There is another aspect of moving all active worth discussing, and that is the impact of the passive filters (crossovers) on the sound.
1. Going all active increases the efficiency of the speakers:
All of the UBR62 drivers have a DC resistance slightly over 4 Ohm (the woofer is 4.15 Ohm if I remember correctly). The stock passive crossovers implement two inductors in series with the woofer, one having 1.2 Ohm DCR and the other having 0.4 Ohm, for a total series DCR of 1.6 Ohm. The inductor in series with the midrange has 1 Ohm DCR.
Thus, the inductors in series with the woofer are dissipating somewhere between 25-30% of the power driving the woofer, and this is ignoring inductor core losses. The inductor in series with the midrange is air core, so no core losses, but still is dissipating 15-20% of the power driving the midrange. (The impedance of the drivers varies with frequency, so these are just estimates.)
2. Going all active increases the damping factor (DF), significantly:
DF correlates with the amplifier's ability to control speaker motion. A high DF results in a more controlled (e.g., tighter) bass response. DF is defined as the ratio of the rated impedance of a loudspeaker (the actual driver) to the source impedance of the power amplifier (it's output impedance), and is calculated as DF = (ZL + ZS)/ZS, where ZL is the load impedance (of the driver) and ZS is the amplifier's output impedance. (
https://en.wikipedia.org/wiki/Damping_factor). The more simple form of the equation, DF = ZL/ZS, commonly is used.
This definition is overly simplistic for passive speakers, though. It only considers, for the source impedance, which is the output impedance of the amplifier, without any consideration to the impact of passive filters (crossovers), speaker wire, etc., in the circuit between the driver and the amplifier. There is much confusion in the audio industry regarding these considerations. Even KEF confuses this issue, taking into consideration the speaker wire, but completely ignoring the significantly larger issue of passive filter components in the circuit (
https://us.kef.com/blogs/news/damping-factor-explained).
Here is an article that explains DF pretty thoroughly:
https://sound-au.com/biamp-vs-passive.htm. As explained in that article, passive filter components do need to be considered when determining DF. From the view of the driver for which DF is computed, the passive filter components add to the source impedance (ZS).
With my speakers, let's do a very simplistic computation of DF for the woofer, assuming the output impedance of the amplifier is very low so as to be negligible (mine is) and the DCR of the speaker wire is low enough, in comparison to the passive filter components, to be negligible. Thus, this computation just is using the DCR of the inductors, and ignoring all other contributors to the source impedance to make this calculation simple while still getting into the ballpark: DF = (4.15 + 1.6)/1.6 = 3.6. That is very low, and may be one of the issues causing me to perceive a lack of dynamics in the stock speakers - the amplifier does not have adequate control over the woofers, and thus they have sloppy bass.
Going all active, my source impedance is the sum of my amplifier's output impedance (< 50 uOhm) and the speaker cable (< 150 mOhm). Now, DF = (4.15 + 0.15)/0.15 = 28.7. That is nearly 8x higher than the DF computed based on using the passive filter.
One big caveat to the above calculations is that I only computed DF using DCR and did a lot of hand waiving to make the calculations simple, but in reality the DF is determined by the actual impedances, which vary with frequency. Still, these simple calculations show the benefit of going all active and the positive impact on speaker dynamics. The article to which I posted the link delves much further into this topic.