Difference between revisions of "Electromagnetic wave"

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A transverse wave composed of an oscillating electrical field and a magnetic field that oscillates perpendicular to the electric field.<ref>Wile, Dr. Jay L. ''Exploring Creation With Physical Science''. Apologia Educational Ministries, Inc. 1999, 2000</ref>
 
A transverse wave composed of an oscillating electrical field and a magnetic field that oscillates perpendicular to the electric field.<ref>Wile, Dr. Jay L. ''Exploring Creation With Physical Science''. Apologia Educational Ministries, Inc. 1999, 2000</ref>
  
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Electromagnetic waves was predicted by the classical laws of electricity and magnetism, known as Maxwell's equations, which is a system of [[partial differential equations]].
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Electromagnetic waves was predicted 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"
 +
! 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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| 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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|}
 
[[Category:Physics]]
 
[[Category:Physics]]
  
 
== References ==
 
== References ==
 
<references />
 
<references />

Revision as of 02:56, March 31, 2007

A transverse wave composed of an oscillating electrical field and a magnetic field that oscillates perpendicular to the electric field.[1]

Electromagnetic waves was predicted by the classical laws of electricity and magnetism, known as Maxwell's equations:

Name Partial Differential Equations Integral Equations
Gauss's law of Conservation: <math>\nabla \cdot \mathbf{D} = \rho</math> <math>\oint_S \mathbf{D} \cdot \mathrm{d}\mathbf{A} = \int_V \rho\, \mathrm{d}V</math>
Gauss' law Of Magnetism: <math>\nabla \cdot \mathbf{B} = 0</math> <math>\oint_S \mathbf{B} \cdot \mathrm{d}\mathbf{A} = 0</math>
Faraday's Law of Induction: <math>\nabla \times \mathbf{E} = -\frac{\partial \mathbf{B}} {\partial t}</math> <math>\oint_C \mathbf{E} \cdot \mathrm{d}\mathbf{l} = - \int_S \frac{\partial\mathbf{B}}{\partial t} \cdot \mathrm{d} \mathbf{A}</math>
Ampère's Law of Circulation
<math>\nabla \times \mathbf{H} = \mathbf{J} + \frac{\partial \mathbf{D}} {\partial t}</math> <math>\oint_C \mathbf{H} \cdot \mathrm{d}\mathbf{l} = \int_S \mathbf{J} \cdot \mathrm{d} \mathbf{A} +
\int_S \frac{\partial\mathbf{D}}{\partial t} \cdot \mathrm{d} \mathbf{A}</math>

References

  1. ↑ Wile, Dr. Jay L. Exploring Creation With Physical Science. Apologia Educational Ministries, Inc. 1999, 2000