vault backup: 2025-03-23 12:18:57
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],
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"metadata": {
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"metadata": {
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"kernelspec": {
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"display_name": "TagUIFocus5",
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"language": "python",
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"name": "python",
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"name": "python",
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"nbconvert_exporter": "python",
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"nbconvert_exporter": "python",
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"pygments_lexer": "ipython3",
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"pygments_lexer": "ipython3",
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"version": "3.12.4"
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"source": [
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"source": [
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"P1.vel(N).express(N)"
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"P1.vel(N).express(N)"
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]
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]
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},
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{
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"cell_type": "markdown",
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"metadata": {},
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"source": [
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"# 两杆连接"
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]
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}
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}
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],
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"name": "python",
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"pygments_lexer": "ipython3",
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"version": "3.12.4"
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"version": "3.11.8"
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}
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}
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},
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},
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"nbformat": 4,
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"nbformat": 4,
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1344
补课/多体动力学/17_Equations_of_Motions.excalidraw.md
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1344
补课/多体动力学/17_Equations_of_Motions.excalidraw.md
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补课/多体动力学/17_Equations_of_Motions.ipynb
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补课/多体动力学/17_Equations_of_Motions.ipynb
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{
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"cells": [],
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},
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"language_info": {
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"name": "python",
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"version": "3.11.8"
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}
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},
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"nbformat": 4,
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"nbformat_minor": 2
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}
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11
补课/多体动力学/框架.canvas
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补课/多体动力学/框架.canvas
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{
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"nodes":[
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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},
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{"id":"04fa17192ff0596c","x":-242,"y":160,"width":250,"height":60,"type":"text","text":"GAF Generalized Active Force 左端项"},
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{"id":"c574d94bf9b233b4","x":50,"y":160,"width":250,"height":60,"type":"text","text":"GIF Generalized Inertia Force 右端项"}
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],
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"edges":[
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{"id":"f33ddf845b3a3ff4","fromNode":"330ceae2327436f1","fromSide":"bottom","toNode":"04fa17192ff0596c","toSide":"top"},
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{"id":"79d807d4f3d87b22","fromNode":"330ceae2327436f1","fromSide":"bottom","toNode":"c574d94bf9b233b4","toSide":"top"}
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]
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}
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