... change everything, make no difference / change nothing, make a difference ... Really?



For decades controversy has raged in HiFi audio as to the variability of electronics and cables. Most could agree that loudspeakers sound different but that elements of a HiFi system that amplify and conduct the energy that makes the speakers move could not.

Loudspeaker crossovers are constructed with Inductors [L], Capacitors [C] and Resistors [R] to shape the energy to match divers drivers and the cabinet for the desired response. LCR combine to form Impedance [Z]. For more information, Wikipedia has excellent pages on Inductance, Capacitance, Resistance and Impedance. Impedance is frequency dependent as thus varies across the audio band.

It is counter intuitive that electrical energy in a series of electronics and cables could be immune from changes in LCR. Given loudspeakers with sufficient resolution, the changes should be apparent. However, just as some are colorblind and others tone deaf, some will not have the ability to discern subtle differences.

Amplifier outputs and cables all have LCR properties. When one chains together LCR components, frequency and phase response alter. Loudspeaker XOvers are essentially Tone Controls to contour the audio for each driver. Since LCR are cable properties cables are also Tone Controls, albeit at a much finer level. An electronics engineer knows what is driving and following his Tone Control circuit and can thus tailor it for precise control. No such luck for a cable manufacturer. A cable's performance is system dependent. An arguably better cable could make a system less pleasant if it exposes existing flaws. Some cables are well engineered, some are clearly not!

PS Audio Copper Magazine has an excellent series of articles on audio cables by Garen Galeis of Belden. The Belden cables are marketed under the Iconoclast label, but there is currently very little information available [Apr 2018]

Time is of the Essence Part 1   Time is of the Essence Part 2   Time is of the Essence Part 3
XLR Interconnect Design   Speaker Cable Design, Part 1   Speaker Cable Design, Part 2

 Crossovers, Frequency and Phase 

Crossovers are built with LCR and alter both the amplitude and phase of the signal. The designer may use multiple sections to adjust the slope [rate] in different bands to compensate for driver anomalies. As slope increases, so does phase shift and group delay. Unfortunately, very few loudspeakers are minimum possible phase error and thus a great many have never heard such a system. For those who appreciate what phase coherence accomplishes, non-aligned loudspeakers can have artifacts that make them less than ideal.

Humans localize sound from several cues including time- and level-differences between both ears. With a naturally occurring sound directly in front of the listener the fundamental and harmonics arrive in each ear at the same time. Humans are most sensitive to (i.e. able to discern at lowest intensity) frequencies between 2KHz and 5Hz. Most music has little content above 8KHz.

With a 2nd order 440Hz crossover [12db/oct] the 2nd harmonic of A440 is shifted a few hundred µS or inches relative to the fundamental. As cables have LCR properties, they also alter the amplitude, phase and delay. Whether these changes enhance or detract is completely system dependent! What works well in one system may not in another.


Inductors and Capacitors change the phase relationship between the voltage and current of an AC signal. Taken together with Resistance, they form Impedance. In the ubiquitous 75Ω CATV RG-6, 75Ω refers to its Impedance, not resistance.

In general, loudspeaker cables should strive to minimize L as it has the most impact at audio frequencies and loudspeaker impedances.


This graph shows the relative impedances of the cables used in the simulations. The Multi cables are ribbon cable wired as alternating Signal+/Signal* parallel cables. Note how the impedance of these multiple cables is flatter than typical 'speaker wire' or 'zip cord'. Geometry has everything to do with Impedance and just because a cable is flat, it does not necessarily mean better.

* Signal– is preferable to Ground as Earth Ground it may not be. Misuse of the term Ground leads to all manner of confusion in audio. The same current flows in Signal– as Signal+ but in the opposite direction.


HiFi is extremely personal and one man's meat is another's poison. Some like it very loud with lots of bass and others cherish the silky treble and apparent sound stage of tube electronics. Others prize Time Coherence and accurate phase response. Still others have no problem listening to distorted Lossy Encoding on portable devices. Others cannot abide Lossy Encoding in any form. See why Lossy Encoding sounds bad for more information.

In absolute terms, HiFi should be indistinguishable from a live performance meaning that all localization clues are accurately reproduced. Our objective is to show how cables affect those cues and that cables interact with both the driving and driven end.


There are many additional parameters that are not included in the models and simulation. Dielectric, skin & proximity effects, voice coil temperature, loudspeaker connector LCR, loudspeaker internal wiring LCR, XOver PCB LCR, etc. Most of these are small in relation to variances due cable LCR. Others only become operative at the very top of the audio band. A 3-way system will have response variations in completely different areas. A cable that works well with a 2-way system may not on a 3-way. A cable that works well on a complex loudspeaker Z and a tube amp may not on a flatter Z and a solid state amplifier. There is no free lunch!

Cables have different effects in different systems. The only true way to know if a cable is better is to try it in YOUR system. Another listener may totally disagree as they prefer alternate colorations. Audio store demos are not always valid for your system. Cables that are initially impressive can wear thin very quickly. When auditioning any component, always replug ALL current cables in the whole system. Listen to your reference materials on a fully warmed system. See Winter Blues for possible thermal effects.


[Click Thumbnails for a larger image]



Solid State Amplifier output stage model is an idealized source configured with emitter resistor, output inductor with parallel resistor and output connector capacitance. It has no bandwidth limitation. An actual amplifier has bandwidth limitations and its implementation can affect response within the audio band when interacting with cable and loudspeaker Z.

Emitter Resistor - Each output transistor has an emitter resistor to stabilize its bias current. These resistors are typically on the order of about 0.22Ω. Small amplifiers may have one or two output transistors while large amplifiers can have a dozen. In the simulations we have used 0.11R for two output devices for an amplifier around 100W and 0.025 for an amplifier with eight output devices for an amplifier of around 400W. This output R reacts with the cable impedance.

Loudspeaker Cables

Amp Single
Multi Wire

Loudspeaker Cables are modeled as single 2 conductor wire and a cable made of 10 pairs of parallel wires. Two types of single wire are modeled: a 12ga OFC commercial loudspeaker cable and 18ga zip cord. The Multiple wire cable is based on a 22ga ribbon configured as 10-way Signal± pairs. This equalizes R with the Single model. Note that Signal- may or may not be at earth potential and current flows in both conductors equally. LCR values are divided equally between the two conductors.

LCR values:

Single: 12ga L 150nH/ft - C 22pF/ft - R 0.0016Ω/ft** - Polyolefin - Src: manufacturers data sheet

Multi: 22ga L 150nH/ft* - C 11pF/ft* - R 0.016Ω/ft** - PVC - Src: manufacturers data sheet*

Zip: 18ga L 212nH/ft - C 14.6pF/ft - R 0.0064Ω/ft** - PVC - Src: calculated from materials and geometry

* - LC values based on Gnd-Signal-Gnd. Single 22ga Gnd-Signal calculated value is 250nH and 13pF
** - DC R values per conductor


Computer Optimized XOver Cookbook XOver

Loudspeakers are modeled as two way with 2KHz crossover. One uses a computer [Comp] model that incorporates driver impedance and performance. Missing from this model is the parallel C across inductors and drivers. The other uses a 'cookbook' [CkBk] 2nd order crossover calculated simply from the driver R values.

NOTE: Loudspeaker models ignore driver resonances or cabinet loading, as indicated by the simulation responses below 500Hz. This Google link for Loudspeaker Impedance Curves should disabuse even the most skeptical that their loudspeakers are a constant 8Ω.

Simulation Results

10Hz to 20MHz Response
Graph at left shows simulation response to 20MHz. Response below 100Hz and above 20KHz are not plotted for comparison graph clarity. As can be seen from loudspeaker impedance curves, Z below 500Hz varies enormously. Modeling it is beyond this scope. Suffice it to say that interaction below 500Hz is far more significant than shown. Response above 20KHz could vary significantly with amplifier design. These examples are for illustration ONLY and are not intended for any other purpose.

Single Wire Cookbook XOver Single 12ga Wire to Cookbook XOver            Single Wire Computer XOver Single 12ga Wire to Computer XOver
Single Wire Cookbook XOver Multi 22ga Wire to Cookbook XOver            Single Wire Computer XOver Multi 22ga Wire to Computer XOver
Zip Cord Wire Cookbook XOver Zip 18ga Wire to Cookbook XOver            Zip Cord Computer XOver Zip 18ga Wire to Computer XOver
18ga PET Cookbook XOver 18ga Mylar Wire to Cookbook XOver            Zip Cord Computer XOver 18ga Mylar Wire to Computer XOver
Zip Cord Wire Cookbook XOver Teflon Zip 18ga Wire to Cookbook XOver            Zip Cord Computer XOver Teflon Zip 18ga Wire to Computer XOver

 Amplifier Output R 

0L 0.025R Level 0L 0.025R Phase 0L 0.11R Level 0L 0.11R Phase
This simulation shows how the amplifier output R may interact with cable LCR and the loudspeaker Z. Notice the difference in the upper frequency slopes and how they interact with the different crossovers. This simulates the change that could be expected with identical amps differing only in number of output devices, all other things being equal.

 Amplifier Output L and R 

Varying Amp Op Single Level Varying Amp Op Single Phase Varying Amp Op Multi Level Varying Amp Op Multi Phase Varying Amp Op Zip Level Varying Amp Op Zip Phase

This simulation shows how the amplifier output L and R may interact with cable LCR and the loudspeaker Z. Notice the difference in the upper frequency slopes with the addition of the 2µH inductor. The parallel R has very little effect in the audio band but could help with a higher capacitance cable and low impedance loudspeaker in preventing parasitic oscillation.

The above two simulations give insight into an amplifier output property fault wherein the output Z is dynamically affected in a frequency-dependent manner as a function of output level. Loudspeaker impedance varies with frequency and to a lesser extent with input level. In the amplifier, as the output level and frequency vary, output impedance varies. Output transformers suffer badly in this area and contribute to the tube sound. OTL [Output TransformerLess] tube designs are an attempt to mitigate this problem trading power for fidelity. Solid state is not immune. Unless the power supply has sufficient reserve capacity, the output can be starved by large peaks in the loudspeaker Z minima. If the output Z is varying dynamically, its interaction with the cable is also varying dynamically in proportion to the cable's impedance. And thus, the loudspeaker is not fed an identically phased signal at -10db as at -9 or -11. This fault could render a store demo or another's opinion suspect even when conducted on identical equipment unless the listening and amplifier drive levels are matched. Room interactions play a significant part in the perceived sound and may ameliorate or exacerbate cable colorations.

 Cable Comparisons to Cookbook and Computer Optimized XOvers 

Var Wire CkBk Lvl Var Wire CkBk Phs Var Wire Comp Lvl Var Wire Comp Phs
Level and Phase comparisons for Cables to Cookbook and Computer Optimized 2-way 2Khz XOvers.

 Cable Comparisons with Single Parameter Change 

LCR depends on wire diameter, wire spacing and dielectric material. LCR all increase linearly with cable length. Ignoring permeability, L depends on size and spacing. C depends on size, spacing and dielectric. It is not trivial to fabricate two physically different cables and achieve the same impedance.

12ga PO vs 18ga PET Lvl 12ga PO vs 18ga PET Phs

In this cable pair, diameter and spacing were adjusted to maintain L and dielectric changed from Polyolefin to Mylar to keep capacitance constant. R varies in this example, 18ga being 4x more resistive than 12ga.

18ga PVC vs Teflon Lvl 18ga PVC vs Teflon Phs

In this cable pair, diameter and spacing were maintained to keep L & R constant, and dielectric changed from PVC to Teflon. C drops from 14.59pF to 9.76pF / ft.

Note how the traces overlay, indicating very little difference.

Zip PVC vs PTFE Deltas

This graph of Level and Phase deltas show just how little difference there is between PVC and Teflon in the audio band for Zip cord geometry cables. Maximum Level is about 0.00005db and Phase about 0.0005° @ 20KHz!

Zip PVC vs PTFE 10MHz Phase Zip PVC vs PTFE 10MHz Phase

These graphs show how little difference there is between PVC and Teflon to 1MHz. Above 5MHz is where capacitive differences begins to tell. Teflon has a lower dielectric absorption factor which may improve smearing over PVC.


TC-50 BiWire Conn

Bi-Wiring uses two cables to separate Woofer and Mid/Tweeter connectors on the speaker from a single amplifier output. Some claim that it makes an improvement and others say there is no benefit. Some critical listeners who can reliably detect cable differences also claim to detect BiWiring. As always it will be system dependent and subject to listener bias as to better or not.

BiWire CkBk Driver Level BiWire CkBk Driver Phase

These graphs show the Driver responses measured at the Driver / XOver connection in the loudspeaker at the lines marked Woofer and Tweeter in the model images above. Only the Single wire Cookbook is shown as in all cases responses overlay similarly. This is expected from Y-Axis XOver attenuation magnitudes. Frequency is ±2 octaves from the XOver frequency.

BiWire Driver Level Delta BiWire Driver Phase Delta

These graphs show the deltas between one cable to the speaker and Bi-Wired with two runs for Single Cookbook and MultiWire Computer models. The single lead is subtracted from the Bi-Wire. The differences are slight, but quite probably within the detectability range of critical listeners. It is interesting to note that more complex MultiWire / Computer

XOver combination has more rapid rates of change, perhaps enhancing detectability.

 Bi-Wiring Bridging 

TC-50 BiWire Conn

Many BiWire capable loudspeakers are delivered with a pair of Bridges between the Plus and Negative terminal pairs to allow single cable connection. Of course this led to the inevitable "Which BiWire Bridge Mode Sounds Best?" opinion controversy. There FOUR possible 4 conductor BiWire combinations plus the TriWire variant:

  • • None - Normal 4 conductor BiWire
  • • Negative - Bridge between Negative terminals only
  • • Positive - Bridge between Positive terminals only
  • • Both - Negative and Positive terminals bridged BUT with a cable connected to each
  • • TriWire - Single conductor to Positive or Negative Bridged terminals and two wires to opposite polarity

TC-50 BiWire Tweet TC-50 BiWire Woofer Cookbook BiWire Tweet Cookbook BiWire Woofer

The images above are deltas to a standard 4 conductor BiWire. It is readily apparent that each Bridge Mode differs and the magnitudes are system dependent. In short, listen with a jaundiced ear upon all claims and recommendations unless the systems are identical from source onwards.


Some claim all cables sound the same. Some claim two cables with the same R will sound the same. Some cable manufacturers make all kinds of wild claims, provide no engineering insight as to problems solved and charge ever increasing prices for something that may not be any better than, or even different from, what the customer is currently using as cables interact with the system! Everything interacts and any claims for guaranteed improvements may be proved ephemera.

Caveat emptor.