Analyzing the Setup
Welcome to this fascinating problem on semiconductor diodes! We are given the V−I characteristics of a forward-biased diode.
Our primary objective is to find its dynamic resistance at a specific operating current, which is ID=3 mA.
Unlike a simple ohmic resistor, a diode is a non-linear device. This means its resistance is not constant; it changes depending on the voltage applied across it.
The Master Equation
So, what exactly is dynamic resistance? It is defined as the inverse of the slope of the V−I curve at a specific operating point.
Mathematically, it represents the ratio of a small change in voltage to the corresponding small change in current. We can write this as:
To find this slope, we don't look at the curve itself, but rather at the tangent line drawn at our operating point of 3 mA.
Extracting Data from the Graph
We need to pick two easy-to-read points on this tangent line to calculate ΔV and ΔI.
If we look closely at the grid in the provided graph, the tangent line crosses exactly at a current of 1 mA when the voltage is 0.65 V.
Similarly, it crosses a current of 5 mA when the voltage is 0.75 V.
These two points, (0.65 V,1 mA) and (0.75 V,5 mA), are perfect for our calculation because they lie exactly on the grid intersections.
Substituting the Values
Now, let's substitute these extracted values into our dynamic resistance formula.
The change in voltage, ΔV, is simply the difference between the two voltage readings: 0.75−0.65 V.
The change in current, ΔI, is the difference between the two current readings: 5−1 mA.
Crucial Step: We must remember to convert milliamperes to standard SI unit amperes by multiplying by 10−3.
Final Calculation
Let's simplify the numerator and the denominator.
The numerator becomes 0.10 V, and the denominator becomes 4×10−3 A.
To resolve the fraction, the 10−3 in the denominator moves to the numerator and becomes 1000.
Multiplying 0.10 by 1000 gives us 100. Finally, dividing 100 by 4 yields exactly 25Ω.
Conclusion
The dynamic resistance of the diode at 3 mA is 25Ω.
Notice how this resistance would be entirely different if we picked a point lower on the curve where it is flatter. The resistance there would be much higher!
Always remember, for non-linear devices like diodes, resistance is a local property that depends entirely on where you are operating on the curve.