So I fed ChatGPT Pro (paid) this prompt:
"consider the paper published Paper on Measurements of RCA Cables by Kunchur"
It wrote back this response which was clearly influenced by my prior interactions with it:
Yes—Kunchur’s 2021 RCA-only measurement paper is the relevant one: “An Electrical Study of Single-Ended Analog Interconnect Cables.”
It removes the most obvious flaw in his AES listening paper—comparing different RCA and XLR signal paths—but it still establishes only this:
- Different RCA cables can have measurably different noise pickup and time-domain responses.
- The reported reflection/deviation effects are driven by very-fast-edge tests, far beyond audio bandwidth.
- A measured difference is not evidence of an audible difference unless its magnitude is quantified at the receiving component under realistic source/load impedances and shown to survive an audio-bandwidth, level-matched comparison.
The potentially consequential finding is noise, not nominal resistance, capacitance, or the reflection plots. But that noise must be separated from ordinary system-specific ground-loop/RF pickup: cable routing, shield termination, connected equipment, and local RF environment can dominate it. The paper does not demonstrate that its microsecond-scale residual behavior produces an audible alteration of program material.
So it is fair to say: the paper shows RCA interconnects are not electrically identical; it does not demonstrate that the identified differences explain audible cable-quality differences. The paper’s own leap from microsecond behavior to audibility is especially unsupported by its measurements. iosrjournals.org
---
So I prompted again:
"do that analysis, ignoring any interactions with me."
It seems to have followed that advice:
Bottom line
This is a useful demonstration that three particular RCA interconnects have different electrical properties, especially RF pickup. It does
not demonstrate that their time-domain differences alter music audibly, nor that one is intrinsically “better” in normal audio use.
Its strongest result is:
unbalanced interconnect shielding and grounding can matter for noise pickup. Its central claim—microsecond-scale capacitive/reflection behavior as a likely explanation for audible cable character—is not established.
What the paper actually measures
It compares one 2 m cable each at roughly $500 (“S”), $50 (“M”), and <$5 (“G”), then measures RLC parameters, frequency response, pulse response, RF reflections, and noise pickup. The normal-audio test uses a 600 Ω source and 10 kΩ load. Under that condition, the measured frequency response is flat within ±0.03 dB and phase variation within ±0.06°—including the generic cable. iosrjournals.org
That result is important: for the stated, representative source/load condition, the paper finds no consequential conventional audio-band transfer error.
The major technical problem: frequency-dependent capacitance is not proof of nonlinearity
The paper says that dielectric behavior means a cable “cannot be represented by a fixed transfer function” and introduces history-dependent convolution as evidence. iosrjournals.org
That is incorrect reasoning.
A linear time-invariant network is
defined by its impulse response/convolution: it necessarily has output dependent on prior input history. Frequency-dependent capacitance, dielectric loss, dispersion, and dielectric absorption can all be represented by a fixed linear transfer function—typically a distributed RC model or a sum of RC branches.
To establish nonlinearity, the paper would need to show that the response changes with signal amplitude: e.g., measure intermodulation, harmonic distortion, or impulse/transfer response at several voltages with carefully controlled error. It does not do that. The 5 V pulse tests show that cables behave differently at RF; they do not show relevant nonlinear signal alteration at line level.
Why the pulse/reflection results do not support an audio conclusion
The reflection experiment uses 4 ns pulses and a 500 MHz measurement chain. That is an RF test, deliberately examining content tens to hundreds of MHz above audio. With a 100 Ω source and a 10 kΩ load—nearly open at RF—the cable is badly mismatched as a transmission line, so reflections are expected. The paper itself identifies a ~23.8 ns reflection period consistent with the cable round-trip delay. iosrjournals.org
That is real RF behavior. But it does not follow that a music signal is materially altered:
- Audio content does not contain 4 ns edges.
- A ~1–2 µs decay is associated principally with ultrasonic behavior; its existence alone says nothing about residual magnitude within 20 kHz.
- The paper’s own audio-band frequency-response result already constrains any linear, baseband effect.
- The relevant quantity would be the difference between cables after band-limiting to audio, referenced to program material, then tested for audibility.
Invoking microsecond auditory timing does not bridge that gap. Temporal discrimination or binaural timing acuity is not a general detector for arbitrarily tiny, mostly ultrasonic artifacts. The amplitude, spectrum, and masking relationship of the artifact must still be demonstrated.
The capacitance experiment is deliberately nonrepresentative
To magnify the capacitance effect, the paper uses a
1 MΩ source resistance, a 1 MΩ load, and doubles cable length to 4 m.
iosrjournals.org
That is legitimate as a sensitivity experiment, but it is not representative of the 600 Ω/10 kΩ audio connection subsequently called typical. It can show a difference in capacitance or loss behavior; it cannot, by itself, establish a relevant effect in ordinary line-level use.
Also, the paper infers a large frequency variation in the generic cable’s capacitance from a transfer measurement in that extreme high-impedance setup. An independent impedance/complex-admittance measurement across frequency, with calibration and uncertainty, would be needed before treating the inferred change as a material property of the cable rather than the full fixture.
Noise: the credible and potentially meaningful finding
The paper measures substantially different RF and audio-band noise voltages among the three cables. Its quoted ITU-R 468-weighted values are 25.3, 40.6, and 44.5 µV RMS for S, M, and G; the full 0–2.5 MHz figures for M and G are far larger because of RF pickup. iosrjournals.org
That is plausible and useful. Shield construction, source impedance, cable routing, ground reference, and the receiving equipment’s RF rejection absolutely can make an RCA interconnect behave differently in a given installation.
But the conclusion should be narrower than the paper’s:
- The test is a cable-plus-fixture-plus-local-RF-environment result, not a universal cable ranking.
- The DSO input is 1 MΩ with 500 MHz bandwidth—not an actual preamp input and not a measurement of the receiving device’s demodulated output.
- To claim audible RF effects, one must measure the audio-band output of representative receiving electronics while the interference is present, or demonstrate audibility under controlled conditions.
- The conclusion that shielding is more important than balanced topology is not supported by this experiment. A properly implemented balanced interface rejects common-mode interference through the receiver’s CMRR; measuring one well-shielded RCA cable does not test that mechanism. iosrjournals.org
The finding that the one single-point-shielded cable is direction-dependent is unsurprising and practically useful: shield termination and system grounding determine the best orientation. It is not evidence for directional conductor behavior. iosrjournals.org
Experimental-design limitations
The “grade” conclusion is heavily confounded:
| Claimed variable | Also changes between S, M, and G |
|---|
| Cable grade / price | dielectric, geometry, shielding, connector construction, gauge, channel spacing, shield termination |
| Direction | shield ground connection for M |
| Noise performance | test layout, local RF field, grounding, receiving impedance/bandwidth |
| Manufacturing quality | only one example of each cable class; no production sample replication |
A monotonic ranking across three deliberately chosen cables is not evidence that price or “audiophile grade” causes the claimed improvements. It is compatible with the simpler conclusion that these three designs differ, especially in shielding and RF behavior.
What would make the paper persuasive
A decisive follow-up would:
- Use several samples of each design and comparable cables differing in one construction variable at a time.
- Measure impedance and S-parameters over frequency with calibrated fixtures.
- Measure the actual output of representative preamps/power amps under injected, controlled RF exposure.
- Band-limit and level-match cable-difference residuals, then quantify them relative to masking thresholds.
- Run blinded listening tests on the specific, measured condition.
The paper contains real electrical observations, but it turns them into an audibility theory too quickly. Its evidence supports good shielding, sensible grounding, and avoidance of obviously poor or damaged RCA cables—not a general claim that expensive interconnects preserve musical transients better.