A What is meant by ##\rho_{xx}##?

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The discussion centers on the interpretation of $$\rho_{xx}$$ in a specific paper, where it is clarified that $$\rho_{xx}$$ refers to a component of the resistivity tensor rather than a scalar density. Participants note that the paper treats electrons as a continuum fluid, suggesting that $$\rho$$ represents the density of this fluid. There is a consensus that equation 3 in the paper is not a definition but rather a calculation related to resistivity. The conversation also touches on the differences in notation between physicists and mathematicians, highlighting potential confusion in interpreting terms like $$E_x$$. Overall, the discussion emphasizes the importance of understanding context and notation in scientific literature.
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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, E_x is the x-component of the electric field vector: \quad \hat x \cdot \vec E.
To mathematicians and advanced mathematics students, E_x is the partial-derivative of E with respect to x: \quad \displaystyle\frac{\partial E}{\partial x}.
(I'd be curious to how \vec\nabla\cdot \vec E would be expanded out... presumably, one would define \vec E= F(x,y,z) \hat x+ G(x,y,z) \hat y + H(x,y,z) \hat z)

(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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