1. Diode Equation and Models
 The general equation linking the diode current I to the applied voltage V is:

2. Diode Equation and Models
Here:
Io is the reverse saturation current.
k is Boltzmann's constant= x JK-1.
T is the working temperature in Kelvin.
e is the magnitude of the electronic charge.
n is called the ideality factor. (n= 1 from theory. From experiments on silicon diodes n= 2 at low current and 1 for large currents).

3. Diode Equation and Models
As an exercise satisfy yourself that this explains the facts discussed in the Semiconductor Diodes section of the module. (The ‘exponential’ term corresponds to majority carrier flow whilst the ‘–1’ term relates to the ‘reverse saturation’ component)
You can now tackle questions 1-4 on Example Sheet1!

4. Diode Equation and Models
By plotting out this equation on a ‘practical scale’ we see that to a good approximation

5. Diode Equation and Models
Diode eqn

6. Diode Equation and Models
An ideal diode would show an abrupt transition from perfectly conducting (diode short circuit) to perfectly non-conducting (diode open circuit) states at 0V I V

7. Diode Equation and Models
It acts as switch since
In the ON state it is a short and in the OFF state it is open circuit I V ON
OFF
Smith/Dorf symbol for ideal diode

8. Diode Equation and Models
An silicon diode approximates this ideal but the transition from conducting to non-conducting circuit states is at around 0.6V because of the barrier potential. This voltage is called the cut-in voltage I V
0.6

9. Diode Equation and Models
Experiment

10. Diode Equation and Models
A closer approximation to the diode I-V equation (experiment) also includes the bulk resistance. This gives the diode’s I-V curve a finite slope above cut-in. I V
0.6

11. Diode Equation and Models
Diodes formed in other materials have different cut-in voltages.
Diodes breakdown for large reverse bias (Breakdown voltage)

12. Diode Equation and Models
We are now in a position to draw some models that represent diode behaviour.
We can use these models instead of the diode equation in circuit analysis
Later on in the Module we will be developing similar models (or equivalent circuits) to represent the behaviour of transistors when they are used as linear amplifiers.

13. Diode Equation and Models
Diode circuit symbol
Anode
Cathode p n

14. Diode Equation and Models
BS3939, IEC symbol (For information only, Smith and Dorf’s symbols will be used in the module)

15. Diode Equation and Models
In forward bias the equivalent circuit is a forward bias drop (Vc ~ 0.6V) in series with a small (forward) resistance. I + - V V
0.6 VC
R f

16. Diode Equation and Models
In many cases Rf can be ignored. I V
0.6
0.6V

17. Diode Equation and Models
In reverse bias (strictly in the ‘off’ state below Vc) the diode can be represented by a very large resistor Rr.
We shall assume Rr. to be infinitely large so that the piecewise linear model for the diode is:

18. Diode Equation and Models
Incremental Diode Model
Another important principle that we will need for transistor analysis is that of the‘incremental modelling’ of a non-linear device.
Basically this assumes the diode I-V curve is linear for small variations in I and V about some operating or bias point. (Also known as the ‘Q’ or quiescent point.)

19. Diode Equation and Models
We introduce important notation used throughout the module. As noted, the (small) a.c. signal sits on top of a d.c. bias level.
Lower-case symbols are used for the time varying signals (i, v).
Upper-case symbols are used for the d.c. bias levels (I, V).

20. Diode Equation and ModelsVQ
I, i
V, v v i t

21. Diode Equation and Models
The diode is biased to operate about a point Q on the I-V curve
The small a.c. signal is superimposed on this bias.
The diode can then be modelled by a resistance equal to the inverse slope of the tangent to the bias point (Linear approximation to diode curve)

22. Diode Equation and Models

23. Diode Equation and Models
We will, in the examples class, use the diode equation to show that, for an ideality factor of 1, the dynamic (small signal) resistance is:

24. Zener Diode
This is simply a diode whose breakdown voltage is controlled to be a specific value.
It finds wide use in limiting and voltage regulator circuits (see diode application section of the module)