Understanding Basic Calculus: Limits, Differentials, and Integrals Explained

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Discussion Overview

The discussion revolves around understanding the concepts of limits, differentials, and integrals in calculus, particularly in the context of a specific equation involving mass flow and force. Participants explore the transition from finite differences to differentials and the implications of integrating both sides of an equation.

Discussion Character

  • Exploratory
  • Technical explanation
  • Mathematical reasoning

Main Points Raised

  • One participant expresses confusion about how the limit as \(\delta s \rightarrow 0\) leads to the differential form in the equation.
  • Another participant suggests rewriting the first equation to clarify the limit process and agrees with the transition to the second equation.
  • A participant questions the validity of multiplying through by \(ds\) during integration and seeks clarification on this operation.
  • Another participant confirms that the two integrals will have the same value and discusses the rigorous approach to understanding equality between differentials.
  • One participant introduces a separable differential equation as an example to illustrate the use of the chain rule in this context.
  • Participants discuss the paradox of multiplying by \(ds\) and its implications in calculus, noting that while it may seem meaningless, it can yield correct results under certain conditions.

Areas of Agreement / Disagreement

Participants generally agree on the mathematical processes involved but express differing views on the appropriateness of certain operations, such as multiplying by \(ds\). The discussion remains unresolved regarding the best approach to understanding these concepts.

Contextual Notes

There are limitations in the discussion regarding the definitions of differentials and the assumptions underlying the operations discussed. The conversation does not resolve the complexities associated with these mathematical concepts.

Who May Find This Useful

This discussion may be useful for students or individuals seeking to deepen their understanding of calculus, particularly in the areas of limits, differentials, and integration techniques.

ryan88
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I have been going over some lecture notes and have some questions about some of the mathematics shown in these notes.

They start off with the following equation:

\delta F_x = \dot{m} \frac{dV_x}{ds} \delta s

and then impose the limit as \delta s \rightarrow 0, and gets:

\frac{dF_x}{ds} = \dot{m}\frac{dV_x}{ds}

I guess I am kind of confused as to how \delta s \rightarrow 0 would form the differential seen on the left hand side of the equation.

Then the next line of the notes goes from the previous equation to:

dF_x = \dot{m}dV_x

Is this because both sides have been integrated with respect to s? Or have I missed something else here too?

Sorry if these seem like simple questions, but I guess I am not as confident with limits and the difference between \Delta, \delta and d as I thought I was.

Any help would be appreciated.

Thanks,

Ryan
 
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Well, from your first equation, you may re-write this as:
\frac{\delta{F}_{x}}{\delta{s}}=\dot{m}\frac{dV_{x}}{ds}
When now taking the limit as \delta\to{0}, your second equation should appear, agreed?
 
I had wondered if it was just as simple as that or whether or not I was missing something, thanks for that.

But I am still stuck with the second part of my question. If i integrate both sides with respect to s, I get:

\int \frac{dF_x}{ds} ds = \dot{m} \int \frac{dV_x}{ds} ds

Which can then be simplified to:

\int dF_x = \dot{m} \int dV_x

But this will not give the answer I got from the course notes.

The only way I can think of to get that answer is to multiply through by ds, but I didn't think that you were "allowed" to do this. Please correct me if I am wrong.

Thanks,

Ryan
 
ryan88 said:
Which can then be simplified to:

\int dF_x = \dot{m} \int dV_x

Indeed.
And at your level, this is the ONLY rigorous manner inb which you should think of equality between differentials.
The two integrals will have the same value.

It is possible to make an entirely different, equally rigorous maths in which differentials can be PROPERLY defined, but this is not basic level courses (and what you learn at basic level is NOT invalid, or of little use, but you've got to start somewhere, leaving other stuff out!)


But this will not give the answer I got from the course notes.

The only way I can think of to get that answer is to multiply through by ds, but I didn't think that you were "allowed" to do this.

Again, fine thinking!

But, the clever thing about the chain rule of differentiation, CONNECTED with the integral above will yield the same results AS IF you could have multiplied with ds!

Thus, somewhat paradoxically, a formally meaningless operation (multiplying with ds) necessarily yields good results.

(The basic reason why it is meaningless is that "ds" is not a real number, and hence can't be multiplied with. The other way I mentioned basically creates another "number system" within, indeed, multiplication of differentials is a meaningful operation.)
Please correct me if I am wrong.

Thanks,

Ryan


Hope this helped!
 
Yeah thanks that does help, but would it be possible to provide an example on how the chain rule would be used in this context? I think this may help me understand it a bit better.

Thanks,

Ryan
 
Okay.

Let us have a separable differential equation:
\frac{dy}{dx}=\frac{1}{g(y(x))}
where g(y) is some function of y.

We may solve this as follws:
g(y(x))\frac{dy}{dx}=1,
or, by integration:
\int_{x_{0}}^{X}g(y(x))\frac{dy}{dx}dx=\int_{x_{0}}^{X}1dx=X-x_{0}
where I use X as an arbitrary x-value, x_0 as some initial value.
Supposing there is a function G(y), so that \frac{dG}{dy}=g(y)[/itex].<br /> <br /> Then, by the technique of substitution (i.e, the inverse chain rule, if you like!),<br /> we may rewrite the left-hand side as:<br /> G(y(X))-g(y(x_{0})=\int_{x_{0}}^{X}\frac{dG}{dy}\frac{dy}{dx}dx,<br /> <br /> yielding the solution in (implicit form for Y=y(X), y_0=y(x_0)):<br /> G(Y)-G(y_{0})=X-x_{0}<br /> <br /> Now, all this is very cumbersome!<br /> <br /> Instead, we cut over the niceties as follows:<br /> \frac{dy}{dx}=\frac{1}{g(y)}<br /> we multiply with g(y)dx, yielding:<br /> g(y)dy=dx<br /> and we then integrate the left-hand side from y_0 to Y, and the righthand-side from x_0 to X, giving us the same answer.
 
Right, now I understand! Thank you very much for all your help arildno!
 

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