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{"id":"330ceae2327436f1","type":"text","text":"牛顿-欧拉方程\n\n$$\n\\begin{split}\\bar{F} = & \\frac{{}^N d \\bar{p}}{dt} \\quad \\textrm{ where } \\bar{p} = m_B{}^N\\bar{v}^{B_o} \\\\\\bar{M} = & \\frac{{}^N d\\bar{H}}{dt} \\quad \\textrm{ where }\\bar{H} = \\breve{I}^{B/B_o} \\cdot {}^N\\bar{\\omega}^{B}\\end{split}|","x":-242,"y":-194,"width":542,"height":174},
{"id":"04fa17192ff0596c","x":-242,"y":160,"width":250,"height":60,"type":"text","text":"GAF Generalized Active Force 左端项"},
{"id":"c574d94bf9b233b4","x":50,"y":160,"width":250,"height":60,"type":"text","text":"GIF Generalized Inertia Force 右端项"}
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