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I have moved this conversation out of the other discussion. I did some measurements, I repeated the same for 8 times.
Questions:
My experience is that I am nowhere near the 3% (its more like 10% if I take out the obvious outliers from the 8 repeats, because I get 0.067 with this method). So I wonder what could improve this. I will do the kayak erg as well as there I have a rather accurate value from the engineer that made it and see how that works. EDIT: I re-did the measurements with a strudier sawing string (previously I used knitting string that had some springiness). And there is a massive improvement. With the original weight I get 0.075 but with the increased weight (of 167gramm) it produced 0.0775 inertia which is very close to the CAD calculation. Especially if I round it up which should be plausible considering friction and air drag (while I suppose normally the latter should be nominal at such a low speed) So one conclusion of mine currently is that a bit heavier weight produce better results especially on machines that have more friction (mine is rather old) which is logical as friction is constant and its constant effect on higher speed is relatively reduced. |
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Apologies for being unclear!
This video explains a lot, I think/hope. It depicts a "standard" way of measuring inertia. It is fundamentally more accurate than the "pendulum method". It is a "standard" undergrad physics experiment. Note that in the video, the rotation axis points vertical, wheras the rower flywheel axis points horizontal. This makes it even easier, since no idler pulley is required.
This thread shows the 12 encoder lines on the flywheel of my concept2 model C, causing 12 pulses per revolution. Normally used for determining the angular speed during rowing, but now I use it for determining$\frac{d\omega}{dt}$ to estimate the moment of inertia.
From de the delta-times I calculate$\omega = \frac{2\pi}{12\Delta t}$ . Plotting $\omega$ versus time gives slope $\frac{d\omega}{dt}$ as a constant, which can be plugged in in $J=mr^2(\frac{g}{r\dot\omega}-1)$ , were $m$ represents the mass attached to the string, $r$ is the radius of the "fan-drum" and g is acceleration due to gravity.
In my case it was particularly/surprisingly easy to carry out. The only thing I had to do is take off the screen from the flywheel housing (instead of just the front cover of my model C) and wind a string with weight around the "fan-drum". And I lifted the flywheel assembly 1 meter up such that I had more "drop-height". I did the experiment with two different weights: 172 [g] and 35 [g]. Results for$J$ were very similar, but I preferred the data obtained with the higher weight. I also had to make one or two tweaks in my analysis software, since during rowing, very low speed (<200 [rpm]) data is discarded.
@kamp169
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