I 2nd derivative of angular displacement wrt time

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The discussion clarifies that the second derivative of angular displacement with respect to time, represented as d²θ/dt², does not equal (dθ/dt)². Using examples like θ = sin(t) and θ(t) = t, it is shown that the second derivative can yield negative or zero values, while the square of the first derivative remains non-negative. This indicates a fundamental difference in their meanings, despite dimensional agreement. The conversation raises critical questions about the implications of these results on rotational motion, particularly regarding constant rotation rates and the behavior of angular velocity. Overall, the proposed equation is deemed incorrect based on these analyses.
Prez Cannady
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If ##\theta## is angular displacement, does ##\frac{d^2\theta}{dt^2} = (\frac{d\theta}{dt})^2##? Proof?
 
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Parameterized, I think not. A contradiction:

$$ \theta = sin(t) $$
$$ \frac{d\theta}{dt} = cos(t) $$
$$ \frac{d^2\theta}{dt^2} = -sin(t) $$
$$ \left(\frac{d\theta}{dt}\right)^2 = (cos(t))^2 $$
 
How about this:
$$
\begin{align}
\theta(t) &= t \\
\frac{d\theta}{dt} &= 1 \\
\frac{d^2\theta}{dt^2} &= 0 \neq \left( \frac{d\theta}{dt} \right)^2
\end{align}
$$
 
Yeah. Dimensionally they agree because ##\theta## is dimensionless, but they're not equivalent. Thanks.
 
Try a couple of sanity checks of the proposed equation:
1) If the rotation rate is not changing, the second derivative is zero. Does that mean that it is not rotating at all?
2) Since the right hand side is always positive, does that mean that the rotation rate can only get more positive?
 
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