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Proof of charge neutrality inside a homogeneous conductor


We show that no charges exist inside the conductors $ A$ and $ B$. With (8) and (28) we obtain from (26) and (27) for the electric field

$\displaystyle \vec E = \left(Q - \frac{1}{e} \left(\frac{\partial \mu}{\partial...
... \frac{1}{e}
 \left(\frac{\partial
 \mu}{\partial n}\right)_T \vec\nabla n \, .$ (31)

We denote the coefficient of $ \vec\nabla T$ on the r.h.s. by $ Q^\prime$. Taking the divergence and neglecting a spatial variation of this coefficient and of the derivative $ (\partial\mu/\partial n)_T$, which may result from the temperature variation, we obtain, using the Maxwell equation

$\displaystyle -e \delta n(\vec r)/\varepsilon_0= \rm {div}\,\, \vec E (\vec r)$ (32)

the following equation for the charge density $ -e\delta n (\vec
r)$:

$\displaystyle -e \delta n ( \vec r) = \varepsilon_0 \left( Q^\prime \Delta
 T(\...
...e} \left(\frac{\partial \mu}{\partial
 n}\right)_T \Delta n (\vec r) \right)\,.$ (33)

$ \Delta$ stands for the Laplacian. Under stationary conditions as assumed the heat conduction equation

$\displaystyle C \dot T - \lambda \Delta T =0,$ (34)

where $ C$ denotes the specific heat per volume, leads to

$\displaystyle \Delta T (\vec r) = 0\, ,$ (35)

which reduces eqn. (33) to the homogeneous differential equation

$\displaystyle \Delta n(\vec r) = \xi^{-2} \delta n(\vec r)\, ,$ (36)

where

$\displaystyle \xi = \left(\frac{\varepsilon_0}{e^2} \left(\frac{\partial
 \mu}{\partial n}\right)_T \right)^{1/2}$ (37)

is a screening length of atomic dimension. Inside a conductor the solution of eqn. (36) decays to zero exponentially within a distance from the surface given by $ \xi$. (We note the following analogy: In the London theory of supraconductivity an equation of the same form as eqn. (36) describes the expulsion of the magnetic field from the interior of a superconductor (Meissner-Ochsenfeld effect) [3].) On a macroscopic scale, therefore, the condition of charge neutrality

$\displaystyle \delta n (\vec r) = 0\, .$ (38)

holds. The charges generating the thermoelectric potential must be located exclusively at surfaces and interfaces!
next up previous
Next: Non-stationary conditions Up: Where do the electric Previous: Where do the electric
Klaus Froboese 2000-11-07