Nernst effect

In physics and chemistry, the Nernst Effect (also termed first Nernst–Ettingshausen effect, after Walther Nernst and Albert von Ettingshausen) is a thermoelectric (or thermomagnetic) phenomenon observed when a sample allowing electrical conduction is subjected to a magnetic field and a temperature gradient normal (perpendicular) to each other. An electric field will be induced normal to both.

This effect is quantified by the Nernst coefficient |N|, which is defined to be

where ${\displaystyle E_{Y}}$ is the y-component of the electric field that results from the magnetic field's z-component ${\displaystyle B_{Z}}$ and the temperature gradient ${\displaystyle dT/dx}$.

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