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Current Flow ECE 2204.

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Presentation on theme: "Current Flow ECE 2204."— Presentation transcript:

1 Current Flow ECE 2204

2 n+-n and p+-p Junctions
In the previous set of slides on diffusion currents, we showed that a diffusion current flowed when an n+ layer was in contact with an n layer But, current can’t flow continuously without some source of energy Violation of the conservation of energy and momentum

3 Continuity of Fermi Energies
The slope in the conduction band energy and the valence band energy indicate that an electric field has been induced at the n+-n junction as the electrons

4 Induced Electric Field
There are charged donors, ND+, left behind in the n+ region as electrons diffuse into the n region. Another source of positive charge in the n+ region is a result of the diffusion of holes from the n region into the n+ region There is an increase in negative charges in the n region because of the inflow of electrons from the n+ region and the loss of holes as the holes move into the n+ region. Seen as the sloped region between the n+ and n regions The electric field causes a drift current in the opposite direction that counters the diffusion current.

5 Total Carrier Flow diffusion drift e e e e e e e e e e
e e e e e e e e e e e e h h h h h h h h h h drift diffusion Drift currents flows because of the electric field that balance the diffusion currents

6 Total Current Flow is the sum of the drift and diffusion currents
J is the current density or current I divided by the cross-sectional area A through which the carriers move.

7 When no voltage is applied

8 A more subtle balance All electron flow must sum to zero and all hole flow must sum to zero.

9 p+-p junction You should be able to determine the direction of carrier flow and determine whether the currents are diffusion or drift.


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