> The whole idea of impedance matching in audio..... was to balance the line and match the line to 600 Ohms. This minimizes losses and pickup of noise.
Uh, no?
Impedance and balance are different things.
Lowest loss of voltage requires infinite load impedance.
Least voltage pickup requires a zero impedance.
Impedance "matching" is important when audio power is VERY expensive and limited by source impedance.
Early telephone systems had no amplifiers (other than the carbon-mike). The source (microphone) has an impedance. To get the most of this small power out of the mike and into a load, you "match".
Even when vacuum-tubes came, they were not that powerful and VERY expensive. Power out of things generally, and triodes particularly, is limited by internal impedance. Once again, you get the most load-power with "match".
(You might be thinking: tubes have high input impedance. Yeah, so we use step-up transformers for "free voltage gain". What matches? Actually the tube input capacitance at the highest frequency specified, complicated by transformer reactances at high impedance. So while it is not a simple resistive "match", the idea is the same.)
An ideal long transmission line has zero series resistance, zero leakage, zero capacitance, zero inductance. Real lines have some of everything. For low frequency, you "match" the geometric-mean of series and shunt resistance; but anything better than soggy paper has such a broad range between series and shunt resistance that it hardly matters above dozens of ohms. For high frequency you get squeezed between inductance and capacitance, which usually force you toward the 100-1K ohm range.
Very long (relative to a wavelength) lines are terminated to kill reflections. There is "NO" quality-audio situation where reflections matter. The miles of round-trip path-length needed to hear an echo also attenuate the echo.
Without reflections, the "best" way to drive most audio lines is with a low non-Zero source impedance and a very high load impedance. This also leads to simple-splitting: just add loads in parallel like holiday lights. There is a long-broadcast-line convention for 50 ohm source and 1Meg load. In small-studio work we often run 22r-470r source and 10K-50K load.
Since the 1930s, gain has been cheap. And cheaper again in the 1950s and 1970s. "Modern" stuff does NOT need matching, though into the 1960s much stuff clung to match-load convention to replace older gear without confusion. Low-Z sources are standard, though watch the difference between "output impedance" (may be 47r) and "minimum load impedance" (may be 1K).
> I want to have a 1:1 input transformer
The transformer "reflects" whatever it sees, although there is a "design goal" impedance which it works best at.
You want primary Z higher than source Z. Sound-card is likely to be low-Z and able to drive 600r or higher. It may be cleaner with higher Z.
You want secondary Z <= actual load, which is a resistor-pot network around 50K.
600:10K gives 1:4 voltage step-up. Input impedance may be 600 ohms near 20Hz, more like 3K over most of the audio band. Works. 600 ohms is a heavy load for some chips.
600:600 also works, unity voltage.
10K:10K works, and is going to be many-K impedance all across the audio band.