it seems like the ELR of 6l6 tubes is 3800 ohms with a plate voltage of 360vdc
While 6L6Gc are 5600 with a plate voltage 450vdc
Does it change the effective ELR of the 6L6Gc if you run them at 365vdc on the plates like in a vibrolux 6G11?
The output tube doesn't have "ELR" as you've described it. In fact, if you look at the plate curves for the 6L6, above some low plate voltage, and individual gridline turns and runs mostly horizontal, indicating a
very high internal plate resistance. But we really don't care what a pentode or beam power tube's internal resistance is; it doesn't matter the way a triode's internal plate resistance does.
Instead, think of a pentode or beam power tube as a "voltage-controlled current source". Applied grid voltage causes these tubes to pass more/less plate current, and the differing position of the grid voltage lines on the sheet show this. Also recall this when noting that you generally don't see Mu or plate resistance for the tube listed, but you
always see Gm for these tubes. For a 6L6, 6,000 micromhos is typical, but Europeans specify this as 6mA/V (same quantity with a different way of expressing the units).
You could have a short hunk of wire with an ammeter between the power supply and 6L6 plate, effectively 0Ω load resistance. And for a changing grid voltage, you will see a changing plate current. But that's not useful in an amp. You need a load impedance through which that plate current flows so that, in accordance with Ohm's Law, a voltage can be developed across that load impedance. And Power = Voltage * Current, so now you have power developed across the primary winding of the OT, to be passed to the secondary.
What load impedance to use? Depends on the supply voltage, the limit of plate current for the tube used, and how much power you need.
If (especially screen) supply voltage is low, plate current swing will be low and you might need a bigger load impedance to develop a bigger voltage swing to hit your power target; this accounts for higher load impedance at lower plate voltages.
If you don't need as much power, you can keep supply voltage and idle conditions the same and use a smaller load impedance. Smaller load "R" when plugged into Ohm's Law (Volts = Current * Resistance) yields smaller plate voltage swing. Power is then smaller because (Smaller Volts) times (Same Current) equals Smaller Power. This matches the somewhat lower power output for the 3.8kΩ condition compared to the 6.6kΩ condition for the same supply voltage.
In the third condition listed, the designers went further into class AB. The supply voltage, idle current and bias went up. Idle current is ~32% more than the other conditions. But load impedance went down compared to the first condition, which allowed a max-signal plate current 59% greater than the first condition. Power output nearly doubles.