{
  "schema_version": 1,
  "kind": "ConceptView",
  "producer": "concept-view-1",
  "concept_id": "urn:uuid:4f329e32-44d0-4b99-86ea-6081a59ce73d",
  "labels": {
    "zh-CN": "动力学变量",
    "en": "dynamical variable"
  },
  "alternative_labels": [],
  "scope_note": "",
  "identity_status": "active",
  "identity_revision": "6c40a3293d48c9b5910d6c70f20d8e605f9e8ec4702d95dac11e34bb2d26bf29",
  "occurrences": [
    {
      "concept_id": "urn:uuid:4f329e32-44d0-4b99-86ea-6081a59ce73d",
      "book_id": "szekeres",
      "edition_id": "source-snapshot-bc3404156f6e",
      "lang": "zh-CN",
      "route": "zh/chapter-16/05-classical-mechanics",
      "anchor": "first-ec9af8e84a0c2190a4c3-zh",
      "chapter": "16",
      "section": "16.5",
      "offset": 28129,
      "range": [
        35909,
        36153
      ],
      "source_revision": "aac6045c8f792acfb5c9989193835b417610f4c945fe5f70074b9b0c3fb0e939",
      "source_category": "translation",
      "review_status": "unreviewed",
      "role": "occurrence",
      "role_basis": {
        "kind": "explicit-source-uuid-marker"
      },
      "label": "动力学变量(dynamical variable)",
      "context": {
        "range": [
          35886,
          36279
        ],
        "quote": "任何函数 $f : M \\to R$ 都称为 <u class=\"concept-term\" data-concept-identity=\"urn:uuid:4f329e32-44d0-4b99-86ea-6081a59ce73d\" data-concept-route=\"/concept-identities#concept-4f329e32-44d0-4b99-86ea-6081a59ce73d\" id=\"first-ec9af8e84a0c2190a4c3-zh\">动力学变量(dynamical variable)</u>。对于任意动力学变量 $f$，我们令 $X _ { f } = { \\overline { { \\mathrm { d } } } } { \\overline { { f } } }$ 为由 $f .$ 生成的哈密顿向量场。那么对于任意向量场 $Y$，",
        "quote_sha256": "303ad81b719e35f00888164df1635e7cb5fe1eef332335aadee487d9dac60ef3",
        "environment": null,
        "excerpt_omitted": false
      },
      "parallel_readings": [
        {
          "route": "en/chapter-16/05-classical-mechanics",
          "lang": "en",
          "source_category": "original_transcription",
          "basis": "registered-book-edition-section-language-context; not-concept-equivalence"
        }
      ],
      "id": "occ-b8865d60d5c306eb228a937b"
    },
    {
      "concept_id": "urn:uuid:4f329e32-44d0-4b99-86ea-6081a59ce73d",
      "book_id": "szekeres",
      "edition_id": "source-snapshot-bc3404156f6e",
      "lang": "en",
      "route": "en/chapter-16/05-classical-mechanics",
      "anchor": "first-ec9af8e84a0c2190a4c3-en",
      "chapter": "16",
      "section": "16.5",
      "offset": 37658,
      "range": [
        44967,
        45204
      ],
      "source_revision": "6ba31cc0cea910b2bb1780c9e846e4e265229202d450afd615e6b7053ad533bb",
      "source_category": "original_transcription",
      "review_status": "unreviewed",
      "role": "occurrence",
      "role_basis": {
        "kind": "explicit-source-uuid-marker"
      },
      "label": "dynamical variable",
      "context": {
        "range": [
          44926,
          45404
        ],
        "quote": "Any function $f : M \\to R$ is known as a <u class=\"concept-term\" data-concept-identity=\"urn:uuid:4f329e32-44d0-4b99-86ea-6081a59ce73d\" data-concept-route=\"/concept-identities#concept-4f329e32-44d0-4b99-86ea-6081a59ce73d\" id=\"first-ec9af8e84a0c2190a4c3-en\">dynamical variable</u>. For any dynamical variable $f$ we set $X _ { f } = { \\overline { { \\mathrm { d } } } } { \\overline { { f } } }$ to be the Hamiltonian vector field generated by $f .$ . Then for any vector field $Y$,",
        "quote_sha256": "f097ac7e97c8a87dc75ee63d65efe4d9dca2af5d0871de1f039a41a99acb676b",
        "environment": null,
        "excerpt_omitted": false
      },
      "parallel_readings": [
        {
          "route": "zh/chapter-16/05-classical-mechanics",
          "lang": "zh-CN",
          "source_category": "translation",
          "basis": "registered-book-edition-section-language-context; not-concept-equivalence"
        }
      ],
      "id": "occ-8d4ce82114a539f115cb668d"
    }
  ],
  "registered_positions": [
    {
      "route": "en/chapter-16/05-classical-mechanics",
      "lang": "en",
      "section": "16.5",
      "signal": "term-mark",
      "label": "dynamical variable",
      "english": "dynamical variable",
      "offset": 35557
    },
    {
      "route": "zh/chapter-16/05-classical-mechanics",
      "lang": "zh-CN",
      "section": "16.5",
      "signal": "term-mark",
      "label": "动力学变量",
      "english": "dynamical variable",
      "offset": 26028
    }
  ],
  "statements": [],
  "resolved_references": [],
  "reading_order": [
    "occ-b8865d60d5c306eb228a937b",
    "occ-8d4ce82114a539f115cb668d"
  ],
  "recorded_dependencies": [],
  "reading_paths": [],
  "coverage": {
    "registered_positions": 2,
    "located_occurrences": 2,
    "whole_book_search_complete": false,
    "registered_positions_truncated": false,
    "independent_human_review_implied": false
  },
  "unresolved": [],
  "base_revision": "c14d5e2b3e9deabbdb7a1c8613eec3c6ac4f6f70cf8852580d583758c00f0afa",
  "optional_enrichments": []
}