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        "quote": "最后一步要么通过对$L = { \\textstyle { \\frac { 1 } { 2 } } } g _ { i j } \\dot { q } ^ { i } \\dot { q } ^ { j } - U ( q )$直接求导得到，要么通过对$T ( q ^ { j } , \\lambda \\dot { q } ^ { i } ) = \\lambda ^ { 2 } T ( q ^ { j } , \\dot { q } ^ { i } )$应用齐次函数的欧拉定理得到。动量1-形式的分量$p _ { i }$由<a href=\"#equation-16-30\" class=\"cross-reference\" id=\"xref-05-classical-mechanics-6\" data-reference=\"equation-16-30\">式(16.30)</a>给出，称为与广义坐标$q ^ { i }$共轭的<u class=\"concept-term\" data-concept-identity=\"urn:uuid:fa2ca729-0b3e-4cc8-8d07-b3c46fd2db3f\" data-concept-route=\"/concept-identities#concept-fa2ca729-0b3e-4cc8-8d07-b3c46fd2db3f\" id=\"first-6c194196dbcd9b6544b3-zh\">广义动量(generalized momentum)</u>",
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