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The Errors & Animadversions of Honest Isaac Newton by Sheldon ...

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to any mysterious forces. <strong>The</strong>y moved freely and erratically with randomvelocities, occasionally suffering elastic impacts with one another or with thecontaining vessel. But this correct and brilliant insight would languish forwell over a century. “Why was [Bernouilli’s] theory forgotten?” asked thecontemporary historian <strong>of</strong> science Stephen Brush. It was because “<strong>Newton</strong>’stheory... had been firmly established as the explanation <strong>of</strong> Boyle’s Law, both<strong>by</strong> the reputation <strong>of</strong> <strong>Newton</strong> and <strong>by</strong> its simplicity... Once the <strong>Newton</strong>ianswere in power, no prudent scientist (at least in England) would dare to contradictthe real or supposed opinions <strong>of</strong> the ‘autocrat <strong>of</strong> science’ until late inthe 19th century.”<strong>Newton</strong>’s flawed understanding <strong>of</strong> the elasticity <strong>of</strong> air did not preventhim from seeking to understand the propagation <strong>of</strong> sound, which he wrote“can be nothing else but pulses <strong>of</strong> the air propagated through it,” that is,sound waves. From an ingenious but rather difficult to understand argument,he deduced a simple formula for the speed <strong>of</strong> sound in air:V =√PressureDensity .But for a multiplicative factor that is not so different from unity, <strong>Newton</strong>’sresult is correct. It stands as a triumph <strong>of</strong> <strong>Newton</strong>’s physical intuition. Hecould not have known that sound propagation is not isothermal, and that thecorrect result involves an additional thermodynamic parameter.<strong>Newton</strong> would not be satisfied with a result that was only approximatelycorrect. He was compelled to swindle his way to exactitude: Of the precedingcalculation, he wrote, “We have made no allowance for the crassitude <strong>of</strong> thesolid particles <strong>of</strong> the air, <strong>by</strong> which the sound is propagated instantaneously.”(In <strong>Newton</strong>’s time ‘crassitude’ meant ‘thickness’. <strong>Newton</strong> was arguing thatthe physical size <strong>of</strong> air molecules somehow enhanced the velocity <strong>of</strong> sound.)With this dreadfully spurious argument, <strong>Newton</strong> augmented his estimate <strong>of</strong>the speed <strong>of</strong> sound <strong>by</strong> about 10%, but his modified result was still significantlysmaller than its known speed. He then appealed to an even more absurdargument: “<strong>The</strong> vapors floating in the air being <strong>of</strong> another spring, and adifferent tone, will hardly, if at all, partake <strong>of</strong> the motion <strong>of</strong> the true air inwhich the sounds are propagated.... So if the atmosphere consists <strong>of</strong> 10 parts <strong>of</strong>true air and one part <strong>of</strong> vapors [If indeed!], the motion <strong>of</strong> sounds will be swifter<strong>by</strong> the subduplicate ratio [that is, the square root] <strong>of</strong> 11 to 10...” Having6

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