Voltage feedback and current feedback.

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SUMMARY

The discussion focuses on the differences between voltage feedback (vfb) and current feedback (cfb) in amplifier configurations, specifically in common cathode tube amplifiers and cathode followers. The gain equation for a common cathode amplifier is defined as \(\frac{\mu R_{l}}{R_{p} + R_{k}(\mu +1) + R_{l}}\), highlighting the impact of unbypassed cathode resistance on gain and dynamic plate resistance. The transition from cfb to vfb is explained through the change in feedback mechanism when the output is taken from the cathode instead of the anode, emphasizing the nature of the error signal as either current or voltage.

PREREQUISITES
  • Understanding of amplifier gain equations, specifically for common cathode tube amplifiers.
  • Familiarity with the concepts of voltage feedback (vfb) and current feedback (cfb).
  • Knowledge of resistive dividers and their role in feedback loops.
  • Basic principles of tube amplifier configurations, including cathode followers and their characteristics.
NEXT STEPS
  • Study the gain equations for common cathode tube amplifiers in detail.
  • Explore the principles of voltage feedback (vfb) and current feedback (cfb) in various amplifier designs.
  • Investigate the effects of unbypassed resistors on amplifier performance.
  • Learn about the implementation of feedback loops in transistor amplifier circuits.
USEFUL FOR

Electronics engineers, audio amplifier designers, and students studying amplifier theory who seek to deepen their understanding of feedback mechanisms in tube and transistor amplifiers.

bitrex
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Looking at the equations for the gain of a common cathode tube amplifier with the cathode resistor unbypassed (though the question in general could apply to similar configurations with BJTs and FETs) I see that the gain of the amplifier is something like \frac{\mu R_{l}}{R_{p} + R_{k}(\mu +1) + R_{l}}, where Rl is the load resistance, Rp is the dynamic plate resistance, mu is the amplification factor, and Rk is the unbypassed cathode resistance. This is degenerative feedback where the feedback is proportional to the current through the device - the gain of the amplifier is reduced and the dynamic plate resistance is increased. However, in a cathode follower, when the emitter resistor is unbypassed the dynamic plate resistance is decreased by the factor \frac{R_{p}}{\mu +1}}. This must be voltage feedback since the input impedance is increased and the output impedance is reduced. What I can't see is how the feedback changed from current feedback to voltage feedback by just taking the output from the cathode instead of the anode.
 
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It's current feedback, cfb, because the error signal is a current. In a voltage feedback loop, vfb, the error signal is a voltage.

With vfb, the output voltage (or current with a sense resistor) is fed back through a resistive divider, to the base of the input transistor which is driven until the differential voltage across the 2 bases (input is a differential pair) is reduced to virtual zero.

With cfb, the output voltage (or current with a sense resistor) is fed back through a resistive divider, to the common emitter of a totem pole emitter follower. The upper emitter sources current and the lower emitter sinks current. The output drives the feedback current to virtual zero when the loop is closed.

It's all about the error signal. The terms cfb & vfb refer to the error signal being a current or a voltage resp. Does this help?

Claude
 

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