l'incertitude-type compos\u00e9e<\/h3>\n\n\n\n<p class=\"has-medium-font-size\">Dans le cas o\u00f9 les grandeurs d'entr\u00e9e sont ind\u00e9pendantes, l'incertitude-type de la grandeur de sortie <math data-latex=\"y\"><semantics><mi>y<\/mi><annotation encoding=\"application\/x-tex\">y<\/annotation><\/semantics><\/math> o\u00f9 <math data-latex=\"y\"><semantics><mi>y<\/mi><annotation encoding=\"application\/x-tex\">y<\/annotation><\/semantics><\/math> est l'estimation du mesurande <math data-latex=\"Y\"><semantics><mi>Y<\/mi><annotation encoding=\"application\/x-tex\">Y<\/annotation><\/semantics><\/math>, donc le r\u00e9sultat du mesurage obtenus \u00e0 partir des estimations <math data-latex=\"x_1, x_2,\\ldots,x_N\"><semantics><mrow><msub><mi>x<\/mi><mn>1<\/mn><\/msub><mo separator=\"true\">,<\/mo><msub><mi>x<\/mi><mn>2<\/mn><\/msub><mo separator=\"true\">,<\/mo><mo>\u2026<\/mo><mo separator=\"true\">,<\/mo><msub><mi>x<\/mi><mi>N<\/mi><\/msub><\/mrow><annotation encoding=\"application\/x-tex\">x_1, x_2,\\ldots,x_N<\/annotation><\/semantics><\/math> des grandeurs d'entr\u00e9es <math data-latex=\"X_1, X_2, \\dots, X_N\"><semantics><mrow><msub><mi>X<\/mi><mn>1<\/mn><\/msub><mo separator=\"true\">,<\/mo><msub><mi>X<\/mi><mn>2<\/mn><\/msub><mo separator=\"true\">,<\/mo><mo>\u2026<\/mo><mo separator=\"true\">,<\/mo><msub><mi>X<\/mi><mi>N<\/mi><\/msub><\/mrow><annotation encoding=\"application\/x-tex\">X_1, X_2, \\dots, X_N<\/annotation><\/semantics><\/math> et de la fonction <math data-latex=\"f\"><semantics><mi>f<\/mi><annotation encoding=\"application\/x-tex\">f<\/annotation><\/semantics><\/math>.<\/p>\n\n\n\n<div class=\"wp-block-katex-display-block katex-eq\" data-katex-display=\"true\"><pre>u_c(y) = \\sqrt{\\sum\\limits_{i=1}^{N}\\left(\\frac{\\partial f}{\\partial x_i}u\\right)^2 u^2(x_i)}<\/pre><\/div>\n\n\n\n<p class=\"has-medium-font-size\">Cette relation porte le nom de loi de propagation de l'incertitude. Les d\u00e9riv\u00e9es partielles <math data-latex=\"\\frac{\\partial f}{\\partial x_i}\"><semantics><mfrac><mrow><mi>\u2202<\/mi><mi>f<\/mi><\/mrow><mrow><mi>\u2202<\/mi><msub><mi>x<\/mi><mi>i<\/mi><\/msub><\/mrow><\/mfrac><annotation encoding=\"application\/x-tex\">\\frac{\\partial f}{\\partial x_i}<\/annotation><\/semantics><\/math> portent le nom de coefficients de sensibilit\u00e9 <math data-latex=\"c_i\"><semantics><msub><mi>c<\/mi><mi>i<\/mi><\/msub><annotation encoding=\"application\/x-tex\">c_i<\/annotation><\/semantics><\/math> et les termes  <math data-latex=\"\\frac{\\partial f}{\\partial x_i}u(x_i)\"><semantics><mrow><mfrac><mrow><mi>\u2202<\/mi><mi>f<\/mi><\/mrow><mrow><mi>\u2202<\/mi><msub><mi>x<\/mi><mi>i<\/mi><\/msub><\/mrow><\/mfrac><mi>u<\/mi><mo form=\"prefix\" stretchy=\"false\">(<\/mo><msub><mi>x<\/mi><mi>i<\/mi><\/msub><mo form=\"postfix\" stretchy=\"false\">)<\/mo><\/mrow><annotation encoding=\"application\/x-tex\">\\frac{\\partial f}{\\partial x_i}u(x_i)<\/annotation><\/semantics><\/math> sont les composantes de l'incertitude. L'incertitude compos\u00e9e est donc la racine carr\u00e9 de la somme quadratique des composantes de l'incertitude <math data-latex=\"u_i(y) = c_iu(x_i)\"><semantics><mrow><msub><mi>u<\/mi><mi>i<\/mi><\/msub><mo form=\"prefix\" stretchy=\"false\">(<\/mo><mi>y<\/mi><mo form=\"postfix\" stretchy=\"false\">)<\/mo><mo>=<\/mo><msub><mi>c<\/mi><mi>i<\/mi><\/msub><mi>u<\/mi><mo form=\"prefix\" stretchy=\"false\">(<\/mo><msub><mi>x<\/mi><mi>i<\/mi><\/msub><mo form=\"postfix\" stretchy=\"false\">)<\/mo><\/mrow><annotation encoding=\"application\/x-tex\">u_i(y) = c_iu(x_i)<\/annotation><\/semantics><\/math>.<\/p>\n\n\n<div style=\"border: 3px outset #fab300; border-radius: 26px; background-color: #fff6e2; \" class=\"ub-styled-box ub-bordered-box wp-block-ub-styled-box\" id=\"ub-styled-box-9f5368b2-760c-435b-bde9-24a1f99a74e6\">\n<p class=\"has-small-font-size\" id=\"ub-styled-box-bordered-content-\">Exemple : Puissance dissip\u00e9e dans une r\u00e9sistance.<\/p>\n\n\n\n<ul class=\"wp-block-list\">\n<li class=\"has-small-font-size\">La puissance dissip\u00e9e dans une r\u00e9sistance  <math data-latex=\"R\"><semantics><mi>R<\/mi><annotation encoding=\"application\/x-tex\">R<\/annotation><\/semantics><\/math> est fonction de la tension \u00e0 ces bornes <math data-latex=\"U\"><semantics><mi>U<\/mi><annotation encoding=\"application\/x-tex\">U<\/annotation><\/semantics><\/math>. La r\u00e9sistance  <math data-latex=\"R\"><semantics><mi>R<\/mi><annotation encoding=\"application\/x-tex\">R<\/annotation><\/semantics><\/math> varie en fonction de la temp\u00e9rature selon une loi : <math data-latex=\"R=R_0\\left(1+\\alpha (T-T_0)\\right)\"><semantics><mrow><mi>R<\/mi><mo>=<\/mo><msub><mi>R<\/mi><mn>0<\/mn><\/msub><mrow><mo fence=\"true\" form=\"prefix\">(<\/mo><mn>1<\/mn><mo>+<\/mo><mi>\u03b1<\/mi><mo form=\"prefix\" stretchy=\"false\">(<\/mo><mi>T<\/mi><mo>\u2212<\/mo><msub><mi>T<\/mi><mn>0<\/mn><\/msub><mo form=\"postfix\" stretchy=\"false\">)<\/mo><mo fence=\"true\" form=\"postfix\">)<\/mo><\/mrow><\/mrow><annotation encoding=\"application\/x-tex\">R=R_0\\left(1+\\alpha (T-T_0)\\right)<\/annotation><\/semantics><\/math> o\u00f9 <math data-latex=\"R_0\"><semantics><msub><mi>R<\/mi><mn>0<\/mn><\/msub><annotation encoding=\"application\/x-tex\">R_0<\/annotation><\/semantics><\/math> est la valeur de r\u00e9sistance \u00e0 la temp\u00e9rature <math data-latex=\"T_0\"><semantics><msub><mi>T<\/mi><mn>0<\/mn><\/msub><annotation encoding=\"application\/x-tex\">T_0<\/annotation><\/semantics><\/math>. On a donc <math data-latex=\"P=f(U, R_0, \\alpha, T) = \\frac{U^2}{R_0\\left(1+\\alpha(T-T_0)\\right)}\"><semantics><mrow><mi>P<\/mi><mo>=<\/mo><mi>f<\/mi><mo form=\"prefix\" stretchy=\"false\">(<\/mo><mi>U<\/mi><mo separator=\"true\">,<\/mo><msub><mi>R<\/mi><mn>0<\/mn><\/msub><mo separator=\"true\">,<\/mo><mi>\u03b1<\/mi><mo separator=\"true\">,<\/mo><mi>T<\/mi><mo form=\"postfix\" stretchy=\"false\">)<\/mo><mo>=<\/mo><mfrac><msup><mi>U<\/mi><mn>2<\/mn><\/msup><mrow><msub><mi>R<\/mi><mn>0<\/mn><\/msub><mrow><mo fence=\"true\" form=\"prefix\">(<\/mo><mn>1<\/mn><mo>+<\/mo><mi>\u03b1<\/mi><mo form=\"prefix\" stretchy=\"false\">(<\/mo><mi>T<\/mi><mo>\u2212<\/mo><msub><mi>T<\/mi><mn>0<\/mn><\/msub><mo form=\"postfix\" stretchy=\"false\">)<\/mo><mo fence=\"true\" form=\"postfix\">)<\/mo><\/mrow><\/mrow><\/mfrac><\/mrow><annotation encoding=\"application\/x-tex\">P=f(U, R_0, \\alpha, T) = \\frac{U^2}{R_0\\left(1+\\alpha(T-T_0)\\right)}<\/annotation><\/semantics><\/math>.<\/li>\n\n\n\n<li class=\"has-small-font-size\"><math data-latex=\"c_1 = \\frac{\\partial f}{\\partial U} = \\frac{2U}{R_0\\left(1+\\alpha(T-T_0)\\right)}=\\frac{2P}{V}\"><semantics><mrow><msub><mi>c<\/mi><mn>1<\/mn><\/msub><mo>=<\/mo><mfrac><mrow><mi>\u2202<\/mi><mi>f<\/mi><\/mrow><mrow><mi>\u2202<\/mi><mi>U<\/mi><\/mrow><\/mfrac><mo>=<\/mo><mfrac><mrow><mn>2<\/mn><mi>U<\/mi><\/mrow><mrow><msub><mi>R<\/mi><mn>0<\/mn><\/msub><mrow><mo fence=\"true\" form=\"prefix\">(<\/mo><mn>1<\/mn><mo>+<\/mo><mi>\u03b1<\/mi><mo form=\"prefix\" stretchy=\"false\">(<\/mo><mi>T<\/mi><mo>\u2212<\/mo><msub><mi>T<\/mi><mn>0<\/mn><\/msub><mo form=\"postfix\" stretchy=\"false\">)<\/mo><mo fence=\"true\" form=\"postfix\">)<\/mo><\/mrow><\/mrow><\/mfrac><mo>=<\/mo><mfrac><mrow><mn>2<\/mn><mi>P<\/mi><\/mrow><mi>V<\/mi><\/mfrac><\/mrow><annotation encoding=\"application\/x-tex\">c_1 = \\frac{\\partial f}{\\partial U} = \\frac{2U}{R_0\\left(1+\\alpha(T-T_0)\\right)}=\\frac{2P}{V}<\/annotation><\/semantics><\/math><\/li>\n\n\n\n<li class=\"has-small-font-size\"><math data-latex=\"c_2 = \\frac{\\partial f}{\\partial R_0} = - \\frac{U^2}{R_0^2\\left(1+\\alpha(T-T_0)\\right)}=-\\frac{P}{R_0}\"><semantics><mrow><msub><mi>c<\/mi><mn>2<\/mn><\/msub><mo>=<\/mo><mfrac><mrow><mi>\u2202<\/mi><mi>f<\/mi><\/mrow><mrow><mi>\u2202<\/mi><msub><mi>R<\/mi><mn>0<\/mn><\/msub><\/mrow><\/mfrac><mo>=<\/mo><mo form=\"prefix\" stretchy=\"false\">\u2212<\/mo><mfrac><msup><mi>U<\/mi><mn>2<\/mn><\/msup><mrow><msubsup><mi>R<\/mi><mn>0<\/mn><mn>2<\/mn><\/msubsup><mrow><mo fence=\"true\" form=\"prefix\">(<\/mo><mn>1<\/mn><mo>+<\/mo><mi>\u03b1<\/mi><mo form=\"prefix\" stretchy=\"false\">(<\/mo><mi>T<\/mi><mo>\u2212<\/mo><msub><mi>T<\/mi><mn>0<\/mn><\/msub><mo form=\"postfix\" stretchy=\"false\">)<\/mo><mo fence=\"true\" form=\"postfix\">)<\/mo><\/mrow><\/mrow><\/mfrac><mo>=<\/mo><mo form=\"prefix\" stretchy=\"false\">\u2212<\/mo><mfrac><mi>P<\/mi><msub><mi>R<\/mi><mn>0<\/mn><\/msub><\/mfrac><\/mrow><annotation encoding=\"application\/x-tex\">c_2 = \\frac{\\partial f}{\\partial R_0} = - \\frac{U^2}{R_0^2\\left(1+\\alpha(T-T_0)\\right)}=-\\frac{P}{R_0}<\/annotation><\/semantics><\/math><\/li>\n\n\n\n<li class=\"has-small-font-size\"><math data-latex=\"c_3 = \\frac{\\partial f}{\\partial \\alpha} = - \\frac{U^2(T-T_0)}{R_0\\left(1+\\alpha(T-T_0)\\right)}=-\\frac{P(T-T_0)}{1+\\alpha (T-T_0)}\"><semantics><mrow><msub><mi>c<\/mi><mn>3<\/mn><\/msub><mo>=<\/mo><mfrac><mrow><mi>\u2202<\/mi><mi>f<\/mi><\/mrow><mrow><mi>\u2202<\/mi><mi>\u03b1<\/mi><\/mrow><\/mfrac><mo>=<\/mo><mo form=\"prefix\" stretchy=\"false\">\u2212<\/mo><mfrac><mrow><msup><mi>U<\/mi><mn>2<\/mn><\/msup><mo form=\"prefix\" stretchy=\"false\">(<\/mo><mi>T<\/mi><mo>\u2212<\/mo><msub><mi>T<\/mi><mn>0<\/mn><\/msub><mo form=\"postfix\" stretchy=\"false\" lspace=\"0em\" rspace=\"0em\">)<\/mo><\/mrow><mrow><msub><mi>R<\/mi><mn>0<\/mn><\/msub><mrow><mo fence=\"true\" form=\"prefix\">(<\/mo><mn>1<\/mn><mo>+<\/mo><mi>\u03b1<\/mi><mo form=\"prefix\" stretchy=\"false\">(<\/mo><mi>T<\/mi><mo>\u2212<\/mo><msub><mi>T<\/mi><mn>0<\/mn><\/msub><mo form=\"postfix\" stretchy=\"false\">)<\/mo><mo fence=\"true\" form=\"postfix\">)<\/mo><\/mrow><\/mrow><\/mfrac><mo>=<\/mo><mo form=\"prefix\" stretchy=\"false\">\u2212<\/mo><mfrac><mrow><mi>P<\/mi><mo form=\"prefix\" stretchy=\"false\">(<\/mo><mi>T<\/mi><mo>\u2212<\/mo><msub><mi>T<\/mi><mn>0<\/mn><\/msub><mo form=\"postfix\" stretchy=\"false\" lspace=\"0em\" rspace=\"0em\">)<\/mo><\/mrow><mrow><mn>1<\/mn><mo>+<\/mo><mi>\u03b1<\/mi><mo form=\"prefix\" stretchy=\"false\">(<\/mo><mi>T<\/mi><mo>\u2212<\/mo><msub><mi>T<\/mi><mn>0<\/mn><\/msub><mo form=\"postfix\" stretchy=\"false\" lspace=\"0em\" rspace=\"0em\">)<\/mo><\/mrow><\/mfrac><\/mrow><annotation encoding=\"application\/x-tex\">c_3 = \\frac{\\partial f}{\\partial \\alpha} = - \\frac{U^2(T-T_0)}{R_0\\left(1+\\alpha(T-T_0)\\right)}=-\\frac{P(T-T_0)}{1+\\alpha (T-T_0)}<\/annotation><\/semantics><\/math><\/li>\n\n\n\n<li class=\"has-small-font-size\"><math data-latex=\"c_4 = \\frac{\\partial f}{\\partial T} = - \\frac{U^2\\alpha}{R_0\\left(1+\\alpha(T-T_0)\\right)^2}=-\\frac{P\\alpha}{1+\\alpha (T-T_0)}\"><semantics><mrow><msub><mi>c<\/mi><mn>4<\/mn><\/msub><mo>=<\/mo><mfrac><mrow><mi>\u2202<\/mi><mi>f<\/mi><\/mrow><mrow><mi>\u2202<\/mi><mi>T<\/mi><\/mrow><\/mfrac><mo>=<\/mo><mo form=\"prefix\" stretchy=\"false\">\u2212<\/mo><mfrac><mrow><msup><mi>U<\/mi><mn>2<\/mn><\/msup><mi>\u03b1<\/mi><\/mrow><mrow><msub><mi>R<\/mi><mn>0<\/mn><\/msub><msup><mrow><mo fence=\"true\" form=\"prefix\">(<\/mo><mn>1<\/mn><mo>+<\/mo><mi>\u03b1<\/mi><mo form=\"prefix\" stretchy=\"false\">(<\/mo><mi>T<\/mi><mo>\u2212<\/mo><msub><mi>T<\/mi><mn>0<\/mn><\/msub><mo form=\"postfix\" stretchy=\"false\">)<\/mo><mo fence=\"true\" form=\"postfix\">)<\/mo><\/mrow><mn>2<\/mn><\/msup><\/mrow><\/mfrac><mo>=<\/mo><mo form=\"prefix\" stretchy=\"false\">\u2212<\/mo><mfrac><mrow><mi>P<\/mi><mi>\u03b1<\/mi><\/mrow><mrow><mn>1<\/mn><mo>+<\/mo><mi>\u03b1<\/mi><mo form=\"prefix\" stretchy=\"false\">(<\/mo><mi>T<\/mi><mo>\u2212<\/mo><msub><mi>T<\/mi><mn>0<\/mn><\/msub><mo form=\"postfix\" stretchy=\"false\" lspace=\"0em\" rspace=\"0em\">)<\/mo><\/mrow><\/mfrac><\/mrow><annotation encoding=\"application\/x-tex\">c_4 = \\frac{\\partial f}{\\partial T} = - \\frac{U^2\\alpha}{R_0\\left(1+\\alpha(T-T_0)\\right)^2}=-\\frac{P\\alpha}{1+\\alpha (T-T_0)}<\/annotation><\/semantics><\/math><\/li>\n\n\n\n<li class=\"has-small-font-size\"><math data-latex=\"u(P) = \\sqrt{c_1^2u^2(U)+c_2^2u^2(R_0)+c_3^2u^2(\\alpha)+c_4^2u^2(T)}\"><semantics><mrow><mi>u<\/mi><mo form=\"prefix\" stretchy=\"false\">(<\/mo><mi>P<\/mi><mo form=\"postfix\" stretchy=\"false\">)<\/mo><mo>=<\/mo><msqrt><mrow><msubsup><mi>c<\/mi><mn>1<\/mn><mn>2<\/mn><\/msubsup><msup><mi>u<\/mi><mn>2<\/mn><\/msup><mo form=\"prefix\" stretchy=\"false\">(<\/mo><mi>U<\/mi><mo form=\"postfix\" stretchy=\"false\">)<\/mo><mo>+<\/mo><msubsup><mi>c<\/mi><mn>2<\/mn><mn>2<\/mn><\/msubsup><msup><mi>u<\/mi><mn>2<\/mn><\/msup><mo form=\"prefix\" stretchy=\"false\">(<\/mo><msub><mi>R<\/mi><mn>0<\/mn><\/msub><mo form=\"postfix\" stretchy=\"false\">)<\/mo><mo>+<\/mo><msubsup><mi>c<\/mi><mn>3<\/mn><mn>2<\/mn><\/msubsup><msup><mi>u<\/mi><mn>2<\/mn><\/msup><mo form=\"prefix\" stretchy=\"false\">(<\/mo><mi>\u03b1<\/mi><mo form=\"postfix\" stretchy=\"false\">)<\/mo><mo>+<\/mo><msubsup><mi>c<\/mi><mn>4<\/mn><mn>2<\/mn><\/msubsup><msup><mi>u<\/mi><mn>2<\/mn><\/msup><mo form=\"prefix\" stretchy=\"false\">(<\/mo><mi>T<\/mi><mo form=\"postfix\" stretchy=\"false\" lspace=\"0em\" rspace=\"0em\">)<\/mo><\/mrow><\/msqrt><\/mrow><annotation encoding=\"application\/x-tex\">u(P) = \\sqrt{c_1^2u^2(U)+c_2^2u^2(R_0)+c_3^2u^2(\\alpha)+c_4^2u^2(T)}<\/annotation><\/semantics><\/math><\/li>\n<\/ul>\n\n\n<\/div>\n\n\n<p class=\"has-medium-font-size\">Si <math data-latex=\"Y = c_1X_1 + c_2X_2 + \\ldots c_NX_N\"><semantics><mrow><mi>Y<\/mi><mo>=<\/mo><msub><mi>c<\/mi><mn>1<\/mn><\/msub><msub><mi>X<\/mi><mn>1<\/mn><\/msub><mo>+<\/mo><msub><mi>c<\/mi><mn>2<\/mn><\/msub><msub><mi>X<\/mi><mn>2<\/mn><\/msub><mo>+<\/mo><mo>\u2026<\/mo><msub><mi>c<\/mi><mi>N<\/mi><\/msub><msub><mi>X<\/mi><mi>N<\/mi><\/msub><\/mrow><annotation encoding=\"application\/x-tex\">Y = c_1X_1 + c_2X_2 + \\ldots c_NX_N<\/annotation><\/semantics><\/math> alors l'incertitude combin\u00e9e s'\u00e9crit simplement :<\/p>\n\n\n\n<div class=\"wp-block-katex-display-block katex-eq\" data-katex-display=\"true\"><pre>u_c(y) = \\sqrt{\\sum\\limits_{i=1}^{N}c_i^2 u^2(x_i)}<\/pre><\/div>\n\n\n\n<p class=\"has-medium-font-size\">Si <math data-latex=\"Y = cX_1^{p_1} + c_2X_2^{p_2} + \\ldots c_NX_N^{p_N}\"><semantics><mrow><mi>Y<\/mi><mo>=<\/mo><mi>c<\/mi><msubsup><mi>X<\/mi><mn>1<\/mn><msub><mi>p<\/mi><mn>1<\/mn><\/msub><\/msubsup><mo>+<\/mo><msub><mi>c<\/mi><mn>2<\/mn><\/msub><msubsup><mi>X<\/mi><mn>2<\/mn><msub><mi>p<\/mi><mn>2<\/mn><\/msub><\/msubsup><mo>+<\/mo><mo>\u2026<\/mo><msub><mi>c<\/mi><mi>N<\/mi><\/msub><msubsup><mi>X<\/mi><mi>N<\/mi><msub><mi>p<\/mi><mi>N<\/mi><\/msub><\/msubsup><\/mrow><annotation encoding=\"application\/x-tex\">Y = cX_1^{p_1} + c_2X_2^{p_2} + \\ldots c_NX_N^{p_N}<\/annotation><\/semantics><\/math> alors l'incertitude combin\u00e9e s'\u00e9crit simplement :<\/p>\n\n\n\n<div class=\"wp-block-katex-display-block katex-eq\" data-katex-display=\"true\"><pre>\\frac{u_c(y)}{y} = \\sqrt{\\sum\\limits_{i=1}^{N}p_i^2 \\left(\\frac{u(x_i)}{x_i}\\right)^2}<\/pre><\/div>\n\n\n\n<p class=\"has-medium-font-size\">Si les grandeurs d'entr\u00e9e sont corr\u00e9l\u00e9es, la loi de propagation de l'incertitude s\u2019\u00e9crit en tenant compte des  covariances des grandeurs d'entr\u00e9e :<\/p>\n\n\n\n<div class=\"wp-block-katex-display-block katex-eq\" data-katex-display=\"true\"><pre>u_c^2(y) = \\sum\\limits_{i=1}^{N}\\left(\\frac{\\partial f}{\\partial x_i}u\\right)^2 u^2(x_i)+ 2 \\sum\\limits_{i=1}^{N-1}\\sum\\limits_{j=i+1}^{N}\\frac{\\partial f}{\\partial x_i}\\frac{\\partial f}{\\partial x_j}u(x_i,x_j)<\/pre><\/div>\n\n\n\n<h3 class=\"wp-block-heading\">Incertitude \u00e9largie<\/h3>\n\n\n\n<p class=\"has-medium-font-size\">Pour une meilleure compr\u00e9hension de l'incertitude-type, il est parfois n\u00e9cessaire de d\u00e9finir un intervalle \u00e0 l\u2019int\u00e9rieur duquel on puisse esp\u00e9rer voire se situer une large fraction de la distribution des valeurs qui pourraient \u00eatre attribu\u00e9es au mesurande. Cet intervalle est appel\u00e9 incertitude \u00e9largie <math data-latex=\"U\"><semantics><mi>U<\/mi><annotation encoding=\"application\/x-tex\">U<\/annotation><\/semantics><\/math> et s'obtient en multipliant l'incertitude-type par un facteur d\u2019\u00e9largissement <math data-latex=\"k\"><semantics><mi>k<\/mi><annotation encoding=\"application\/x-tex\">k<\/annotation><\/semantics><\/math>.<\/p>\n\n\n\n<div class=\"wp-block-katex-display-block katex-eq\" data-katex-display=\"true\"><pre>U = ku(y)<\/pre><\/div>\n\n\n\n<p class=\"has-medium-font-size\">On exprime alors le r\u00e9sultat d'un mesurage sous la forme <math data-latex=\"Y=y\\pm U\"><semantics><mrow><mi>Y<\/mi><mo>=<\/mo><mi>y<\/mi><mo>\u00b1<\/mo><mi>U<\/mi><\/mrow><annotation encoding=\"application\/x-tex\">Y=y\\pm U<\/annotation><\/semantics><\/math>.<\/p>\n\n\n\n<p class=\"has-medium-font-size\">La valeur du facteur d'\u00e9largissement est fonction du niveau de confiance correspondant \u00e0 la probabilit\u00e9 qu'une fraction \u00e9lev\u00e9e <math data-latex=\"p\"><semantics><mi>p<\/mi><annotation encoding=\"application\/x-tex\">p<\/annotation><\/semantics><\/math> de la loi de distribution qui caract\u00e9rise le mesurande <math data-latex=\"Y\"><semantics><mi>Y<\/mi><annotation encoding=\"application\/x-tex\">Y<\/annotation><\/semantics><\/math> se trouve dans l'intervalle <math data-latex=\"Y-U\"><semantics><mrow><mi>Y<\/mi><mo>\u2212<\/mo><mi>U<\/mi><\/mrow><annotation encoding=\"application\/x-tex\">Y-U<\/annotation><\/semantics><\/math>, <math data-latex=\"Y+U\"><semantics><mrow><mi>Y<\/mi><mo>+<\/mo><mi>U<\/mi><\/mrow><annotation encoding=\"application\/x-tex\">Y+U<\/annotation><\/semantics><\/math>. Si la loi de distribution des valeurs <math data-latex=\"y\"><semantics><mi>y<\/mi><annotation encoding=\"application\/x-tex\">y<\/annotation><\/semantics><\/math> de la grandeur  <math data-latex=\"Y\"><semantics><mi>Y<\/mi><annotation encoding=\"application\/x-tex\">Y<\/annotation><\/semantics><\/math> ob\u00e9it approximativement a une loi normale, le choix <math data-latex=\"k=2\"><semantics><mrow><mi>k<\/mi><mo>=<\/mo><mn>2<\/mn><\/mrow><annotation encoding=\"application\/x-tex\">k=2<\/annotation><\/semantics><\/math> fournit un intervalle avec un niveau de confiance de 95% et e choix 3 fournit un intervalle avec un niveau de confiance de 99% environ.<\/p>\n\n\n\n<p class=\"has-medium-font-size\">Dans le cas o\u00f9 le nombre d'observations est faible (<math data-latex=\"N&lt;30)\"><semantics><mrow><mi>N<\/mi><mo>&lt;<\/mo><mn>30<\/mn><mo form=\"postfix\" stretchy=\"false\">)<\/mo><\/mrow><annotation encoding=\"application\/x-tex\">N&lt;30)<\/annotation><\/semantics><\/math> et ne permet pas de v\u00e9rifier si la distribution des valeurs suit une loi normale, il convient de choisir une loi de <em>t<\/em>  (loi de Student) \u00e0 <math data-latex=\"N-1\"><semantics><mrow><mi>N<\/mi><mo>\u2212<\/mo><mn>1<\/mn><\/mrow><annotation encoding=\"application\/x-tex\">N-1<\/annotation><\/semantics><\/math> degr\u00e9s de libert\u00e9. Le coefficient d'\u00e9largissement <math data-latex=\"k\"><semantics><mi>k<\/mi><annotation encoding=\"application\/x-tex\">k<\/annotation><\/semantics><\/math> est alors donn\u00e9 dans la table de Student en fonction du niveau de confiance <math data-latex=\"1-\\alpha\"><semantics><mrow><mn>1<\/mn><mo>\u2212<\/mo><mi>\u03b1<\/mi><\/mrow><annotation encoding=\"application\/x-tex\">1-\\alpha<\/annotation><\/semantics><\/math>.<\/p>\n\n\n\n<h3 class=\"wp-block-heading\">Expression de l'incertitude<\/h3>\n\n\n\n<p class=\"has-medium-font-size\">Le r\u00e9sultat d'un mesurage comporte  :<\/p>\n\n\n\n<ol class=\"wp-block-list\">\n<li class=\"has-medium-font-size\"> la description compl\u00e8te de la mani\u00e8re dont le mesurande est d\u00e9fini, le mode op\u00e9ratoire permettant son estimation et la relation entre le mesurande et les grandeurs d'entr\u00e9e dont il d\u00e9pend. Les unit\u00e9s utilis\u00e9es doivent \u00eatre pr\u00e9cis\u00e9es.<\/li>\n\n\n\n<li class=\"has-medium-font-size\">la liste les  composantes de l'incertitude et leur \u00e9valuation.<\/li>\n\n\n\n<li class=\"has-medium-font-size\">l'estimation <math data-latex=\"y \"><semantics><mi>y<\/mi><annotation encoding=\"application\/x-tex\">y <\/annotation><\/semantics><\/math> du mesurande <math data-latex=\"Y\"><semantics><mi>Y<\/mi><annotation encoding=\"application\/x-tex\">Y<\/annotation><\/semantics><\/math> et son incertitude compos\u00e9e <math data-latex=\"u_c(y)\"><semantics><mrow><msub><mi>u<\/mi><mi>c<\/mi><\/msub><mo form=\"prefix\" stretchy=\"false\">(<\/mo><mi>y<\/mi><mo form=\"postfix\" stretchy=\"false\">)<\/mo><\/mrow><annotation encoding=\"application\/x-tex\">u_c(y)<\/annotation><\/semantics><\/math>. Lorsque cela est appropri\u00e9,  l'incertitude-type relative <math data-latex=\"\\left|\\frac{u_C(y)}{y}\\right|\"><semantics><mrow><mo fence=\"true\" form=\"prefix\">|<\/mo><mfrac><mrow><msub><mi>u<\/mi><mi>C<\/mi><\/msub><mo form=\"prefix\" stretchy=\"false\">(<\/mo><mi>y<\/mi><mo form=\"postfix\" stretchy=\"false\" lspace=\"0em\" rspace=\"0em\">)<\/mo><\/mrow><mi>y<\/mi><\/mfrac><mo fence=\"true\" form=\"postfix\">|<\/mo><\/mrow><annotation encoding=\"application\/x-tex\">\\left|\\frac{u_C(y)}{y}\\right|<\/annotation><\/semantics><\/math> doit \u00eatre fournie.<\/li>\n\n\n\n<li class=\"has-medium-font-size\">l'incertitude \u00e9largie en pr\u00e9cisant le facteur d'\u00e9largissement et le niveau de confiance.<\/li>\n<\/ol>\n\n\n<div style=\"border: 3px outset #fab300; border-radius: 26px; background-color: #fff6e2; \" class=\"ub-styled-box ub-bordered-box wp-block-ub-styled-box\" id=\"ub-styled-box-bb5091a8-7dca-4b63-8e2f-71feaa353a34\">\n<p class=\"has-small-font-size\" id=\"ub-styled-box-bordered-content-\">Exemple : une masse <math data-latex=\"m\"><semantics><mi>m<\/mi><annotation encoding=\"application\/x-tex\">m<\/annotation><\/semantics><\/math> a \u00e9t\u00e9 mesur\u00e9e en effectuant dix observations dans les conditions de r\u00e9p\u00e9tabilit\u00e9. Le r\u00e9sultat du mesurage doit \u00eatre not\u00e9 pas<\/p>\n\n\n\n<ul class=\"wp-block-list\">\n<li class=\"has-small-font-size\"><math data-latex=\"m = 100,02147(35)\\,\\mathrm{g}\"><semantics><mrow><mi>m<\/mi><mo>=<\/mo><mn>100,02147<\/mn><mo form=\"prefix\" stretchy=\"false\">(<\/mo><mn>35<\/mn><mo form=\"postfix\" stretchy=\"false\">)<\/mo><mspace width=\"0.1667em\"><\/mspace><mrow><mi mathvariant=\"normal\">g<\/mi><\/mrow><\/mrow><annotation encoding=\"application\/x-tex\">m = 100,02147(35)\\,\\mathrm{g}<\/annotation><\/semantics><\/math> o\u00f9 le nombre entre parenth\u00e8ses est la valeur num\u00e9rique de l'incertitude-type qui porte sur les deux dernier chiffres du r\u00e9sultat fourni.<\/li>\n\n\n\n<li class=\"has-small-font-size\"><math data-latex=\"m = (100,02157\\pm0,00079)\\,\\mathrm{g}\"><semantics><mrow><mi>m<\/mi><mo>=<\/mo><mo form=\"prefix\" stretchy=\"false\">(<\/mo><mn>100,02157<\/mn><mo>\u00b1<\/mo><mn>0,00079<\/mn><mo form=\"postfix\" stretchy=\"false\">)<\/mo><mspace width=\"0.1667em\"><\/mspace><mrow><mi mathvariant=\"normal\">g<\/mi><\/mrow><\/mrow><annotation encoding=\"application\/x-tex\">m = (100,02157\\pm0,00079)\\,\\mathrm{g}<\/annotation><\/semantics><\/math>  o\u00f9 le nombre qui suit le <math data-latex=\"\\pm\"><semantics><mo lspace=\"0em\" rspace=\"0em\">\u00b1<\/mo><annotation encoding=\"application\/x-tex\">\\pm<\/annotation><\/semantics><\/math> est la valeur num\u00e9rique de l'incertitude \u00e9largie d\u00e9termin\u00e9e \u00e0 partir de l'incertitude-type <math data-latex=\"u_C(m) = 0,35\\,\\mathrm{mg}\"><semantics><mrow><msub><mi>u<\/mi><mi>C<\/mi><\/msub><mo form=\"prefix\" stretchy=\"false\">(<\/mo><mi>m<\/mi><mo form=\"postfix\" stretchy=\"false\">)<\/mo><mo>=<\/mo><mn>0,35<\/mn><mspace width=\"0.1667em\"><\/mspace><mrow><mtext><\/mtext><mi>mg<\/mi><\/mrow><\/mrow><annotation encoding=\"application\/x-tex\">u_C(m) = 0,35\\,\\mathrm{mg}<\/annotation><\/semantics><\/math> et du facteur d'\u00e9largissement <math data-latex=\"k = 2,26\"><semantics><mrow><mi>k<\/mi><mo>=<\/mo><mn>2,26<\/mn><\/mrow><annotation encoding=\"application\/x-tex\">k = 2,26<\/annotation><\/semantics><\/math> sur la base de la loi de Student pour 9 degr\u00e9s de libert\u00e9, et d\u00e9finit un intervalle estim\u00e9 avoir un niveau de confiance de 95%.<\/li>\n\n\n\n<li class=\"has-small-font-size\">L'incertitude doit \u00eatre arrondie au chiffre sup\u00e9rieur plut\u00f4t qu\u2019au chiffre le plus proche et ne doit comporter que 2 chiffres significatifs.<\/li>\n<\/ul>\n\n\n<\/div>\n\n\n<h2 class=\"wp-block-heading\">Bibliographie<\/h2>\n\n\n\n<p class=\"has-medium-font-size\">\n<div id='zp-InTextBib-zotpress-d0177b31e4b6a8af1c6e8b00988f4690' class='zp-Zotpress zp-Zotpress-InTextBib wp-block-group zp-Post-1'>\r\n\t\t<span class=\"ZP_ITEM_KEY ZP_ATTR\">{20404111:GTVNKYYL};{20404111:4EFUZV59}<\/span>\r\n\t\t<span class=\"ZP_STYLE ZP_ATTR\">apa<\/span>\r\n\t\t<span class=\"ZP_SORTBY ZP_ATTR\">default<\/span>\r\n\t\t<span class=\"ZP_ORDER ZP_ATTR\"><\/span>\r\n\t\t<span class=\"ZP_TITLE ZP_ATTR\"><\/span>\r\n\t\t<span class=\"ZP_SHOWIMAGE ZP_ATTR\"><\/span>\r\n\t\t<span class=\"ZP_SHOWTAGS ZP_ATTR\"><\/span>\r\n\t\t<span class=\"ZP_DOWNLOADABLE ZP_ATTR\"><\/span>\r\n\t\t<span class=\"ZP_NOTES ZP_ATTR\"><\/span>\r\n\t\t<span class=\"ZP_ABSTRACT ZP_ATTR\"><\/span>\r\n\t\t<span class=\"ZP_CITEABLE ZP_ATTR\"><\/span>\r\n\t\t<span class=\"ZP_TARGET ZP_ATTR\"><\/span>\r\n\t\t<span class=\"ZP_URLWRAP ZP_ATTR\"><\/span>\r\n\t\t<span class=\"ZP_FORCENUM ZP_ATTR\">0<\/span>\r\n\t\t<span class=\"ZP_HIGHLIGHT ZP_ATTR\"><\/span>\r\n\t\t<span class=\"ZP_POSTID ZP_ATTR\">1<\/span><div class='zp-List loading'>\n<div class=\"zp-SEO-Content\">\t\t\t\t<span class=\"ZP_JSON 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Universit\u00e9 de Franche-Comt\u00e9.<\/div>\n<\/div>\n\t\t\t\t<\/div><!-- .zp-Entry .zpSearchResultsItem -->\t\t\t\t<div id=\"zp-ID-1-20404111-QBNXGKW6\" data-zp-author-date='Jardino-et-al.-1974' data-zp-date-author='1974-Jardino-et-al.' data-zp-date='1974' data-zp-year='1974' data-zp-itemtype='journalArticle' class=\"zp-Entry zpSearchResultsItem\">\n<div class=\"csl-bib-body\" style=\"line-height: 2; padding-left: 1em; text-indent:-1em;\">\n  <div class=\"csl-entry\">Jardino, M., Deloche, R., & Lambert, F. (1974). \u00c9volution des densit\u00e9s d\u2019atomes et mol\u00e9cules m\u00e9tastables dans une post-d\u00e9charge d\u2019h\u00e9lium entre 7 et 40 Torr. <i>Comptes Rendus de l\u2019Acad\u00e9mie des Sciences, Serie B<\/i>, <i>278<\/i>, 5.<\/div>\n<\/div>\n\t\t\t\t<\/div><!-- .zp-Entry .zpSearchResultsItem --><\/div><!-- .zp-zp-SEO-Content -->\n<\/div><!-- .zp-List --><\/div><!--.zp-Zotpress-->\n\n<\/p>\n\n\n\n<p><\/p>\n","protected":false},"excerpt":{"rendered":"<p>La m\u00e9trologie est la science de la mesure. Elle s&rsquo;int\u00e9resse aux grandeurs physiques, chimique ou biologiques, \u00e0 leurs unit\u00e9s et [&hellip;]<\/p>\n","protected":false},"author":2,"featured_media":37,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"site-sidebar-layout":"default","site-content-layout":"","ast-site-content-layout":"default","site-content-style":"default","site-sidebar-style":"default","ast-global-header-display":"","ast-banner-title-visibility":"","ast-main-header-display":"","ast-hfb-above-header-display":"","ast-hfb-below-header-display":"","ast-hfb-mobile-header-display":"","site-post-title":"","ast-breadcrumbs-content":"","ast-featured-img":"","footer-sml-layout":"","ast-disable-related-posts":"","theme-transparent-header-meta":"","adv-header-id-meta":"","stick-header-meta":"","header-above-stick-meta":"","header-main-stick-meta":"","header-below-stick-meta":"","astra-migrate-meta-layouts":"default","ast-page-background-enabled":"default","ast-page-background-meta":{"desktop":{"background-color":"var(--ast-global-color-5)","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-opacity":"","overlay-gradient":""},"tablet":{"background-color":"","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-opacity":"","overlay-gradient":""},"mobile":{"background-color":"","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-opacity":"","overlay-gradient":""}},"ast-content-background-meta":{"desktop":{"background-color":"var(--ast-global-color-4)","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-opacity":"","overlay-gradient":""},"tablet":{"background-color":"var(--ast-global-color-4)","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-opacity":"","overlay-gradient":""},"mobile":{"background-color":"var(--ast-global-color-4)","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-opacity":"","overlay-gradient":""}},"footnotes":""},"categories":[5],"tags":[],"class_list":["post-1","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-cours"],"featured_image_src":"https:\/\/sciences-physiques.org\/wp-content\/uploads\/2026\/01\/metrologie.png","author_info":{"display_name":"lemessagerceleste","author_link":"https:\/\/sciences-physiques.org\/index.php\/author\/lemessagerceleste\/"},"_links":{"self":[{"href":"https:\/\/sciences-physiques.org\/index.php\/wp-json\/wp\/v2\/posts\/1","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/sciences-physiques.org\/index.php\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/sciences-physiques.org\/index.php\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/sciences-physiques.org\/index.php\/wp-json\/wp\/v2\/users\/2"}],"replies":[{"embeddable":true,"href":"https:\/\/sciences-physiques.org\/index.php\/wp-json\/wp\/v2\/comments?post=1"}],"version-history":[{"count":89,"href":"https:\/\/sciences-physiques.org\/index.php\/wp-json\/wp\/v2\/posts\/1\/revisions"}],"predecessor-version":[{"id":174,"href":"https:\/\/sciences-physiques.org\/index.php\/wp-json\/wp\/v2\/posts\/1\/revisions\/174"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/sciences-physiques.org\/index.php\/wp-json\/wp\/v2\/media\/37"}],"wp:attachment":[{"href":"https:\/\/sciences-physiques.org\/index.php\/wp-json\/wp\/v2\/media?parent=1"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/sciences-physiques.org\/index.php\/wp-json\/wp\/v2\/categories?post=1"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/sciences-physiques.org\/index.php\/wp-json\/wp\/v2\/tags?post=1"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}