... change everything, make no difference / change nothing, make a difference ... Really?
Background
Contention
Crossovers, Frequency and Phase
Impedance
Click thumbnails for a larger image
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.
Objective
Caveats
Models
Amplifier
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 may have more than 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
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
Loudspeakers
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
Response below 100Hz and above 20KHz are not plotted in the comparison graphs below for 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 12ga Wire to Cookbook XOver
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Single 12ga Wire to Computer XOver
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Multi 22ga Wire to Cookbook XOver
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Multi 22ga Wire to Computer XOver
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Zip 18ga Wire to Cookbook XOver
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Zip 18ga Wire to Computer XOver
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18ga Mylar Wire to Cookbook XOver
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18ga Mylar Wire to Computer XOver
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Teflon Zip 18ga Wire to Cookbook XOver
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Teflon Zip 18ga Wire to Computer XOver
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Amplifier Output R
Amplifier Output L and R
Cable Comparisons to Cookbook and Computer Optimized XOvers
Cable Comparisons with Single Parameter Change
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.
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.
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! Nevertheless, some attribute dielectric with a significant sonic signature.
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.
Cable Burn In
Bi-Wiring
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 Bi-Wiring. As always it will be system dependent and subject to listener bias as to better or not.
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.
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
Bi-Wiring Bridging
Many Bi-Wire 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 Bi-Wire Bridge Mode Sounds Best?'. There FOUR possible 4 conductor Bi-Wire combinations plus the Tri-Wire variant:
- • None - Normal 4 conductor Bi-Wire
- • 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
A/C Wiring
Much ado is made in some circles about the inadequacy of 14ga wiring and how it will diminish dynamics.
14ga Copper wire has an ampacity of 28 amps. The U.S. National Electrical Code [NEC] rates 14ga THHN for 20A @ 75°C. Romex 14/2 is electrically equivalent to THHN. NEC limits 14ga to 15A circuits for a very adequate safety margin. See NEC 310.15(B)(16).
To find how much loss is incurred on a heavily loaded 14ga circuit, a SemiProfessional espresso machine, plugged into the first socket on a circuit and the only device, was measured. It has a 1600w heating element with a resistance of ≈8.25Ω or ≈14A current draw. The heating element is PID controlled. This duty cycle is a square wave and presents transients far in excess of anything in a HiFi system. Using a digital sampling oscilloscope [DSO], 100%, ≈50% and 0% duty cycle load voltages were recorded.
No load measured 117.81vrms, load 114.02vrms integrating samples over 1 period for periods
While the deltas in the numbers are large relative to the magnitudes, these are DC values. Power transformer primary inductance makes them irrelevant. A 125w tube amp power transformer has a DC resistance of ≈700mΩ, which would allow a peak current of ≈250A on 120VAC were it not for the inductance.
People prattle on about A/C line current draw as though it is continuous. Musical peaks are asynchronous to the line frequency! The image shows 3 samples: Bass Drum, A/C Line Hz and a snippet from Jefferson Airplane's "White Rabbit". In the drum sample, the peak signal is out of phase with the line. All power is supplied from the capacitor filter bank that was charged on the previous half cycle. In the "White Rabbit" snippet, the signal is primarily out of phase with the line. Later, the signal is as much in as out of phase with the A/C.
Mains Voltage
50+ years on since 120V became the U.S. nominal in 1967, line voltages are still all over the map.
Many manufacturers still rate equipment @ 1945 US standard 117V or 115V for the North American market. A 5% overvoltage may be detrimental, particularly with older tube gear. A
Bucking Transformer can reduce the voltage and risk.
Conclusion