Charge Motion in Metals: Difference between revisions

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==References==
==References==
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/conins.html#c1
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/conins.html#c1
http://physics.bu.edu/~okctsui/PY543/1_notes_Drude_2013.pdf




[[Category:Fields]]
[[Category:Fields]]

Revision as of 18:33, 4 December 2015

Written by Will Rountree

Mobile Electron Sea

Metals, like all matter, are made of atoms. These atoms consist of a nucleus surrounded by electrons. The majority of metals have few electrons in the outer orbitals, and these valence electrons aren't tightly bound to the nucleus. As a result they are "free" and able to move through the material. The electrons aren't shared or transferred between atoms; they are available to all nuclei in the metal. Often there is only one free electron per atom, but that is all it takes to create a "sea" of electrons surrounding the atoms. Due to every atom lacking a negatively charged electron, the atoms are positively charged and remain bound together by the "sea." There is an even distribution of positive and negative charges, so the net electric field inside of metal is zero.

Charge Motion

Electrons naturally repel each other. When an electric field is applied to a metal, the mobile electrons begin to experience a force and accelerate. The electron continues to accelerate until it collides with another electron in the mobile electron sea. This process continues to propagate throughout the metal for as long as an external field is applied to the metal.

Examples

Simple

Middling

Difficult

Connectedness

History

This model for the motion of electrons in metal is credited to physicist Paul Drude, who first proposed the model in 1900. Subsequently called the Drude Model, this theory

See also

Further reading

External links

References

http://hyperphysics.phy-astr.gsu.edu/hbase/electric/conins.html#c1 http://physics.bu.edu/~okctsui/PY543/1_notes_Drude_2013.pdf