|
|
|
|
|
by mannykannot
1327 days ago
|
|
That's an interesting point of view, but is it not the case that the length of the synodic day varies throughout the year, on account of Kepler's 2nd. law? - IIRC, this is the first-order effect in explaining the analemma. The length of the sidereal day is also variable, but more slowly (at least if we put aside atmospheric and earthquake effects, which I guess affect both equally.) I think we need both a way to reckon our everyday experience of passing time and a constant measure, and one cannot be just a special case of the other. Personally, I feel that introducing leap seconds into Unix time just muddied the waters. As to the sidereal day being of little interest outside of astronomy, James Watt's patron/partner Matthew Boulton built a sidereal clock and tried hard to find a purchaser (even having it shipped to Catherine the Great in hopes of sparking some interest) without success. It was on display in his Birmingham home when we visited a few years ago. https://www.thefreelibrary.com/Boulton+clocks+on+to+the+past... |
|
I don't see the relevance; the length of the sidereal day isn't constant either.
Variation in the length of the synodic day is the reason a day may contain other than 86400 seconds. If days are not of constant length, you could vary the length of a second on a day-to-day basis, or you could define the length of a "reference day" and then define the second as a convenient fraction of that. We have taken the second approach (though the first was used historically).
But we don't care about the vibration of cesium; if that were to change, we would adjust by changing the definition of a second, not by accepting that seconds were now of a different duration than before. Thus, the fact that cesium is referenced in an "official" definition of the duration of a second is meaningless. The officialness of that definition is illusory; in reality, seconds continue to be defined as a convenient fraction of an average day.