khaliss
Active Member
Hi All,
I finally took the plunge & acquired a used pair of Martin Logan Classic ESL-9s (to upgrade my ESLs, I just love the sound of electrostatic speakers). Although I was already 90% happy with my previous speakers (& setup), I always wondered about the concept of true bi-amping, and how it may have a "real" impact on some type of speakers... in particular, electrostatic speakers (in this case, the ESL9 (on paper) can drop as low as 0.8 ohms(?) When paired with a certain type of amplifier (class A/B, but has class-A bias... as claimed by the manufacturer).
Speakers: Martin Logan Classic ESL-9
Configuration: horizontal bi-amplification
Amplifiers: dual Musmys E-406 (XLR/balanced)
Preamp: Musmys C2860+ (XLR/balanced)
DAC: Topping E70 Velvet (via USB)
Streamer: PC (intel i3 13th-gen, 16GB DDR4)
Tube/EQ: Douk Audio T8-pro (GE tubes)
Technical Specs of Musmys E-406 amplifier:
* Rated continuous output power (20HZ-20000HZ)
* Pure Class A: 60W/4 ohm output
* Pure Class A: 30W/8 ohm output
** Class AB: 320W/4 ohm output
** Class AB: 180W/8 ohm output
* Frequency response: Continuous rated output: 20-20000Hz +0 -0.2db
* 1W output :05-160000HZ +0 -3dB
* S/N signal-to-noise ratio: 120dB across the entire frequency band
* Input impedance: 40K (balanced input), 20K (RCA input)
* Input sensitivity: 0.87V rated continuous average output 0.11V output 1 watt power
* Distortion of 0.005%
* Amplification factor of 28dB
Martin Logan ESL-9 technical specs:
Frequency Response = 34–23,000 Hz ±3dB
Sensitivity = 90 dB/2.83 volts/meter
Impedance = 4 Ohms, 0.8 at 20kHz Compatible with 4, 6, or 8 Ohm rated amplifiers.
Crossover Frequency = 380Hz
High Frequency Transducer = XStat™ CLS™ electrostatic transducer » Panel Dimensions: 44" x 9.2" (112 x 23cm) » Radiating Area: 405 in² (2,576 cm² )
Low Frequency Transducer = Two 8” (20.3 cm) cast basket, high excursion, rigid aluminium cone woofers with extended throw drive assembly, non-resonance asymmetrical chamber format
I just got these all setup yesterday... one of the ESL-9s though has an issue, it had a lower output of -6 to -8db compared to the other electrostatic transducer panel (no problems with the woofer section), so I had to compensate the difference by balancing them out using software (HighPass Filter setting via EQ-APO). Anyways, that's another story for another day.
video:
(background music had to be changed, as youtube restricts the actual track I was playing)
Measurements:
I had AI put together the wall of text below, as it was easier to put my thoughts into something that is a bit more technical for the audience to dive on & maybe share some thoughts/opinions?
Contemplating on the technical advantages of running a horizontal bi-amp configuration when pairing high-bias Class-A/AB amplifiers with highly capacitive electrostatic panels, specifically the Martin Logan Classic ESL 9s.
Now, from a strict engineering standpoint, a fixed idling current (Iq) dictated by physics usually means that when load impedance halves, the pure Class-A wattage envelope actually cuts in half because the speaker demands more current per volt. Seeing a manufacturer claim that the Class-A window doubles into 4 Ohms usually points to either a sliding/dynamic bias design that scales current draw with the input signal, or marketing that treats the Class-A envelope as a fixed percentage of total linear current capability.
But here is where horizontal bi-amping turns this mathematical debate into a moot point(?)
If running a single amplifier:
By isolating the panels, it eliminates power supply sag and intermodulation distortion induced by heavy bass transients. The delicate, highly revealing electrostatic panels receive a pristine, low-distortion signal without any transistor glare, allowing the system to fully realize the transient speed and transparency electrostatics are famous for.
Curious to hear thoughts from those who have modeled or measured distortion profiles on high-bias amps when isolated from low-frequency current draws(?)
I finally took the plunge & acquired a used pair of Martin Logan Classic ESL-9s (to upgrade my ESLs, I just love the sound of electrostatic speakers). Although I was already 90% happy with my previous speakers (& setup), I always wondered about the concept of true bi-amping, and how it may have a "real" impact on some type of speakers... in particular, electrostatic speakers (in this case, the ESL9 (on paper) can drop as low as 0.8 ohms(?) When paired with a certain type of amplifier (class A/B, but has class-A bias... as claimed by the manufacturer).
Speakers: Martin Logan Classic ESL-9
Configuration: horizontal bi-amplification
Amplifiers: dual Musmys E-406 (XLR/balanced)
Preamp: Musmys C2860+ (XLR/balanced)
DAC: Topping E70 Velvet (via USB)
Streamer: PC (intel i3 13th-gen, 16GB DDR4)
Tube/EQ: Douk Audio T8-pro (GE tubes)
Technical Specs of Musmys E-406 amplifier:
* Rated continuous output power (20HZ-20000HZ)
* Pure Class A: 60W/4 ohm output
* Pure Class A: 30W/8 ohm output
** Class AB: 320W/4 ohm output
** Class AB: 180W/8 ohm output
* Frequency response: Continuous rated output: 20-20000Hz +0 -0.2db
* 1W output :05-160000HZ +0 -3dB
* S/N signal-to-noise ratio: 120dB across the entire frequency band
* Input impedance: 40K (balanced input), 20K (RCA input)
* Input sensitivity: 0.87V rated continuous average output 0.11V output 1 watt power
* Distortion of 0.005%
* Amplification factor of 28dB
Martin Logan ESL-9 technical specs:
Frequency Response = 34–23,000 Hz ±3dB
Sensitivity = 90 dB/2.83 volts/meter
Impedance = 4 Ohms, 0.8 at 20kHz Compatible with 4, 6, or 8 Ohm rated amplifiers.
Crossover Frequency = 380Hz
High Frequency Transducer = XStat™ CLS™ electrostatic transducer » Panel Dimensions: 44" x 9.2" (112 x 23cm) » Radiating Area: 405 in² (2,576 cm² )
Low Frequency Transducer = Two 8” (20.3 cm) cast basket, high excursion, rigid aluminium cone woofers with extended throw drive assembly, non-resonance asymmetrical chamber format
I just got these all setup yesterday... one of the ESL-9s though has an issue, it had a lower output of -6 to -8db compared to the other electrostatic transducer panel (no problems with the woofer section), so I had to compensate the difference by balancing them out using software (HighPass Filter setting via EQ-APO). Anyways, that's another story for another day.
video:
Measurements:
I had AI put together the wall of text below, as it was easier to put my thoughts into something that is a bit more technical for the audience to dive on & maybe share some thoughts/opinions?
Contemplating on the technical advantages of running a horizontal bi-amp configuration when pairing high-bias Class-A/AB amplifiers with highly capacitive electrostatic panels, specifically the Martin Logan Classic ESL 9s.
The Hardware & The Spec Riddle
Using a pair of Musmys E-406 dual-mono amplifiers (the massive Accuphase-inspired topologies utilizing 24 high-current MOSFETs and a heavy capacitor bank per chassis).Now, from a strict engineering standpoint, a fixed idling current (Iq) dictated by physics usually means that when load impedance halves, the pure Class-A wattage envelope actually cuts in half because the speaker demands more current per volt. Seeing a manufacturer claim that the Class-A window doubles into 4 Ohms usually points to either a sliding/dynamic bias design that scales current draw with the input signal, or marketing that treats the Class-A envelope as a fixed percentage of total linear current capability.
But here is where horizontal bi-amping turns this mathematical debate into a moot point(?)
The Real-World Challenge: ESL 9 Impedance
The ESL 9 is a hybrid design: dual 8-inch aluminum woofers handling everything below 380 Hz (nominal 4 ohms), and a massive XStat electrostatic panel handling everything above 380 Hz. Like all large capacitive panels, the impedance drops like a stone as frequency rises, bottoming out at a brutal 0.8ohms at 20 kHz.If running a single amplifier:
- The low-frequency woofers demand massive voltage swings and the lion's share of the current.
- This heavy low-end power demand constantly exhausts the amplifier's idling current, instantly kicking the amp out of its clean Class-A window and into Class-AB push-pull operation just to keep up with the bass.
Why Horizontal Bi-Amping can be a big advantage(?)
By dedicating one E-406 chassis strictly to the woofers (below 380 Hz) and a completely separate E-406 chassis to the electrostatic panels (above 380 Hz), this could fundamentally rewrite the system's thermodynamics and signal integrity.- Liberation from Bass Energy: The "panel amplifier" is completely decoupled from the heavy low-frequency lifting. Below 380 Hz, it sees an open circuit, meaning its power supply rails face virtually zero demand from the bass.
- The High-Frequency Power Realities: While the electrostatic panel's sub-1-Ohm impedance at 20 kHz technically compresses the amp's theoretical Class-A wattage ceiling, actual musical energy tapers off significantly in the upper registers.
Intent: Keeping the Panels in Pure Class-A
Whether the Musmys' true Class-A threshold under low impedance is 15 Watts or 60 Watts, horizontal bi-amping ensures that the panel amplifier stays anchored within its ultra-clean Class-A operational window 100% of the time.By isolating the panels, it eliminates power supply sag and intermodulation distortion induced by heavy bass transients. The delicate, highly revealing electrostatic panels receive a pristine, low-distortion signal without any transistor glare, allowing the system to fully realize the transient speed and transparency electrostatics are famous for.
Curious to hear thoughts from those who have modeled or measured distortion profiles on high-bias amps when isolated from low-frequency current draws(?)
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