How Do You Calculate Resistance in a Diode Circuit for Specific Voltage Changes?

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Discussion Overview

The discussion revolves around calculating the resistance in a diode circuit to achieve a specific output voltage change in response to varying load current. Participants explore the small-signal model of the diode, the relationship between diode current and resistance, and the implications of these calculations for circuit design.

Discussion Character

  • Homework-related
  • Technical explanation
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • One participant expresses confusion about how to find the resistance R using the small-signal model, noting an initial calculation for diode current based on voltage differences.
  • Another participant suggests determining the diode voltage required for the output to be at 3 V under no load and proposes writing a nodal equation to relate the output voltage change to load current.
  • There is a discussion about the expected diode voltage drop, with one participant asserting it should be 0.75 V for each diode in series.
  • Participants clarify that the small signal model suppresses the DC source and focuses on the load current as the varying signal, leading to a nodal equation involving the resistances and load current.
  • One participant derives an expression for the output voltage change per load current change and substitutes values to find the resistance R, arriving at approximately 2.42 kΩ.
  • Concerns are raised about the negative sign in the derived expression for voltage change per load current change, with participants reflecting on the implications of output voltage decreasing as load current increases.
  • Another participant calculates the saturation current for the diodes based on the derived resistance and voltage drop.

Areas of Agreement / Disagreement

Participants generally agree on the approach to use the small-signal model and the calculations involved, but there is some uncertainty regarding the implications of the negative sign in the voltage change expression and the direction of voltage change with respect to load current.

Contextual Notes

Participants note that the small signal model does not include the DC operating point condition and that the load current serves as the varying signal in the analysis. There is also discussion about the assumptions made regarding diode behavior and the saturation current calculations.

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Homework Statement



Design the circuit in the following figure so that ##V_o = 3V## when ##I_L = 0## and ##V_o## changes by ##20mV## per ##1mA## of load current.

(a) Use the small-signal model of the diode to find the value of ##R##.
(b) Specify the value of ##I_S## (saturation current) of each of the diodes.

Screen Shot 2015-02-07 at 9.55.16 PM.png


Homework Equations

The Attempt at a Solution



I don't understand how part (a) is to be accomplished. Assuming a diode current ##I_D## flows from top to bottom, the current can be found from:

$$I_D = \frac{15V - 3V}{R}$$

The small signal resistance is given by:

$$r_d = \frac{V_T}{I_D}$$

The answer is listed as ##2.4k##, but I am unsure how to proceed.
 
Last edited:
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Okay, so you have an expression relating the operating point current ##I_D## and the resistance R. You should also be able to determine what the diode voltage ##V_D## has to be in order for the output to be at 3 V under no load. (It looks pretty high for a silicon diode that must be passing a fairly modest current, so we can anticipate that the diode saturation current is going to be pretty darn small).

Next I think you'll want to turn to the small signal model. Maybe write a nodal equation at the Vout node. The voltage there will be the Δv that results from a load current Δi. See if you can't arrange the equation to equate Δv/Δi to something involving the unknown resistances ##r_d## and R since you're given some information about what you want Δv/Δi to be. Your expression for ##r_d## in your post will let you bridge these results back to the large signal stuff by getting rid of ##r_d## using ##V_T/I_D##.

See where that takes you.
 
If I wanted ##V_o = 3V##, would I not say ##V_D = 0.75V## for each diode in series?

The small signal model consists of a source ##v_s## in series with the resistor ##R## and the small signal resistance ##r_d## (the series combination of the diodes). I don't think I can write a node equation for this series circuit, did you mean a voltage divider?
 
Zondrina said:
If I wanted ##V_o = 3V##, would I not say ##V_D = 0.75V## for each diode in series?
Yup.
The small signal model consists of a source ##v_s## in series with the resistor ##R## and the small signal resistance ##r_d## (the series combination of the diodes). I don't think I can write a node equation for this series circuit, did you mean a voltage divider?
The only source in the small signal model will be the load current. The 15 V DC source is suppressed, and it never had an AC signal component.
 
gneill said:
Yup.

The only source in the small signal model will be the load current. The 15 V DC source is suppressed, and it never had an AC signal component.

Ah, short circuit the voltage and open circuit the current, sorry it's pretty early. So the DC analysis has already been done.

The small signal model has a resistor ##R## in series with ##r_d## and a common ground.

Since ##I_L = 0##, the voltage at the node above ##r_d## is ##V_o = 3V##. Does that mean the current across ##r_d## is ##i_d = \frac{V_o}{r_d}##?

I'm still a bit lost, i'll try after getting some sleep.
 
In the small signal model the Vo = 3 V disappears. That's a DC operating point condition and doesn't enter into the small signal model. The load current is of interest in the small signal model though, it is the "signal" in the small signal model. So what you're left with is the resistance R, the diode small signal resistances rd, and a load current as the signal. I know it seems strange to have the load as a signal, but it's what is varying according to the problem. Here's what we're looking at:

Fig1.gif
 
gneill said:
In the small signal model the Vo = 3 V disappears. That's a DC operating point condition and doesn't enter into the small signal model. The load current is of interest in the small signal model though, it is the "signal" in the small signal model. So what you're left with is the resistance R, the diode small signal resistances rd, and a load current as the signal. I know it seems strange to have the load as a signal, but it's what is varying according to the problem. Here's what we're looking at:

View attachment 78753

I thought about replacing the diodes with ##4 r_d## in the model before I slept, but I didn't know if it had any merit. So it turns out the load current IS the signal in the small signal model.

So writing a nodal equation at the only node in the circuit:

$$I_R - I_{r_d} - \Delta i = 0 \Rightarrow \frac{0 - \Delta v}{R} - \frac{\Delta v - 0}{4 r_d} = \Delta i \Rightarrow - \frac{\Delta v}{R} - \frac{\Delta v}{4 r_d} = \Delta i$$

So we can conlcude:

$$\Delta v \left[- \frac{1}{R} - \frac{1}{4 r_d} \right] = \Delta i \Rightarrow \frac{\Delta v}{\Delta i} = - \frac{1}{\left[ \frac{1}{R} + \frac{1}{4 r_d} \right]} \Rightarrow \frac{\Delta v}{\Delta i} = - \frac{4 R r_d}{R + 4r_d}$$

Substituting in for ##r_d = \frac{V_T}{I_D} = \frac{V_T}{\frac{12 V}{R}} = \frac{(25 \times 10^{-3} V)R}{12 V} = 0.002083 R##:

$$\frac{\Delta v}{\Delta i} = - \frac{4 R (0.002083 R)}{R + 4(0.002083 R)} = - 0.00826315 R$$

So we know ##\frac{\Delta v}{\Delta i} = \frac{20 mV}{1 mA} = 20 \Omega##, hence:

$$R = \frac{20 \Omega}{0.00826315} = 2420.4 \Omega = 2.42 k \Omega$$

The only thing bothering me at this point is why there's a negative sign, which I had to ignore (since ##|R| \geq 0##). Is this relevant?

Sleeeep <3

EDIT: I forgot to mention the saturation current:

$$I_S = \frac{I_D}{e^{\frac{V_D}{V_T}}} = \frac{\frac{12 V}{2.42 \times 10^3 \Omega}}{e^{\frac{0.75 V}{25 \times 10^{-3} V}}} = 4.64 \times 10^{-16} A$$
 
Last edited:
Well done! Just a little niggle:

Zondrina said:
The only thing bothering me at this point is why there's a negative sign, which I had to ignore (since |R|≥0|R| \geq 0). Is this relevant?


Do a little thinking about Δv/Δvi. The problem statement says that Vout changes by 20 mV per 1 mA of load current. It doesn't say it which direction it changes. Reflect on what should happen to Vout as the load draws more current.
 
gneill said:
Well done! Just a little niggle:

Do a little thinking about Δv/Δvi. The problem statement says that Vout changes by 20 mV per 1 mA of load current. It doesn't say it which direction it changes. Reflect on what should happen to Vout as the load draws more current.

Ah I see, so as the load current ##I_L## increases by ##1mA## at a time, the output voltage ##V_o## is going to decrease. Hence why the negative sign was there.
 
  • #10
Zondrina said:
Ah I see, so as the load current ILI_L increases by 1mA1mA at a time, the output voltage VoV_o is going to decrease. Hence why the negative sign was there.
Yes indeed!
 

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