Smarter way to solve a continuity equation?

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Homework Help Overview

The problem involves a continuity equation related to a conserved substance in three-dimensional space, defined by a density function and a corresponding flux vector. The task is to show that these functions satisfy the conservation equation under a specific condition regarding constants.

Discussion Character

  • Exploratory, Assumption checking

Approaches and Questions Raised

  • Participants discuss potential methods for solving the problem, including the use of the divergence theorem and spherical coordinates. There is uncertainty about how to handle the position vector and the complexity of the calculations involved.

Discussion Status

Some participants are exploring different approaches to the problem, while others express confusion about the initial steps and the implications of the position vector in the context of spherical coordinates. There is no explicit consensus on a preferred method yet.

Contextual Notes

Participants note the complexity of the calculations and the potential for misunderstanding the role of the position vector in the equations provided. There is a mention of the time constraints related to formatting the discussion, which may affect the problem-solving process.

stufletcher
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Homework Statement


The density in 3-D space of a certain kind of conserved substance is given by
[tex]\[\rho (x,y,z, t) = At^{-\frac{3}{2}}e^{-\frac{r^2}{4kt}}\][/tex]

where [tex]\mathbf r = x\mathbf i + y\mathbf j +z\mathbf k[/tex] and [tex]r = |\mathbf r|[/tex]. The corresponding flux vector is given by
[tex]\mathbf J(\mathbf r, t) = Bt^{-\frac{5}{2}}e^{-\frac{r^2}{4kt}}\mathbf r[/tex]
Here, A, B, k and positive constants.

Homework Equations



Show that [tex]$\rho, \mathbf J$[/tex] satisfy the conservation equation [tex]\frac{\partial \rho}{\partial t}[/tex][tex]+ \nabla \cdot \mathbf J = 0[/tex] only if [tex]$ A = 2B$[/tex]

The Attempt at a Solution


So I've looked at this, found the derivative for the density function, had a fair play with the div function, I'm just wondering if there is a smarter way to solve this then actually deriving the partial derivative and the div function and re-arranging? I have a feeling there is something inherent, for example like the divergence theorum, that i can use?

mind you in the time it took me to get the tex working i could have solved the thing, but I'm still curious
 
Last edited:
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One smarter way would be by using (first understanding the derivation, of course) Eqs. (49,50) from the entry "http://mathworld.wolfram.com/SphericalCoordinates.html" ".
 
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Hmm. To be honest I don't know where to start. For example, how to i manage the position vector? Do i replace x, y, z with [tex]r cos \theta sin \phi[/tex] etc, then do the divergence? It starts to look very messy ... [tex]t^{-\frac{5}{2}}e^{-\frac{r}{4kt}} r cos \theta sin \phi[/tex] for the x component for example
 
stufletcher said:
Hmm. To be honest I don't know where to start. For example, how to i manage the position vector? Do i replace x, y, z with [tex]r cos \theta sin \phi[/tex] etc, then do the divergence? It starts to look very messy ... [tex]t^{-\frac{5}{2}}e^{-\frac{r}{4kt}} r cos \theta sin \phi[/tex] for the x component for example

[tex]r[/tex] in the exponential is not the position vector. It is its length - one of the coordinates of the spherical system. It will stay as such. [tex]\theta,\phi[/tex] simply do not appear in the formula - which simplifies the calculations.
 

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