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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>
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]].
Electromagnetic waves was predicted by the classical laws of electricity and magnetism, known as Maxwell's equations:
{| class="wikitable" border="1" cellpadding="8" cellspacing="0"
! 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<br />
| <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>
|}
[[Category:Physics]]
[[Category:Physics]]
== References ==
== References ==
<references />
<references />