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null,\n    'Su pianeti diversi'\n);\n\nvar _ref28 = Object(preact_min[\"h\"])(\n    'p',\n    null,\n    'Per pianeti diversi dalla Terra vale la stessa regola:'\n);\n\nvar _ref29 = Object(preact_min[\"h\"])(\n    'p',\n    null,\n    'L\\'unica differenza \\xE8 che cambia la ',\n    Object(preact_min[\"h\"])(\n        'i',\n        null,\n        'costante di gravit\\xE0'\n    ),\n    ':'\n);\n\nvar _ref30 = Object(preact_min[\"h\"])(\n    'h2',\n    null,\n    'Forze di contatto'\n);\n\nvar _ref31 = Object(preact_min[\"h\"])(\n    panel_Panel,\n    null,\n    Object(preact_min[\"h\"])(\n        'h3',\n        null,\n        'Normale'\n    ),\n    Object(preact_min[\"h\"])(\n        'p',\n        null,\n        'Si oppone alle forze applicate alla superficie di contatto.'\n    ),\n    Object(preact_min[\"h\"])(\n        'p',\n        null,\n        'Un libro appoggiato su un tavolo ha la ',\n        Object(preact_min[\"h\"])(\n            'b',\n            null,\n            'forza di gravit\\xE0'\n        ),\n        ' che lo attira verso il terreno e la ',\n        Object(preact_min[\"h\"])(\n            'b',\n            null,\n            'forza normale'\n        ),\n        ' che lo trattiene dal cadere.'\n    )\n);\n\nvar _ref32 = Object(preact_min[\"h\"])(\n    'h3',\n    null,\n    'Attrito statico'\n);\n\nvar _ref33 = Object(preact_min[\"h\"])(\n    'p',\n    null,\n    'Impedisce a un corpo di muoversi se non viene spinto da una forza che supera una certa soglia:'\n);\n\nvar _ref34 = Object(preact_min[\"h\"])(\n    'h3',\n    null,\n    'Attrito dinamico'\n);\n\nvar _ref35 = Object(preact_min[\"h\"])(\n    'p',\n    null,\n    'Rallenta i corpi che si stanno muovendo finch\\xE8 essi non si fermano:'\n);\n\nvar _ref36 = Object(preact_min[\"h\"])(\n    panel_Panel,\n    null,\n    Object(preact_min[\"h\"])(\n        'h3',\n        null,\n        'Tensione'\n    ),\n    Object(preact_min[\"h\"])(\n        'p',\n        null,\n        'E\\' forza trasmessa tra due estremi di una fune.'\n    ),\n    Object(preact_min[\"h\"])(\n        'p',\n        null,\n        'Pu\\xF2 essere redirezionata per mezzo di carrucole.'\n    )\n);\n\nvar _ref37 = Object(preact_min[\"h\"])(\n    'h3',\n    null,\n    'Elastica'\n);\n\nvar _ref38 = Object(preact_min[\"h\"])(\n    'p',\n    null,\n    'Una molla cerca sempre di tornare alla sua posizione indeformata con forza:'\n);\n\nvar _ref39 = Object(preact_min[\"h\"])(\n    'p',\n    null,\n    '(E\\' negativa perch\\xE8 la forza \\xE8 opposta a quella applicata per deformarla.)'\n);\n\nvar _ref40 = Object(preact_min[\"h\"])(\n    'h2',\n    null,\n    'Cinematica'\n);\n\nvar _ref41 = Object(preact_min[\"h\"])(\n    'h3',\n    null,\n    'Spostamento'\n);\n\nvar _ref42 = Object(preact_min[\"h\"])(\n    'p',\n    null,\n    '\\xC8 un vettore che indica la posizione di un corpo rispetto a un\\'origine.'\n);\n\nvar _ref43 = Object(preact_min[\"h\"])(\n    'h3',\n    null,\n    'Velocit\\xE0'\n);\n\nvar _ref44 = Object(preact_min[\"h\"])(\n    'p',\n    null,\n    '\\xC8 un vettore che misura la variazione di posizione nel tempo.'\n);\n\nvar _ref45 = Object(preact_min[\"h\"])(\n    'p',\n    null,\n    'Se si considera un intervallo di tempo infinitesimale si dice ',\n    Object(preact_min[\"h\"])(\n        'i',\n        null,\n        'velocit\\xE0 istantanea'\n    ),\n    ':'\n);\n\nvar _ref46 = Object(preact_min[\"h\"])(\n    'h3',\n    null,\n    'Accelerazione'\n);\n\nvar _ref47 = Object(preact_min[\"h\"])(\n    'p',\n    null,\n    '\\xC8 un vettore che misura la variazione di velocit\\xE0 nel tempo.'\n);\n\nvar _ref48 = Object(preact_min[\"h\"])(\n    'p',\n    null,\n    'Se si considera un intervallo di tempo infinitesimale si dice ',\n    Object(preact_min[\"h\"])(\n        'i',\n        null,\n        'accelerazione istantanea'\n    ),\n    ':'\n);\n\nvar _ref49 = Object(preact_min[\"h\"])(\n    'h3',\n    null,\n    'Quantit\\xE0 di moto ',\n    Object(preact_min[\"h\"])(\n        'small',\n        null,\n        '(momento lineare)'\n    )\n);\n\nvar _ref50 = Object(preact_min[\"h\"])(\n    'p',\n    null,\n    'La quantit\\xE0 di moto \\xE8 una propriet\\xE0 vettoriale dei corpi:'\n);\n\nvar _ref51 = Object(preact_min[\"h\"])(\n    'p',\n    null,\n    'Se la forza risultante \\xE8 nulla, la quantit\\xE0 di moto non cambia.'\n);\n\nvar _ref52 = Object(preact_min[\"h\"])(\n    'h2',\n    null,\n    'Moto rettilineo uniforme'\n);\n\nvar _ref53 = Object(preact_min[\"h\"])(\n    'h3',\n    null,\n    'Spostamento'\n);\n\nvar _ref54 = Object(preact_min[\"h\"])(\n    'p',\n    null,\n    'La ',\n    Object(preact_min[\"h\"])(\n        'i',\n        null,\n        'legge oraria'\n    ),\n    ' \\xE8:'\n);\n\nvar _ref55 = Object(preact_min[\"h\"])(\n    'h3',\n    null,\n    'Velocit\\xE0'\n);\n\nvar _ref56 = Object(preact_min[\"h\"])(\n    'p',\n    null,\n    '\\xC8 costante:'\n);\n\nvar _ref57 = Object(preact_min[\"h\"])(\n    'h3',\n    null,\n    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Object(preact_min[\"h\"])(\n    'h3',\n    null,\n    'Velocit\\xE0'\n);\n\nvar _ref64 = Object(preact_min[\"h\"])(\n    'p',\n    null,\n    '\\xC8 una retta:'\n);\n\nvar _ref65 = Object(preact_min[\"h\"])(\n    'h3',\n    null,\n    'Accelerazione'\n);\n\nvar _ref66 = Object(preact_min[\"h\"])(\n    'p',\n    null,\n    '\\xC8 costante:'\n);\n\nvar _ref67 = Object(preact_min[\"h\"])(\n    panel_Panel,\n    null,\n    Object(preact_min[\"h\"])(\n        'h3',\n        null,\n        'Forze'\n    ),\n    Object(preact_min[\"h\"])(\n        'p',\n        null,\n        'Si applica la prima legge di Newton:'\n    ),\n    Object(preact_min[\"h\"])(\n        'p',\n        null,\n        Object(preact_min[\"h\"])(\n            latex_Latex,\n            null,\n            'f(t) = m a'\n        )\n    )\n);\n\nvar _ref68 = Object(preact_min[\"h\"])(\n    'h2',\n    null,\n    'Moto armonico semplice'\n);\n\nvar _ref69 = Object(preact_min[\"h\"])(\n    panel_Panel,\n    null,\n    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)\n);\n\nvar _ref80 = Object(preact_min[\"h\"])(\n    'h3',\n    null,\n    'Moto circolare uniforme'\n);\n\nvar _ref81 = Object(preact_min[\"h\"])(\n    'h2',\n    null,\n    'Moto circolare uniforme'\n);\n\nvar _ref82 = Object(preact_min[\"h\"])(\n    'h3',\n    null,\n    'Velocit\\xE0 angolare'\n);\n\nvar _ref83 = Object(preact_min[\"h\"])(\n    'p',\n    null,\n    'Quanto cambia la fase nel tempo.'\n);\n\nvar _ref84 = Object(preact_min[\"h\"])(\n    'h3',\n    null,\n    'Fase'\n);\n\nvar _ref85 = Object(preact_min[\"h\"])(\n    'p',\n    null,\n    'E\\' l\\'angolo percorso dal corpo rispetto alla posizione iniziale.'\n);\n\nvar _ref86 = Object(preact_min[\"h\"])(\n    'h3',\n    null,\n    'Velocit\\xE0'\n);\n\nvar _ref87 = Object(preact_min[\"h\"])(\n    'p',\n    null,\n    'Si applicano le formule per la circonferenza:'\n);\n\nvar _ref88 = Object(preact_min[\"h\"])(\n    'h3',\n    null,\n    'Accelerazione'\n);\n\nvar _ref89 = Object(preact_min[\"h\"])(\n    'p',\n    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'Forze conservative'\n);\n\nvar _ref105 = Object(preact_min[\"h\"])(\n    'p',\n    null,\n    'Sono conservative le forze per le quali il lavoro compiuto non dipende dal percorso seguito per andare dalla partenza all\\'arrivo.'\n);\n\nvar _ref106 = Object(preact_min[\"h\"])(\n    'p',\n    null,\n    'Ad esempio, \\xE8 conservativa la ',\n    Object(preact_min[\"h\"])(\n        'b',\n        null,\n        'forza di gravit\\xE0'\n    ),\n    ', ma non \\xE8 conservativa la ',\n    Object(preact_min[\"h\"])(\n        'del',\n        null,\n        'forza di attrito'\n    ),\n    '.'\n);\n\nvar _ref107 = Object(preact_min[\"h\"])(\n    'p',\n    null,\n    'Se in un sistema ci sono solo forze conservative, allora l\\'energia meccanica totale si conserva:'\n);\n\nvar _ref108 = Object(preact_min[\"h\"])(\n    'h3',\n    null,\n    'Potenza'\n);\n\nvar _ref109 = Object(preact_min[\"h\"])(\n    'p',\n    null,\n    '\\xC8 la velocit\\xE0 di trasferimento di energia:'\n);\n\nvar 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          latex_Latex,\n                            null,\n                            r(_templateObject10)\n                        )\n                    )\n                ),\n                Object(preact_min[\"h\"])(\n                    panel_Panel,\n                    null,\n                    _ref18,\n                    _ref19,\n                    Object(preact_min[\"h\"])(\n                        'p',\n                        null,\n                        Object(preact_min[\"h\"])(\n                            latex_Latex,\n                            null,\n                            r(_templateObject11)\n                        )\n                    )\n                )\n            ),\n            _ref20,\n            Object(preact_min[\"h\"])(\n                split_Split,\n                null,\n                Object(preact_min[\"h\"])(\n                    panel_Panel,\n                    null,\n                    _ref21,\n                    _ref22,\n         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class={style.split}>{children}</div>;\n\t}\n}\n\n\n// WEBPACK FOOTER //\n// ./components/split.js","import style from './fisica.css';\nimport { Component } from 'preact';\nimport Latex from '../components/latex';\nimport Panel from '../components/panel';\nimport Split from '../components/split';\n\nconst r = String.raw;\n\nexport default class Fisica extends Component {\n\trender() {\n        return (\n            <div>\n                <h1>Fisica</h1>\n                <h2>Vettori</h2>\n                <Split>\n                    <Panel>\n                        <h3>\n                            Componenti cartesiane\n                        </h3>\n                        <p>\n                            Usa le regole base della trigonometria:\n                        </p>\n                        <p>\n                            <Latex>{r`\\vec{v} = \\vec{v}_x + \\vec{v}_y`}</Latex>\n                        </p>\n                        <p>\n                            <Latex>{r`\\left | \\vec{v}_x \\right | = \\left | \\vec{v} \\right | \\sin \\alpha`}</Latex>\n                        </p>\n                        <p>\n                            <Latex>{r`\\left | \\vec{v}_y \\right | = \\left | \\vec{v} \\right | \\cos \\alpha`}</Latex>\n                        </p>\n                    </Panel>\n                    <Panel>\n                        <h3>\n                            Somma\n                        </h3>\n                        <p>\n                            Scomponi in componenti, poi sommali:\n                        </p>\n                        <p>\n                            <Latex>{r`\\vec{v} + \\vec{w} = (\\vec{v}_x + \\vec{w}_x) + (\\vec{v}_y + \\vec{w}_y)`}</Latex>\n                        </p>\n                        <p>\n                            Produce il vettore risultante dall'applicazione della regola del parallelogramma.\n                        </p>\n                    </Panel>\n                    <Panel>\n                        <h3>\n                            Differenza\n                        </h3>\n                        <p>\n                            Alla fine è sempre una somma:\n                        </p>\n                        <p>\n                            <Latex>{r`\\vec{v} - \\vec{w} = (\\vec{v}_x - \\vec{w}_x) + (\\vec{v}_y - \\vec{w}_y)`}</Latex>\n                        </p>\n                        <p>\n                            Produce il vettore che parte da <Latex>w</Latex> e arriva a <Latex>v</Latex>.\n                        </p>\n                    </Panel>\n                    <Panel>\n                        <h3>\n                            Prodotto scalare\n                        </h3>\n                        <p>\n                            Si chiama scalare perchè il risultato è uno scalare, non un vettore.\n                        </p>\n                        <p>\n                            <Latex>{r`\\vec{v} \\cdot \\vec{w} = \\left | \\vec{v} \\right | \\left | \\vec{w} \\right | \\cos \\alpha`}</Latex>\n                        </p>\n                        <p>\n                            Produce il modulo della proiezione di <Latex>{r`\\vec{a}`}</Latex> su <Latex>{r`\\vec{b}`}</Latex>.\n                        </p>\n                    </Panel>\n                </Split>\n                <h2>\n                    Leggi di Newton\n                </h2>\n                <Split>\n                    <Panel>\n                        <h3>\n                            1ᵃ: Inerzia\n                        </h3>\n                        <p>\n                            Se un corpo puntiforme ha forza risultante nulla, allora la sua velocità non cambia.\n                        </p>\n                        <p>\n                            <Latex>{r`\\Sigma \\vec{F} = 0 \\Longleftrightarrow \\Delta v = 0`}</Latex>\n                        </p>\n                    </Panel>\n                    <Panel>\n                        <h3>\n                            2ᵃ: Proporzionalità\n                        </h3>\n                        <p>\n                            La forza risultante di un corpo è direttamente proporzionale alla sua accelerazione, e la costante di proporzionalità è la <i>massa</i>.\n                        </p>\n                        <p>\n                            <Latex>{r`\\Sigma \\vec{F} = m \\vec{a}`}</Latex>\n                        </p>\n                    </Panel>\n                    <Panel>\n                        <h3>\n                            3ᵃ: Azione e reazione\n                        </h3>\n                        <p>\n                            Due corpi esercitano forze uguali e opposte uno sull'altro. \n                        </p>\n                        <p>\n                            <Latex>{r`\\vec{F}_{21} = -\\vec{F}_{12}`}</Latex>\n                        </p>\n                    </Panel>\n                </Split>\n                <h2>\n                    Forza di gravità\n                </h2>\n                <Split>\n                    <Panel>\n                        <h3>\n                            Tra due corpi\n                        </h3>\n                        <p>\n                            Due corpi puntiformi si attirano uno verso l'altro con forza:\n                        </p>\n                        <p>\n                            <Latex>{r`\\left | \\vec{F} \\right | = G \\frac{m_1 m_2}{s^2}`}</Latex>\n                        </p>\n                        <p>\n                            <Latex>G</Latex> è la <i>costante di gravitazione universale</i> e vale:\n                        </p>\n                        <p>\n                            <Latex>{r`G = 6.67 \\cdot 10^{-11} \\frac{N m^2}{{kg}^2}`}</Latex>\n                        </p>\n                    </Panel>\n                    <Panel>\n                        <h3>\n                            Verso la Terra\n                        </h3>\n                        <p>\n                            Se nel sistema di riferimento consideriamo la Terra ferma, allora un corpo è attratto verso la Terra con forza <i>peso</i> uguale a:\n                        </p>\n                        <p>\n                            <Latex>{r`\\left | \\vec{F} \\right | = g m`}</Latex>\n                        </p>\n                        <p>\n                            <Latex>g</Latex> è la <i>costante di gravità</i> della Terra, e vale:\n                        </p>\n                        <p>\n                            <Latex>{r`g = 9.81 \\frac{m}{s^2}`}</Latex>\n                        </p>\n                    </Panel>\n                    <Panel>\n                        <h3>\n                            Su pianeti diversi\n                        </h3>\n                        <p>\n                            Per pianeti diversi dalla Terra vale la stessa regola:\n                        </p>\n                        <p>\n                            <Latex>{r`\\left | \\vec{F} \\right | = g m`}</Latex>\n                        </p>\n                        <p>\n                            L'unica differenza è che cambia la <i>costante di gravità</i>:\n                        </p>\n                        <p>\n                            <Latex>{r`g_{luna} = 1.62 \\frac{m}{s^2}`}</Latex>\n                        </p>\n                        <p>\n                            <Latex>{r`g_{marte} = 3.71 \\frac{m}{s^2}`}</Latex>\n                        </p>\n                    </Panel>\n                </Split>\n                <h2>\n                    Forze di contatto\n                </h2>\n                <Split>\n                    <Panel>\n                        <h3>\n                            Normale\n                        </h3>\n                        <p>\n                            Si oppone alle forze applicate alla superficie di contatto.\n                        </p>\n                        <p>\n                            Un libro appoggiato su un tavolo ha la <b>forza di gravità</b> che lo attira verso il terreno e la <b>forza normale</b> che lo trattiene dal cadere. \n                        </p>\n                    </Panel>\n                    <Panel>\n                        <h3>\n                            Attrito statico\n                        </h3>\n                        <p>\n                            Impedisce a un corpo di muoversi se non viene spinto da una forza che supera una certa soglia:\n                        </p>\n                        <p>\n                            <Latex>{r`\\left | \\vec{F} \\right | \\leq \\mu_{s} \\left | \\vec{F}_{normale} \\right |`}</Latex>\n                        </p>\n                    </Panel>\n                    <Panel>\n                        <h3>\n                            Attrito dinamico\n                        </h3>\n                        <p>\n                            Rallenta i corpi che si stanno muovendo finchè essi non si fermano:\n                        </p>\n                        <p>\n                            <Latex>{r`\\left | \\vec{F} \\right | \\leq \\mu_{d} \\left | \\vec{F}_{normale} \\right |`}</Latex>\n                        </p>\n                    </Panel>\n                    <Panel>\n                        <h3>\n                            Tensione\n                        </h3>\n                        <p>\n                            E' forza trasmessa tra due estremi di una fune.\n                        </p>\n                        <p>\n                            Può essere redirezionata per mezzo di carrucole.\n                        </p>\n                    </Panel>\n                    <Panel>\n                        <h3>\n                            Elastica\n                        </h3>\n                        <p>\n                            Una molla cerca sempre di tornare alla sua posizione indeformata con forza:\n                        </p>\n                        <p>\n                            <Latex>{r`F = -k x`}</Latex>\n                        </p>\n                        <p>\n                            (E' negativa perchè la forza è opposta a quella applicata per deformarla.)\n                        </p>\n                    </Panel>\n                </Split>\n                <h2>\n                    Cinematica\n                </h2>\n                <Split>\n                    <Panel>\n                        <h3>\n                            Spostamento\n                        </h3>\n                        <p>\n                            È un vettore che indica la posizione di un corpo rispetto a un'origine.\n                        </p>\n                        <p>\n                            <Latex>{r`\\Delta \\vec{s} = \\vec{s}(fine) - \\vec{s}(inizio)`}</Latex>\n                        </p>\n                    </Panel>\n                    <Panel>\n                        <h3>\n                            Velocità\n                        </h3>\n                        <p>\n                            È un vettore che misura la variazione di posizione nel tempo.\n                        </p>\n                        <p>\n                            <Latex>{r`\\vec{v} = \\frac{\\Delta \\vec{s}}{\\Delta t}`}</Latex>\n                        </p>\n                        <p>\n                            Se si considera un intervallo di tempo infinitesimale si dice <i>velocità istantanea</i>:\n                        </p>\n                        <p>\n                            <Latex>{r`\\vec{v} = \\lim_{\\Delta t \\to 0} \\frac{\\Delta \\vec{s}}{\\Delta t} = \\frac{d \\vec{s}}{dt}`}</Latex>\n                        </p>\n                    </Panel>\n                    <Panel>\n                        <h3>\n                            Accelerazione\n                        </h3>\n                        <p>\n                            È un vettore che misura la variazione di velocità nel tempo.\n                        </p>\n                        <p>\n                            <Latex>{r`\\vec{a} = \\frac{\\Delta \\vec{v}}{\\Delta t}`}</Latex>\n                        </p>\n                        <p>\n                            Se si considera un intervallo di tempo infinitesimale si dice <i>accelerazione istantanea</i>:\n                        </p>\n                        <p>\n                            <Latex>{r`\\vec{a} = \\lim_{\\Delta v \\to 0} \\frac{\\Delta \\vec{v}}{\\Delta t} = \\frac{d \\vec{v}}{d t} = \\frac{d^2 \\vec{s}}{d t^2}`}</Latex>\n                        </p>\n                    </Panel>\n                    <Panel>\n                        <h3>\n                            Quantità di moto <small>(momento lineare)</small>\n                        </h3>\n                        <p>\n                            La quantità di moto è una proprietà vettoriale dei corpi:\n                        </p>\n                        <p>\n                            <Latex>{r`\\vec{p} = m \\vec{v}`}</Latex>\n                        </p>\n                        <p>\n                            Se la forza risultante è nulla, la quantità di moto non cambia.\n                        </p>\n                        <p>\n                            <Latex>{r`\\Sigma \\vec{F} = 0 \\Longleftrightarrow \\Delta \\vec{p} = 0`}</Latex>\n                        </p>\n                    </Panel>\n                </Split>\n                <h2>\n                    Moto rettilineo uniforme\n                </h2>\n                <Split>\n                    <Panel>\n                        <h3>\n                            Spostamento\n                        </h3>\n                        <p>\n                            La <i>legge oraria</i> è:\n                        </p>\n                        <p>\n                            <Latex>{r`s(t) = v \\cdot \\Delta t + s(0)`}</Latex>\n                        </p>\n                    </Panel>\n                    <Panel>\n                        <h3>\n                            Velocità\n                        </h3>\n                        <p>\n                            È costante:\n                        </p>\n                        <p>\n                            <Latex>{r`v(t) = k`}</Latex>\n                        </p>\n                    </Panel>\n                    <Panel>\n                        <h3>\n                            Accelerazione\n                        </h3>\n                        <p>\n                            La velocità non varia:\n                        </p>\n                        <p>\n                            <Latex>{r`a(t) = 0`}</Latex>\n                        </p>\n                    </Panel>\n                    <Panel>\n                        <h3>\n                            Forze\n                        </h3>\n                        <p>\n                            Si applica la prima legge di Newton:\n                        </p>\n                        <p>\n                            <Latex>f(t) = 0</Latex>\n                        </p>\n                    </Panel>\n                </Split>\n                <h2>\n                    Moto rettilineo uniformemente accelerato\n                </h2>\n                <Split>\n                    <Panel>\n                        <h3>\n                            Spostamento\n                        </h3>\n                        <p>\n                            La <i>legge oraria</i> è:\n                        </p>\n                        <p>\n                            <Latex>{r`s(t) = \\frac{1}{2} a \\cdot (\\Delta t)^2 + v(0) \\cdot (\\Delta t) + s(0)`}</Latex>\n                        </p>\n                    </Panel>\n                    <Panel>\n                        <h3>\n                            Velocità\n                        </h3>\n                        <p>\n                            È una retta:\n                        </p>\n                        <p>\n                            <Latex>{r`v(t) = a \\Delta t + v(0)`}</Latex>\n                        </p>\n                    </Panel>\n                    <Panel>\n                        <h3>\n                            Accelerazione\n                        </h3>\n                        <p>\n                            È costante:\n                        </p>\n                        <p>\n                            <Latex>{r`a(t) = k`}</Latex>\n                        </p>\n                    </Panel>\n                    <Panel>\n                        <h3>\n                            Forze\n                        </h3>\n                        <p>\n                            Si applica la prima legge di Newton:\n                        </p>\n                        <p>\n                            <Latex>f(t) = m a</Latex>\n                        </p>\n                    </Panel>\n                </Split>\n                <h2>\n                    Moto armonico semplice\n                </h2>\n                <Split>\n                    <Panel>\n                        <h3>\n                            Ampiezza\n                        </h3>\n                        <p>\n                            E' la distanza dal centro massima che raggiunge il corpo.\n                        </p>\n                        <p>\n                            (L'ampiezza di una sinusoide.)\n                        </p>\n                    </Panel>\n                    <Panel>\n                        <h3>\n                            Velocità angolare\n                        </h3>\n                        <p>\n                            Indica quanto in fretta cambia la posizione del corpo. \n                        </p>\n                        <p>\n                            Dipende dal periodo:\n                        </p>\n                        <p>\n                            <Latex>{r`\\omega = \\frac{2 \\pi}{T}`}</Latex>\n                        </p>\n                    </Panel>\n                    <Panel>\n                        <h3>\n                            Spostamento\n                        </h3>\n                        <p>\n                            E' una sinusoide:\n                        </p>\n                        <p>\n                            <Latex>{r`s(t) = A \\sin (\\omega \\cdot t + \\phi)`}</Latex>\n                        </p>\n                    </Panel>\n                    <Panel>\n                        <h3>\n                            Velocità\n                        </h3>\n                        <p>\n                            E' la sinusoide dello spostamento, sfasata di <Latex>{r`\\frac{\\pi}{2}`}</Latex>:\n                        </p>\n                        <p>\n                            <Latex>{r`s(t) = A \\sin (\\omega \\cdot t + \\phi + \\frac{\\pi}{2})`}</Latex>\n                        </p>\n                    </Panel>\n                    <Panel>\n                        <h3>\n                            Accelerazione\n                        </h3>\n                        <p>\n                            E' la sinusoide della velocità, sfasata di <Latex>{r`\\frac{\\pi}{2}`}</Latex>:\n                        </p>\n                        <p>\n                            <Latex>{r`s(t) = A \\sin (\\omega \\cdot t + \\phi + \\pi)`}</Latex>\n                        </p>\n                    </Panel>\n                    <Panel>\n                        <h3>\n                            Forze\n                        </h3>\n                        <p>\n                            Si applica la prima legge di Newton:\n                        </p>\n                        <p>\n                            <Latex>f(t) = m a</Latex>\n                        </p>\n                    </Panel>\n                </Split>\n                <h2>\n                    Moti composti\n                </h2>\n                <Split>\n                    <Panel>\n                        <h3>\n                            Moto parabolico\n                        </h3>\n                        <p>\n                            Il moto parabolico è dato sommando un moto rettilineo uniforme sull'asse orizzontale e un moto rettilineo uniformemente accelerato sull'asse verticale.\n                        </p>\n                    </Panel>\n                    <Panel>\n                        <h3>\n                            Moto circolare uniforme\n                        </h3>\n                        <p>\n                            Il moto parabolico è dato sommando due moti armonici semplici: uno sull'asse X, e l'altro, sfasato di <Latex>{r`\\frac{\\pi}{2}`}</Latex>, sull'asse Y.\n                        </p>\n                    </Panel>\n                </Split>\n                <h2>\n                    Moto circolare uniforme\n                </h2>\n                <Split>\n                    <Panel>\n                        <h3>\n                            Velocità angolare\n                        </h3>\n                        <p>\n                            Quanto cambia la fase nel tempo.\n                        </p>\n                        <p>\n                            <Latex>{r`\\omega = \\frac{2 \\pi}{T}`}</Latex>\n                        </p>\n                    </Panel>\n                    <Panel>\n                        <h3>\n                            Fase\n                        </h3>\n                        <p>\n                            E' l'angolo percorso dal corpo rispetto alla posizione iniziale.\n                        </p>\n                        <p>\n                            Si indica con <Latex>{r`\\phi`}</Latex>, e generalmente si usa in radianti.\n                        </p>\n                    </Panel>\n                    <Panel>\n                        <h3>\n                            Velocità\n                        </h3>\n                        <p>\n                            Si applicano le formule per la circonferenza:\n                        </p>\n                        <p>\n                            <Latex>{r`v = \\frac{\\Delta s}{t} = \\frac{2 \\pi \\cdot r}{T}`}</Latex>\n                        </p>\n                    </Panel>\n                    <Panel>\n                        <h3>\n                            Accelerazione\n                        </h3>\n                        <p>\n                            Il corpo ha sempre un accelerazione verso il centro che gli impedisce di abbandonare il moto: \n                        </p>\n                        <p>\n                            <Latex>{r`a = \\frac{v^2}{r} = r \\cdot \\omega^2 = v \\cdot \\omega`}</Latex>\n                        </p>\n                    </Panel>\n                    <Panel>\n                        <h3>\n                            Forza centripeta\n                        </h3>\n                        <h3>\n                            È verso il centro e si calcola con:\n                        </h3>\n                        <p>\n                            <Latex>{r`F = m \\cdot a`}</Latex>\n                        </p>\n                    </Panel>\n                </Split>\n                <h2>\n                    Lavoro ed energia\n                </h2>\n                <Split>\n                    <Panel>\n                        <h3>\n                            Lavoro\n                        </h3>\n                        <p>\n                            E' compiuto da una forza che sposta un corpo.\n                        </p>\n                        <p>\n                            <Latex>{r`W = \\vec{F} \\cdot \\vec{s} = F \\cdot \\Delta s \\cdot cos(\\alpha )`}</Latex>\n                        </p>\n                        <p>\n                            (Se la forza non è parallela allo spostamento, il prodotto scalare ci fa considerare solo la componente parallela.)\n                        </p>\n                    </Panel>\n                    <Panel>\n                        <h3>\n                            Energia cinetica\n                        </h3>\n                        <p>\n                            Un corpo ha energia cinetica in ogni momento uguale a:\n                        </p>\n                        <p>\n                            <Latex>{r`E_c = \\frac{1}{2} m v^2`}</Latex>\n                        </p>\n                        <p>\n                            Se una forza effettua lavoro su un corpo, cambia la sua energia cinetica pari al lavoro effettuato:\n                        </p>\n                        <p>\n                            <Latex>{r`\\Delta E_c = W`}</Latex>\n                        </p>\n                    </Panel>\n                    <Panel>\n                        <h3>\n                            Energia potenziale gravitazionale\n                        </h3>\n                        <p>\n                            Un corpo ha energia potenziale in ogni momento pari a: \n                        </p>\n                        <p>\n                            <Latex>{r`E_{p_g} = m \\cdot g \\cdot h`}</Latex>\n                        </p>\n                        <p>\n                            (Con <Latex>h</Latex> uguale a un altezza scelta come punto di riferimento.)\n                        </p>\n                    </Panel>\n                    <Panel>\n                        <h3>\n                            Energia potenziale elastica\n                        </h3>\n                        <p>\n                            Una molla ha sempre energia potenziale elastica pari a:\n                        </p>\n                        <p>\n                            <Latex>{r`E_{p_e} = \\frac{1}{2} k x^2`}</Latex>\n                        </p>\n                    </Panel>\n                    <Panel>\n                        <h3>\n                            Forze conservative\n                        </h3>\n                        <p>\n                            Sono conservative le forze per le quali il lavoro compiuto non dipende dal percorso seguito per andare dalla partenza all'arrivo.\n                        </p>\n                        <p>\n                            Ad esempio, è conservativa la <b>forza di gravità</b>, ma non è conservativa la <del>forza di attrito</del>.\n                        </p>\n                        <p>\n                            Se in un sistema ci sono solo forze conservative, allora l'energia meccanica totale si conserva:\n                        </p>\n                        <p>\n                            <Latex>{r`E = E_k + E_p`}</Latex>\n                        </p>\n                    </Panel>\n                    <Panel>\n                        <h3>\n                            Potenza\n                        </h3>\n                        <p>\n                            È la velocità di trasferimento di energia:\n                        </p>\n                        <p>\n                            <Latex>{r`P = \\frac{\\Delta E}{\\Delta t}`}</Latex>\n                        </p>\n                    </Panel>\n                </Split>\n            </div>\n        )\n\t}\n}\n\n\n\n// WEBPACK FOOTER //\n// ./pages/fisica.js","import style from \"./copyright.css\";\r\nimport { Component } from 'preact';\r\n\r\nexport default class Copyright extends Component {\r\n\trender() {\r\n\t\treturn <div class={style.copyright}>© 2019 - Stefano Pigozzi - <a href=\"https://creativecommons.org/licenses/by-sa/4.0/\">CC BY-SA 4.0</a></div>;\r\n\t}\r\n}\n\n\n// WEBPACK FOOTER //\n// ./components/copyright.js","import './index.css';\nimport { Component } from 'preact';\nimport Fisica from './pages/fisica';\nimport Copyright from './components/copyright';\n\nexport default class App extends Component {\n\trender() {\n\t\treturn 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