Miller effect

This pole is moved down in frequency by the Miller effect.

This interesting phenomenon is known as the Miller effect.

This eliminates the Miller effect and thus contributes to a much higher bandwidth.

This will typically reduce the Miller effect and increase the bandwidth of the amplifier.

The Miller effect may also be exploited to synthesize larger capacitors from smaller ones.

Because of the Miller effect in the common source amplifier the input and the output transmission line are coupled.

The input impedance of the circuit is almost zero because of the Miller effect.

The original Miller effect is implemented by capacitive impedance connected between the two nodes.

Since the input side has no load there is no gain on that side and the Miller effect does not come into play.

The Miller effect negatively affects the performance of the common-source amplifier in the same way (and has similar solutions).

These properties of the Miller effect are generalized in the Miller theorem.

The Miller effect may be undesired in many cases, and approaches may be sought to lower its impact.

The bandwidth of the common-emitter amplifier tends to be low due to high capacitance resulting from the Miller effect.

In analog amplifiers this curtailment of frequency response is a major implication of the Miller effect.

Voltage can be amplified by a common gate transistor, which shows no miller effect and no unit gain frequency cut off.

The Miller effect was named after John Milton Miller.

The inverting integrators from this list are examples of useful and desired applications of the Miller effect in its extreme manifestation.

As most amplifiers are inverting ( as defined above is positive), the effective capacitance at their inputs is increased due to the Miller effect.

Miller theorem generalizes Miller effect as it implies arbitrary impedance Z connected between the nodes.

This configuration holds the transistor's collector voltage roughly constant, thus making the base to collector gain zero and hence (ideally) removing the Miller effect.

A well-know example of this is the Miller effect, in which an unavoidable feedback capacitance appears increased (i.e. its impedance appears reduced) by negative feedback.

In some of them, the Miller phenomenon appears as desired (bootstrapping) or undesired (Miller effect) unintentional effects; in other cases it is intentionally introduced.

The emitter-coupled amplifier is compensated for temperature drifts, V is cancelled, and the Miller effect and transistor saturation are avoided.

Miller effect - John Milton Miller (John M. Miller)

To combat the stability problems and limited voltage gain due to the Miller effect, the physicist Walter H. Schottky invented the tetrode tube in 1919.