User:John R. Brews/CZ psychology authors: Difference between revisions
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==Operation== | ==Operation== | ||
The figure shows a JFET with an ''n-''type body and a ''p-''type gate region. For a discussion of dopant impurities and the terminology ''p-'' and ''n-''type. see [[Semiconductor#Dopant_impurities|dopant impurities]]. | The figure shows a JFET with an ''n-''type body and a ''p-''type gate region. For a discussion of dopant impurities and the terminology ''p-'' and ''n-''type. see [[Semiconductor#Dopant_impurities|dopant impurities]]. | ||
The dark-colored portion of the body is conducting, due to the electrons in this region, and is called the ''channel''. The light-colored portion of the body is depleted of electrons and is not electrically conducting. | |||
The n-type body in the figure conducts electricity when a voltage drop is applied between source and drain. The amount of current depends, among other things, upon the cross-section of the device that is conducting. This cross section is controlled by the gate, which makes ohmic contact to a p-type region. If the gate-source [[pn diode|pn-junction]] is reverse biased by applying a negative voltage to the gate and holding the source at ground, the depletion region within the pn-junction widens, restricting the cross section of the conducting channel. | The n-type body in the figure conducts electricity when a voltage drop is applied between source and drain. The amount of current depends, among other things, upon the cross-section of the device that is conducting. This cross section is controlled by the gate, which makes ohmic contact to a p-type region. If the gate-source [[pn diode|pn-junction]] is reverse biased by applying a negative voltage to the gate and holding the source at ground, the depletion region within the pn-junction widens, restricting the cross section of the conducting channel. | ||
The insulating portion of the body varies in width from source to drain because the current through the body causes a voltage drop as suggested by [[Ohm's law]] that varies with distance and increases the amount of reverse bias between the gate and body as a function of distance down the channel. | The insulating portion of the body varies in width from source to drain because the current through the body causes a voltage drop as suggested by [[Ohm's law]] that varies with distance and increases the amount of reverse bias between the gate and body as a function of distance down the channel. | ||
Revision as of 12:24, 26 March 2012
A junction field-effect transistor or JFET is a three-terminal device that conducts a current that can be controlled by an applied voltage. It is made of two semiconductor layers.
Operation
The figure shows a JFET with an n-type body and a p-type gate region. For a discussion of dopant impurities and the terminology p- and n-type. see dopant impurities.
The dark-colored portion of the body is conducting, due to the electrons in this region, and is called the channel. The light-colored portion of the body is depleted of electrons and is not electrically conducting.
The n-type body in the figure conducts electricity when a voltage drop is applied between source and drain. The amount of current depends, among other things, upon the cross-section of the device that is conducting. This cross section is controlled by the gate, which makes ohmic contact to a p-type region. If the gate-source pn-junction is reverse biased by applying a negative voltage to the gate and holding the source at ground, the depletion region within the pn-junction widens, restricting the cross section of the conducting channel.
The insulating portion of the body varies in width from source to drain because the current through the body causes a voltage drop as suggested by Ohm's law that varies with distance and increases the amount of reverse bias between the gate and body as a function of distance down the channel.