{
  "schema_version": 1,
  "kind": "ConceptView",
  "producer": "concept-view-1",
  "concept_id": "urn:uuid:f807579a-57c3-403d-aada-e8bec3d29d6e",
  "labels": {
    "zh-CN": "内能",
    "en": "internal energy"
  },
  "alternative_labels": [],
  "scope_note": "",
  "identity_status": "active",
  "identity_revision": "62c6efe449aec0979508bdc8ae0ce2bb402119143ae09fb7e09614ee8d0b86ad",
  "occurrences": [
    {
      "concept_id": "urn:uuid:f807579a-57c3-403d-aada-e8bec3d29d6e",
      "book_id": "szekeres",
      "edition_id": "source-snapshot-bc3404156f6e",
      "lang": "zh-CN",
      "route": "zh/chapter-16/04-thermodynamics",
      "anchor": "first-4d1ca1566ddc76193750-zh",
      "chapter": "16",
      "section": "16.4",
      "offset": 5061,
      "range": [
        9733,
        9971
      ],
      "source_revision": "4735d1e90df7c488c244eeb0006b5ef32a5616b3bde3dcf69a3414bd828dfb44",
      "source_category": "translation",
      "review_status": "unreviewed",
      "role": "occurrence",
      "role_basis": {
        "kind": "explicit-source-uuid-marker"
      },
      "label": "内能(internal energy)",
      "context": {
        "range": [
          9702,
          10344
        ],
        "quote": "热力学第一定律：能量。对每个热力学系统 $K$，存在一个称为 <u class=\"concept-term\" data-concept-identity=\"urn:uuid:f807579a-57c3-403d-aada-e8bec3d29d6e\" data-concept-route=\"/concept-identities#concept-f807579a-57c3-403d-aada-e8bec3d29d6e\" id=\"first-4d1ca1566ddc76193750-zh\">内能(internal energy)</u> 的函数 $U : K  \\mathbb { R }$，以及一个称为 <u class=\"concept-term\" data-concept-identity=\"urn:uuid:640cbf2a-bf3f-465e-a7f9-0d97c48f0e1f\" data-concept-route=\"/concept-identities#concept-640cbf2a-bf3f-465e-a7f9-0d97c48f0e1f\" id=\"first-bf7505bc87a493212805-zh\">功形式(work form)</u> 的 1-形式 $\\omega \\in \\Lambda _ { 1 } ( K )$，使得系统在任何可逆过程 $\\gamma : [ t _ { 1 } , t _ { 2 } ]  K$ 中所做的功由下式给出",
        "quote_sha256": "ae1b32942ab07b51ce3c738da8945dc0ef5692ed7afdd340ae994fce5614d775",
        "environment": null,
        "excerpt_omitted": false
      },
      "parallel_readings": [
        {
          "route": "en/chapter-16/04-thermodynamics",
          "lang": "en",
          "source_category": "original_transcription",
          "basis": "registered-book-edition-section-language-context; not-concept-equivalence"
        }
      ],
      "id": "occ-7cad2a8a30915f3760e73c4d"
    },
    {
      "concept_id": "urn:uuid:f807579a-57c3-403d-aada-e8bec3d29d6e",
      "book_id": "szekeres",
      "edition_id": "source-snapshot-bc3404156f6e",
      "lang": "en",
      "route": "en/chapter-16/04-thermodynamics",
      "anchor": "first-4d1ca1566ddc76193750-en",
      "chapter": "16",
      "section": "16.4",
      "offset": 9159,
      "range": [
        13361,
        13595
      ],
      "source_revision": "9240a01d2a6f17071128730ac11f0ece82cb8c622db6a3fe2bc4ab3df0015dcd",
      "source_category": "original_transcription",
      "review_status": "unreviewed",
      "role": "occurrence",
      "role_basis": {
        "kind": "explicit-source-uuid-marker"
      },
      "label": "internal energy",
      "context": {
        "range": [
          13237,
          13999
        ],
        "quote": "First law of thermodynamics: energy. For every thermodynamic system $K$ there is a function $U : K  \\mathbb { R }$ known as <u class=\"concept-term\" data-concept-identity=\"urn:uuid:f807579a-57c3-403d-aada-e8bec3d29d6e\" data-concept-route=\"/concept-identities#concept-f807579a-57c3-403d-aada-e8bec3d29d6e\" id=\"first-4d1ca1566ddc76193750-en\">internal energy</u> and a 1-form $\\omega \\in \\Lambda _ { 1 } ( K )$ known as the <u class=\"concept-term\" data-concept-identity=\"urn:uuid:5c46b2ed-4fca-4687-ba8b-563256d5f2f4\" data-concept-route=\"/concept-identities#concept-5c46b2ed-4fca-4687-ba8b-563256d5f2f4\" id=\"first-a89c8f244ce4c9186d29-en\">workform</u> such that the work done by the system in any reversibleprocess $\\gamma : [ t _ { 1 } , t _ { 2 } ]  K$ is given by",
        "quote_sha256": "e49411300cfff2533128275ac89e84982a8369677caeef423a97c95c2b55a305",
        "environment": null,
        "excerpt_omitted": false
      },
      "parallel_readings": [
        {
          "route": "zh/chapter-16/04-thermodynamics",
          "lang": "zh-CN",
          "source_category": "translation",
          "basis": "registered-book-edition-section-language-context; not-concept-equivalence"
        }
      ],
      "id": "occ-999c3187c32f1978fff31c09"
    }
  ],
  "registered_positions": [
    {
      "route": "en/chapter-16/04-thermodynamics",
      "lang": "en",
      "section": "16.4",
      "signal": "term-mark",
      "label": "internal energy",
      "english": "internal energy",
      "offset": 7822
    },
    {
      "route": "zh/chapter-16/04-thermodynamics",
      "lang": "zh-CN",
      "section": "16.4",
      "signal": "term-mark",
      "label": "内能",
      "english": "internal energy",
      "offset": 3724
    }
  ],
  "statements": [],
  "resolved_references": [],
  "reading_order": [
    "occ-7cad2a8a30915f3760e73c4d",
    "occ-999c3187c32f1978fff31c09"
  ],
  "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": "04e0a9259898b22a793125210956471eefa9a562dc2476d0cc700b551f4867ac",
  "optional_enrichments": []
}