Undergrad Differentiation is Exact or Approximation

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The discussion explores whether differentiation is exact or merely an approximation, particularly in the context of uniform circular motion. It highlights the confusion surrounding the relationship between angular displacement and linear displacement, questioning the accuracy of the equations derived from these concepts. The conversation emphasizes that differentiation, defined as a limit, provides an exact outcome without uncertainty. It contrasts differential quotients with differentials of differences, suggesting that while they can yield similar results, they are fundamentally different. Ultimately, the discussion concludes that while approximations can be useful, differentiation itself is an exact mathematical process.
Devil Moo
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Is Differentiation exact or just an approximation?

I am wonder whether this question is meaningful or not. Slope is expressed as "it is approaching to a value as x is approaching 0" so it is inappropriate to ask such question. But when I deal with uniform circular motion, it is very confusing.

Suppose ##A## is constant for vector ##\mathbf A##. And the angle between ##\mathbf A(t+\Delta t)## and ##\mathbf A(t)## is ##\Delta \theta##.
##\begin{align}
\Delta \mathbf A & = \mathbf A (t + \Delta t) - \mathbf A(t) \nonumber \\
| \Delta \mathbf A | & = 2A \sin (\Delta \theta / 2) \nonumber
\end{align}##

if ##\Delta \theta \ll 1##, ##\sin (\Delta \theta / 2) \approx \Delta \theta / 2##
##\begin{align} | \Delta \mathbf A | & \approx 2A (\Delta \theta / 2 \nonumber \\
& =A \Delta \theta \nonumber \\
| \Delta \mathbf A / \Delta t | & \approx A (\Delta \theta / \Delta t) \nonumber
\end{align}##

if ##\Delta t \rightarrow 0##,
##| d \mathbf A / dt | = A (d \theta / dt)##

But isn't it ##| d \mathbf A / dt | = 2A (d \sin (\Delta \theta / 2) / dt)##?

Is ##v = r \omega## not accurate compared with ##v = 2r (d \sin (\Delta \theta / 2) / dt)##?
 
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Differentiation is exact: it is expressed as a limit and that makes for an outcome without uncertainty.

##| d \mathbf A / dt | = 2A (d \sin (\Delta \theta / 2) / dt)##
On the left you have a differential quotient, but on the right you have a differential of a difference.
With ##\theta/2 = \omega t/2## you do get the same differential ##\omega r##.
 
By chain rule,

##\begin{align}
\frac {d\sin(\theta/2)} {d(\theta /2)}\frac {d(\theta / 2)} {d\theta} & = \frac {1} {2} \cos\frac {\theta} {2} \frac {d\theta} {dt} \nonumber \\
|\frac {d\mathbf A} {dt} | & = A\cos\frac {\theta} {2} \frac {d\theta} {dt} \nonumber
\end{align}##

It seems they are not the same differential.

Also,

##| \frac {\Delta A} {\Delta t} | \approx A\frac {\Delta \theta} {\Delta t}##

when ##t \rightarrow 0##, why it will become equality?
 
Here is a little puzzle from the book 100 Geometric Games by Pierre Berloquin. The side of a small square is one meter long and the side of a larger square one and a half meters long. One vertex of the large square is at the center of the small square. The side of the large square cuts two sides of the small square into one- third parts and two-thirds parts. What is the area where the squares overlap?

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