In the context of diodes, dynamic resistance refers to the incremental or small-signal resistance exhibited by a diode when it is operating in its forward-biased region. Diodes are semiconductor devices that allow current to flow in one direction only, from the anode to the cathode, when a forward voltage is applied across them. When a diode is forward-biased (i.e., the anode voltage is greater than the cathode voltage), it allows a significant current to flow through it.
However, the relationship between the voltage and current in a diode is nonlinear. The diode follows the exponential Shockley diode equation:
=
(
−
1
)
I
D
=I
s
(e
nV
T
V
D
−1)
where:
I
D
is the diode current.
I
s
is the reverse saturation current (a small current that flows in reverse bias).
V
D
is the voltage across the diode (anode voltage minus cathode voltage).
n is the ideality factor, typically a value between 1 and 2.
V
T
is the thermal voltage, approximately 25 mV at room temperature (300 K).
Since the diode equation is exponential, the current-voltage (I-V) curve of the diode is very steep. In practical applications, we often need to analyze the behavior of diodes for small variations around an operating point, which is called small-signal analysis. This analysis is crucial in designing electronic circuits, especially those using diodes in amplifiers, oscillators, and other applications.
To simplify the analysis, we can approximate the exponential I-V curve of the diode to a linear relationship by considering the dynamic resistance. The dynamic resistance, denoted as
r
d
, is defined as the incremental change in voltage divided by the incremental change in current at a given operating point of the diode.
=
Δ
Δ
r
d
=
ΔI
D
ΔV
D
For small variations in voltage and current (
Δ
ΔV
D
and
Δ
ΔI
D
), the diode can be approximated as a resistor with resistance
r
d
around the operating point. This dynamic resistance is also sometimes called "differential resistance" since it represents the resistance at a particular point on the diode's I-V curve.
The use of dynamic resistance in small-signal analysis allows us to replace the diode with an equivalent linear circuit around the operating point, making it easier to perform calculations and design circuits using diodes. This approximation holds as long as the variations in voltage and current are small enough not to significantly deviate from the operating point.
It's important to note that dynamic resistance is just an approximation for small-signal analysis and does not accurately represent the diode's behavior for large signal variations or in reverse-biased regions. For precise and accurate modeling of diodes in more complex circuits, the full nonlinear diode equation must be used. However, dynamic resistance provides a valuable tool for quick and simplified analysis in small-signal circuits.