Department of Electronics and Communication
College of Engineering Karunagappally
What You will Learn
- You will plot the V-I characteristics of Si and Ge diodes and understand the difference in cut in voltage and slope of the characteristics.
Theory
Semiconductor diode is a $p-n$ junction that conducts well on forward bias and conducts very little on reverse bias. The relation between diode current and voltage is \begin{equation}\label{diodeeqcurrent} I=I_{o}[e^{\frac{V_{D}}{\eta V_{T}}}-1] \end{equation} where $I_{o}$ is the reverse saturation current, $V_{D}$ is the voltage across the diode and $V_{T}=\frac{kT}{q}$. $k$ is the Boltzmann constant and $T$ is the absolute temperature. The ideality factor $\eta$ varies from $1$ to $2$.Experiment - Forward Characteristics
Experiment - Reverse Characteristics
The Qucs schematic for plotting reverse characteristics of Si diode is shown below. In the $\fbox{Parameter Sweep}$, set the diode reverse voltage between $0$ V and $10$ V to study the saturation of reverse current. Run the simulation and observe the dpl file as shown below. The transient simulation with parameter sweep results in the reverse characteristic prior to break down as shown below. If the diode voltage is allowed to sweep to $100\,V$, then the break down happens at around $50\,V$, as shown below. Repeat the experiment for a Ge diode as well.Observations
- Forward resistance of Si diode =$\ldots\ldots\ldots\ldots\ldots\ldots\ldots\ldots\, $ $\Omega$
- Forward resistance of Ge diode =$\ldots\ldots\ldots\ldots\ldots\ldots\ldots\ldots\,$ $\Omega$
- Reverse resistance of Si diode =$\ldots\ldots\ldots\ldots\ldots\ldots\ldots\ldots\,$ $k\,\Omega$
- Reverse resistance of Ge diode =$\ldots\ldots\ldots\ldots\ldots\ldots\ldots\ldots\,$ $k\,\Omega$
What You Learned
- You plotted the V-I characteristics of diodes under forward and reverse condition on the simulator
- You measured the cut in voltage, forward and reverse resistances of Si and Ge diodes
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