 Collins (2009) points out an uncomfortable consequence of this objection, that the fine-tuning argument would be compelling if only \(\neg D\) were more life-friendly. Imagine that the laws of physics only permitted a finite range of possible expansion speeds, say 0–100 km/s, with a speed of 9–10 km/s required to support life. Then premise (1) would hold and the fine-tuning argument would succeed: \(p(F\mid \neg D)=1/100\), with \(p(F\mid D)\) presumably much higher, maybe even 1. Now imagine the possible range to be much larger, say 0–\(10^{10}\) km/s. The argument then becomes even stronger, with \(p(F\mid \neg D)=1/10^{10}\). As the upper limit on possible expansion speeds increases, the argument becomes stronger and stronger…until the limit becomes infinite, at which point the argument fails, according to the present objection.