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| | The spectrum of electromagnetic waves has an extremely wide range from radio waves, micro waves, TeraHertz radiation, infrared (IR) radiation, visible light, ultraviolett (UV) light, far UV radiation, soft X-rays, hard X-rays and <math>\gamma</math>-radiation. | | The spectrum of electromagnetic waves has an extremely wide range from radio waves, micro waves, TeraHertz radiation, infrared (IR) radiation, visible light, ultraviolett (UV) light, far UV radiation, soft X-rays, hard X-rays and <math>\gamma</math>-radiation. |
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| − | Electromagnetic waves are well described by the classical laws of electricity and magnetism, known as Maxwell's equations: | + | Electromagnetic waves are well described by the classical laws of electricity and magnetism, known as [[Maxwell's equations]]. |
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| − | {| class="wikitable" border="1" cellpadding="8" cellspacing="0"
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| − | ! Name
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| − | ! [[Partial Differential Equations]]
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| − | ! [[Integral Equations]]
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| − | |-
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| − | | Gauss's Law of Conservation:
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| − | | <math>\nabla \cdot \mathbf{D} = \rho</math>
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| − | | <math>\oint_S \mathbf{D} \cdot \mathrm{d}\mathbf{A} = \int_V \rho\, \mathrm{d}V</math>
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| − | |-
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| − | | Gauss' Law Of Magnetism:
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| − | | <math>\nabla \cdot \mathbf{B} = 0</math>
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| − | | <math>\oint_S \mathbf{B} \cdot \mathrm{d}\mathbf{A} = 0</math>
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| − | |-
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| − | | Faraday's Law of Induction:
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| − | | <math>\nabla \times \mathbf{E} = -\frac{\partial \mathbf{B}} {\partial t}</math>
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| − | | <math>\oint_C \mathbf{E} \cdot \mathrm{d}\mathbf{l} = - \int_S \frac{\partial\mathbf{B}}{\partial t} \cdot \mathrm{d} \mathbf{A}</math>
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| − | |-
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| − | | Ampère's Law of Circulation<br />
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| − | | <math>\nabla \times \mathbf{H} = \mathbf{J} + \frac{\partial \mathbf{D}} {\partial t}</math>
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| − | | <math>\oint_C \mathbf{H} \cdot \mathrm{d}\mathbf{l} = \int_S \mathbf{J} \cdot \mathrm{d} \mathbf{A} +
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| − | \int_S \frac{\partial\mathbf{D}}{\partial t} \cdot \mathrm{d} \mathbf{A}</math>
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| − | |}
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| − | where '''B''' denotes the [[magnetic field]], '''E''' denotes the [[electric field]], '''H''' denotes the auxiliary magnetic field, '''J''' denotes the free [[current density]], and <math>\rho</math> denotes the free [[electric charge density]].
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| − | In the language of [[Exterior Calculus]], Maxwell's equations can be rewritten much more compactly as:
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| − | :<math>\mathrm{d}\bold{F}=0</math>
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| − | :<math>\mathrm{d} * {\bold{F}}=\bold{J}</math>
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| − | where '''d''' is [[exterior derivative]] operator, '''*''' is the [[Hodge star]] operator, and '''F''' is the force exerted upon a charged particle by the electric field and magnetic field.
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| | [[Category:Physics]] | | [[Category:Physics]] |