2ND look, you're right, that doesn't make any sense. Like saying it doesn't matter what the voltage across a ...
There's a lot of unstated baggage and implications in that article. If you're not clued-in to what's unsaid, you'll mis-read what
is said.
You apply an input signal to a power amp; whether the amp acts like a current source or a voltage source depends on which quantity tracks the input signal in the face of a changing load impedance.
Transistor power amps tend to act like voltage sources; users assume the amp will output more power if they use a 4Ω load instead of an 8Ω load. Because the amplifier tries to maintain a constant voltage output (ratio) based on the input signal, halving the load impedance doubles the current, and double-current times same voltage equals double power.
You know that doesn't work well with tubes, and that we try to match whenever possible because mismatch in either direction yields less power. Mismatching a transistor amp be attaching a higher load yields less output power (but in a predictable way that's often exploited by headphone users), while mismatching lower yields more power until you burn out the output transistors.
It doesn't help that tubes or transistors can be configured as voltage or current sources, based on the nature of the device and how feedback is (or isn't) applied around the amplifier. And discussions like the article assume theoretical perfect sources when in reality we run into limitations pretty quickly.
At a certian frequency speaker A is 10 ohms and speaker B is 20 ohm. ... in series ... there's 50W across the 30 ohm load.
... I came up with:
Speaker A 16.6W
Speaker B 33.3W
If power stays constant, then yes, the power is divided as you've shown.
For a series circuit, you'd remember that there's only 1 path for current so all elements of the circuit see the same current. Therefore the one with the highest impedance has the greatest voltage drop and therefore the greatest power (output or dissipation).
... I then imagined them in parallel. ... 50W across the 6.666 load
...
Speaker A 33.3W
Speaker B 16.6W
Yes. For a parallel circuit, each branch sees the same applied voltage between their terminals (because each branch has their terminals connected together where the paths split). Now there will be less current in the high impedance path, so same voltage times less current equals less power. Now the low impedance path has the greatest power output/dissipation.
So one way one speaker is getting twice the watts because it's at twice the voltage, the other way the other speaker gets twice the watts because it's at twice the current
What(if anything) does this mean?(besides I have too much time on my hands
)
You have confirmed for yourself what I posted originally.

All that's happening is you are re-discovering fundamental electrical principles known as Kirchhoff's Laws, Ohm's Law and the equation for power.