A two way passive crossover as an example separates the low frequency audio and the high frequency audio. It does so by placing magic resistors in line with the tweeters and with the woofers. The magic is that these resistors change resistance (impedance) with frequency.
For the tweeter we use a magic resistor that gets higher in impedance as the frequency decreases. At 10kHz this resistor might be 0 ohms, at 5kHz it might be 1 ohms, and at 2.5kHz it might be 4 ohms and at 1.25kHz it is 12 ohms, at 612Hz it is 48 ohms; and so on. If we are using a 4 ohm tweeter and the magic resistor hits 4 ohms at 2.5kHz, this means only half of the power will be going to the tweeter at 2.5kHz vs when the magic resistor isn't active. This half power point is called the -3dB point or the crossover point. Also notice that as the frequency halves, the impedance of the magic resistor goes up by 4x. This indicates a 6dB per octave crossover. In a 12dB per octave crossover the magic resistor goes up by 16x per frequency half.
The same thing happens with the woofer, but the magic resistors used for this work the other way. As frequency goes up by 2x, the impedance goes up by 4x. (6db per octave).
So with our 2 way component set lets do an example of what happens with impedance vs freq. We will use a 2kHz crossover point and a 12dB per octave crossover for high and low pass. We will also use 4 ohm woofers and tweeters. We are going to ignore impedance rise of the drivers themselves for this example. This will demonstrate how a properly designed component set can maintain 4 ohms at any frequency even.
Frequency Impedance of Woofer + magic R Impedance of Tweeter + magic R Parallel impedance (what amp sees)
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31 Hz 4 ohms 12 Mohm 4 ohms
63 Hz 4 ohms 1 Mohm 4 ohms
125 Hz 4 ohms 84 kohms 4 ohms
250 Hz 4 ohms 6916 ohms 4 ohms
500 Hz 4 ohms 580 ohms 4 ohms
1 kHz 4.3 ohms 52 ohms 4 ohms
2 kHz 8 ohms 8 ohms 4 ohms
4 kHz 52 ohms 4.3 ohms 4 ohms
8 kHz 580 ohms 4 ohms 4 ohms
16 kHz 6916 ohms 4 ohms 4 ohms
This magic resistor is made from capacitors and inductors; and sometimes resistors too.
So as to how this relates to the AMM-1, it depends if you are trying to measure the actual power going to one of the speakers in the component set, or if you are trying to measure the amplifier output into the complete component set.