in forward biasing depletion region width decreases and in reverse biasing it increases .
Because Reverse bias constrained the majority carries to repel from both side (P side & N side)hence Depletion layer is formed with a large extant of majority carriers hence the depletion region is wider in reverse bias.
The capacitance of a varactor diode can be changed by varying the reverse bias voltage applied across it. As the reverse voltage increases, the depletion region widens, which reduces the capacitance. Conversely, decreasing the reverse bias voltage narrows the depletion region, increasing the capacitance. This property allows varactor diodes to be effectively used in tuning applications, such as in voltage-controlled oscillators.
when the diode is applied forward bias voltage the width of depletion region gets reduced the barrier voltage decreases there by facilitating the easy exchange of holes and electrons. when the diode is reverse biased the width of depletion region increases there by hindering the flow or exchange of charge carriers.
For an abrupt junction varactor diode, the device capacitance (C) inversely depends on the applied reverse bias voltage (V). As the reverse bias increases, the depletion region widens, leading to a decrease in capacitance. The relationship can be approximated by the equation ( C \propto V^{-1/2} ), indicating that capacitance decreases as the square root of the increase in reverse bias voltage. Thus, higher reverse bias results in lower device capacitance.
Reverse Bias
Because Reverse bias constrained the majority carries to repel from both side (P side & N side)hence Depletion layer is formed with a large extant of majority carriers hence the depletion region is wider in reverse bias.
any capacitance is given by equation C = (epsilon * A/ d) where d is distance between two plates, thus as d reduces C increases. Now, in depletion region as we increase reverse bias, the depletion region width increases. Now consider depletion region as a parallel plate capacitor, with positive charges on n side and negative charges on p side. Thus, as reverse bias increases, d of junction capacitance increases thus capacitance reduces. On other hand, as reverse bias reduces, d of junction capacitance reduces, thus capacitance increases. -Amey Churi
The capacitance of a varactor diode can be changed by varying the reverse bias voltage applied across it. As the reverse voltage increases, the depletion region widens, which reduces the capacitance. Conversely, decreasing the reverse bias voltage narrows the depletion region, increasing the capacitance. This property allows varactor diodes to be effectively used in tuning applications, such as in voltage-controlled oscillators.
depletion region will decrease.
A depletion region will form at the junction of a p-type and n-type semiconductor in a semiconductor diode. This region is depleted of charge carriers, creating an electric field that prevents further flow of current in the reverse bias direction.
when the diode is applied forward bias voltage the width of depletion region gets reduced the barrier voltage decreases there by facilitating the easy exchange of holes and electrons. when the diode is reverse biased the width of depletion region increases there by hindering the flow or exchange of charge carriers.
For an abrupt junction varactor diode, the device capacitance (C) inversely depends on the applied reverse bias voltage (V). As the reverse bias increases, the depletion region widens, leading to a decrease in capacitance. The relationship can be approximated by the equation ( C \propto V^{-1/2} ), indicating that capacitance decreases as the square root of the increase in reverse bias voltage. Thus, higher reverse bias results in lower device capacitance.
Zener diodes are heavily doped to create a narrow depletion region, allowing them to operate in the reverse breakdown region where they exhibit the Zener effect. This effect causes the diode to conduct in reverse bias at a specific voltage, ideal for voltage regulation applications.
Reverse Bias
Because the bulk charge and surface charge interacting with electric field (forward bias) creates the depletion region.
The depletion layer width at the collector junction is typically wider than that at the emitter junction due to the differences in doping concentrations. The collector region is generally lightly doped compared to the heavily doped emitter region, resulting in a larger electric field and a broader depletion region. Additionally, the collector junction must accommodate a higher reverse bias, which further expands the depletion region to maintain charge neutrality and facilitate efficient charge separation.
Generally, the depletion region thickness is proportional to thehttp://www.answers.com/topic/square-root of the applied voltage; and http://www.answers.com/topic/capacitanceis inversely proportional to the depletion region thickness. Thus, the capacitance is inversely proportional to the square root of applied voltage.