Engineering Sciences 154
See nice reference on Diode Applications from the Georgia State University, Hyperphysics project.
Typical power supply applications
- Half-Wave Rectification
"Figure shows a half-wave rectifier circuit. The signal is exactly the top half of the input voltage signal, and for an ideal diode does not depend at all on the size of the load resistor.
"The rectified signal is now a combination of an AC signal and a DC component. Generally, it is the DC part of a rectified signal that is of interest, and the un-welcomed AC component is described as ripple. It is desirable to move the ripple to high frequencies where it is easier to remove by a low-pass filter.
"When diodes are used in small-signal applications - a few volts - their behaviour is not closely approximated by the ideal model because of the PN turn-on voltage. The equivalent circuit model can be used to evaluate the detailed action of the rectifier under these conditions. During the part of the wave when the input is positive but less than the PN turn-on voltage, the model predicts no loop current and the output signal voltage is therefore zero. When the input exceeds this voltage, the output signal becomes proportional to, or about 0.6 V lower than the source voltage."
|Op Amp solution to PN turn-on problem
Half-wave rectifier with filter capacitor or peak detector
- Full-Wave Retification
- Version 1 - Center-Tap Full-Wave Rectifier
- Version 2 - Bridge Full-Wave Rectifier
"The diode bridge circuit shown ÷ is a full-wave rectifier. The diodes act to route the current from both halves of the AC wave through the load resistor in the same direction, and the voltage developed across the load resistor becomes the rectified output signal. The diode bridge is a commonly used circuit and is available as a four-terminal component in a number of different power and voltage ratings."
Go to Diode Bridge Modules for a collection of pdf data sheets on many integrated diode bridges.
Op Amp solution to PN turn-on problem
Split Power Supply
"Often a circuit requires a power supply that provides negative voltage as well as positive voltage. By reversing the direction of the diode and the capacitor (if it is polarized), the half-wave rectification circuit with low-pass filter provides a negative voltage. Similarly, reversing the direction of the diodes and capacitor in the full-wave rectified supply produces a negative voltage supply. A split power supply is shown in figure ÷"
Also called a "dc restorer" in Sedra & Smith"When a signal drives an open-ended capacitor the average voltage level on the output terminal of the capacitor is determined by the initial charge on that terminal and may therefore be quite unpredictable. Thus it is necessary to connect the output to ground or some other reference voltage via a large resistor. This action drains any excess charge and results in an average or DC output voltage of zero.
"A simple alternative method of establishing a DC reference for the output voltage is by using a diode clamp as shown in figure ÷. By conducting whenever the voltage at the output terminal of the capacitor goes negative, this circuit builds up an average charge on the terminal that is sufficient to prevent the output from ever going negative. Positive charge on this terminal is effectively trapped."
"A diode clipping circuit can be used to limit the voltage swing of a signal. Figure ÷ shows a diode circuit that clips both the positive and negative voltage swings to references voltages."
Limiting with ordinary diodes: Limiting with Zener diodes: Multiplier
- Doubler - Version 1: A dc restorer followed by a peak detector
- Doubler - Version 2
"A voltage multiplier circuit is shown in figure÷. We can think of it as two half-wave rectifier circuits in series. During the positive half-cycle one of the diodes conducts and charges a capacitor. During the negative half-cycle the other diode conducts negatively to charge the other capacitor. The voltage across the combination is therefore equal to twice the peak voltage. In this type of circuit we have to assume that the load does not draw a significant charge from the capacitors."
- For more on multipliers see:
"To the left (above) you see a basic Diode Logic OR gate. We'll assume that a logic 1 is represented by +5 volts, and a logic 0 is represented by ground, or zero volts. In this figure, if both inputs are left unconnected or are both at logic 0, output Z will also be held at zero volts by the resistor, and will thus be a logic 0 as well. However, if either input is raised to +5 volts, its diode will become forward biased and will therefore conduct. This in turn will force the output up to logic 1. If both inputs are logic 1, the output will still be logic 1. Hence, this gate correctly performs a logical OR function.
"To the right (above) is the equivalent AND gate. We use the same logic levels, but the diodes are reversed and the resistor is set to pull the output voltage up to a logic 1 state. For this example, +V = +5 volts, although other voltages can just as easily be used. Now, if both inputs are unconnected or if they are both at logic 1, output Z will be at logic 1. If either input is grounded (logic 0), that diode will conduct and will pull the output down to logic 0 as well. Both inputs must be logic 1 in order for the output to be logic 1, so this circuit performs the logical AND function."
Consider the following circuit:
Using the Shockley Diode Equation we can write
This is a pretty complicated expression, but we can get a reasonable and useful result with a bit algebra and analysis. Let us assume that there are dc biases on the signals (usual case) so that
where are fluctuations around the bias values .
With much algebra we can show that
The important point is that the output has components