. . . . . . . . . . . . . . . . . . . . . . . "\u975E\u9F50\u6B21\u7684\u7535\u78C1\u6CE2\u65B9\u7A0B"@zh . . . . . . . . . . . . . . "\u5C40\u57DF\u5316\u7684\u6642\u8B8A\u7535\u8377\u548C\u7535\u6D41\u5BC6\u5EA6\u5728\u771F\u7A7A\u4E2D\u662F\u7535\u78C1\u6CE2\u7684\u6E90\u3002\u5728\u6709\u6E90\u7684\u60C5\u5F62\u4E0B\uFF0C\u9EA6\u514B\u65AF\u97E6\u65B9\u7A0B\u7EC4\u53EF\u4EE5\u5199\u6210\u4E00\u4E2A\u975E\u9F50\u6B21\u7684\u7535\u78C1\u6CE2\u65B9\u7A0B\uFF08\u82F1\u6587\uFF1AInhomogeneous electromagnetic wave equation\uFF09\u7684\u5F62\u5F0F\uFF0C\u6B63\u662F\u56E0\u4E3A\u6CE2\u6E90\u7684\u5B58\u5728\u4F7F\u5F97\u504F\u5FAE\u5206\u65B9\u7A0B\u53D8\u4E3A\u975E\u9F50\u6B21\u3002"@zh . . . . "4603613"^^ . "In electromagnetism and applications, an inhomogeneous electromagnetic wave equation, or nonhomogeneous electromagnetic wave equation, is one of a set of wave equations describing the propagation of electromagnetic waves generated by nonzero source charges and currents. The source terms in the wave equations make the partial differential equations inhomogeneous, if the source terms are zero the equations reduce to the homogeneous electromagnetic wave equations. The equations follow from Maxwell's equations."@en . . "Inhomogeneous electromagnetic wave equation"@en . . . "\u5C40\u57DF\u5316\u7684\u6642\u8B8A\u7535\u8377\u548C\u7535\u6D41\u5BC6\u5EA6\u5728\u771F\u7A7A\u4E2D\u662F\u7535\u78C1\u6CE2\u7684\u6E90\u3002\u5728\u6709\u6E90\u7684\u60C5\u5F62\u4E0B\uFF0C\u9EA6\u514B\u65AF\u97E6\u65B9\u7A0B\u7EC4\u53EF\u4EE5\u5199\u6210\u4E00\u4E2A\u975E\u9F50\u6B21\u7684\u7535\u78C1\u6CE2\u65B9\u7A0B\uFF08\u82F1\u6587\uFF1AInhomogeneous electromagnetic wave equation\uFF09\u7684\u5F62\u5F0F\uFF0C\u6B63\u662F\u56E0\u4E3A\u6CE2\u6E90\u7684\u5B58\u5728\u4F7F\u5F97\u504F\u5FAE\u5206\u65B9\u7A0B\u53D8\u4E3A\u975E\u9F50\u6B21\u3002"@zh . . . . . . . . . . . . "In electromagnetism and applications, an inhomogeneous electromagnetic wave equation, or nonhomogeneous electromagnetic wave equation, is one of a set of wave equations describing the propagation of electromagnetic waves generated by nonzero source charges and currents. The source terms in the wave equations make the partial differential equations inhomogeneous, if the source terms are zero the equations reduce to the homogeneous electromagnetic wave equations. The equations follow from Maxwell's equations."@en . . . . . . . . . . . . . . . . . . . . . . . "13610"^^ . . . . . . . "1117574382"^^ . . . . . . . . . . . . . .