{"id":3270,"date":"2022-07-15T16:43:34","date_gmt":"2022-07-15T07:43:34","guid":{"rendered":"https:\/\/home.hirosaki-u.ac.jp\/relativity\/?page_id=3270"},"modified":"2024-06-12T15:05:09","modified_gmt":"2024-06-12T06:05:09","slug":"%e7%84%a1%e7%90%86%e9%96%a2%e6%95%b0%e3%81%ae%e7%a9%8d%e5%88%86","status":"publish","type":"page","link":"https:\/\/home.hirosaki-u.ac.jp\/relativity\/%e7%90%86%e5%b7%a5%e7%b3%bb%e3%81%ae%e6%95%b0%e5%ad%a6b\/%e7%84%a1%e7%90%86%e9%96%a2%e6%95%b0%e3%81%ae%e7%a9%8d%e5%88%86\/","title":{"rendered":"\u7121\u7406\u95a2\u6570\u306e\u7a4d\u5206"},"content":{"rendered":"<p dir=\"ltr\">\u591a\u9805\u5f0f\u306e\u5e73\u65b9\u6839\u306a\u3069\u306e\u7121\u7406\u95a2\u6570\u3092\u542b\u3080\u5834\u5408\u306e\u7a4d\u5206\u3002\u5fc5\u305a\u7a4d\u5206\u3067\u304d\u308b\u3068\u3044\u3046\u308f\u3051\u3067\u306f\u306a\u3044\u304c\uff0c\u7f6e\u63db\u7a4d\u5206\u306a\u3069\u306b\u3088\u3063\u3066\u7a4d\u5206\u3067\u304d\u308b\u3044\u304f\u3064\u304b\u306e\u4f8b\u3092\u3042\u3052\u3066\u304a\u304f\u3002\uff08\u7121\u7406\u95a2\u6570\u306e\u7a4d\u5206\u306f\u7121\u7406\u3067\u3059\uff01\u306a\u3093\u3066\u8a00\u308f\u305a\u306b&#8230; \uff09<!--more--><\/p>\n<h3 dir=\"ltr\">\u4f8b 1 \\(\\displaystyle \\int \\frac{dx}{x \\sqrt{x+1}} \\)<\/h3>\n<p dir=\"ltr\">\\( \\sqrt{x+1} = t\\) \u3068\u304a\u304f\u3068\uff0c<\/p>\n<p id=\"yui_3_17_2_1_1657870978428_1403\" dir=\"ltr\">\\begin{eqnarray}<br \/>\nx + 1 &amp;=&amp; t^2 \\\\<br \/>\nx &amp;=&amp; t^2 -1 \\\\<br \/>\ndx &amp;=&amp; 2t dt<br \/>\n\\end{eqnarray}<\/p>\n<p dir=\"ltr\">\u3057\u305f\u304c\u3063\u3066\uff0c<\/p>\n<p dir=\"ltr\">\\begin{eqnarray}<br \/>\n\\int \\frac{dx}{x \\sqrt{x+1}} &amp;=&amp; \\int \\frac{2 t dt}{(t^2 -1) t} \\\\<br \/>\n&amp;=&amp; \\int \\frac{2}{t^2-1} dt\\\\<br \/>\n&amp;=&amp; \\int \\left( \\frac{1}{t-1} -\\frac{1}{t+1}\\right) dt\\\\<br \/>\n&amp;=&amp; \\log |t-1| -\\log |t + 1| + C \\\\<br \/>\n&amp;=&amp; \\log \\left| \\frac{\\sqrt{x+1} -1}{\\sqrt{x+1} + 1}\\right| + C<br \/>\n\\end{eqnarray}<\/p>\n<h3 dir=\"ltr\">\u4f8b 2 \\(\\displaystyle \\int \\frac{dx}{\\sqrt{x^2+1}} \\)<\/h3>\n<p dir=\"ltr\">\\( \\sqrt{x^2 + 1} = t\\) \u3067\u306f\u306a\u304f\uff0c\\( \\sqrt{x^2 + 1} = t {\\color{red} { -x}}\\) \u3068\u304a\u304f\u3068\u3088\u3044\u3053\u3068\u304c\u77e5\u3089\u308c\u3066\u3044\u308b\u3002<\/p>\n<p dir=\"ltr\">\\begin{eqnarray}<br \/>\n\\sqrt{x^2+1} &amp;=&amp; t -x \\\\<br \/>\nx^2 + 1 &amp;=&amp; t^2 -2 t x + x^2 \\\\<br \/>\n\\therefore\\ \\ x &amp;=&amp; \\frac{t^2-1}{2t} \\\\<br \/>\ndx &amp;=&amp; \\frac{t^2 + 1}{2t^2} dt \\\\<br \/>\n\\sqrt{x^2+1} &amp;=&amp; t -x \\\\<br \/>\n&amp;=&amp; t -\\frac{t^2 -1}{2t} \\\\<br \/>\n&amp;=&amp; \\frac{t^2 + 1}{2t}<br \/>\n\\end{eqnarray}<\/p>\n<p dir=\"ltr\">\u3057\u305f\u304c\u3063\u3066<\/p>\n<p dir=\"ltr\">\\begin{eqnarray}<br \/>\n\\int \\frac{dx}{\\sqrt{x^2+1}} &amp;=&amp; \\int \\frac{2t}{t^2 + 1} \\frac{t^2 + 1}{2t^2} dt\\\\<br \/>\n&amp;=&amp; \\int \\frac{1}{t} dt \\\\<br \/>\n&amp;=&amp; \\log |t| + C \\\\<br \/>\n&amp;=&amp; \\log \\left|x + \\sqrt{x^2 + 1}\\right| + C \\\\<br \/>\n&amp;=&amp; \\log \\left(x + \\sqrt{x^2 + 1}\\right) + C<br \/>\n\\end{eqnarray}<\/p>\n<h4 dir=\"ltr\">\u5225\u89e3\uff1a<\/h4>\n<p dir=\"ltr\">\u9006\u53cc\u66f2\u7dda\u95a2\u6570\u306e\u5fae\u5206\u3092\u601d\u3044\u51fa\u3059\u3068<\/p>\n<p dir=\"ltr\">$$ \\frac{d}{dx} \\sinh^{-1} x = \\frac{d}{dx} \\log\\left(x + \\sqrt{x^2+1}\\right) = \\frac{1}{\\sqrt{x^2+1}}$$<\/p>\n<p dir=\"ltr\">\u3060\u3063\u305f\u304b\u3089\uff0c\u305f\u3060\u3061\u306b<\/p>\n<p dir=\"ltr\">$$\\int\\frac{dx}{\\sqrt{x^2+1}} = \\sinh^{-1} x + C = \\log\\left(x + \\sqrt{x^2+1}\\right) + C$$<\/p>\n<h3 dir=\"ltr\">\u4f8b 3 \\(\\displaystyle \\int \\sqrt{x^2+1} dx\\)<\/h3>\n<p dir=\"ltr\">\u3053\u306e\u5834\u5408\u3082 \\( \\sqrt{x^2 + 1} = t -x\\) \u3068\u304a\u304f\u3068\u3088\u3044\u3053\u3068\u304c\u77e5\u3089\u308c\u3066\u3044\u308b\u3002<\/p>\n<p dir=\"ltr\">\\begin{eqnarray}<br \/>\n\\int \\sqrt{x^2+1} dx &amp;=&amp; \\int \\frac{t^2+1}{2t} \\frac{t^2 + 1}{2t^2} dt\\\\<br \/>\n&amp;=&amp; \\frac{1}{4} \\int \\frac{t^4 + 2 t^2 + 1}{t^3} dt \\\\<br \/>\n&amp;=&amp; \\frac{1}{4} \\int \\left(t + \\frac{2}{t} + \\frac{1}{t^3} \\right)dt\\\\<br \/>\n&amp;=&amp; \\frac{1}{4} \\left( \\frac{t^2}{2} + 2 \\log |t| -\\frac{1}{2 t^2} \\right) + C \\\\<br \/>\n&amp;=&amp; \\frac{1}{2} \\log |t| + \\frac{1}{2} \\frac{t^2 + 1}{2t} \\frac{t^2 -1}{2t} + C\\\\<br \/>\n&amp;=&amp; \\frac{1}{2} \\log \\left(x + \\sqrt{x^2+1}\\right)+ \\frac{1}{2} x \\sqrt{x^2+1}+ C \\\\<br \/>\n&amp;=&amp; \\frac{1}{2} \\sinh^{-1} x + \\frac{1}{2} x \\sqrt{x^2+1}+ C<br \/>\n\\end{eqnarray}<\/p>\n<p>&nbsp;<\/p>\n<h4>\u5225\u89e3\uff1a<\/h4>\n<p>\u90e8\u5206\u7a4d\u5206\u3092\u3057\u3066\uff0c\u4f8b 2 \u306e\u7d50\u679c\u3092\u4f7f\u3046\u3002<\/p>\n<p>\\begin{eqnarray}<br \/>\n\\int \\sqrt{x^2+1} dx &amp;=&amp; x \\sqrt{x^2 + 1} -\\int x \\frac{x}{\\sqrt{x^2+1}} dx \\\\<br \/>\n&amp;=&amp; x \\sqrt{x^2 + 1} -\\int\u00a0 \\frac{x^2 + 1}{\\sqrt{x^2+1}} dx + \\int\u00a0 \\frac{1}{\\sqrt{x^2+1}} dx\\\\<br \/>\n&amp;=&amp; \\int\u00a0 \\frac{1}{\\sqrt{x^2+1}} dx + x \\sqrt{x^2 + 1} -\\int \\sqrt{x^2 + 1} dx \\\\ \\ \\\\<br \/>\n\\therefore\\ \\ \\int \\sqrt{x^2+1} dx &amp;=&amp; \\frac{1}{2} \\left\\{ \\int\u00a0 \\frac{1}{\\sqrt{x^2+1}} dx + x \\sqrt{x^2 + 1}\\right\\} \\\\<br \/>\n&amp;=&amp; \\frac{1}{2} \\log \\left(x + \\sqrt{x^2+1}\\right) + \\frac{1}{2} x \\sqrt{x^2+1}+ C \\\\<br \/>\n&amp;=&amp; \\frac{1}{2} \\sinh^{-1} x + \\frac{1}{2} x \\sqrt{x^2+1}+ C<br \/>\n\\end{eqnarray}<\/p>\n<h3>\u4f8b 4 \\(\\displaystyle \\int \\sqrt{1 -x^2} \\,dx\\)<\/h3>\n<h4>\u7f6e\u63db\u7a4d\u5206\u3067\u89e3\u304f\u4f8b<\/h4>\n<p>$x = \\sin t, \\ dx = \\cos t\\, dt$ \u3068\u3057\u3066<\/p>\n<p>\\begin{eqnarray}<br \/>\n\\int \\sqrt{1 -x^2}\\, dx &amp;=&amp; \\int \\sqrt{1 -\\sin^2 t} \\, \\cos t\\, dt \\\\<br \/>\n&amp;=&amp; \\int \\cos^2 t\\, dt \\\\<br \/>\n&amp;=&amp; \\frac{1}{2} \\int (\\cos 2 t +1)\\, dt \\\\<br \/>\n&amp;=&amp; \\frac{1}{2} \\left(\\frac{1}{2} \\sin 2 t + t\\right) \\\\<br \/>\n&amp;=&amp; \\frac{1}{2} \\left(\\sin\u00a0 t \\cos t + t\\right) \\\\<br \/>\n&amp;=&amp; \\frac{1}{2} \\left(x \\sqrt{1 -x^2} + \\sin^{-1} x \\right)<br \/>\n\\end{eqnarray}<\/p>\n<h4>\u90e8\u5206\u7a4d\u5206\u3067\u89e3\u304f\u4f8b<\/h4>\n<p>\\begin{eqnarray}<br \/>\nI &amp;\\equiv&amp; \\int \\sqrt{1-x^2}\\, dx \\\\<br \/>\n&amp;=&amp; x \\sqrt{1 -x^2} -\\int x\\, \\left(\\frac{d}{dx} \\sqrt{1 -x^2}\\right) \\,dx\\\\<br \/>\n&amp;=&amp; x \\sqrt{1-x^2} + \\int \\frac{x^2}{\\sqrt{1-x^2}}\\,dx \\\\<br \/>\n&amp;=&amp; x \\sqrt{1-x^2} + \\int \\frac{1}{\\sqrt{1-x^2}} \\,dx -\\int \\frac{1-x^2}{\\sqrt{1-x^2}}\\, dx \\\\<br \/>\n&amp;=&amp; x \\sqrt{1-x^2} + \\int \\frac{1}{\\sqrt{1-x^2}} \\,dx -I \\\\<br \/>\n\\therefore\\ \\ I &amp;=&amp; \\frac{1}{2} \\left(x \\sqrt{1-x^2} + \\int \\frac{1}{\\sqrt{1-x^2}} \\,dx \\right) \\\\<br \/>\n&amp;=&amp; \\frac{1}{2}\\left(x\\sqrt{1-x^2} +\\sin^{-1} x\\right)<br \/>\n\\end{eqnarray}<\/p>\n<h3>\u7df4\u7fd2\u554f\u984c 1. \\(\\displaystyle \\int \\frac{dx}{x \\sqrt{x-1}} \\)<\/h3>\n<p>$\\sqrt{x-1} = t$\u00a0 \u3068\u304a\u304f\u3068&#8230;<\/p>\n<p>\u3053\u306e\u7a4d\u5206\u306f<a href=\"https:\/\/home.hirosaki-u.ac.jp\/relativity\/%e4%b8%80%e8%88%ac%e7%9b%b8%e5%af%be%e8%ab%96%e7%9a%84%e5%ae%87%e5%ae%99%e8%ab%96\/%e8%a7%92%e5%be%84%e8%b7%9d%e9%9b%a2\/#Omega_Lambda_0\">\u76f8\u5bfe\u8ad6\u7684\u5b87\u5b99\u8ad6\u306e\u307b\u3046\u3067\u5fc5\u8981\u306b\u306a\u3063\u305f\u308a\u3059\u308b<\/a>\u3093\u3067\u3059\u3088\u3002<\/p>\n<h3>\u7df4\u7fd2\u554f\u984c 2. \\(\\displaystyle \\int \\frac{\\sqrt{x}}{\\sqrt{1-x}} dx \\)<\/h3>\n<h3>\u7df4\u7fd2\u554f\u984c 3. \\(\\displaystyle \\int \\frac{\\sqrt{x}}{\\sqrt{1-x^3}} dx \\)<\/h3>\n<p>\u3053\u3093\u306a\u7a4d\u5206\uff0c\u793e\u4f1a\u306b\u51fa\u305f\u3089\u7d76\u5bfe\u4f7f\u308f\u306a\u3044\u3057\uff0c\u5f79\u306b\u306a\u3093\u304b\u305f\u305f\u306a\u3044\u306a\u3069\u3068\u601d\u3063\u3066\u3044\u307e\u305b\u3093\u304b\uff1f\u3053\u308c\u3089\u306e\u7a4d\u5206\u3082<a href=\"https:\/\/home.hirosaki-u.ac.jp\/relativity\/%e4%b8%80%e8%88%ac%e7%9b%b8%e5%af%be%e8%ab%96%e7%9a%84%e5%ae%87%e5%ae%99%e8%ab%96\/%e5%ae%87%e5%ae%99%e8%ab%96%e3%83%91%e3%83%a9%e3%83%a1%e3%83%bc%e3%82%bf%e3%81%a8%e5%ae%87%e5%ae%99%e5%b9%b4%e9%bd%a2\/#i-5\" target=\"_blank\" rel=\"noopener\">\u5b87\u5b99\u5e74\u9f62\u3092\u77e5\u308b\u305f\u3081\u306b\u5fc5\u8981\u306b\u306a\u3063\u305f\u308a\u3059\u308b<\/a>\u3093\u3067\u3059\u3088\u3002<\/p>\n<h3>\u7df4\u7fd2\u554f\u984c 4. \\(\\displaystyle \\int \\frac{1}{\\left(a^2 +x^2\\right)^{\\frac{3}{2}}} dx \\)<\/h3>\n<p>\u3053\u3093\u306a\u7a4d\u5206\uff0c\u3044\u3063\u305f\u3044\u3044\u3064\u3069\u3053\u3067\u4f7f\u3046\u3093\u3060\u3068\u601d\u3063\u3066\u3044\u307e\u305b\u3093\u304b\uff1f\u3053\u306e\u7a4d\u5206\u306f1\u5e74\u751f\u5f8c\u671f\u306e\u96fb\u78c1\u6c17\u5b66I\u3067<a href=\"https:\/\/home.hirosaki-u.ac.jp\/relativity\/%e9%9b%bb%e7%a3%81%e6%b0%97%e5%ad%a6-i\/%e9%9d%99%e9%9b%bb%e5%a0%b4%ef%bc%9a%e9%9b%bb%e8%8d%b7%e5%af%86%e5%ba%a6%e3%81%8b%e3%82%89%e7%9b%b4%e6%8e%a5%e9%9b%bb%e5%a0%b4%e3%82%92%e6%b1%82%e3%82%81%e3%82%8b\/#i-5\">\u4e00\u69d8\u306a\u7dda\u96fb\u8377\u306b\u3088\u308b\u96fb\u5834<\/a>\u3092\u6c42\u3081\u308b\u969b\u306b\u4f7f\u3046\u3093\u3067\u3059\u3088\uff01<\/p>\n","protected":false},"excerpt":{"rendered":"<p dir=\"ltr\">\u591a\u9805\u5f0f\u306e\u5e73\u65b9\u6839\u306a\u3069\u306e\u7121\u7406\u95a2\u6570\u3092\u542b\u3080\u5834\u5408\u306e\u7a4d\u5206\u3002\u5fc5\u305a\u7a4d\u5206\u3067\u304d\u308b\u3068\u3044\u3046\u308f\u3051\u3067\u306f\u306a\u3044\u304c\uff0c\u7f6e\u63db\u7a4d\u5206\u306a\u3069\u306b\u3088\u3063\u3066\u7a4d\u5206\u3067\u304d\u308b\u3044\u304f\u3064\u304b\u306e\u4f8b\u3092\u3042\u3052\u3066\u304a\u304f\u3002\uff08\u7121\u7406\u95a2\u6570\u306e\u7a4d\u5206\u306f\u7121\u7406\u3067\u3059\uff01\u306a\u3093\u3066\u8a00\u308f\u305a\u306b&#8230; \uff09<\/p><p><a class=\"more-link btn\" href=\"https:\/\/home.hirosaki-u.ac.jp\/relativity\/%e7%90%86%e5%b7%a5%e7%b3%bb%e3%81%ae%e6%95%b0%e5%ad%a6b\/%e7%84%a1%e7%90%86%e9%96%a2%e6%95%b0%e3%81%ae%e7%a9%8d%e5%88%86\/\">\u7d9a\u304d\u3092\u8aad\u3080<\/a><\/p>\n","protected":false},"author":33,"featured_media":0,"parent":2068,"menu_order":28,"comment_status":"closed","ping_status":"closed","template":"","meta":{"inline_featured_image":false,"footnotes":""},"class_list":["post-3270","page","type-page","status-publish","hentry","nodate","item-wrap"],"aioseo_notices":[],"_links":{"self":[{"href":"https:\/\/home.hirosaki-u.ac.jp\/relativity\/wp-json\/wp\/v2\/pages\/3270","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/home.hirosaki-u.ac.jp\/relativity\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/home.hirosaki-u.ac.jp\/relativity\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/home.hirosaki-u.ac.jp\/relativity\/wp-json\/wp\/v2\/users\/33"}],"replies":[{"embeddable":true,"href":"https:\/\/home.hirosaki-u.ac.jp\/relativity\/wp-json\/wp\/v2\/comments?post=3270"}],"version-history":[{"count":15,"href":"https:\/\/home.hirosaki-u.ac.jp\/relativity\/wp-json\/wp\/v2\/pages\/3270\/revisions"}],"predecessor-version":[{"id":8886,"href":"https:\/\/home.hirosaki-u.ac.jp\/relativity\/wp-json\/wp\/v2\/pages\/3270\/revisions\/8886"}],"up":[{"embeddable":true,"href":"https:\/\/home.hirosaki-u.ac.jp\/relativity\/wp-json\/wp\/v2\/pages\/2068"}],"wp:attachment":[{"href":"https:\/\/home.hirosaki-u.ac.jp\/relativity\/wp-json\/wp\/v2\/media?parent=3270"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}