Master equation -> diffusion equation

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Homework Help Overview

The discussion revolves around the derivation of the diffusion equation from the Master equation in the context of a one-dimensional discrete chain. The original poster is exploring how to transition from the Master equation to the diffusion equation, specifically focusing on the behavior of particles jumping between states in the chain.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • The original poster attempts to connect the Master equation to the diffusion equation using a limit process and questions the application of the derivative definition in this context. Other participants provide clarifications on the expressions for derivatives at specific points and suggest using central differences for a clearer approach.

Discussion Status

The discussion is progressing with participants actively engaging in clarifying the mathematical steps involved. Some guidance has been offered regarding the use of central differences, which may help in understanding the transition to the diffusion equation.

Contextual Notes

Participants are working within the constraints of a homework assignment, which may limit the depth of exploration into the underlying concepts. There is an emphasis on understanding the mathematical definitions and their applications rather than arriving at a final solution.

Mikhail_MR
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Homework Statement


I am trying to understand the derivation of the diffusion equation from the Master equation for a 1D chain. We have an endless 1D discrete chain. State from ##n## can jump to ##n+1## and ##n-1## with equal probabilities. The distance between chain links is ##a##.

Homework Equations


Master equation: $$\frac{d\rho_n}{dt} = W\left(-2\rho_n + \rho_{n+1} + \rho_{n-1}\right)$$

The Attempt at a Solution


With ##\Delta n = 1## we have $$\frac{d\rho_n}{dt}=Wa^2 \frac{(\rho_{n-1}-\rho_n) + (\rho_{n+1}-\rho_n)}{(\Delta n)^2 a^2},$$ where we could write ##(\Delta n)^2 a^2 = (\Delta x)^2##, since ##na=x##. In limit ##\Delta x \rightarrow 0## we get $$\frac{d\rho_n}{dt} = Wa^2 \frac{\partial^2 \rho_n}{\partial x^2}$$.
Unfortunately, I can not understand the last step. The definition of a derivative is ##f(x_0+\Delta x) - f(x_0) /\Delta x##, but I do not understand how it is used here.

Any help would be appreciated.
 
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Using your definition (with brackets inserted correctly), what is the expression for dρ/dx at x0 = n-1? What is the expression at x0 = n? So what is d(dρ/dx)/dx ?
 
##d\rho/dx## would be ##\frac{\rho_n - \rho_{n-1}}{\Delta x}## at ##x_0=n-1## and ##\frac{\rho_{n+1} - \rho_{n}}{\Delta x}## at ##x_0=n##.
Then: $$d(d\rho/dx)dx= [(d\rho/dx)_{x_0=n} - (d\rho/dx)_{x_0=n-1}] / \Delta x$$. Oh, now I see it. Thank you!
 
A better way of doing this would be in terms of central differences: ##d\rho/dx## would be ##\frac{\rho_n - \rho_{n-1}}{\Delta x}## at ##x_0=n-1/2## and ##\frac{\rho_{n+1} - \rho_{n}}{\Delta x}## at ##x_0=n+1/2##
 

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