DC bias current and small-signal resistance

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SUMMARY

The discussion centers on calculating the DC bias current and small-signal resistance using the diode equation, specifically ##i_D = 8\cdot 10^{-12} (e^{v_D/20m} - 1)##. The user attempts to derive small-signal parameters but encounters discrepancies in the results, particularly with the calculated current I_D. The suggestion is made to manipulate the diode equation to express V_D as a function of I_D and differentiate to obtain the impedance. Additionally, significant figures in the I_S value are highlighted as a potential source of error.

PREREQUISITES
  • Understanding of the diode equation and its parameters
  • Familiarity with small-signal analysis in electronic circuits
  • Knowledge of differentiation in the context of electrical engineering
  • Basic principles of significant figures in calculations
NEXT STEPS
  • Manipulate the diode equation to express V_D as a function of I_D
  • Learn about differentiating current-voltage relationships to find impedance
  • Review significant figures and their impact on electronic calculations
  • Explore small-signal resistance calculations in semiconductor devices
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Electrical engineers, students studying semiconductor physics, and anyone involved in circuit design and analysis, particularly in understanding diode behavior and small-signal modeling.

JessicaHelena
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Homework Statement
Consider the diode D_1 shown in Fig 7-1.

The diode is a non-linear device with the following I-V characteristics:

##i_D = I_S \cdot (e^{\frac{v_D}{v_{TH}} - 1)##

where i_D is the current through the diode, I_S is the reverse bias saturation current, v_D is the voltage across the diode, and V_TH is the thermal voltage. Assume ##I_S = 8*10^{-12}## and ##V_{TH} = 20mV##.

Although the diode is a non-linear device, it can be modeled as a resistor for small signals. Calculate the numerical value of the DC bias current I_D in mA such that its small-signal resistance is 5 Ohms.
Relevant Equations
iD = ID + id
(i.e., total variable iD = DC output ID + small signal id)

also,
##I_D + \delta i_D \approx## (iD evaluated at v_D) + (derivative of iD evaluated at v_D)*##\delta v_D##
##I_D = ## (iD evaluated at v_D)
##\delta i_D = ## (derivative of iD evaluated at v_D) *##\delta v_D##
We are given that ##i_D = 8\cdot 10^{-12} (e^{v_D/20m} - 1)##

Hence ##i_D' = e^{50 v_D}/2500000000## and ##i_D'' = e^{50 v_D}/50000000##

Then I have that ##\delta i_D \approx\frac{ e^{50 v_D}}{2500000000} \cdot \delta v_D = \delta v_D / 5## Cancelling ##\delta v_D## from boh sides and solving for the v_D, I have that ##v_D = 0.400602##.

Plugging this value into the original function for iD, I can get I_D, which gives me 0.004. However, this is not right. What am I doing wrong?
 

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I didn't go through your calculation in detail, but I'd be inclined to manipulate the diode equation to get Vd as a function of Id, and differentiate to get the impedance, then substitute in the point Id = 20mA...

Z(Vd) = \frac{dVd}{dId}
 
Or just differentiate the ##I_D## function w.r.t. ##V_D##. Conductance is the reciprocal of resistance.
 
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@JessicaHelena : is it possible that you're running into significant figures issues when entering your results? It looks like your ##I_S## value is only specified to one sig fig.

Edit: I ask because I've run the calculations and come up with results that match yours. So I have to wonder where the underlying issue lies.
 
Last edited:

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