Differentiation is Exact or Approximation

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SUMMARY

The discussion centers on the nature of differentiation in the context of uniform circular motion and its implications for exactness versus approximation. It establishes that differentiation is exact as it is defined as a limit, leading to outcomes without uncertainty. The conversation highlights the relationship between angular displacement and linear velocity, specifically addressing the equations \(v = r \omega\) and \(v = 2r \frac{d \sin(\Delta \theta / 2)}{dt}\). The participants conclude that while both expressions can yield similar results under certain conditions, they are fundamentally different in their derivation and implications.

PREREQUISITES
  • Understanding of calculus, specifically limits and differentiation.
  • Familiarity with angular motion concepts, including angular velocity and displacement.
  • Knowledge of trigonometric functions and their derivatives.
  • Basic principles of vector analysis in physics.
NEXT STEPS
  • Study the concept of limits in calculus to reinforce understanding of differentiation.
  • Explore the relationship between linear and angular velocity in circular motion.
  • Investigate the application of the chain rule in differentiation, particularly in trigonometric contexts.
  • Examine the implications of approximations in physics, especially in the context of small-angle approximations.
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Students and professionals in physics, mathematics, and engineering who are interested in the precise nature of differentiation and its applications in motion analysis.

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?
 

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