written 7.8 years ago by | • modified 7.8 years ago |
Mumbai University > Electronics ana telecommunication engineering > Sem 3 > Analog electronics 1
Marks: 4M
Years: Dec 2014, May 2016
written 7.8 years ago by | • modified 7.8 years ago |
Mumbai University > Electronics ana telecommunication engineering > Sem 3 > Analog electronics 1
Marks: 4M
Years: Dec 2014, May 2016
written 7.8 years ago by |
The diode current depends on the voltage applied to it. The relationship between applied voltage V and the diode current I is exponential and is mathematically given by the equation called diode current equation. It is expressed as,
I = $I_0 (e^\frac{V}{(ηV_T )} -1) A$
Where $I_0$ = Reverse saturation current in amperes
V = Applied voltage
η = 1 for germanium diode
= 2 for silicon diode
$V_T$ = Voltage equivalent of temperature in volts
The voltage equivalent of temperature indicates dependence of diode current on temperature. The voltage equivalent of temperature $V_T$ for a given diode at temperature T is calculated as,
$V_T$ = kT volts
Where k = Boltzmann's constant = $8.62 x10^(-5) eV/° K$
T = Temperature in °K.
Thus at room temperature of 27 °C i.e. T = 27 + 273 = 300 ° K the value of $V_T$ is,
$V_T= 8.62 x 10^(-5) x 300 $= 0.02586 V = 26 mV
The value of V_T also can be expressed as,
$V_T= \frac{T}{\frac{1}{K}}= \frac{T}{\frac{1}{8.62x10^(-5)}}= \frac{T}{11600}$
Thus at room temperature of T = 300 ° K, we get $V_T$ = 26 mV.
The diode current equation is applicable for all the conditions of diode i.e. unbiased, forward biased and reverse biased.
When unbiased, V = 0 hence we get,
$I = I_0 (e^0 -1) A = 0 A$
Thus there is no current through diode when unbiased.