What is meant by ##\rho_{xx}##?

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Discussion Overview

The discussion centers around the meaning of the notation $$\rho_{xx}$$ as presented in a specific paper. Participants explore its implications in the context of physics, particularly regarding its definition and relationship to density and resistivity tensors.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Conceptual clarification

Main Points Raised

  • Some participants suggest that $$\rho$$ typically represents density, but question why it would be treated as a scalar in this context.
  • Others point out that $$\rho_{xx}$$ is defined in equation 3 of the paper, indicating it may not relate to density as initially assumed.
  • One participant proposes that $$\rho_{xx}$$ could represent the second derivative of density with respect to position, $$\rho_{xx}=\frac{\partial^2\rho}{\partial x^2}$$.
  • Another participant asserts that $$\rho_{xx}$$ is a component of the resistivity tensor, challenging the initial density interpretation.
  • Some participants express difficulty in following the paper, suggesting that it treats electrons as a continuum fluid and applies fluid dynamics equations.
  • There is a mention of the relationship between $$\rho_{xx}$$ and other tensor components, such as $$\eta_{xx}$$ and $$\eta_{xy}$$, indicating a broader context of tensor analysis.
  • One participant critiques the paper's clarity and notation, suggesting it exemplifies poor writing practices in scientific communication.
  • Several side notes discuss the differences in notation between physicists and mathematicians, particularly regarding vector components and partial derivatives.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the interpretation of $$\rho_{xx}$$, with multiple competing views regarding its definition and implications. The discussion remains unresolved as participants explore different interpretations and clarify their understanding.

Contextual Notes

There are limitations in the discussion regarding the assumptions made about the notation and its definitions. The relationship between density and resistivity tensor components is not fully resolved, and the context of the equations in the paper may influence interpretations.

aliens123
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I was wondering what was meant by $$\rho_{xx}$$ in the following paper: https://arxiv.org/abs/1703.07325

I would guess that $$\rho$$ is the density, however I don't see why $$\rho$$ would be treated like a scalar. Unless what they mean is derivatives... Thank you!
 
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It's defined in equation 3.
 
Normally it should be $$\rho_{xx}=\frac{\partial^2\rho}{\partial x^2}$$

Usually density is a scalar, at least that's how I know it when studying most of physics.
 
Delta2 said:
Usually density is a scalar
Yes, but ##\rho_{xx}## has nothing to do with density - see how it's defined in equation 3 in the paper.
 
Ibix said:
Yes, but ##\rho_{xx}## has nothing to do with density - see how it's defined in equation 3 in the paper.
I am having big trouble following the paper, but i think equation 3 is not an equation of definition but an equation of calculation.

Moreover i think the paper tries to study the electron flow as the electrons being some sort of continuum fluid and by applying fluid dynamics equations. Most likely ##\rho## is the density of the "electron continuum fluid"
 
Delta2 said:
Most likely ##\rho## is the density of the "electron continuum fluid"
No - check the units. It's a component of the resistivity tensor.
 
Ibix said:
No - check the units. It's a component of the resistivity tensor.
Hmmm, maybe you are right, it seems that they are tensor components cause it also refers to ##\eta_{xx}## and ##\eta_{xy}## as components of the kinematic viscosity tensor.
 
Delta2 said:
Hmmm, maybe you are right
Furthermore, there is an explicit statement in the paragraph between equations 11 and 12 that equation 3 is the resistivity tensor.
 
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Yes, it's the inverse conductivity tensor and thus the resistivity tensor. It's an example, how not to write a paper and that referees are sometimes not picky enough :frown:.
 
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  • #10
Side note:
Delta2 said:
Normally it should be $$\rho_{xx}=\frac{\partial^2\rho}{\partial x^2}$$

Usually density is a scalar, at least that's how I know it when studying most of physics.

When I taught Griffith's level E&M the first time,
I realized another example of notational differences between mathematicians and physicists.
To physicists and advanced physics students, [itex]E_x[/itex] is the x-component of the electric field vector: [itex]\quad[/itex] [itex]\hat x \cdot \vec E[/itex].
To mathematicians and advanced mathematics students, [itex]E_x[/itex] is the partial-derivative of [itex]E[/itex] with respect to [itex]x[/itex]: [itex]\quad[/itex] [itex]\displaystyle\frac{\partial E}{\partial x}[/itex].
(I'd be curious to how [itex]\vec\nabla\cdot \vec E[/itex] would be expanded out... presumably, one would define [itex]\vec E= F(x,y,z) \hat x+ G(x,y,z) \hat y + H(x,y,z) \hat z[/itex])

(Long ago, I was a double major in physics and math, but I guess I probably compartmentalized notations.)

Possibly interesting reading:
http://sites.science.oregonstate.edu/math/bridge/papers/bridge.pdf
"Bridging the Gap between Mathematics and the Physical Sciences"
Tevian Dray and Corinne A. Manogue

http://sites.science.oregonstate.edu/physics/bridge/papers/CMJspherical.pdf
"Spherical Coordinates"
Tevian Dray and Corinne A. Manogue
 
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  • #11
Never ever use the Notation ##E_x## for the partial derivative of a function ##E## with respect to ##x##. You'll run into a lot of trouble doing so. The mathematicians turn to make their lives very difficult by not using a thoughtful notation. This I learned when I attended a pure mathematicians' lecture on functional analysis. The mathematicians never use ornaments to clearly specify what's a vector, a vector component, a scalar etc. They were very confused when it came to solve problems. Usually I first translated the problem into physicists's notation and solved it in this notation. After that I translated it to the mathematicians's notation, because the mathematicians never accept physicists's notation (particularly they don't like the Dirac bra-ket notation for Hilbert spaces and make the scalar product semilinear in the 2nd argument instead in the first just to make their lives more difficult; nor do they appreciate the Ricci calculus when they deal with vector/tensor algebra and calculus, again to make their lives more difficult).

The physicists had to learn the much more powerful and error-minimizing notation themselves. If you look at Maxwell's treatise or even the early writings by Einstein and Minkowski you get into a crisis too!
 
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