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HDE 226868
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In his 1905 paper on Brownian motion, Einstein derived the equation $$D=\frac{RT}{N}\frac{1}{6\pi kP}\tag{7}$$ where $T$ is temperature, $k$ is viscosity, $P$ is the radius of a spherical molecule (the Stokes radius) and $R$ and $N$ are constants.

A more familiar form used by Wikipedia is $$D=\frac{k_BT}{6\pi\eta r}$$ where $k_B$ is Boltzmann's constant, $\eta$ is viscosity, and $r$ is the radius. The variant you have, $$\frac{D}{\mu}=V_t$$ arises from defining the thermal voltage as $$V_t\equiv\frac{k_BT}{q}$$ and writing the electrical mobility $\mu$ in terms of $q$ and $6\pi\eta r$.

Sutherland and Smoluchowski also did similar work to arrive at variations of the equation, so they, too, deserve some credit. That said, neither Smoluchowski nor Einstein (I don't have access to the full text of Sutherland's work) used thermal voltage to compactify the diffusion equation.

In his 1905 paper on Brownian motion, Einstein derived the equation $$D=\frac{RT}{N}\frac{1}{6\pi kP}\tag{7}$$ where $T$ is temperature, $k$ is viscosity, $P$ is the radius of a spherical molecule (the Stokes radius) and $R$ and $N$ are constants.

A more familiar form used by Wikipedia is $$D=\frac{k_BT}{6\pi\eta r}$$ where $k_B$ is Boltzmann's constant, $\eta$ is viscosity, and $r$ is the radius. The variant you have, $$\frac{D}{\mu}=V_t$$ arises from defining the thermal voltage as $$V_t\equiv\frac{k_BT}{q}$$ and writing the electrical mobility $\mu$ in terms of $q$ and $6\pi\eta r$.

Sutherland and Smoluchowski also did similar work to arrive at the equation, so they, too, deserve some credit.

In his 1905 paper on Brownian motion, Einstein derived the equation $$D=\frac{RT}{N}\frac{1}{6\pi kP}\tag{7}$$ where $T$ is temperature, $k$ is viscosity, $P$ is the radius of a spherical molecule (the Stokes radius) and $R$ and $N$ are constants.

A more familiar form used by Wikipedia is $$D=\frac{k_BT}{6\pi\eta r}$$ where $k_B$ is Boltzmann's constant, $\eta$ is viscosity, and $r$ is the radius. The variant you have, $$\frac{D}{\mu}=V_t$$ arises from defining the thermal voltage as $$V_t\equiv\frac{k_BT}{q}$$ and writing the electrical mobility $\mu$ in terms of $q$ and $6\pi\eta r$.

Sutherland and Smoluchowski also did similar work to arrive at variations of the equation, so they, too, deserve some credit. That said, neither Smoluchowski nor Einstein (I don't have access to the full text of Sutherland's work) used thermal voltage to compactify the diffusion equation.

Typo.
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HDE 226868
  • 10.9k
  • 5
  • 43
  • 77

In his 1905 paper on Brownian motion, Einstein derived the equation $$D=\frac{RT}{N}\frac{1}{6\pi kP}\tag{7}$$ where $T$ is temperature, $k$ is viscosity, $P$ is the radius of a spherical molecule (the Stokes radius) and $R$ and $N$ are constants.

A more familiar form used by Wikipedia is $$D=\frac{k_BT}{6\pi\eta r}$$ where $4k_B$$k_B$ is Boltzmann's constant, $\eta$ is viscosity, and $r$ is the radius. The variant you have, $$\frac{D}{\mu}=V_t$$ arises from defining the thermal voltage as $$V_t\equiv\frac{k_BT}{q}$$ and writing the electrical mobility $\mu$ in terms of $q$ and $6\pi\eta r$.

Sutherland and Smoluchowski also did similar work to arrive at the equation, so they, too, deserve some credit.

In his 1905 paper on Brownian motion, Einstein derived the equation $$D=\frac{RT}{N}\frac{1}{6\pi kP}\tag{7}$$ where $T$ is temperature, $k$ is viscosity, $P$ is the radius of a spherical molecule (the Stokes radius) and $R$ and $N$ are constants.

A more familiar form used by Wikipedia is $$D=\frac{k_BT}{6\pi\eta r}$$ where $4k_B$ is Boltzmann's constant, $\eta$ is viscosity, and $r$ is the radius. The variant you have, $$\frac{D}{\mu}=V_t$$ arises from defining the thermal voltage as $$V_t\equiv\frac{k_BT}{q}$$ and writing the electrical mobility $\mu$ in terms of $q$ and $6\pi\eta r$.

Sutherland and Smoluchowski also did similar work to arrive at the equation, so they, too, deserve some credit.

In his 1905 paper on Brownian motion, Einstein derived the equation $$D=\frac{RT}{N}\frac{1}{6\pi kP}\tag{7}$$ where $T$ is temperature, $k$ is viscosity, $P$ is the radius of a spherical molecule (the Stokes radius) and $R$ and $N$ are constants.

A more familiar form used by Wikipedia is $$D=\frac{k_BT}{6\pi\eta r}$$ where $k_B$ is Boltzmann's constant, $\eta$ is viscosity, and $r$ is the radius. The variant you have, $$\frac{D}{\mu}=V_t$$ arises from defining the thermal voltage as $$V_t\equiv\frac{k_BT}{q}$$ and writing the electrical mobility $\mu$ in terms of $q$ and $6\pi\eta r$.

Sutherland and Smoluchowski also did similar work to arrive at the equation, so they, too, deserve some credit.

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HDE 226868
  • 10.9k
  • 5
  • 43
  • 77

In his 1905 paper on Brownian motion, Einstein derived the equation $$D=\frac{RT}{N}\frac{1}{6\pi kP}\tag{7}$$ where $T$ is temperature, $k$ is viscosity, $P$ is the radius of a spherical molecule (the Stokes radius) and $R$ and $N$ are constants.

A more familiar form used by Wikipedia is $$D=\frac{k_BT}{6\pi\eta r}$$ where $4k_B$ is Boltzmann's constant, $\eta$ is viscosity, and $r$ is the radius. The variant you have, $$\frac{D}{\mu}=V_t$$ arises from defining the thermal voltage as $$V_t\equiv\frac{k_BT}{q}$$ and writing the electrical mobility $\mu$ in terms of $q$ and $6\pi\eta r$.

Sutherland and Smoluchowski also did similar work to arrive at the equation, so they, too, deserve some credit.