Understanding dy/dx in Calculus

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SUMMARY

The notation dy/dx in calculus, originating from Leibniz's notation, represents the instantaneous rate of change of y with respect to x. It behaves like a fraction, allowing for operations such as cancellation in the Chain Rule, where dy/dx = dy/du * du/dx. While dy/dx is not strictly a fraction, it can be treated as one due to its definition as the limit of a fraction. Understanding the distinction between "derivative" and "differential" is crucial, as dy and dx must correspond in equations unless in integrals.

PREREQUISITES
  • Understanding of basic calculus concepts, including derivatives and differentials.
  • Familiarity with Leibniz's notation for derivatives.
  • Knowledge of the Chain Rule in calculus.
  • Basic understanding of limits and their properties.
NEXT STEPS
  • Study the Chain Rule in more detail, focusing on its applications and proofs.
  • Explore the concept of differentials and their symbolic definitions in calculus.
  • Research differential forms and their relevance in advanced calculus.
  • Review the distinction between derivatives and differentials through textbooks or online resources.
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Students in calculus courses, mathematics educators, and anyone seeking to deepen their understanding of derivatives and their applications in calculus.

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I don't get the concept of the notation dy/dx. Sometimes my physics teacher puts dx in the back of an equation and cross multiply with other number. Does this mean dx can be multiply like numbers? I just don't get the overall concept of dy/dx.

I'm in 3rd year calculus and I understand that derivative is the instantaneous rate of change but how does it relates to the notation?
 
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I hope I don't confuse you more (I'm not entirely certain myself).

The notation dy/dx comes from Leibniz's notation of derivatives. Originally, he used the Greek small delta (δ) which looks a bit like a 'd'. Anyway, the d or delta represents 'a small change in'. So dy/dx means 'the small change in y, with relation to x'.

Now the dy/dx notation has one useful property to it, and that is that it can behave as a fraction. Consider the Chain Rule:

dy/dx = dy/du * du/dx

The du's can cancel as though they were in fractions, to give you dy/dx again.

This becomes more pointed with differential equations and the relation with integration, where you can 'move' the dx to be able to integrate a DE.

I think that should about cover the very basic info about dy/dx notation... you'll probably get a better answer from a real mathematician...

Good luck. :smile:
 
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One of the things your textbook should make clear (and you should ask your teacher about) is the distinction between "derivative" and "differential".

The derivative (represented y'(Newton's notation) or dy/dx (Leibniz' notation)) is NOT defined as a fraction. Strictly speaking it is incorrect to separate the "dy" from the "dx" in the derivative.

HOWEVER! dy/dx IS defined as the "limit of a fraction". One can prove "fraction-like" properties (chain rule: dy/dz= (dy/dx)(dx/dz) for example) by going back before the limit, cancelling parts of fractions, and then taking the limit. That is, we can always TREAT a derivative like a fraction. To take advantage of that, we define "dx" purely symbolically and then define dy by "dy= f'(x) dx". Given that definition, dy/dx DOES represent a fraction! Since dx is only defined symbolically, you should never have a dx in an equation without a corresponding dy (or vice-versa) unless it is in an integral (which effectively removes the derivative).

If you are wondering what I mean by "define symbolically", well, we can define differentials precisely in "differential forms" but that is beyond calculus so just "think" of it as symbolic.
You might want to check out Lethe's thread "differential forms" under the differential equation forum.
 
I've encountered a few different definitions of "indefinite integral," denoted ##\int f(x) \, dx##. any particular antiderivative ##F:\mathbb{R} \to \mathbb{R}, F'(x) = f(x)## the set of all antiderivatives ##\{F:\mathbb{R} \to \mathbb{R}, F'(x) = f(x)\}## a "canonical" antiderivative any expression of the form ##\int_a^x f(x) \, dx##, where ##a## is in the domain of ##f## and ##f## is continuous Sometimes, it becomes a little unclear which definition an author really has in mind, though...

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