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LECTURE NO. 3
INCREMENTAL MODEL OF A PN JUNCTION DIODE
Fig.1. A dc diode circuit.
V DD = V D + I D .R D _____(1) This describes DC load line.
I D = I D0 exp(V D /V T )_____(2) This is the device characteristics.
Q-point or the quiescent point is the DC operating point and is obtained as the intersection of DC load line and the device characteristics.
Figure 2. The dc load line , the device characteristics and the Q point.
Tan(α)= slope of the load line= (-1/R D )
Under signal conditions:
Figure 3. Signal is being coupled with the diode circuit.
i D = I D + i d where i D is the instantaneous diode current.
I D is the DC diode current.
i d is the incremental diode current.
And v D (instantaneous diode voltage) = V D (DC Diode Voltage) + v d _(incremental diode voltage)
Now the loop or the mesh equation is:-
(V DD +v s )=v D +i D R D _______(3)
Rewriting the above equation we get:-
(V DD +v s )= (V D + v d )+( I D + i d ) R D _____(4)
Now we have (Instantaneous – DC) = Incremental part,
that is Eq.(4)-Eq.(1) :
v s = v d + i d R D = v d + v o ;
Incremental circuit will be:-
Figure 4. The incremental circuit of the Diode Circuit with signal.
A diode under instantaneous conditions has two parts :-
The above is a relation between the diode current and the diode voltage.
We know that
e Ɵ = 1+Ɵ+(Ɵ 2 /2!)+ (Ɵ 3 /3!)+………….
If Ɵ<<1; e Ɵ = 1+Ɵ This now becomes a linear equation.
If incremental voltage across the diode is less than 5 mV then Ɵ<<1.
To maintain linearity, we maintain all the signals small.
So under small signal approximations,
e Ɵ = 1+Ɵ will hold good.
Now we note that V T =26mV and the room temperature=300K and if V d <5 mV then we satisfy the small signal condition and we obtain:
Then we have;
Thus;
Let:
Putting V T =26mV and I D =1mA we get r d =26Ω.
Thus the incremental part of the diode circuit was determined as follows:
Incremental resistance r d = (Thermal Resistance V T / Quiescent Current through the diode)
This is small signal approximation. Thus Diode equivalent circuit is composed of linear elements only under small signal condition. Hence the circuit in Figure 4 is incremental circuit or small signal equivalent circuit. The incremental resistance r d offered by the diode under small signal condition is a linear resistance and is included in the circuit only under incremental condition.
Table 1. Values of incremental resistance at 300K offered by a diode under various DC diode currents.
I D (mA) | r d (ohms)=V T /I D at Room Temerature(300K |
1µA | 26 kohms |
10µA | 2.6 kohms |
100µA | 260 ohms |
1 mA | 26 ohms |
10mA | 2.6ohms |
100mA | 0.26 ohms. |
Amplitude or Harmonic Distortion.
As can be seen from Figure 3, input sinusoidal voltage v S appears as addition and subtraction to V DD . Hence under signal condition, the load line is being shifted as shown in Figure 5. In doing so Q pint also shifts generating sinusoidal current swing. As can be seen in the figure, a small segment of I-V curve of the diode(which is the case under small signal condition) is essentially a straight line. Hence Q moves along a straight segment and in the process generates a sinusoidal swing in the current.
Figure 5. Diode Current Sinusoidal Swing under Sinusoidal Input Voltage under small signal condition.
But as seen in Figure 6, if input voltage is a large signal then Q traces a non-linear segment of I-V curve. This results in non-sinusoidal current swing in the diode. This means a sinusoidal voltage is not giving rise to a sinusoidal current in the output load resistance R L . Hence the output voltage will be non-sinusoidal and its Fourier Series Expansion will contain Fundamental and Harmonics. This is known as Amplitude or Harmonic Distortion.
Figure 6. Non-sinusoidal diode current swing when input voltage is a large voltage.
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