Infinitesimal volume element in different coordinate system

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Discussion Overview

The discussion revolves around the transformation of infinitesimal volume elements during coordinate changes, specifically from Cartesian to polar coordinates. Participants explore the mathematical relationships and properties of differentials in this context, including the Jacobian and the behavior of differential forms.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant presents a formula for the transformation of volume elements involving the Jacobian, questioning their calculations when transitioning from Cartesian to polar coordinates.
  • Another participant challenges the correctness of the differential expressions for \( dr \) and \( d\theta \), suggesting an alternative interpretation based on the geometry of the transformation.
  • A different approach is proposed using the cross product to derive the area element, leading to a different expression for the volume element in polar coordinates.
  • Participants discuss the properties of differential forms, including the anticommutation rule and the implications of higher-order differentials being zero.
  • There is a suggestion to recalculate the original expressions with an understanding of the commutation rules for differentials.
  • Some participants express confusion about the geometric and algebraic interpretations of the anticommutation rule and its implications for the calculations being discussed.

Areas of Agreement / Disagreement

Participants express differing views on the correctness of the differential transformations and the properties of differential forms. There is no consensus on the proper approach to the calculations or the interpretations of the rules governing differentials.

Contextual Notes

Participants note the importance of understanding the properties of differential forms, particularly regarding the commutation and anticommutation rules, which may affect the calculations being performed. Some assumptions about the nature of the transformations and the definitions of the differentials remain unresolved.

teddd
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I've already post this, but I've done it in the wrong section!

So here I go again..

I've a doubt on the way the infinitesimal volume element transfoms when performing a coordinate transformation from [itex]x^j[/itex] to [itex]x^{j'}[/itex]
It should change according to [tex]dx^1dx^2...dx^n=\frac{\partial (x^1,x^2...x^n)}{\partial (x^{1'}x^{2'}...x^{n'})}dx^{1'}dx^{2'}...dx^{n'}[/tex]where [itex]\frac{\partial (x^1,x^2...x^n)}{\partial (x^{1'}x^{2'}...x^{n'})}[/itex] is the Jacobian of the transformation.So i tried to do this in a concrete example: the transformation between cartesian [itex]x,y[/itex] to polar [itex]r,\theta[/itex] coordinates.
The jacobian of this transformation is [itex]r[/itex] and so, according to what I've written above[tex]dxdy=rdrd\theta[/tex]but since [itex]dr=cos\theta dx+sin\theta dy[/itex] and [itex]d\theta=-\frac{1}{r}sin\theta dx+\frac{1}{r}cos\theta dy[/itex] i get to [tex]dV=r(cos\theta dx+sin\theta dy)(-\frac{1}{r}sin\theta dx+\frac{1}{r}cos\theta dy)=(-sin\theta cos\theta dx^2+sin\theta cos\theta dy^2+cos^2\theta dxdy-sin^2\theta dxdy)[/tex]and this is not equal to [itex]dxdy[/itex], the volume element in cartesian coordinate, as it should be!

Where am I mistaking?

Thanks!
 
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Are you sure that [itex]\mathrm{d}r=\cos\theta\;\mathrm{d}x+\sin\theta\; \mathrm{d}y[/itex]? It seems to me that
[tex]\mathrm{d}r=\sqrt{\mathrm{d}x^2+\mathrm{d}y^2}.[/tex]
Also, the formula for the angle also seems to be wrong. Please explain your formulas.
 
[itex]x= r cos(\theta)[/itex], [itex]y= r sin(\theta)[/itex]
so that [itex]dx= cos(\theta)dr- r sin(\theta)d\theta[/itex] and
[tex]dy= sin(\theta)dr+ r cos(\theta)d\theta[/tex]

The differential of area is
[tex]dxdy= (cos(\theta)dr- r sin(\theta)dy)\times(sin(\theta)dr+ r cos(\theta)d\theta)[/tex]
where the "[itex]\times[/itex] is the cross product:
[tex]\left|\begin{array}{ccc} \vec{i} & \vec{j} & \vec{k} \\ cos(\theta)dr & -r sin(\theta)d\theta) & 0 \\ sin(\theta)dr & r cos(\theta) d\theta & 0 \end{array}\right|= (r cos^2(\theta)+ rsin^2(\theta))drd\theta\vec{k}= r drd\theta\vec{k}[/tex]
 
My [itex]dr[/itex] and [itex]d\theta[/itex] are the differentials of[tex]r=\sqrt{x^2+y^2}[/tex]and[tex]\theta=arctg\frac{y}{x}[/tex]

Isn't this the right way to perform the calculation?
 
Two important properties of differential forms:
[tex]dx \, dx = 0[/tex]
[tex]dx \, dy = -dy \, dx[/tex]​
Try doing your original calculation again, now that you know that the product of differential forms don't commute. (In particular, be careful when you expand the product so as not to reorder things!)

EDIT: I guess I really out to also point out that
[tex]f \, dx = dx \, f[/tex]​
where f is real-valued. (or complex-valued)
 
Last edited:
I knew that there was some sort of commutation rule for infinitesimal!

The [itex]dx^{n}=0[/itex] with [itex]n>1[/itex] propriety is ok (they re higher order terms in a taylor expansion of the function, so I guess they're trascurable by definition); but where does the anticommutation rule come from??
 
teddd said:
The [itex]dx^{n}=0[/itex] with [itex]n>1[/itex] propriety is ok (they re higher order terms in a taylor expansion of the function, so I guess they're trascurable by definition); but where does the anticommutation rule come from??
Geometrically, it deals with orientation.

Algebraically, it's the same rule. :smile: Let [itex]z = x+y[/itex], and simplify this expression in two different ways:
[tex](dz)^2 - (dx)^2 - (dy)^2[/tex]​
 
teddd said:
The [itex]dx^{n}=0[/itex] with [itex]n>1[/itex] propriety is ok (they re higher order terms in a taylor expansion of the function, so I guess they're trascurable by definition); but where does the anticommutation rule come from??
Geometrically, it deals with orientation.

Algebraically, it's the same rule. :smile: Let [itex]z = x+y[/itex]. Then:
[tex](dz)^2 = (dx + dy)^2[/tex]​
and so...
 
So becaouse [itex](dz)^2[/itex] must be zero, we have [itex]dxdy=-dydx[/itex] !

Thanks a lot for your help guys!
 
  • #10
teddd said:
My [itex]dr[/itex] and [itex]d\theta[/itex] are the differentials of[tex]r=\sqrt{x^2+y^2}[/tex]and[tex]\theta=arctg\frac{y}{x}[/tex]

Isn't this the right way to perform the calculation?
Since it is dxdy you want to replace, it make more sense to me to calculate dx and dy in terms of [itex]dr[/itex] and [itex]d\theta[/itex].
 
  • #11
Isn't [itex]\mathrm{d}y\mathrm{d}x[/itex] equal to 0? (I haven't really learned the rules but it seems more intuitive that way).
 
  • #12
No, it isn't. It is, however, a "second order differential" so that while "dx" and "dy" separately are differentials of length, "dxdy" is a differential of area.
 
  • #13
You're absolutely right HallsofIvy; but I wanted to check the rule by doing the backwards calculation!
 

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