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Routledge History of Philosophy Volume IV

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RENAISSANCE AND SEVENTEENTH-CENTURY RATIONALISM 119<br />

motion whose degree <strong>of</strong> speed was half <strong>of</strong> the last and highest degree <strong>of</strong><br />

speed <strong>of</strong> the former uniformly accelerated motion. 40<br />

The medieval version <strong>of</strong> this theorem is now usually referred to as the Merton<br />

rule, after its probable origins in Merton College, Oxford, in the first half <strong>of</strong> the<br />

fourteenth century. There has been much discussion <strong>of</strong> the possibility <strong>of</strong><br />

medieval influence on Galileo in this regard, but it seems ill-advised to look for<br />

anything more specific than the important step <strong>of</strong> (implicitly or explicitly)<br />

representing the intensities <strong>of</strong> speeds by segments <strong>of</strong> straight lines.<br />

The second theorem and its corollary descend from speeds, or their intensities,<br />

to distances. The theorem shows that in a uniformly accelerated motion the<br />

distances traversed are as the squares <strong>of</strong> the times, and the corollary that the<br />

successive distances traversed in equal times, starting from rest, are as the<br />

successive odd numbers 1, 3, 5, 7,…. We are now reaching directly measurable<br />

quantities, and so the stage is set for Simplicio to ask for experimental evidence<br />

to show whether this is in fact the mode <strong>of</strong> acceleration employed by nature in<br />

the case <strong>of</strong> falling bodies. Salviati willingly complies.<br />

As a true man <strong>of</strong> science [scienziato] you make a very reasonable demand,<br />

and one that is customary and appropriate in the sciences which apply<br />

mathematical demonstrations to physical conclusions, as is seen with<br />

perspectivists, with astronomers, with mechanicians, with musicians, and<br />

others who confirm with sensory experiences their principles, which are<br />

the foundations <strong>of</strong> the whole succeeding structure. 41<br />

The experiments involved rolling well-prepared bronze balls down different<br />

lengths <strong>of</strong> an extremely smooth channel arranged at different inclinations to the<br />

horizontal, and measuring the times <strong>of</strong> their descents by water running out <strong>of</strong> a<br />

hole in a pail <strong>of</strong> water. One’s initial impression may be that the set-up smacks <strong>of</strong><br />

Heath Robinson (or Rube Goldberg), but repetitions <strong>of</strong> the experiments in recent<br />

years have shown that they can be surprisingly accurate, and so we may say that<br />

they did indeed give Galileo strong support for his ‘law’ <strong>of</strong> falling bodies.<br />

The burden <strong>of</strong> the Fourth Day <strong>of</strong> the Discorsi is to combine the horizontal and<br />

the vertical, and so produce a general description <strong>of</strong> the behaviour <strong>of</strong> unimpeded<br />

‘natural’ motion. The result is the famous parabolic path for projectiles. This was<br />

admirable mathematically but less satisfactory empirically for, as gunners and<br />

others were quick to point out, the maximum horizontal trajectory was not to be<br />

achieved by firing at an elevation <strong>of</strong> 45°, nor did actual cannon balls follow a<br />

neat mathematical parabola. 42 All this goes to show the extent to which, despite<br />

his practical rhetoric, such as that provided by setting the Discorsi in the Arsenal<br />

at Venice, the success <strong>of</strong> Galileo’s mechanics depended on his focusing on ideal<br />

situations and ignoring many <strong>of</strong> the messy complexities <strong>of</strong> the actual physical<br />

world.

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