@ Langston: Let's say it is supposed to..... It won't and it can't, but if it was a very simple filter the differences would be worse by far.
The LAB fP is not a good comparison, as it (depending on the way you look at the design) has an active, dynamical filter circuit.
The K10 obviously has a lp filter of pretty high order, making me think about phase issues up there. Do you have some phase measurements too?
@ Bink:
Michael 'Bink' Knowles wrote on Sat, 16 December 2006 22:14 |
Quote: | ...Sound is "tighter"...
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Would this observation be measurable as a faster rise time? Just curious.
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I'm not the original poster of your quote, but I dare to answer anyways.
I don't think so. You can calculate, how fast of a rise time is needed for that power in bass range. I don't think that there is ANY current design that would be limited by the rise time/slew rate in bass range. There WOULD be limitations with SOME designs in HF range, but OTOH no one needs 2x5kW at HF from one amp, so the demands up there aren't that high.
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How much steady state power (24/7/365) can it deliver at 240v in bridge mode? Willing to guess?
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I did not measure the K10 for that, but I can tell from the old DigAm7000 (which couldn't be bridged) that it would do 2x500W continous at any load (not below 2 ohms!) 24/7. That's enough to keep up the rated power for typical rock music, but not with 'electronic music' (I know that from experience). The K-series will have a similar design, allowing maybe 800-1000W per channel at any load. That means they'd have to step down the output power if the RMS would be too high for a too long time.