# The Diffusion Constant

- Page ID
- 5284

The diffusive flow of particles can be studied by applying a constant force \(f\) to a system using the microscopic equations of motion

\[\dot{\textbf r}_i = { {\textbf p}_i \over m_i}\]

\[\dot{\textbf p}_i = {\textbf F}_i({\textbf q}_1,..,{\textbf q}_N) + f\hat{\textbf x} \]

which have the conserved energy

\[ H' = \sum_{i=1}^N {{\textbf p}_i^2 \over 2m_i} + U({\textbf q}_1,...,{\textbf q}_N) -f\sum_{i=1}^Nx_i \]

Since the force is applied in the \( \hat{\textbf x} \) direction, there will be a net flow of particles in this direction, i.e., a current \(J_x \). Since this current is a thermodynamic quantity, there is an estimator for it:

\[ u_x = \sum_{i=1}^N \dot{x}_i \]

and \(J_x = \langle u_x \rangle \). The constant force can be considered as arising from a potential field

\[ \phi(x) = -xf \]

The potential gradient \( \partial \phi/\partial x \) will give rise to a concentration gradient \(\partial c / \partial x \) which is opposite to the potential gradient and related to it by

\[ {\partial c \over \partial x} = -{1 \over kT}{\partial \phi \over \partial x} \]

However, Fick's law tells how to relate the particle current \(J_x \) to the concentration gradient

\[ J_x = D{\partial c \over \partial x} = -{D \over kT}{\partial \phi \over \partial x}= {D \over kT}f \]

where \(D\) is the *diffusion constant*. Solving for \(D\) gives

\[ D = kT{J_x \over f} = kT\lim_{t\rightarrow\infty}{\langle u_x(t)\rangle \over f} \]

Let us apply the linear response formula again to the above nonequilibrium average. Again, we make the identification:

\[ F_e(t) = 1\;\;\;\;\;\;{\textbf D}_i = f\hat{\textbf x}\;\;\;\;\;{\textbf C}_i=0 \]

Thus,

\[\langle u_x(t) \rangle = \langle u_x\rangle_0 + \beta\int_0^t dsf\langle \left(\sum_{i=1}^N\dot{x}_i(0)\right)\left(\sum_{i=1}^N\dot{x}_i(t-s)\right)\rangle_0 \]

\[\langle u_x \rangle_0 + \beta f\int_0^t ds\sum_{i,j}\langle \dot{x}_i(0)\dot{x}_j(t-s)\rangle_0\]

In equilibrium, it can be shown that there are no cross correlations between different particles. Consider the initial value of the correlation function. From the virial theorem, we have

\[ \langle \dot{x}_i\dot{x}_j\rangle_0 = \delta_{ij}\langle \dot{x}_i^2\rangle_0 \]

which vanishes for \(i \ne j \). In general,

\[ \langle \dot{x}_i(0)\dot{x}_j(t)\rangle_0 = \delta_{ij}\langle \dot{x}_i(0)\dot{x}_i(t-s)\rangle_0 \]

Thus,

\[ \langle u_x(t)\rangle = \langle u_x\rangle_0 + \beta f \int_0^t ds\sum_{i=1}^N\dot{x}_i(0)\dot{x}_i(t-s)\rangle_0 \]

In equilibrium, \(\langle u_x \rangle _0 = 0 \) being linear in the velocities (hence momenta). Thus, the diffusion constant is given by, when the limit \( t \rightarrow \infty \) is taken,

\[ D = \int_0^{\infty} \sum_{i=1}^N\langle\dot{x}_i(0)\dot{x}_i(t)\rangle_0 \]

However, since no spatial direction is preferred, we could also choose to apply the external force in the \(\underline {y} \) or \(z \) directions and average the result over the these three. This would give a diffusion constant

\[ D = {1 \over 3}\int_0^{\infty} dt \sum_{i=1}^N\langle \dot{\textbf r}_i(0)\cdot\dot{\textbf r}_i(t)\rangle_0\]

The quantity

\[ \sum_{i=1}^N\langle \dot{\textbf r}_i(0)\cdot\dot{\textbf r}_i(t)\rangle_0 \]

is known as the *velocity autocorrelation function*, a quantity we will encounter again in other contexts.