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Colpitts oscillators are similar to the shunt fed Hartley oscillator circuit except the Colpitts oscillator, instead of having a tapped inductor, utilizes two series capacitors in its LC circuit With the Colpitts oscillator the connection between these two capacitors is used as the center tap for the circuit A Colpitts oscillator circuit is shown at Figure 2-5, and you will see some similarities with the Hartley oscillator The simplest Colpitts oscillator to construct and get running is the series tuned version, more often referred to as the Clapp Oscillator Because there is no load on the inductor, a high Q circuit results with a high L/C ratio and of course much less circulating current This aids drift reduction Because larger inductances are required, stray inductances do not have as much impact as perhaps in other circuits The total capacitive reactance of the parallel combination of capacitors depicted as series tuning below the inductor in a series tuned Colpitts oscillator or Clapp oscillator should have a total reactance of

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around 200 ohms Not all capacitors may be required in your particular application Effectively all the capacitors are in series in a Colpitts oscillator, ie they appear as parallel connected but their actual values are in fact in series Ideally, your frequency determining components L1 and the parallel capacitors should be in a grounded metal shield The FET used in the Colpitts oscillator is the readily available 2N4416A Note, the metal FET case is connected to the circuit ground The output from the Colpitts oscillator is through output capacitor 47 pF; this should be the smallest of values possible, consistent with continued reliable operation into the next buffer amplifier stage

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A major benefit of the optgroup element is that although we had nine separate items in three groups, we could fit them all onto the screen in groups of three This means that in this particular case, users don t have to scroll off the end of the screen, and they are led in a very intuitive way to the data that they need To make this even more useful, you can use the onpick attribute of the option element to jump directly to another URL or card In the above case, we could add more cards to give current prices of each item, or a fuller description, or whatever we like I will show you all of the code for the deck to give you the idea The items in bold are those that I have added to the preceding code

HF and higher frequencies without resorting to some sort of crystal control Hence the reason for crystal oscillators The crystal oscillator depicted at Figure 2-6 is a typical example of an RF or radio frequency crystal oscillators which may be used for exciters or RF converters Transistor Q1, can be any transistor which will operate up to 150 MHz, such as a 2N2222A The turns ratio on the tuned circuit depicts an anticipated nominal load of 50 ohms This allows a theoretical 25k ohms on the collector, so typically a 7:1 turns ratio for T1 would be used Use the: L * C = 25330 / F02 formula for determining L and C in the tuned circuits of crystal oscillator Personally I would make L a reactance of around 250 ohms In this case, I d make C1 a smaller trimmer capacitor The crystal at X1 could be an overtone type crystal for the crystal, selecting a L * C for the odd particular multiple of overtone wanted in your crystal oscillators Typically the output of the crystal oscillator would be followed by a buffer circuit A pictorial diagram of the crystal controlled oscillator circuit is shown in Figure 2-7 Note that the components in this diagram are illustrated as component blocks as they might actually look placed on the circuit, rather than as electronic symbols in a circuit diagram or schematic

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Crystal oscillators are oscillators where the primary frequency determining element is a quartz crystal Because of the inherent characteristics of the quartz crystal the crystal oscillator may be held to extreme accuracy of frequency stability Crystal oscillators are, usually, fixed frequency oscillators where stability and accuracy are the primary considerations For example, it is almost impossible to design a stable and accurate LC oscillator for the upper

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