\u82f1\u56fd\u79d1\u5b66\u671f\u520a\u300a\u7269\u7406\u4e16\u754c\u300b\u66fe\u8ba9\u8bfb\u8005\u6295\u7968\u8bc4\u9009\u4e86\u201c\u6700\u4f1f\u5927\u7684\u516c\u5f0f\u201d\uff0c\u6700\u7ec8\u699c\u4e0a\u6709\u540d\u7684\u5341\u4e2a\u516c\u5f0f\u65e2\u6709\u65e0\u4eba\u4e0d\u77e5\u76841+1=2\uff0c\u53c8\u6709\u8457\u540d\u7684$E_0=mc^2$\uff1b\u65e2\u6709\u7b80\u5355\u7684-\u5706\u5468\u516c\u5f0f\uff0c\u53c8\u6709\u590d\u6742\u7684\u6b27\u62c9\u516c\u5f0f\u2026\u2026
\n
\n\u4ece\u4ec0\u4e48\u65f6\u5019\u8d77\u6211\u4eec\u5f00\u59cb\u538c\u6076\u6570\u5b66\uff1f\u8fd9\u4e9b\u4e1c\u897f\u539f\u672c\u5982\u6b64\u7f8e\u4e3d\uff0c\u5982\u6b64\u7cbe\u5999\u3002\u8fd9\u4e2a\u5730\u7403\u4e0a\u6709\u591a\u5c11\u4f1f\u5927\u7684\u667a\u6167\u66fe\u8017\u5c3d\u4e00\u751f\uff0c\u624d\u6700\u7ec8\u5199\u4e0b\u4e00\u4e2a\u7b49\u53f7\u3002\u6bcf\u5f53\u4f60\u89e3\u4e0d\u5f00\u65b9\u7a0b\u7684\u65f6\u5019\uff0c\u4e0d\u59a8\u6362\u4e00\u4e2a\u89d2\u5ea6\u60f3\uff0c\u6682\u4e14\u653e\u4e0b\u5bf9\u7406\u79d1\u7684\u538c\u6076\u548c\u5bf9\u8003\u8bd5\u7684\u75db\u6068\u3002\u56e0\u4e3a\u4f60\u6b63\u5728\u89c1\u8bc1\u7684\uff0c\u662f\u79d1\u5b66\u7684\u7f8e\u4e3d\u4e0e\u4eba\u7c7b\u7684\u5c0a\u4e25\u3002<\/p>\n
$\\large\\textbf { No.10. \u5706\u7684\u5468\u957f\u516c\u5f0f\uff1a( The Length of the Circumference of a Circle )}$
\n\\[c=2 \\pi r\\]<\/p>\n
\u8fd9\u516c\u5f0f\u8d3c\u725b\u903c\u4e86\uff0c\u521d\u4e2d\u5b66\u5230\u73b0\u5728\u3002\u76ee\u524d\uff0c\u4eba\u7c7b\u5df2\u7ecf\u80fd\u5f97\u5230\u5706\u5468\u7387\u76842061\u4ebf\u4f4d\u7cbe\u5ea6\u3002\u8fd8\u662f\u633a\u65e0\u804a\u7684\u3002\u73b0\u4ee3\u79d1\u6280\u9886\u57df\u4f7f\u7528\u7684-\u5706\u5468\u7387\u503c\uff0c\u6709\u5341\u51e0\u4f4d\u5df2\u7ecf\u8db3\u591f\u4e86\u3002\u5982\u679c\u7528 35\u4f4d\u7cbe\u5ea6\u7684-\u5706\u5468\u7387\u503c\uff0c\u6765\u8ba1\u7b97\u4e00\u4e2a\u80fd\u628a\u592a\u9633\u7cfb\u5305\u8d77\u6765\u7684\u4e00\u4e2a\u5706\u7684\u5468\u957f\uff0c\u8bef\u5dee\u8fd8\u4e0d\u5230\u8d28\u5b50\u76f4\u5f84\u7684\u767e\u4e07\u5206\u4e4b\u4e00\u3002\u73b0\u5728\u7684\u4eba\u8ba1\u7b97\u5706\u5468\u7387\uff0c\u591a\u6570\u662f\u4e3a\u4e86\u9a8c\u8bc1\u8ba1\u7b97\u673a\u7684\u8ba1\u7b97 \u80fd\u529b\uff0c\u8fd8\u6709\u5c31\u662f\u4e3a\u4e86\u5174\u8da3\u3002<\/p>\n
$\\large\\textbf { No.9. \u5085\u91cc\u53f6\u53d8\u6362\u65b9\u7a0b\uff1a (The Fourier Transform) }$
\n\\[\\hat{f}(\\xi):=\\int_{-\\infty}^{\\infty} f(x) e^{-2 \\pi i x \\xi} d x\\]<\/p>\n
\u8fd9\u4e2a\u633a\u4e13\u4e1a\u7684\uff0c\u4e00\u822c\u4eba\u5b8c\u5168\u4e0d\u660e\u767d\u3002\u4e0d\u591a\u4f5c\u89e3\u91ca\u3002\u7b80\u8981\u5730\u8bf4\u6ca1\u6709\u8fd9\u4e2a\u5f0f\u5b50\u6ca1\u6709\u4eca\u5929\u7684\u7535\u5b50\u8ba1\u7b97\u673a\uff0c\u6240\u4ee5\u4f60\u80fd\u5728\u8fd9\u91cc\u4e0a\u7f51\u9664\u4e86\u611f\u8c22\u515a\u611f\u8c22\u653f\u5e9c\u8fd8\u8981\u611f\u8c22\u8fd9\u4e2a\u5b8c\u5168\u770b\u4e0d\u61c2\u7684\u5f0f\u5b50\u3002\u53e6\u5916\u5085\u7acb\u53f6\u867d\u7136\u59d3\u5085\uff0c\u4f46\u662f\u6cd5\u56fd\u4eba\u3002<\/p>\n
$\\large\\textbf { No.8. \u5fb7\u5e03\u7f57\u610f\u65b9\u7a0b\u7ec4\uff1a( The de Broglie Relations) }$
\n\\begin{equation}
\n\\begin{array}{l}
\np=\\hbar k \\\\
\nE=\\hbar \\omega
\n\\end{array}
\n\\end{equation}<\/p>\n
\u8fd9\u4e2a\u4e1c\u897f\u4e5f\u633a\u725b\u903c\u7684\uff0c\u9ad8\u4e2d\u7269\u7406\u5b66\u5230\u5149\u5b66\u7684\u8bdd\u5f88\u591a\u6982\u5ff5\u8ddf\u5b83\u662f\u8fdc\u4eb2\u3002\u7b80\u8981\u5730\u8bf4\u5fb7\u5e03\u7f57\u610f\u8fd9\u4eba\u89c9\u5f97\u7535\u5b50\u4e0d\u4ec5\u662f\u4e00\u4e2a\u7c92\u5b50\uff0c\u4e5f\u662f\u4e00\u79cd\u6ce2\uff0c\u5b83\u8fd8\u6709 \u201c\u6ce2\u957f\u201d\u3002\u4e8e\u662f\u641e\u554a\u641e\u5c31\u6709\u4e86\u8fd9\u4e2a\u7269\u8d28\u6ce2\u65b9\u7a0b\uff0c\u8868\u8fbe\u4e86\u6ce2\u957f\u3001\u80fd\u91cf\u7b49\u7b49\u4e4b\u95f4\u7684\u5173\u7cfb\u3002\u540c\u65f6\u4ed6\u83b7\u5f97\u4e861929\u5e74\u8bfa\u8d1d\u5c14\u7269\u7406\u5b66\u5956\u3002<\/p>\n
$\\large\\textbf { No.7. 1 + 1 = 2 } $
\n\u8fd9\u4e2a\u516c\u5f0f\u4e0d\u9700\u8981\u540d\u79f0\uff0c\u4e0d\u9700\u8981\u7ffb\u8bd1\uff0c\u4e0d\u9700\u8981\u89e3\u91ca\u3002<\/p>\n
$\\large\\textbf { No.6. \u859b\u5b9a\u8c14\u65b9\u7a0b\uff1a(The Schrodinger Equation) }$
\n\\[i \\hbar \\frac{\\partial}{\\partial t} \\Psi(\\mathbf{r}, t)=\\hat{H} \\Psi(\\mathbf{r}, t)\\]<\/p>\n
\u4e5f\u662f\u4e00\u822c\u4eba\u5b8c\u5168\u4e0d\u660e\u767d\u7684\u3002\u56e0\u6b64\u6211\u6458\u5f55\u5b98\u65b9\u8bc4\u4ef7\uff1a\u201c\u859b\u5b9a\u8c14\u65b9\u7a0b\u662f\u4e16\u754c\u539f\u5b50\u7269\u7406\u5b66\u6587\u732e\u4e2d\u5e94\u7528\u6700\u5e7f\u6cdb\u3001\u5f71\u54cd\u6700\u5927\u7684\u516c\u5f0f\u3002\u201d\u7531\u4e8e\u5bf9\u91cf\u5b50\u529b\u5b66\u7684\u6770\u51fa\u8d21\u732e\uff0c\u859b\u5b9a\u8c14\u83b7\u5f971933\u5e74\u8bfa\u8d1d\u5c14\u7269\u7406\u5956\u3002
\n\u53e6\u5916\u859b\u5b9a\u8c14\u867d\u7136\u59d3\u859b\uff0c\u4f46\u662f\u5965\u5730\u5229\u4eba\u3002<\/p>\n
$\\large\\textbf { No.5. \u7231\u56e0\u65af\u5766\u8d28\u80fd\u65b9\u7a0b\uff1a(Mass-energy Equivalence) }$
\n\\[E_0=mc^2\\]<\/p>\n
\u597d\u50cf\u4ece\u6765\u6ca1\u6709\u4e00\u4e2a\u79d1\u5b66\u754c\u7684\u516c\u5f0f\u6709\u5982\u6b64\u5e7f\u6cdb\u7684\u610f\u4e49\u3002\u5728\u7269\u7406\u5b66\u201c\u5947\u8ff9\u5e74\u201d1905\u5e74\uff0c\u7531\u4e00\u4e2a\u53eb\u505a\u7231\u56e0\u65af\u5766\u7684\u5e74\u8f7b\u4eba\u63d0\u51fa\u3002\u540c\u5e74\u4ed6\u8fd8\u53d1\u8868\u4e86\u300a\u8bba\u52a8\u4f53\u7684\u7535\u52a8\u529b\u5b66\u300b\u2014\u2014\u4fd7\u79f0\u72ed\u4e49\u76f8\u5bf9\u8bba\u3002
\n\u8fd9\u4e2a\u516c\u5f0f\u544a\u8bc9\u6211\u4eec\uff0c\u7231\u56e0\u65af\u5766\u662f\u725b\u903c\u7684\uff0c\u80fd\u91cf\u548c\u8d28\u91cf\u662f\u53ef\u4ee5\u4e92\u6362\u7684\u3002\u526f\u4ea7\u54c1\uff1a\u539f\u5b50\u5f39\u3002<\/p>\n
$\\large\\textbf { No.4. \u6bd5\u8fbe\u54e5\u62c9\u65af\u5b9a\u7406\uff1a(Pythagorean Theorem) }$
\n\\[a^2 + b^2 = c^2\\]<\/p>\n
\u505a\u6570\u5b66\u4e0d\u53ef\u80fd\u6ca1\u7528\u5230\u8fc7\u5427\uff0c\u4e0d\u591a\u8bb2\u4e86\u3002<\/p>\n
$\\large\\textbf { No.3. \u725b\u987f\u7b2c\u4e8c\u5b9a\u5f8b\uff1a(Newtow’s Second Law of Motion) }$
\n\\[F=ma\\]<\/p>\n
\u6709\u53f2\u4ee5\u6765\u6700\u4f1f\u5927\u7684\u6ca1\u6709\u4e4b\u4e00\u7684\u79d1\u5b66\u5bb6\u5728\u6709\u53f2\u4ee5\u6765\u6700\u4f1f\u5927\u6ca1\u6709\u4e4b\u4e00\u7684\u79d1\u5b66\u5de8\u4f5c\u300a\u81ea\u7136\u54f2\u5b66\u7684\u6570\u5b66\u539f\u7406\u300b\u5f53\u4e2d\u7684\u88ab\u8ba4\u4e3a\u662f\u7ecf\u5178\u7269\u7406\u5b66\u4e2d\u6700\u4f1f\u5927\u7684\u6ca1\u6709\u4e4b\u4e00\u7684\u6838\u5fc3\u5b9a\u5f8b\u3002\u52a8\u529b\u7684\u6240\u6709\u57fa\u672c\u65b9\u7a0b\u90fd\u53ef\u7531\u5b83\u901a\u8fc7\u5fae\u79ef\u5206\u63a8\u5bfc\u51fa\u6765\u3002\u5bf9\u4e8e\u5b66\u8fc7\u9ad8\u4e2d\u7269\u7406\u7684\u4eba\uff0c\u6ca1\u4ec0\u4e48\u597d\u591a\u8bb2\u4e86\u3002<\/p>\n
$\\large\\textbf { No.2. \u6b27\u62c9\u516c\u5f0f\uff1a(Euler’s Identity) }$
\n\\[e^{i\\pi}+ 1 =0 \\]<\/p>\n
\u8fd9\u4e2a\u516c\u5f0f\u662f\u4e0a\u5e1d\u5199\u7684\u4e48\uff1f\u5230\u4e86\u6700\u540e\u51e0\u540d\uff0c\u521b\u9020\u8005\u4e2a\u4e2a\u795e\u4eba\u3002\u6b27\u62c9\u662f\u5386\u53f2\u4e0a\u6700\u591a\u4ea7\u7684\u6570\u5b66\u5bb6\uff0c\u4e5f\u662f\u5404\u9886\u57df\uff08\u5305\u542b\u6570\u5b66\u7684\u6240\u6709\u5206\u652f\u53ca\u529b\u5b66\u3001\u5149\u5b66\u3001\u97f3\u54cd\u5b66\u3001\u6c34\u5229\u3001\u5929\u6587\u3001\u5316 \u5b66\u3001\u533b\u836f\u7b49\uff09\u6700\u591a\u8457\u4f5c\u7684\u5b66\u8005\u3002\u6570\u5b66\u53f2\u4e0a\u79f0\u5341\u516b\u4e16\u7eaa\u4e3a\u201c\u6b27\u62c9\u65f6\u4ee3\u201d\u3002
\n\u6b27\u62c9\u51fa\u751f\u4e8e\u745e\u58eb\uff0c31\u5c81\u4e27\u5931\u4e86\u53f3\u773c\u7684\u89c6\u529b\uff0c59\u5c81\u53cc\u773c\u5931\u660e\uff0c\u4f46\u4ed6\u6027\u683c\u4e50\u89c2\uff0c\u6709\u60ca\u4eba\u7684\u8bb0\u5fc6 \u529b\u53ca\u96c6\u4e2d\u529b\u3002\u4ed6\u4e00\u751f\u8c26\u900a\uff0c\u5f88\u5c11\u7528\u81ea\u5df1\u7684\u540d\u5b57\u7ed9\u4ed6\u53d1\u73b0\u7684\u4e1c\u897f\u547d\u540d\u3002\u4e0d\u8fc7\u8fd8\u662f\u547d\u540d\u4e86\u4e00\u4e2a\u6700\u91cd\u8981\u7684\u4e00\u4e2a\u5e38\u6570\u2014\u2014e\u3002
\n\u5173\u4e8ee\uff0c\u4ee5\u524d\u6709\u4e00\u4e2a\u7b11\u8bdd\u8bf4\uff1a\u5728\u4e00\u5bb6\u7cbe\u795e\u75c5\u9662\u91cc\uff0c\u6709\u4e2a\u75c5\u60a3\u6574\u5929\u5bf9\u7740\u522b\u4eba\u8bf4\uff0c\u201c\u6211\u5fae\u5206\u4f60\u3001\u6211\u5fae\u5206\u4f60\u3002\u201d\u4e5f\u4e0d\u77e5\u4e3a\u4ec0\u4e48\uff0c\u8fd9\u4e9b\u75c5\u60a3\u90fd\u6709\u4e00\u70b9\u7b80\u5355\u7684\u5fae\u79ef\u5206\u6982\u5ff5\uff0c\u603b\u4ee5\u4e3a \u6709\u4e00\u5929\u81ea\u5df1\u4f1a\u50cf\u4e00\u822c\u591a\u9879\u5f0f\u51fd\u6570\u822c\uff0c\u88ab\u5fae\u5206\u5230\u53d8\u6210\u96f6\u800c\u6d88\u5931\uff0c\u56e0\u6b64\u5bf9\u4ed6\u907f\u4e4b\u4e0d\u53ca\uff0c\u7136\u800c\u67d0\u5929\u4ed6\u5374\u9047\u4e0a\u4e86\u4e00\u4e2a\u4e0d\u4e3a\u6240\u52a8\u7684\u4eba\uff0c\u4ed6\u5f88\u610f\u5916\uff0c\u800c\u8fd9\u4e2a\u4eba\u6de1\u6de1\u5730\u5bf9\u4ed6\u8bf4\uff0c\u201c\u6211\u662fe\u7684x\u6b21\u65b9\u3002\u201d
\n\u8fd9\u4e2a\u516c\u5f0f\u7684\u5de7\u5999\u4e4b\u5904\u5728\u4e8e\uff0c\u5b83\u6ca1\u6709\u4efb\u4f55\u591a\u4f59\u7684\u5185\u5bb9\uff0c\u5c06\u6570\u5b66\u4e2d\u6700\u57fa\u672c\u7684$e\u3001i\u3001\\pi$\u653e\u5728\u4e86\u540c\u4e00\u4e2a\u5f0f\u5b50\u4e2d\uff0c\u540c\u65f6\u52a0\u5165\u4e86\u6570\u5b66\u4e5f\u662f\u54f2\u5b66\u4e2d\u6700\u91cd\u8981\u76840\u548c1\uff0c\u518d\u4ee5\u7b80\u5355\u7684\u52a0\u53f7\u76f8\u8fde\u3002
\n\u9ad8\u65af\u66fe\u7ecf\u8bf4\uff1a\u201c\u4e00\u4e2a\u4eba\u7b2c\u4e00\u6b21\u770b\u5230\u8fd9\u4e2a\u516c\u5f0f\u800c\u4e0d\u611f\u5230\u5b83\u7684\u9b45\u529b\uff0c\u4ed6\u4e0d\u53ef\u80fd\u6210\u4e3a\u6570\u5b66\u5bb6\u3002\u201d<\/p>\n
$\\large\\textbf { No.1. \u9ea6\u514b\u65af\u97e6\u65b9\u7a0b\u7ec4\uff1a(The Maxwell’s Equations) }$
\n\u79ef\u5206\u5f62\u5f0f\uff1a
\n\\begin{array}{l}
\n\\oint_{S} \\mathbf{D} \\cdot \\mathrm{d} \\mathbf{A}=Q_{f, S} \\\\
\n\\oint_{S} \\mathbf{B} \\cdot \\mathrm{d} \\mathbf{A}=0 \\\\
\n\\oint_{\\partial S} \\mathbf{E} \\cdot \\mathrm{d} \\mathbf{l}=-\\frac{\\partial \\Phi_{B, S}}{\\partial t} \\\\
\n\\oint_{\\partial S} \\mathbf{H} \\cdot \\mathrm{d} \\mathbf{l}=I_{f, S}+\\frac{\\partial \\Phi_{D, S}}{\\partial t}
\n\\end{array}
\n\u5fae\u5206\u5f62\u5f0f\uff1a
\n\\[\\left\\{ \\begin{array}{l}\\nabla \\cdot B = 0\\\\
\n\\nabla \\cdot D = \\rho \\\\
\n\\nabla \\times H = \u2013 \\frac{{\\partial D}}{{\\partial t}} + j\\\\
\n\\nabla \\times E = \u2013 \\frac{{\\partial B}}{{\\partial t}} \\end{array}
\n\\right.\\]<\/p>\n
\u4efb\u4f55\u4e00\u4e2a\u80fd\u628a\u8fd9\u51e0\u4e2a\u516c\u5f0f\u770b\u61c2\u7684\u4eba\uff0c\u4e00\u5b9a\u4f1a\u611f\u5230\u80cc\u540e\u6709\u51c9\u98ce\u2014\u2014\u5982\u679c\u6ca1\u6709\u4e0a\u5e1d\uff0c\u600e\u4e48\u89e3\u91ca\u5982\u6b64\u5b8c\u7f8e\u7684\u65b9\u7a0b\uff1f\u8fd9\u7ec4\u516c\u5f0f\u878d\u5408\u4e86\u7535\u7684\u9ad8\u65af\u5b9a\u5f8b\u3001\u78c1\u7684\u9ad8\u65af\u5b9a\u5f8b\u3001\u6cd5\u62c9\u7b2c\u5b9a\u5f8b \u4ee5\u53ca\u5b89\u57f9\u5b9a\u5f8b\u3002\u6bd4\u8f83\u8c26\u865a\u7684\u8bc4\u4ef7\u662f\uff1a\u201c\u4e00\u822c\u5730\uff0c\u5b87\u5b99\u95f4\u4efb\u4f55\u7684\u7535\u78c1\u73b0\u8c61\uff0c\u7686\u53ef\u7531\u6b64\u65b9\u7a0b\u7ec4\u89e3\u91ca\u3002\u201d
\n\u5230\u540e\u6765\u9ea6\u514b\u65af\u97e6\u4ec5\u9760\u7eb8\u7b14\u6f14\u7b97\uff0c\u5c31\u4ece\u8fd9\u7ec4\u516c\u5f0f\u9884\u8a00\u4e86\u7535\u78c1\u6ce2\u7684\u5b58 \u5728\u3002\u6211\u4eec\u4e0d\u662f\u603b\u559c\u6b22\u7f16\u4e00\u4e9b\u6545\u4e8b\uff0c\u6bd4\u5982\u7231\u56e0\u65af\u5766\u5c0f\u65f6\u5019\u56e0\u4e3a\u67d0\u4e00\u523a\u6fc0\u4ece\u800c\u8d70\u4e0a\u4e86\u53d1\u594b\u5b66\u4e60\u3001\u62a5\u6548\u7956\u56fd\u7684\u9053\u8def\u4e48\uff1f\u4e8b\u5b9e\u4e0a\uff0c\u8fd9\u4e2a\u523a\u6fc0\u5c31\u662f\u4f60\u770b\u5230\u7684\u8fd9\u4e2a\u65b9\u7a0b\u7ec4\u3002\u4e5f\u6b63\u662f\u56e0\u4e3a\u8fd9\u4e2a\u65b9\u7a0b\u7ec4\u5b8c\u7f8e\u7edf\u4e00\u4e86\u6574\u4e2a\u7535\u78c1\u573a\uff0c\u8ba9\u7231\u56e0\u65af\u5766\u59cb\u7ec8\u60f3\u8981\u4ee5\u540c\u6837\u7684\u65b9\u5f0f\u7edf\u4e00\u5f15\u529b\u573a\uff0c\u5e76\u5c06\u5b8f\u89c2\u4e0e\u5fae\u89c2\u7684\u4e24\u79cd\u529b\u653e\u5728\u540c\u4e00\u7ec4\u5f0f\u5b50\u4e2d\uff1a\u5373\u8457\u540d\u7684\u201c\u5927\u4e00\u7edf\u7406\u8bba\u201d\u3002\u7231\u56e0\u65af\u5766\u76f4\u5230\u53bb\u4e16\u90fd\u6ca1\u6709\u8d70\u51fa\u8fd9\u4e2a\u96a7\u9053\uff0c\u800c\u5982\u679c\u4e00\u65e6\u8d70\u51fa\u53bb\uff0c\u6211\u4eec\u5c06\u4f1a\u5728\u96a7\u9053\u53e6\u4e00\u5934\u770b\u5230\u4e0a\u5e1d\u672c\u4eba\u3002<\/p>\n
\u8fd8\u6709\u4e9b\u65b9\u7a0b,\u8b6c\u5982:
\n$\\large\\textbf { \u7231\u56e0\u65af\u5766\u5f15\u529b\u573a\u65b9\u7a0b\uff1a}$
\n\\[G_{\\mu \\nu}=R_{\\mu \\nu}-\\frac{1}{2} g_{\\mu \\nu} R=\\frac{8 \\pi G}{c^{4}} T_{\\mu \\nu}\\]<\/p>\n","protected":false},"excerpt":{"rendered":"
\u82f1\u56fd\u79d1\u5b66\u671f\u520a\u300a\u7269\u7406\u4e16\u754c\u300b\u66fe\u8ba9\u8bfb\u8005\u6295\u7968\u8bc4\u9009\u4e86\u201c\u6700\u4f1f\u5927\u7684\u516c\u5f0f\u201d\uff0c\u6700\u7ec8\u699c\u4e0a\u6709\u540d\u7684\u5341\u4e2a\u516c\u5f0f\u65e2\u6709\u65e0\u4eba\u4e0d\u77e5\u76841+1=2\uff0c\u53c8<\/p>\n