Impedance bridging
In electronics, especially audio and sound recording, a high impedance bridging, voltage bridging, or simply bridging connection is one in which the load impedance is much larger than the source impedance. In cases where only the load impedance can be varied, maximizing the load impedance serves to minimize the current drawn by the load, and maximize the voltage signal across the load. Essentially, the load is measuring the source's voltage without affecting it. In cases where only the source impedance can be varied, minimizing the source impedance will maximize the power (and the current) delivered to the  load and, as before, maximize the voltage signal across the load. A different (unrelated) configuration is an impedance matching connection in which the source and load impedances are either equal or complex conjugates. Such a configuration serves to either prevent reflections when transmission lines are involved, or to maximize power delivered to the load given an unchangeable source impedance. Explanation. When the output of a device (consisting of the voltage source "V" and output impedance "Z" in illustration) is connected to the input of another device (the load impedance "Z" in the illustration), it is a "bridging connection" if the  input impedance ("Z") of the load device is much greater than (typically at least ten times) the output impedance ("Z") of the source device. Given an unchangeable "Z", one can maximize the voltage across "Z" by making "Z" as large as possible. This also correspondingly minimizes the current drawn from the source device. This has a number of effects including: This situation is typically encountered in line or mic level connections where the source device (such as the line-out of an audio player or the output of a microphone) has a fixed output impedance which cannot be changed . In such cases, maximum signal level with minimum distortion is obtained with a receiving device that has as high an input impedance as possible (this also optimizes noise as it minimizes attenuation). In the cases of devices with very high output impedances, such as with a guitar or a high-Z mic, a DI box can be used to convert the high output impedances to a lower impedance so as to not require the receiving device to have outrageously high input impedance and thus suffer drawbacks such as increased noise pickup with long cable runs. In such cases, the DI  box is placed close to the source device (such as the guitar and mic), and any long cables are attached to the output of the DI box (which usually also converts unbalanced signals to balanced signals to further increase noise immunity). Given an unchangeable "Z", one can maximize both the voltage and current (and therefore, the power) at the load by minimizing "Z". This is because the power delivered to the load in the above circuit (assuming all impedances are purely real) is: As can be seen, to maximize "P", one needs to minimize "R". This situation is mostly encountered  in the interface between an audio amplifier and a loudspeaker. In such cases, the impedance of the loudspeaker is fixed (a typical value being 8Ω), so to deliver the maximum power to the speaker, the output impedance of the amplifier should be as small as possible (ideally zero). Again, this is for a case where "Z" cannot be changed while "Z" can be freely changed. In tube amplifiers where "Z" is high by nature, maximum power delivery to the speaker (a much lower impedance) is achieved through a transformer that matches the high output impedance of the tube amp  to the lower impedance of the speaker. Maximizing power transfer given a fixed source impedance. A related case, but one which does not occur often in audio, is to optimize the power delivered to the load when the source impedance is unchangeable. In such cases, power delivery is maximized when the load impedance is matched to the source. (See Maximum power transfer theorem.) The only typical audio application where power delivery (as opposed to voltage delivery) is important is the situation mentioned above of an amplifier driving a loudspeaker. A loudspeaker's impedance is a function of its various electrical  and mechanical characteristics, and this impedance typically takes on a value between 2 and 16 ohms without much room for variation. It is however, relatively easy these days to design an audio amplifier with any of a range of output impedances, even down to nearly zero. In a hypothetical situation with an amplifier having an output impedance much higher than zero, say 8Ω, then it is true that maximum power will be delivered if the loudspeaker also has an 8Ω impedance. This is assuming that the amplifier is modeled by "V" and "Z" as shown above, and that the "V  between the two example amplifiers have the same value. The matched impedance situation is encountered much more in non-audio-related situations, for example in antenna design where the impedance at the antenna terminals takes on a set value due to requirements in its geometry. In such cases, in reception, the impedance of the circuit stage connected to the antenna should be matched to the antenna terminal impedance in order to maximize power transfer. Such cases frequently arise in RF circuits, where transmission line effects also dictate impedance matching. Audio amplifiers. In audio amplifier specifications, the input impedance of modern 	Impedance bridging
26604875	op-amp circuits (and many old vacuum tube circuits) is often naturally much higher than the signal source. The value of the output" impedance is also usually desired to be significantly lower than the load impedance. When driving transducers (especially loudspeakers) the output impedance is often described by a ratio, the damping factor, "DF", which is: Here, "Z" is the output impedance of the amplifier. Knowing the "DF", one can easily calculate "Z": "Z" is the impedance of a loudspeaker, usually around 8Ω nominally. The output impedance of the amplifier is typically in the same order of magnitude as the  impedance of the cables connecting it to the speaker (<0.1Ω), so "DF" can be rather high, ranging into the hundreds. While voltage-drives to speakers (reducing back-EMF from the speaker), i.e. high damping factors, are generally taken as a good design goal, there are some engineers who advocate low-nfb power amplifiers with damping factors closer to unity or find high Damping Factors have little effect, such as a mere 0.35 dB difference in real-life results between a high (100) and medium (20) Damping Factor. Really high damping requires a negative source impedance to partly compensate for  the impedance of the voice coil.