Hi guys,
Yes, I meant L-R as in inductor-resistor. Linkwitz-Riley is just a filter shape like Bessel or Butterworth anyway, they come in all orders.
Anyway let's run some numbers on that. The relevant measurement is 12.5H plate to plate. At 100Hz that has a reactance of 7850 ohms, at 50Hz, 3925 ohms, and at 25Hz, 1963 ohms.
DVMs are notorious for failing to measure iron cored inductors properly, but these figures are in the right sort of ballpark so we'll press ahead. Let's say the amp is called to deliver 400W at 33Hz, the low B on a 5 string bass. 400W into an 1100 ohm load is around 660V and 600mA, both RMS. Now with 660V at 33Hz across it, the magnetizing inductance will pass 250mA RMS.
So it will be starting to steal a little power from the speakers. But bearing in mind that eight 6550s can supply something in the region of 1.2A of current, there's plenty to go round.
Now remove half of the tubes and calculate what will happen when you hit that low B again.
Yes, I meant L-R as in inductor-resistor. Linkwitz-Riley is just a filter shape like Bessel or Butterworth anyway, they come in all orders.
Anyway let's run some numbers on that. The relevant measurement is 12.5H plate to plate. At 100Hz that has a reactance of 7850 ohms, at 50Hz, 3925 ohms, and at 25Hz, 1963 ohms.
DVMs are notorious for failing to measure iron cored inductors properly, but these figures are in the right sort of ballpark so we'll press ahead. Let's say the amp is called to deliver 400W at 33Hz, the low B on a 5 string bass. 400W into an 1100 ohm load is around 660V and 600mA, both RMS. Now with 660V at 33Hz across it, the magnetizing inductance will pass 250mA RMS.
So it will be starting to steal a little power from the speakers. But bearing in mind that eight 6550s can supply something in the region of 1.2A of current, there's plenty to go round.
Now remove half of the tubes and calculate what will happen when you hit that low B again.
Comment