Line Integral: Solving for \ointr.dr=0

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Homework Help Overview

The discussion revolves around evaluating the line integral \(\oint \vec{r} \cdot d\vec{r}\) and understanding the conditions under which this integral equals zero. The subject area includes vector calculus and line integrals.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants explore the assertion that \(\vec{r} \cdot d\vec{r} = r dr\) and question the parallelism of the vectors involved. There are attempts to express the integral in Cartesian coordinates and polar coordinates, leading to discussions about tangent lines and their implications for the integral's evaluation.

Discussion Status

The discussion is active, with participants providing insights and questioning assumptions about vector relationships. Some guidance has been offered regarding the simplification of the integral, but multiple interpretations of the tangent lines and their angles remain under consideration.

Contextual Notes

Participants are navigating the definitions and properties of vector fields, particularly in relation to conservative fields, which may influence the evaluation of the integral.

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Homework Statement



What is the result of this? [tex]\oint[/tex]r.dr=?

Homework Equations





The Attempt at a Solution



[tex]\oint[/tex]r.dr =[tex]\oint[/tex]rdr=[tex]\int[/tex][tex]^{a}_{a}[/tex]rdr = [tex]\frac{r^2}{2}[/tex] [tex]\left|[/tex] [tex]^{a}_{a}[/tex] = 0

Is it correct?
 
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What argument do you have for asserting that [itex]\vec{r}\cdot d\vec{r}= r dr[/itex]? Generally, the dot product of two vectors is equal to the product of their lengths when the vectors are parallel. Are [itex]\vec{r}[/itex] and [itex]d\vec{r}[/itex] parallel?

In Cartesian coordinates, [itex]\vec{r}= x\vec{i}+ y\vec{j}[/itex] and [itex]d\vec{r}= dx\vec{i}+ dy\vec{j}[/itex] so your integral becomes [itex]\oint xdx+ ydy[/itex] around some closed path.

A circle of radius R can be written as [itex]\vec{r}= Rcos(\theta)\vec{i}+ R sin(\theta)\vec{j}[/itex] and then [itex]d\vec{r}= -Rsin(\theta)d\theta\vec{i}+ Rcos(\theta)d\theta\vec{j}[/itex] so your integral becomes [itex]R^2\int_{\theta= 0}^{2\pi} -sin(\theta)cos(\theta)+ cos(\theta) sin(\theta) d\theta[/itex] which is even simpler.
 
Dear "HallsofIvy" thank you very much for your wonderful help. I thought the angle between r and dr is always zero because the angle between two curves are defined as the angle between their tangent lines.
 
Okay. And what are the tangent lines of "r" and "dr"?
 
HallsofIvy said:
Okay. And what are the tangent lines of "r" and "dr"?

Well now I think that the tangent lines are different because we have two different vectors, but I didn't notice it!
 
I may be pulling your chain a little too hard here! Yes, r and dr are parallel (they both point directly away from the origin) and so their dot product is just rdr. My point was that you have to show that, not just assert it.

But it is simpler to do it as [itex]R^2\int_{\theta= 0}^{2\pi} -sin(\theta)cos(\theta)+ cos(\theta) sin(\theta) d\theta[/itex] because, of course, [itex]-sin(\theta)cos(\theta)+ cos(\theta)sin(\theta)= 0[/itex].
 
HallsofIvy said:
Okay. And what are the tangent lines of "r" and "dr"?

The tangent line of [tex]\vec{r}[/tex] is placed on d[tex]\vec{r}[/tex] and the tangent line of d[tex]\vec{r}[/tex] is placed on itself because it is a straight line (because [tex]\vec{r}[/tex]= x[tex]\vec{i}[/tex] + y[tex]\vec{j}[/tex]) so the angle between [tex]\vec{r}[/tex] and d[tex]\vec{r}[/tex] is zero.
Is it correct? If there is a better interpretation please let me know. And thank you very much in advance for your great help.
 
have you looked at the definition of conservative vector fields at all?
 

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