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Content Maxwell's Equations with No Charges
Maxwell's Equations with No ChargesIn the absence of sources, charges, currentGauss's Law:
Wave EquationsOnce a wave starts, Both Faraday and Ampere equations keep going. Feed one equation into the other:
In other words, both 𝐸 and 𝐵 are waving.Solution of Wave EquationLet 𝐸 be wave of the form:𝐸=𝐸0 𝑧 ∂2∂𝑥2+ ∂2∂𝑦2+ ∂2∂𝑧2 ∂2∂𝑥2 𝑧 1𝑐2 ∂2∂𝑡2 𝐸= −𝜔2𝑐2𝐸0 𝑧 If 𝜔=𝑐𝑘 then left and right terms are the same. And 𝐸=𝐸0 𝑧is the wave solution of 𝐸. For the differential form of Faraday's law, ∇× 𝐸=− ∂, let 𝐸 be wave of the form: 𝐸=𝐸0 𝑧, then ∇× 𝐸= = 𝑦≡− ∂ → 𝑘𝜔 𝑦= 𝐸0𝑐 𝑦 Self-sustaining wave that can go on forever. 𝐸 and 𝐵 are perpendicular to each other, and to the direction of propagation: 𝑣∥ 𝐸× 𝐵where the magnitude of 𝑣 is 𝑐. Electromagnetic SpectrumGamma rays--X rays--Light(Ultra-Violet--Visible light--Infra-Red)--MicroWave--Radio(TV--FM--Amateur band--AM--Long Wave)Accelerated Charges![]() Transverse pulse propagates at speed of light. Since 𝐸(t), there must be 𝐵. Direction of 𝑣 is therefore given by: 𝐸× 𝐵 ![]() Field∼−𝑞 𝑎⟂ 𝐸radiative= 14𝜋𝜀0 𝑎⟂𝑐2𝑟 The direction of the transverse field is opposite to 𝑞 𝑎⟂. The electric field falls off at a rate 1/𝑟. Why is the Sky BlueOn the Moon, the sky looks black. Gas molecules scatter blue/violet light more than red light. Sky is blue for the same reason, the sunset is red.Source and Referencehttps://www.youtube.com/watch?v=jbHgG1iHoY0&list=PLZ6kagz8q0bvxaUKCe2RRvU_h7wtNNxxi&index=27©sideway ID: 200200802 Last Updated: 2/8/2020 Revision: 0 Latest Updated Links
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