Semiconductor & Computer Engineering
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| − | '''Diffusion current''' is [[current]] which occurs in response to [[concentration gradient]]. That is diffusion current is the movement of [[charge carriers]] as a result of [[entropy]] ensuring that carriers move from a region of high concentration into regions of low concentration. This is in contrast to [[drift current]] which is a result of an applied electric field. | + | '''Diffusion current''' is [[current]] which occurs in response to [[concentration gradient]]. That is, diffusion current is the movement of [[charge carriers]] as a result of [[entropy]] ensuring that carriers move from a region of high concentration into regions of low concentration. This is in contrast to [[drift current]] which is a result of an applied electric field. |
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| + | == Overview == | ||
| + | In a given material where particles are uniformly distributed within the lattice, [[charge carriers]] will roam around randomly due to thermal velocity of the material. However, due to the random collisions the net current will result in a net current of zero as the carriers do not really go anywhere. | ||
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| + | :[[File:diffusion current - uniform.svg|500px]] | ||
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| + | In a material where particles are not entirely uniformly distributed, [[entropy]] will ensure that carriers in region of high concentration will move to regions of low concentration. The '''diffusion current''' is therefore the movement of those [[charge carriers]] as they diffuse. | ||
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| + | :[[File:diffusion current - high con.svg|500px]] | ||
Revision as of 17:12, 23 November 2017
Diffusion current is current which occurs in response to concentration gradient. That is, diffusion current is the movement of charge carriers as a result of entropy ensuring that carriers move from a region of high concentration into regions of low concentration. This is in contrast to drift current which is a result of an applied electric field.
Overview
In a given material where particles are uniformly distributed within the lattice, charge carriers will roam around randomly due to thermal velocity of the material. However, due to the random collisions the net current will result in a net current of zero as the carriers do not really go anywhere.
In a material where particles are not entirely uniformly distributed, entropy will ensure that carriers in region of high concentration will move to regions of low concentration. The diffusion current is therefore the movement of those charge carriers as they diffuse.
