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**\u5165\u5c04\u5149\u3001\u53cd\u5c04\u5149\u3001\u5c48\u6298\u5149\u306e\u95a2\u4fc2\u5f0f**\\\\<br \/>\n    \u5165\u5c04\u89d2\u3092 \\(\\theta_i\\)\u3001\u53cd\u5c04\u89d2\u3092 \\(\\theta_r\\)\u3001\u5c48\u6298\u89d2\u3092 \\(\\theta_t\\)\u3001\u5a92\u8cea1\u306e\u5c48\u6298\u7387\u3092 \\(n_1\\)\u3001\u5a92\u8cea2\u306e\u5c48\u6298\u7387\u3092 \\(n_2\\) \u3068\u3057\u307e\u3059\u3002<\/p>\n<p>    \\[<br \/>\n    n_1 \\sin \\theta_i = n_2 \\sin \\theta_t<br \/>\n    \\]<\/p>\n<p>2. **\u96fb\u5834\u3068\u78c1\u5834\u306e\u5883\u754c\u6761\u4ef6**\\\\<br \/>\n    \u96fb\u5834 \\(\\mathbf{E}\\) \u3068\u78c1\u5834 \\(\\mathbf{H}\\) \u306f\u3001\u5a92\u8cea\u306e\u5883\u754c\u3067\u9023\u7d9a\u3057\u3066\u3044\u307e\u3059\u3002\u3053\u308c\u306b\u57fa\u3065\u304d\u6b21\u306e\u65b9\u7a0b\u5f0f\u3092\u8a2d\u5b9a\u3057\u307e\u3059\u3002<\/p>\n<p>    \\[<br \/>\n    E_{i} + E_{r} = E_{t}<br \/>\n    \\]<\/p>\n<p>3. **\u30d5\u30ec\u30cd\u30eb\u306e\u65b9\u7a0b\u5f0f**\\\\<br \/>\n    S\u504f\u5149\u306e\u5834\u5408\u306e\u30d5\u30ec\u30cd\u30eb\u306e\u65b9\u7a0b\u5f0f\u306f\u6b21\u306e\u3088\u3046\u306b\u306a\u308a\u307e\u3059\u3002<\/p>\n<p>    \\[<br \/>\n    r_s = \\frac{E_r}{E_i} = \\frac{n_1 \\cos \\theta_i &#8211; n_2 \\cos \\theta_t}{n_1 \\cos \\theta_i + n_2 \\cos \\theta_t}<br \/>\n    \\]<\/p>\n<p>    \u53cd\u5c04\u4fc2\u6570 \\(r_s\\) \u306f\u3001\u53cd\u5c04\u5149\u306e\u96fb\u5834\u30d9\u30af\u30c8\u30eb\u306e\u632f\u5e45 \\(E_r\\) \u3068\u5165\u5c04\u5149\u306e\u96fb\u5834\u30d9\u30af\u30c8\u30eb\u306e\u632f\u5e45 \\(E_i\\) 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