By the way: Chandlers data has that object accelerating at only 34% of g between t=1.2s and t=1.8s.
Would a massive chunk of perimeter steel fall this slowly?
Also, here is the raw data we see at the 2:00 mark:
t|v
0.4|-35,291
0.6|-35,995
0.8|-37,032
1.0|-38,328
1.2|-39,328
1.4|-39,994
1.6|-40,328
1.8|-41,328
2.0|-44,660
2.2|-47,327
2.4|-48,660
2.6|-50,993
2.8|-52,326
Please take a close look at the digits to the right of the decimal points:
.032 appears once
.291 appears once
.326-8 appears six times
.660 appears twice
.993-5 appears 3 times
It seems like Chandler's software does not nearly achieve the kind of precision suggested by 3 decimal digits, but in fact rounds values to only a few discrete decimals, and all values have an error margin of +/- .166
This would imply that
- At 1.2 s. the true value is in the range -39.167 to -39.493
- At 1.8s, the true value is in the range -41.167 to -41.493
- At 2.2s, the true value is in the range -47.167 to -47.493
So Chandler's raw data has 34% of g between 1.2s and 1.8s, but it could just as well be 40% of g.
And Chandler's raw data has 153% of g between 1.8s and 2.2s, but it could just as well be 145%