If this is your first visit, be sure to check out the FAQ by clicking the link above. You may have to register before you can post: click the register link above to proceed. To start viewing messages, select the forum that you want to visit from the selection below. |
|
|
Thread Tools | Display Modes |
#121
|
|||
|
|||
The disappearance of darkness
In article , Me
wrote: The very reactive load of these speakers may well mean that cable resistance becomes an audible factor, and cable inductance/capacitance becomes significant (impedance is very low at high frequencies, and very high at low frequencies). speakers are a reactive load. wire is a resistive load. inductance and capacitance of straight wire is *so* incredibly tiny that it can be assumed to be zero (nanohenries & picofarads versus milliohms). ESL tend to be /much/ more reactive than conventional speakers - IIRC, impedance can vary from 1 ohm to 100 ohm depending on frequency. They were very effective at frying conventional amplifiers. even at 1 ohm inductance, different speaker wire isn't going to matter. the differences are a tiny fraction of an ohm. |
#122
|
|||
|
|||
The disappearance of darkness
On 2013.05.14 12:10 , Peter Irwin wrote:
Me wrote: Even well regarded companies like B&W IMO make some extremely bold claims about their technology, usually along the lines of acoustic / mechanical properties of some very expensive and hard to copy substance which is very close to unobtanium. They then go on to justify this based on things like linear accuracy of waveform / THD at high frequencies, when apparently the human auditory system can't even discern the difference between a sine wave and a square wave at about 8KHz or higher. While it is true that you can't hear ultrasonic harmonics, the same distortion mechanisms produce intermodulation distortion. It is probable that most tweeters produce audible IM products in the midrange based on high frequency input signal in at least some real world conditions. Practically any tweeter will have audible IM under contrived conditions. (Feed the tweeter with 19khz and 20khz at a fairly high level and while you may not hear those tones, you will hear the 1khz difference tone.) Your ears may not hear the driving tones but the constructive/destructive product is easily heard. (aka: beat). -- "A Canadian is someone who knows how to have sex in a canoe." -Pierre Berton |
#123
|
|||
|
|||
The disappearance of darkness
On 2013.05.14 06:28 , Eric Stevens wrote:
On Mon, 13 May 2013 19:32:22 -0400, Alan Browne wrote: On 2013.05.09 02:28 , nospam wrote: In article , R. Mark Clayton wrote: Indeed one of the more sensible Hi-Fi mags tested regular mains cable against a group of expensive speaker cables. Virtually no difference. I did use [cheap] chunky speaker cable for my mains, but at full pelt they can be carrying quite a lot of current (10A+). i got my speaker cable at a hardware store. 14 gauge wire is 14 gauge wire. there's nothing special about 'audiophile cable.' it's the same stuff, but with a nicer looking insulation and a significantly higher price. Not quite true. For example the more recent fad is "oxygen free" copper cable which has a _measurably_ lower resistance over a given length. It's not a recent fad: I've been using it for +25 years. "Audiophiles" can rejoice because they can ACTUALLY MEASURE THE LOWER RESISTANCE of their expensive cable v. lesser stuff. (The fact that nobody can _hear_ the difference sails way over their heads). I use it to connect my 'current dumping" Quad 606 amplifier to my Quad ESL63 speakers and I can certainly hear the difference. It's not blindingly obvious but using any one of several (vinyl) test records I was able to demonstrate an audible difference via several double blind tests. If you can't hear the difference it may say more about your equipment than the cables. The difference in resistance is negligible for the same gauge and length. If the 'other' cable was truly limiting current to the point of affecting sound, then you would have done as well by just going to a fatter gauge ordinary wire. -- "A Canadian is someone who knows how to have sex in a canoe." -Pierre Berton |
#124
|
|||
|
|||
The disappearance of darkness
On 2013.05.13 20:29 , nospam wrote:
In article , Alan Browne wrote: Indeed one of the more sensible Hi-Fi mags tested regular mains cable against a group of expensive speaker cables. Virtually no difference. I did use [cheap] chunky speaker cable for my mains, but at full pelt they can be carrying quite a lot of current (10A+). i got my speaker cable at a hardware store. 14 gauge wire is 14 gauge wire. there's nothing special about 'audiophile cable.' it's the same stuff, but with a nicer looking insulation and a significantly higher price. Not quite true. it's definitely true. it's all snake oil with a huge price tag for suckers who fall for the deceptive marketing. No ****. Don't you recognize sarcastic posts for what they are? -- "A Canadian is someone who knows how to have sex in a canoe." -Pierre Berton |
#125
|
|||
|
|||
The disappearance of darkness
In article , Alan Browne
wrote: "Audiophiles" can rejoice because they can ACTUALLY MEASURE THE LOWER RESISTANCE of their expensive cable v. lesser stuff. (The fact that nobody can _hear_ the difference sails way over their heads). I use it to connect my 'current dumping" Quad 606 amplifier to my Quad ESL63 speakers and I can certainly hear the difference. It's not blindingly obvious but using any one of several (vinyl) test records I was able to demonstrate an audible difference via several double blind tests. If you can't hear the difference it may say more about your equipment than the cables. The difference in resistance is negligible for the same gauge and length. If the 'other' cable was truly limiting current to the point of affecting sound, then you would have done as well by just going to a fatter gauge ordinary wire. exactly, and save a significant amount of money in the process. |
#126
|
|||
|
|||
The disappearance of darkness
On Tue, 14 May 2013 14:46:03 -0400, nospam
wrote: In article , Eric Stevens wrote: For example the more recent fad is "oxygen free" copper cable which has a _measurably_ lower resistance over a given length. It's not a recent fad: I've been using it for +25 years. so has everyone else. most wire is oxygen free, and silver is a better conductor anyway but the name doesn't sound as cool. "Audiophiles" can rejoice because they can ACTUALLY MEASURE THE LOWER RESISTANCE of their expensive cable v. lesser stuff. (The fact that nobody can _hear_ the difference sails way over their heads). I use it to connect my 'current dumping" Quad 606 amplifier to my Quad ESL63 speakers and I can certainly hear the difference. you may think you can, but you can't. differences in fractions of an ohm make no difference and are not audible. It was a long time ago and my memory is coming back to me. I am using a low-oxygen cable but not the fancy stuff that the audiophiles pay heaps for. I can't the conductor cross section but it is generous. What I was testing against was a fancy cable where the in and out conductors each employed three sets of wires which were interwoven. I think that this may have been the conductor which achieved fame by blowing up a Naim amplifier as soon as it was connected. Fortunately the Quad 606 is "Unconditionally stable with any load and any signal". In any case, I could hear the difference and dumped the fancy cable. It's not blindingly obvious but using any one of several (vinyl) test records I was able to demonstrate an audible difference via several double blind tests. If you can't hear the difference it may say more about your equipment than the cables. of course it's not blindingly obvious, because there is no difference to be heard. if you guessed correctly, it was pure luck. It was much better than pure luck. Cable impedance does play an important part as I am sure you know. Only with zero impedance does the amplifier have 100% control of the speaker. Quad puts it as "For optimum performance it is necessary to ensure that the impedance of the cable is small relative to the impedance of the load". This makes sense as the amplifier is able to poke out more than 10 amps under the right conditions. In fact what I think I may have been hearing was the effect of the unusually high reactance of the quite long interwoven cable. -- Regards, Eric Stevens |
#127
|
|||
|
|||
The disappearance of darkness
On Wed, 15 May 2013 08:28:28 +1200, Me wrote:
On 15/05/2013 8:21 a.m., nospam wrote: In article , Me wrote: "Audiophiles" can rejoice because they can ACTUALLY MEASURE THE LOWER RESISTANCE of their expensive cable v. lesser stuff. (The fact that nobody can _hear_ the difference sails way over their heads). I use it to connect my 'current dumping" Quad 606 amplifier to my Quad ESL63 speakers and I can certainly hear the difference. you may think you can, but you can't. differences in fractions of an ohm make no difference and are not audible. The system that Eric refers to doesn't use conventional speakers - "ESL" = ElectroStatic Loudspeaker. i checked the equipment he mentioned but it doesn't matter. The very reactive load of these speakers may well mean that cable resistance becomes an audible factor, and cable inductance/capacitance becomes significant (impedance is very low at high frequencies, and very high at low frequencies). speakers are a reactive load. wire is a resistive load. inductance and capacitance of straight wire is *so* incredibly tiny that it can be assumed to be zero (nanohenries & picofarads versus milliohms). ESL tend to be /much/ more reactive than conventional speakers - IIRC, impedance can vary from 1 ohm to 100 ohm depending on frequency. They were very effective at frying conventional amplifiers. Quite right, but this applies to most electrostatic speakers. the most that can happen with audiophile wire is that it will be a fraction of an ohm lower (and that's being incredibly optimistic), which isn't going to make any difference. this is measurable. it's not a question of can you hear it. for example, 25 feet of 14 gauge wire is just 0.063 ohms. the impedance of the speaker is typically 8 ohms. that's over 100x as much. http://www.cirris.com/testing/resistance/wire.html If he says he could hear the difference with this setup - then I believe it. if the electrical properties of the wire are the same, the audio will be the same. it's basic physics. moving the speaker closer or further away from the wall will have far more of an effect than any cable could ever have, but you can't sell that. -- Regards, Eric Stevens |
#128
|
|||
|
|||
The disappearance of darkness
In article , Eric Stevens
wrote: "Audiophiles" can rejoice because they can ACTUALLY MEASURE THE LOWER RESISTANCE of their expensive cable v. lesser stuff. (The fact that nobody can _hear_ the difference sails way over their heads). I use it to connect my 'current dumping" Quad 606 amplifier to my Quad ESL63 speakers and I can certainly hear the difference. you may think you can, but you can't. differences in fractions of an ohm make no difference and are not audible. It was a long time ago and my memory is coming back to me. I am using a low-oxygen cable but not the fancy stuff that the audiophiles pay heaps for. I can't the conductor cross section but it is generous. in other words, standard wire. What I was testing against was a fancy cable where the in and out conductors each employed three sets of wires which were interwoven. I think that this may have been the conductor which achieved fame by blowing up a Naim amplifier as soon as it was connected. Fortunately the Quad 606 is "Unconditionally stable with any load and any signal". In any case, I could hear the difference and dumped the fancy cable. woven wire looks nice. electrically it's meaningless. It's not blindingly obvious but using any one of several (vinyl) test records I was able to demonstrate an audible difference via several double blind tests. If you can't hear the difference it may say more about your equipment than the cables. of course it's not blindingly obvious, because there is no difference to be heard. if you guessed correctly, it was pure luck. It was much better than pure luck. it was luck. electrically, the cable is the same, therefore no difference to be heard. Cable impedance does play an important part as I am sure you know. the impedance of wire is for all intents, zero. as noted before, 25' of 14ga wire is 0.063 ohms and any reactive component is many orders of magnitude lower than that. Only with zero impedance does the amplifier have 100% control of the speaker. it's close enough to zero that it can be considered zero. Quad puts it as "For optimum performance it is necessary to ensure that the impedance of the cable is small relative to the impedance of the load". This makes sense as the amplifier is able to poke out more than 10 amps under the right conditions. the impedance of the wire *is* small relative to the load. the wire is 0.063 ohms and the load is nominally 8 ohms. even if the load drops to 1-2 ohms at certain frequencies, the wire is still insignificant. In fact what I think I may have been hearing was the effect of the unusually high reactance of the quite long interwoven cable. definitely not. what you were hearing was what you wanted to hear. |
#129
|
|||
|
|||
The disappearance of darkness
On Wed, 15 May 2013 01:55:14 -0400, nospam
wrote: In article , Eric Stevens wrote: "Audiophiles" can rejoice because they can ACTUALLY MEASURE THE LOWER RESISTANCE of their expensive cable v. lesser stuff. (The fact that nobody can _hear_ the difference sails way over their heads). I use it to connect my 'current dumping" Quad 606 amplifier to my Quad ESL63 speakers and I can certainly hear the difference. you may think you can, but you can't. differences in fractions of an ohm make no difference and are not audible. It was a long time ago and my memory is coming back to me. I am using a low-oxygen cable but not the fancy stuff that the audiophiles pay heaps for. I can't the conductor cross section but it is generous. in other words, standard wire. 'Good' standard wire. The bulk of the advantage is mechanical. What I was testing against was a fancy cable where the in and out conductors each employed three sets of wires which were interwoven. I think that this may have been the conductor which achieved fame by blowing up a Naim amplifier as soon as it was connected. Fortunately the Quad 606 is "Unconditionally stable with any load and any signal". In any case, I could hear the difference and dumped the fancy cable. woven wire looks nice. electrically it's meaningless. Not this lot. Three cores in, three cores out, the whole interwoven to form a six ply tube. As I said, the reactance was such that in the old days Naim amplifiers could not tolerate them even for milliseconds. It's not blindingly obvious but using any one of several (vinyl) test records I was able to demonstrate an audible difference via several double blind tests. If you can't hear the difference it may say more about your equipment than the cables. of course it's not blindingly obvious, because there is no difference to be heard. if you guessed correctly, it was pure luck. It was much better than pure luck. it was luck. electrically, the cable is the same, therefore no difference to be heard. Cable impedance does play an important part as I am sure you know. the impedance of wire is for all intents, zero. as noted before, 25' of 14ga wire is 0.063 ohms and any reactive component is many orders of magnitude lower than that. Note that I did not say 'resistance'. I said 'impedance' of which reactance is a factor. Only with zero impedance does the amplifier have 100% control of the speaker. it's close enough to zero that it can be considered zero. Quad puts it as "For optimum performance it is necessary to ensure that the impedance of the cable is small relative to the impedance of the load". This makes sense as the amplifier is able to poke out more than 10 amps under the right conditions. the impedance of the wire *is* small relative to the load. the wire is 0.063 ohms and the load is nominally 8 ohms. even if the load drops to 1-2 ohms at certain frequencies, the wire is still insignificant. In fact what I think I may have been hearing was the effect of the unusually high reactance of the quite long interwoven cable. definitely not. what you were hearing was what you wanted to hear. Double blind, remember. -- Regards, Eric Stevens |
#130
|
|||
|
|||
The disappearance of darkness
In rec.photo.digital.slr-systems nospam wrote:
In article , Eric Stevens wrote: For example the more recent fad is "oxygen free" copper cable which has a _measurably_ lower resistance over a given length. It's not a recent fad: I've been using it for +25 years. so has everyone else. most wire is oxygen free, and silver is a better conductor anyway but the name doesn't sound as cool. "Audiophiles" can rejoice because they can ACTUALLY MEASURE THE LOWER RESISTANCE of their expensive cable v. lesser stuff. (The fact that nobody can _hear_ the difference sails way over their heads). I use it to connect my 'current dumping" Quad 606 amplifier to my Quad ESL63 speakers and I can certainly hear the difference. you may think you can, but you can't. differences in fractions of an ohm make no difference and are not audible. Except when they do make a difference of course. Such as the notorious case of some amps when driving electrostatic loudspeakers through unusually low resistance cables becoming unstable and distorting because they needed the very slight cable resistance to stay stable with an ELS load. IIRC it was some early models of NAIM amps. -- Chris Malcolm |
Thread Tools | |
Display Modes | |
|
|
Similar Threads | ||||
Thread | Thread Starter | Forum | Replies | Last Post |
[PIC] Between the Light and the Darkness | jimkramer | 35mm Photo Equipment | 12 | February 23rd 09 11:53 AM |
Framing in darkness | steamer | Digital Photography | 10 | January 31st 08 04:59 PM |
Lightness / Darkness of Images | Dave W | Digital Photography | 2 | December 3rd 05 05:55 PM |