Parallel fed Colpits oscillator circuit

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Parallel fed Colpits oscillator
Parallel fed Colpits oscillator

The circuit operates in a parallel-fed configuration, as the DC plate current does not pass through the inductor. R3 can be substituted with an RF choke if desired. Capacitor C3 prevents B+ from appearing across the variable capacitor, which is typically undesirable. Without R1, C3 may fail to charge, resulting in B+ on the variable capacitor. R1 ensures that the inductor and the outer plates of the variable capacitor are maintained at DC ground potential. The tuning capacitor, often referred to as a split stator, is essentially a dual-ganged capacitor. The rotor and drive shaft are at both AC and DC ground potential, effectively creating a center-tapped capacitor. This configuration places the center of the coil at AC ground potential, leading to the AC voltage at one end of the tuned circuit being 180 degrees out of phase with the AC voltage at the opposite end. The plate voltage is also 180 degrees out of phase with the grid voltage, ensuring that the feedback voltage to the grid has the correct phase to reinforce and sustain oscillation.

The two halves of the variable capacitor must be identical in size or maintain a constant ratio. For narrow tuning ranges, a fixed capacitor can be placed in parallel with the variable capacitor on the grid side, while the capacitor on the plate side remains fixed. The AC voltage applied to the grid is substantial; during the positive peak, it drives the grid positive, charging capacitor C2. As the grid becomes positively charged, it attracts electrons, allowing current to flow, which causes the capacitor to charge negatively at the grid end. The grid does not become excessively positive because the capacitor retains its charge. A small amount of charge dissipates through R2 but is replenished during the next positive half-cycle. This results in a significant average DC voltage of up to -50 volts at the grid, enabling the oscillator to self-adjust. The negative bias reduces the tube's gain, allowing it to stabilize at the necessary level to maintain oscillation. When the grid voltage becomes negative, it typically drives the tube into cutoff, causing the plate current to pulse briefly. The tuned circuit resonates, producing a high-quality sine wave at the grid, although the waveform at the plate may not be as clean.

The circuit's design emphasizes stability and efficiency in oscillation. The careful selection of components such as R1, C2, and the variable capacitor ensures that the oscillator operates within desired parameters. The negative DC voltage at the grid is crucial for maintaining the oscillator's performance, allowing for automatic adjustments based on the circuit's operational conditions. The phase relationship between the voltages at the grid and plate is fundamental to the oscillator's effectiveness, ensuring that feedback is constructive and promotes sustained oscillation. Proper tuning and component matching are essential for achieving optimal performance, particularly in applications requiring precise frequency control.It is parallel fed because the DC plate current does not flow through the inductor. R3 may be replaced by an RF choke if desired. C3 keeps B+ from appearing across the variable capacitor which is generally a no no. If R1 were not present, C3 might not charge up and there would be B+ on the variable capacitor anyway. R1 makes sure that the inductor and the outer plates of the variable capacitor are held at DC ground potential.

The tuning capacitor is sometimes known as a split stator but is actually the familiar dual ganged capacitor. The rotor and drive shaft are at both AC and DC ground potential. The capacitor is, in effect, center tapped. This will place the center of the coil at AC ground potential. The effect of this is to cause the AC voltage at one end of the tuned circuit to be 180 degrees out of phase with the AC voltage at the other end.

Since the plate voltage is 180 degrees out of phase with the grid voltage, the voltage fed back to the grid has the proper phase to reinforce and sustain oscillation. The two halves of the variable capacitor need to be the same size or in a constant ratio to one another. If the oscillator is to be tuned over a narrow range, the capacitor on the plate side may be fixed and the variable capacitor on the grid side would have a fixed capacitor in parallel with it to limit its tuning range.

The AC voltage supplied to the grid is considerable. On the positive peak it drives the grid positive and C2 will be charged. When the grid is forced positive it begins to attract electrons to itself and current will flow. The grid acts like the anode of a diode. This current causes the capacitor to charge with the end of the capacitor which is toward the grid being negative. The grid never goes very far positive because the capacitor charges up and holds the charge. A small amount of charge leaks off through R2 but gets replenished on the next positive half cycle. A substantial average DC voltage, as much as -50 volts, is developed at the grid and this voltage makes the oscillator self adjusting.

The negative bias lowers the gain of the tube and it will set itself to exactly what is needed to sustain oscillation. When the grid voltage goes negative, in most oscillators this will drive the tube into cutoff. This will cause the plate current to flow in short pulses but the tuned circuit rings like a bell and the waveform at the grid is a very good sine wave.

The wave at the plate may not be as good. 🔗 External reference