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Material Type: Lab; Class: Introduction to Electronics; Subject: Electrical and Computer Engr; University: University of Illinois - Urbana-Champaign; Term: Unknown 1989;
Typology: Lab Reports
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In lab 2 we discovered that resistors, motors, and incandescent bulbs all have I-V graphs which can be characterized by sloped lines which characterize the resistive behavior, outside of some transition regions and "warming up" areas. The voltage is directly related to the current. However, in order to control the ECE cars, we need our circuits to be able to encode logic. The circuits need to be able to represent the concepts of "true" and "false", "on" and "off" and be able to perform basic Boolean operations using these concepts. This is highly nonlinear behavior – behavior that is exhibited by the simplest device that we have worked with, a switch. Like the one on the back of your vehicle or the one in the test box. To appreciate the complexity of this simple device – a switch, try and draw an I-V curve for a manual switch. Conceptually, this would be the perfect device to implement the two-state logic that you have learned about in lecture and that you will be using to implement the circuitry on your vehicles. A manual switch has an obvious drawbacks for all applications where speed, size, complexity, and autonomy are desired. An electronic device that can behave as a switch, a switch that is small, fast, and can be controlled electronically. These electronic switches will be used to implement the two-state Boolean arithmetic that all of our digital devices use to operate. The beauty of a two-state system is that the simple concept of "on" and "off" can be mapped onto the two states sometimes called "true" and "false" (if we are speaking in terms of logic) or "1" and "0" (if we are speaking in terms of Boolean logic).
In this lab you will play with a new class of device - diodes. These devices are often used as switches and have traditionally been used in building digital logic gates, although there are many other applications that use the analog behavior of the diode. One such application will be investigated at the end of the lab – the voltage regulator where a zener diode is used to provide a constant voltage drop that can be turned on and off. There are several different types of diodes - we will experiment with three types of diodes, a basic diode, a zener diode, and a light emitting diode (invented here by some folks in the microelectronics group).
Build the circuit shown using a 1N5406 diode, 1kΩ resistor, test box, function generator, and an oscilloscope. Be sure to properly orient the diode in the circuit. You should be old hands at building circuits but if you are still confused ask your TA for help. Always build your circuit first without the test equipment (e.g. the oscilloscope probes). Pay particular attention to the polarity of the oscilloscope probes – remember the negative side of both channels of the ocilloscope are tied to the same common point, they are grounded through the outlet.
✔ Turn on the oscilloscope and put it in XY mode. ✔ Invert channel 2. ✔ Position the displayed dot at the center of the screen. ✔ Turn on the function generator and set it to a 100 Hz sine wave with zero DC offset. ✔ Vary the amplitude of the waveform from the function generator and the horizontal and vertical scales on the oscilloscope until you feel you have obtained a good image. ✔ Don't dismantle the setup when you are finished with this part.
Use the same experimental setup as in part 1, but replace the diode with a 1N4734 Zener diode. Again vary the amplitude of the waveform from the function generator and the horizontal and vertical scales on the oscilloscope until you feel you have obtained a good image.
Light Emitting Diodes (LEDs) function in exactly the same way as normal diodes except that they are made of a semiconducting material that emits light when the diode is in the "on" state. For this lab we have a particularly interesting LED that behaves in a unique way. Use the same experimental setup as in part 1, but replace the diode with the white capped LED. Be sure to orient the LED so that the longer of its two wires is connected to the positive terminal and the shorter of its two wires is connected to the negative terminal. Set the function generator to a 100 Hz sine wave with amplitude 9 V P-P and zero DC offset.
The LED can be a very useful tool for checking signals when you are designing the circuit which will control your car, but you must make sure that it turns on and off in the proper voltage ranges to check signals. So if you want to use it later in the semester, you must include a resistor with resistance equal to what you found on each LED you use for testing. You can repeat this test for the other colors if you have time.
As you determined in lab 3 some voltage sources are non-ideal, in the sense that the voltage actually changes as you modify the load attached to it. For many applications this is unacceptable and a circuit is added to the source to regulate the voltage so that it remains the same for a wider range of load resistances. Similar designs can also be used to clip and rectify signals suggesting an application for AC-DC conversion. The voltage regulating circuit you will be experimenting with in this portion of the lab is one that you encountered for homework and is also a simplified version of the circuit inside your vehicle that regulates the voltage from the battery to provide the 5V for the logic circuits. The regulator comprises a simple non-ideal voltage source - such as a battery with some internal resistance and a Zener diode. From the I-V curve of the zener diode (which you just drew in your notebooks) you can see two regions where the diode behaves like a source in the sense that the voltage remains the same across the device for a wide range of currents flowing through the device. The diode is of course not a source since it cannot provide power. In class you modeled its source-like behavior by replacing the zener diode's I-V curve with a piecewise linear model consisting of 2 vertical lines. A slightly more exact model would take into account that the zener does not emulate an ideal source but has some resistance of its own though it is quite small. Ideally, if the value of Vs is a constant value sufficiently large to drive the Zener diode into the breakdown region then any load that is connected across the terminals of the Zener diode will see the voltage across the load held at the zener breakdown voltage – no matter how the load might change. The voltage is regulated or held constant across the zener diode because the the diode is capable of handling a wide range of currents with a very small change in voltage. Let's investigate how the circuit works given a constant, positive Vs and Rs that is sufficient to put the zener diode into the breakdown region for at least some values of the load RL. From what we know of circuit theory we can think about the two extremes of RL. If RL is infinite then the voltage across the diode will be VZ. As the load decreases from infinity eventually it will become small enough that the diode will be almost shorted causing the diode to turn off. So, there are two ranges in all possible RL, one in which the diode is off, and one in which the diode operates in the breakdown region where it can act as a simple voltage regulator. The graph below illustrate how the voltages and currents depend on the value of the load resistance