{"id":213807,"date":"2024-10-20T00:04:56","date_gmt":"2024-10-20T00:04:56","guid":{"rendered":"https:\/\/www.electricity-magnetism.org\/?p=213807"},"modified":"2024-10-20T00:04:56","modified_gmt":"2024-10-20T00:04:56","slug":"%e7%b7%9a%e9%9b%bb%e8%8d%b7%e3%81%ab%e3%82%88%e3%82%8b%e9%9b%bb%e5%a0%b4%e3%81%ae%e6%b1%82%e3%82%81%e6%96%b9","status":"publish","type":"post","link":"https:\/\/www.electricity-magnetism.org\/ja\/%e7%b7%9a%e9%9b%bb%e8%8d%b7%e3%81%ab%e3%82%88%e3%82%8b%e9%9b%bb%e5%a0%b4%e3%81%ae%e6%b1%82%e3%82%81%e6%96%b9\/","title":{"rendered":"\u7dda\u96fb\u8377\u306b\u3088\u308b\u96fb\u5834\u306e\u6c42\u3081\u65b9"},"content":{"rendered":"

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\u7dda\u96fb\u8377\u306b\u3088\u308b\u96fb\u5834\u306e\u6c42\u3081\u65b9<\/h2>\n

\u7dda\u96fb\u8377\u3068\u306f\u3001\u975e\u5e38\u306b\u9577\u3044\u3001\u307e\u305f\u306f\u7121\u9650\u306b\u9577\u3044\u5e2f\u72b6\u306e\u96fb\u8377\u306e\u5206\u5e03\u3092\u6307\u3057\u307e\u3059\u3002\u7dda\u96fb\u8377\u306b\u3088\u308b\u96fb\u5834\u3092\u6c42\u3081\u308b\u305f\u3081\u306b\u306f\u3001\u30ac\u30a6\u30b9\u306e\u6cd5\u5247\u3092\u5229\u7528\u3059\u308b\u306e\u304c\u4e00\u822c\u7684\u3067\u3059\u3002\u4ee5\u4e0b\u3067\u306f\u305d\u306e\u65b9\u6cd5\u306b\u3064\u3044\u3066\u8aac\u660e\u3057\u307e\u3059\u3002<\/p>\n

<\/p>\n

  • \u96fb\u5834\u306e\u5bfe\u79f0\u6027<\/li>\n
  • \u30ac\u30a6\u30b9\u306e\u6cd5\u5247\u306e\u9069\u7528<\/li>\n
  • \u96fb\u5834\u306e\u5177\u4f53\u7684\u306a\u8a08\u7b97<\/li>\n

    <\/u1><\/p>\n

    \u96fb\u5834\u306e\u5bfe\u79f0\u6027<\/h2>\n

    \u7dda\u96fb\u8377\u306e\u96fb\u5834\u306f\u8ef8\u5bfe\u79f0\u3067\u3042\u308a\u3001\u96fb\u8377\u304c\u7121\u9650\u306b\u9577\u3044\u5834\u5408\u306b\u306f\u3001\u96fb\u5834\u306f\u7dda\u96fb\u8377\u306e\u5782\u76f4\u65b9\u5411\u306b\u306e\u307f\u5b58\u5728\u3057\u307e\u3059\u3002\u3053\u306e\u5bfe\u79f0\u6027\u3092\u5229\u7528\u3059\u308b\u3053\u3068\u3067\u3001\u96fb\u5834\u3092\u7c21\u5358\u306b\u6c42\u3081\u308b\u3053\u3068\u304c\u3067\u304d\u307e\u3059\u3002<\/p>\n

    \u30ac\u30a6\u30b9\u306e\u6cd5\u5247\u306e\u9069\u7528<\/h2>\n

    \u30ac\u30a6\u30b9\u306e\u6cd5\u5247\u306f\u4ee5\u4e0b\u306e\u3088\u3046\u306b\u8868\u3055\u308c\u307e\u3059\uff1a<\/p>\n

    \\[
    \n\\oint \\mathbf{E} \\cdot d\\mathbf{A} = \\frac{Q_{\\text{\u5185}}}{\\epsilon_0}
    \n\\]<\/p>\n

    \u3053\u3053\u3067 \\(\\oint \\mathbf{E} \\cdot d\\mathbf{A}\\) \u306f\u4efb\u610f\u306e\u9589\u3058\u305f\u9762\u3092\u8cab\u901a\u3059\u308b\u96fb\u5834\u306e\u30d5\u30e9\u30c3\u30af\u30b9\u3001 \\(Q_{\\text{\u5185}}\\) \u306f\u305d\u306e\u9762\u5185\u306b\u5b58\u5728\u3059\u308b\u96fb\u8377\u3001 \\(\\epsilon_0\\) \u306f\u771f\u7a7a\u306e\u8a98\u96fb\u7387\u3067\u3059\u3002<\/p>\n

    \u96fb\u5834\u306e\u5177\u4f53\u7684\u306a\u8a08\u7b97<\/h2>\n

    \u7dda\u96fb\u8377\u5bc6\u5ea6 \\(\\lambda\\) \u306e\u7121\u9650\u306b\u9577\u3044\u76f4\u7dda\u72b6\u306e\u96fb\u8377\u3092\u8003\u3048\u307e\u3059\u3002\u3053\u306e\u7dda\u96fb\u8377\u304b\u3089\u8ddd\u96e2 \\(r\\) \u306e\u70b9\u306b\u304a\u3051\u308b\u96fb\u5834 \\(E(r)\\) \u3092\u6c42\u3081\u308b\u306b\u306f\u3001\u30ac\u30a6\u30b9\u9762\uff08\u5186\u7b52\u72b6\u306e\u9589\u66f2\u9762\uff09\u3092\u8003\u3048\u307e\u3059\u3002<\/p>\n

    <\/p>\n

  • \u307e\u305a\u3001\u30ac\u30a6\u30b9\u9762\u306e\u5f62\u72b6\u3092\u5186\u7b52\u3068\u3057\u3001\u534a\u5f84 \\(r\\) \u53ca\u3073\u9577\u3055 \\(L\\) \u3092\u6301\u3064\u5186\u7b52\u9762\u3092\u8003\u3048\u307e\u3059\u3002<\/li>\n
  • \u7dda\u96fb\u8377\u306b\u5e73\u884c\u306a\u9762\u304b\u3089\u306e\u96fb\u5834\u306e\u5bc4\u4e0e\u306f\u30bc\u30ed\u3068\u306a\u308a\u3001\u5782\u76f4\u306a\u4e21\u7aef\u9762\u306e\u9762\u7a4d\u306f\u8a08\u7b97\u306b\u542b\u307e\u308c\u307e\u305b\u3093\u3002<\/li>\n
  • \u5186\u7b52\u9762\u4e0a\u306e\u5168\u3066\u306e\u70b9\u3067\u306e\u96fb\u5834\u5f37\u5ea6\u306f\u4e00\u5b9a\u3067\u3042\u308b\u305f\u3081\u3001\u6b21\u306e\u3088\u3046\u306b\u8a08\u7b97\u3067\u304d\u307e\u3059\uff1a\n

    \\[
    \n E \\cdot (2 \\pi r L) = \\frac{\\lambda L}{\\epsilon_0}
    \n \\]<\/p>\n<\/li>\n

  • \u3053\u308c\u3092\u89e3\u304f\u3068:\n

    \\[
    \n E = \\frac{\\lambda}{2 \\pi \\epsilon_0 r}
    \n \\]<\/p>\n<\/li>\n

    <\/o1><\/p>\n

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