Ajoute le pipeline PageSpec (validation, rendu, publication /p/{slug}),
les démos TipTap /demo, et le simulateur Carnot (modes frigo/PAC/moteur,
énergie kJ vs puissance W, unités K/°C/°F) avec correctifs d’équations KaTeX.
Co-authored-by: Cursor <cursoragent@cursor.com>
75 lines
2.8 KiB
TypeScript
75 lines
2.8 KiB
TypeScript
import type { AnimPlugin } from './types'
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/**
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* T–s diagram of the Carnot cycle — the canonical 2nd-law diagram:
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* isotherms are horizontal, adiabatics vertical, heat = area.
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* Same 5 phases as carnot-cycle-anim (piston) so both tell one story.
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*/
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export const tsDiagramAnim: AnimPlugin = {
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family: 'anim',
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id: 'ts-diagram',
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title: {
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fr: 'Le cycle de Carnot sur le diagramme T–s',
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en: 'The Carnot cycle on the T–s diagram',
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},
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summary: {
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fr: 'Diagramme température–entropie (T–s) du cycle de Carnot : isothermes horizontales, adiabatiques verticales, aires = chaleurs Q_h et Q_c, aire du cycle = travail W. 2ᵉ principe, entropie, rendement.',
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en: 'Temperature–entropy (T–s) diagram of the Carnot cycle: horizontal isotherms, vertical adiabatics, areas = heats Q_h and Q_c, cycle area = work W. Second law, entropy, efficiency.',
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},
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keywords: [
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'carnot',
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'entropie',
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'entropy',
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'diagramme t-s',
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't-s diagram',
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'thermodynamique',
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'thermodynamics',
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'deuxième principe',
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'second law',
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'rendement',
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'efficiency',
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'cycle',
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],
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disclaimer: {
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fr: 'Diagramme pédagogique — grandeurs illustratives.',
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en: 'Teaching diagram — illustrative values.',
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},
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beats: [
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{
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id: 'b1',
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speak: {
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fr: '**Détente isotherme** à $T_h$ : l’entropie croît, la chaleur $Q_h = T_h \\Delta s$ est l’aire sous l’isotherme.',
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en: '**Isothermal expansion** at $T_h$: entropy grows, heat $Q_h = T_h \\Delta s$ is the area under the isotherm.',
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},
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},
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{
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id: 'b2',
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speak: {
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fr: '**Détente adiabatique** : verticale — l’entropie est constante, la température chute de $T_h$ à $T_c$.',
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en: '**Adiabatic expansion**: vertical line — entropy is constant, temperature drops from $T_h$ to $T_c$.',
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},
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},
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{
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id: 'b3',
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speak: {
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fr: '**Compression isotherme** à $T_c$ : l’entropie décroît, la chaleur $Q_c = T_c \\Delta s$ est rejetée — l’aire bleue.',
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en: '**Isothermal compression** at $T_c$: entropy decreases, heat $Q_c = T_c \\Delta s$ is rejected — the blue area.',
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},
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},
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{
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id: 'b4',
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speak: {
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fr: '**Compression adiabatique** : remontée verticale de $T_c$ à $T_h$ — le rectangle se referme.',
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en: '**Adiabatic compression**: vertical climb from $T_c$ back to $T_h$ — the rectangle closes.',
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},
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},
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{
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id: 'b5',
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speak: {
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fr: 'Le **travail net** $W = (T_h - T_c)\\Delta s$ est l’aire du rectangle. Rapport des aires = rendement $\\eta = 1 - T_c/T_h$ — le maximum du 2ᵉ principe.',
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en: '**Net work** $W = (T_h - T_c)\\Delta s$ is the rectangle area. Area ratio = efficiency $\\eta = 1 - T_c/T_h$ — the second-law maximum.',
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},
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},
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],
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}
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