Nordost 1.5m SPDIF RCA- BNC Dual Monofilament Silver Plated 99.9999%OFC Ferrites
- Condition: Vom Verkäufer generell überholt
- Price: 149.29 EUR
- Status: unsold
- Item number: 145121641565
- Seller: audio-maniacs (1043|100.0%)
- Seller information: non commercial
- Item location: Hove, East Sussex
- Ships to: GB
- Shipping: 3,0 EUR
- on EBAY
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Description
Nordost 75 Ohm Silver HD SPDIF cable - rare RCA to BNC ideal for CHORD, NAIM LINN DACs etc. We also added a screen and two Wurth High-Frequency Ferrite beads to reduce noise. This is a unique construction to us. We are continually innovating to improve sound quality. It preserves the characteristic fast Nordost sound but eliminates effects of ground plane noise, RFI, etc., on the sound. Tested with the Chord DAVE and Qutest. This is a coaxial DUAL micro monofilament silver-plated 99.9999% OFC - 75 Ohm cable from one of the top brands in audio cables. (YES, THAT IS SILVER-PLATED 6 NINES OXYGEN FREE COPPER) The dual micro-monofilaments are the two plastic filler wires that space the silver-plated conductor from the middle of the FEP tube, thus providing a mostly air dielectric - improving performance. Brand new BNC connectors - Yarbo Audiophile BNC - gold plated copper. Original Nordost 75Ohm RCA. We have repackaged the cable, improved the strain relief, treated the connectors with Deoxit, thoroughly tested, and burned in the cable. These cables were originally sold as 75 Ohm cables in a bundle of three for component video - manufacturers just sold a single version of the same cable for digital SPDIF. (The specification for SPDIF and Component Video is identical) They are precisely the same, just with different labels. This means you get a fabulous quality Nordost cable at a bargain price. n.b. The Chord Qutest is NOT included in the sale, obviously! 1.5m is the minimum length that an SPDIF cable should be – see explanation below. From Nordost This new design introduces more air space between the conductor and the FEP insulation reducing dielectric contact by more than 85%. The result is a cable with much lower capacitance and resistance, resulting in higher signal speed and resolution. Why SPDIF cables should be 1.5m long. · When the SPDIF signal is launched into the cable from the Transport, it is essentially a voltage square wave consisting of rising edges and falling edges. These edges are no more than voltage transitions from about –250mV to +250mV, the rising edge transitioning from minus voltage to plus voltage, and the falling edge transitioning from plus voltage to minus voltage. When an edge transitions, it can be described as having a rise-time or fall time. This is the time for the signal to transition from 10% to 90% of the entire voltage swing. (note that this DOES Not happen instantaneously) · The rise time is important because this causes reflections on the transmission-line. If the rise time were very slow, say 50 nanoseconds, then there would be no reflections on the transmission-line unless it was extremely long. · Alternately, if the rise-time were less than 1 nanosecond, reflections would occur at every boundary, such as the connection from the circuit board to the wires that go to the connector. · Typical stock Transports have around 25 nanosecond rise times. The primary concern for the manufacturer is to pass FCC regulations for emissions and electromagnetic interference and make the interface reliable. When the regulatory testing is done, they attach very inexpensive, inferior cables and measure the emissions. To insure that the manufacturer passes these tests, they take several precautions. One is designing in the slower than necessary 25 nanosecond rise-time. Another is inserting various filters in the Transport to eliminate high frequencies from the signal. As a result of these choices, there is a hazard created by using too short a digital cable. It is a result of the slow rise time. · When a transition is launched into the cable, it takes a period of time to propagate or transmit to the other end. This propagation time is somewhat slower than the speed of light, usually around 2 nanoseconds per foot, but can be longer depending on the dielectrics used in the digital cable. When the transition reaches the end of the transmission line (in the DAC), a reflection can occur that propagates back to the driver in the Transport. Small reflections can occur in even well matched systems. When the reflection reaches the driver, it can again be reflected back toward the DAC. This ping-pong effect can sustain itself for several bounces depending on the losses in the cable. It is not unusual to see 3-5 of these reflections before they finally decay away, particularly when using the best digital cables, which are usually low-loss. · So, how does this affect the jitter? When the first reflection returns to the DAC, if the transition already in process at the receiver has not been completed, the reflection voltage will superimpose itself on the transition voltage, causing the transition to shift in time. The DAC will sample the transition in this time-shifted state, and there you have jitter. · Let’s look at a numerical example: · If the rise time is 25 nanoseconds and the cable length is 3 feet, then the propagation time is about 6 nanoseconds. Once the transition has arrived at the receiver, the reflection propagates back to the driver (6 nanoseconds), and then the driver reflects this back to the receiver (6 nanoseconds) = 12 nanoseconds. So, as seen at the receiver, 12 nanoseconds after the 25 nanosecond transition started, we have a reflection superimposing on the transition. This is right about the time that the receiver will try to sample the transition, right around 0 volts DC. Not good. Now if the cable had been 1.5 meters, the reflection would have arrived 18 nanoseconds after the 25 nanosecond transition started at the receiver. This is much better because the receiver has likely already sampled the transition by this time. Burn In 48 Hours burn in using the Tara Labs Cascade Burn in file – from their website…“The new CASCADE noise burn-in disc is a proprietary combination of white noise with frequency tone bursts and pink noise mixed at different levels. However, what makes it effective is a series of descending and ascending (cascading) multi-octave square sweeps for better and more complete results than any other “burn-in” discs that have been made to date. The CASCADE noise burn-in disc may be used with an audio electronic component and with an audio cable, including cables with attachments such as batteries or filter networks. Before and after results will be obvious with any of these cables.”
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