I agree, slew rate is largely unimportant to most listeners. It's not until you begin using drivers that can offer coinciding rise and decay times that you will be able to appreciate any difference at all. Extremely low mass, low inductance drivers with little to no energy storage and a flat impedance, mounted in enclosures that also do not store energy, will begin to reveal the differences in slew rate as well as different types and amounts of THD. Add in high efficiency and you can even begin to appreciate the difference in various amplifiers' noise floors. Some drivers even offer faster rise times than the very best of amplifiers (the Manger device with it's 13 uS rise time comes to mind) and you will certainly begin to hear differences in amplifiers with those. But most drivers used in the automobile simply don't offer the resolution necessary for splitting these kinds of hairs so it's not an issue. Take a look at the waterfall and impedance plots for some of these drivers and you can see why most suffer from phase distortion that smear detail.