Does Distance from the Fulcrum Decrease Angular Acceleration on a Seesaw?

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On a seesaw, the angular acceleration decreases as the distance from the fulcrum increases, which is supported by the derived formula α = g/r. However, this formula assumes a point mass on a massless seesaw, which may not hold true if the seesaw has significant mass or if the load is large. In such cases, the total rotational inertia must be considered, including the seesaw's mass. The correct approach involves calculating the total rotational inertia as I_total = I_seesaw + mr^2. Therefore, the assumptions about mass significantly impact the accuracy of angular acceleration calculations.
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When I do some physics derivation, I find that on a seesaw, if the object is farther away from the fulcrum, the angular acceleration decreases. Is this true? If not, where did I go wrong?
\tau = I \cdot \alpha

\tau=F \cdot r

Then, \alpha = \frac{F \cdot r}{I} = \frac{F_g \cdot r}{mr^2}=\frac{g \cdot m \cdot r}{mr^2}=\frac{g}{r}, so if the distance "r" increases, angular acceleration decreases...did I do something wrong?
 
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Are you sure? Some people have told me that it's wrong, because I have to account for the mass of the seesaw.
 
It's not that it is wrong, it simply makes some assumptions. The formula you derived is for a point mass on a massless seesaw. If your seesaw is not light enough to approximate as massless or if your load is too large to be considered a point then your formula doesn't apply.
 
What if I cannot assume the masses are negligible? How would I derive that? And in that case, would angular acceleration increase?
 
Just include the rotational inertia of the seesaw as part of the total rotational inertia:
I_{total} = I_{seesaw} + mr^2 = 1/12 M L^2 + mr^2
 
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