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The simplest use of solid-state and tube technologies might be the circuit shown above. Here a silicon diode is used to bias a 12AX7. The diode's cathode connects to ground and its anode attaches to the tube's cathode, which allows it to conduct current. In this regard it functions much like a cathode resistor, but it differs in that the voltage across the diode is fixed (about 0.7 volts). Multiple diodes yield multiples of 0.7 volts, such as 1.4, 2.1, 2.8, 3.5, and 4.2 volts. (Although maybe not strictly necessary, the addition of a small valued bypass capacitor lessens our worries that the diodes will harm the sound by providing a path for the higher frequencies to take from ground to the triode's cathode. The sonic test would be to build and compare two simple line stages: one with a cathode resistor bypassed by a large electrolytic capacitor and one with a diode string bypassed by a small film capacitor.) The next move up in complexity is to replace the diode string with a two-lead current source. These devices look like an ordinary solid-state diode, but actually comprise a FET, which has its gate tied to its source. The FET's IDSS sets the current flow. Replacing the cathode resistor or diode string results in a Grounded Cathode amplifier stage that always idles at the same current draw, in spite of tube aging and B+ voltage drifts. Unlike the diode string, these devices must be heavily bypassed in this application, as otherwise no gain will result. A constant current flow means a constant voltage developed across a resistor; only the idle current should be constant.
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