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  BASIC  
 ELECTRONICS COURSE  
 Page 29 
  
 INDEX 
 
 
                 There is one more
                GATE we need to cover. It is the . . .
                 
                THE
                SCHMITT TRIGGER INVERTER 
                The SCHMITT TRIGGER INVERTER is an INVERTER with a SCHMITT TRIGGER input. 
                 
                  
                It is basically a GATE and can be used as an INVERTER. But the
                Schmitt Trigger input gives it a lot more features. 
                The Schmitt Trigger Inverter is shown on the left and the
                Schmitt symbol must be included to show it is not an ordinary
                inverter.  
                
                
                This is a very useful BUILDING BLOCK and can be used in many
                different ways.   
                It can be used as an Inverter, an oscillator, a Buffer as well as
                other "Building Blocks." It all depends on the surrounding
                components.  
                When you add components to create a circuit that performs a
                "function," the result is called a BLOCK, or BUILDING
                BLOCK or STAGE.  
                There are 6 Schmitt Inverters in the chips we will be discussing
                and this allows 6
                separate "stages" or "blocks" to be
                produced.  That's why complete projects can be designed around
                a single chip.  
                When wired as an oscillator, only two
                external components are needed. If you require the oscillator to
                be turned on and off, a low-frequency oscillator can gate the
                oscillator (as shown previously). If you require the oscillator
                to drive an output device, two Schmitt Inverters can be wired in
                parallel to deliver the drive-current. If you require a
                load but WITHOUT inversion, two Schmitt gates can be placed in
                series. (This is called "double inversion" and is
                equivalent to a BUFFER.) 
                The chip we are referring to is the HEX SCHMITT TRIGGER with the
                basic identification of 74C14.  
                This chip is also known as 40106 or 74F14  or
                74HC14. They are all pin-for-pin compatible devices. The
                advantage of the 74HC14 is it will operate on a voltage as low
                as 3v.  
                
                The range of
                circuits you can design with this chip is endless but before 
                you can start designing, there are two features we need to
                cover.  
                1.  The Hysteresis of
                a Schmitt Trigger 
                2.  The Time Delay Circuit. 
                 
                 
                1.
                THE HYSTERESIS OF A SCHMITT TRIGGER 
                The Hysteresis of
                a Schmitt Trigger is the gap between the low point where the
                gate changes state and the high point. This gap is typically 33%
                of rail voltage and because this gap is so wide, it is very
                difficult for noise to enter the gate and cause false
                triggering. This makes the gate ideal for noisy situations but
                it will not amplify low-level signals and therefore cannot be
                used where small signals are required to be amplified. This is
                the only drawback of a Schmitt Trigger.  
                The hysteresis is
                the "dead gap" between 33% and 66% of rail voltage and
                these two levels are discussed fully below. 
                
                2.
                THE TIME DELAY CIRCUIT 
                
                The time delay circuit is also know as a "TIMING CIRCUIT," "DELAY
                CIRCUIT," or "R-C
                CIRCUIT".
                These names all refer to a CAPACITOR and RESISTOR in
                series. It does not matter if the capacitor is placed above or below
                the resistor as the time delay will be the
                same. The only difference
                will be the value of the voltage at the beginning and end of the timing
                cycle.  
                If the capacitor is above the resistor, as shown in the first diagram
                below,
                the voltage will RISE from zero to rail voltage.  
                If the capacitor is below the resistor, as shown in the second diagram,
                the voltage will fall from rail voltage to  zero.  
                The join of the two components is the point where the voltage is
                detected and is called the "Detection Point."  
                The Detection Point is monitored by a Detection Circuit.
                This can be any of the gates we
                have described or a transistor or a multimeter.  
                The detection circuit  must not load the timing
                circuit. In other words the detection circuit must have a very
                high input impedance and as we have already described, CMOS
                gates have a very high input impedance. That's why they are
                ideal for detecting the voltage on a DELAY CIRCUIT.  
                
                When voltage is
                applied to a TIMING CIRCUIT, the capacitor begins to charge. If
                we monitor the voltage across the capacitor, we can determine
                when it is at a particular voltage level. It will take a
                PERIOD OF TIME to reach this level and this is the TIME DELAY we
                require.  
                In the animation below we see the capacitor charging via a
                resistor, with a meter showing the approx voltage across the
                capacitor. We have already mentioned the capacitor does not
                charge at a constant rate, but this characteristic does not
                concern us at the moment.  
                The point to remember is the TIME it takes for the capacitor to
                charge.  
                
                 
                 
                
                In the animation
                below, the meter is monitoring the voltage across the RESISTOR.
                As you can see, the voltage across it is falling as the
                capacitor charges.  
 As the voltage across the capacitor
                INCREASES, the voltage across the resistor DECREASES because the
                total voltage across the combination is 10v, and the voltage
                across each must add up to 10v.    
                
                
                  
                
                If we connect the
                DELAY CIRCUIT to the output of a gate (any gate can be used -
                but we will choose an INVERTER and since we are discussing the
                Schmitt Inverter, we will use it)  we can CHARGE the
                capacitor when the output of the Schmitt Inverter is HIGH
                and DISCHARGE the capacitor when the output is LOW.
                The animation below shows how the voltage across the capacitor
                rises and falls during the cycle. The actual shape of the graph
                does not concern us. We are only interested in VOLTAGE LEVELS
                and the TIME TAKEN for the voltage to rise and fall.   
                We will discuss the voltage levels in a moment. For the moment
                you need to know the levels detected by a SCHMITT
                INVERTER are: 33% and 66% of rail voltage. These two levels are
                shown on the graph. 
                 
                
                
                 
                 
                 
                
                Here comes the
                clever part. Instead of the voltmeter monitoring the voltage
                across the capacitor, the input of the Schmitt Inverter can be
                connected to the capacitor.  
                If the voltage across the capacitor is less than 66% of rail
                voltage, the output of the gate is HIGH and the capacitor begins
                to charge. When the voltage reaches 67%, the output goes LOW and
                the capacitor begins to discharge. When the voltage across it
                reaches 32% of rail voltage, the Schmitt Inverter changes state
                and the output goes HIGH. In this way we need only one gate to create an oscillator. 
                There are two very important things to observe in the animation
                below. 
                1. The output is a square wave. In other words the output goes
                from one state to the other VERY QUICKLY  and this
                produces the characteristic waveshape.  
                2. The voltage across the capacitor is EXACTLY 32% to 67% of
                rail voltage.  
                The
                animation below shows the gate in operation.  
                You will notice that the diagram does not show the chip
                connected to the positive and negative rail. It is ASSUMED
                the chip is connected to the supply voltage and that's how the
                output produces the HIGH.  
                
                
                  
                
                 
                A point to remember: 
                1. The output of the chip is always the reverse (opposite) of
                the input. The chip INVERTS the level (HIGH or LOW) on
                the input and makes the output the OPPOSITE. 
                If the Input is HIGH, the output will be LOW
                etc.  
                 
                HOW
                THE SCHMITT OSCILLATOR WORKS
                 
                
                Suppose the input is LOW. The output will be HIGH. The voltage
                across the resistor will cause current to flow through it and
                charge the capacitor. When the voltage on the capacitor reaches
                67% of rail voltage, the gate will change state.  
                The energy in the capacitor will "bleed" through the
                resistor and the voltage across the capacitor will gradually
                fall. When it reaches 32% of rail voltage, the gate will change
                state.   
                
                By selecting the
                correct values for R and C, the Schmitt Oscillator can flash an
                LED at a low flash rate.  The 470R resistor in series with the LED
                has nothing to do with the flash rate. It must be included
                so that the output of the gate goes HIGH. If it is omitted,
                the output will not rise above 1.7v. This is the characteristic
                voltage across a LED and has been discussed in the first pages
                of this course. If the resistor is reduced in resistance, it
                will load the output and the output will not rise to rail voltage. If
                this occurs, the input will not see 67% of rail voltage and the
                gate will not change state.  
                The output of a 74C14 Schmitt gate will deliver about 15 - 20mA.
                If the load requires more than about 20mA, a buffer (driver)
                transistor will be needed. The output will deliver
                more than 20mA but the output will not be full rail voltage. A
                small drop will not affect the performance of the oscillator,
                but if the load current is increased, a
                point will come when the output will not rise to 67% of rail voltage
                and the input will not allow the gate to change state.  
                
                 
                
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