# Thermoelectric Effect

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 Date Published: March 16, 2021 Last Modified: March 16, 2021

## Seebeck Effect

The Seebeck Effect is the electro-motive force (EMF, can be thought of as a voltage) which appears across two points of an electrically conductive material when there is a temperature difference between them. The amount of EMF depends on the material used.

The following diagram shows the basic environment to create the Seebeck Effect.

Note that in practise, the EMF generated across a single conductor moving through a temperature gradient is not really useful for anything, since to measure this voltage and/or conduct any current, you need a return path. However, if you used the same material wire for the return path, it would experience the exact same temperature gradient but in reverse, the two EMF’s would cancel each other out, and you would measure no voltage across the loop. This is where a second trick is is used to generate a working thermocouple — a second wire of different material is used for the second half of the loop. The different material ideally has a widely different Seebeck coefficient and hence generates a different EMF for the same temperature differential, thus creating a measurable voltage and/or current.

Don’t think you can cheat by measuring the voltage across a single wire with a multimeter…the second temperature gradient will still be there, in the wires of the multimeter. The following diagram shows a practical thermocouple design using dissimilar conductors to form a complete circuit:

The Seebeck Effect is primarily used to make thermocouple based temperature sensors and thermoelectric power generators (fun fact: the power source aboard the Mars rover Perseverance uses the Seebeck Effect, it uses radioactive decay to create the required temperature differential to then generate electric power.

### The Seebeck Coefficient

The Seebeck coefficient is calculated from the following equation:

\begin{align} S = -\frac{\Delta V}{\Delta T} \end{align}

where:
$$S$$ is the Seebeck coefficient, in $$VK^{-1}$$
$$\Delta V$$ is the change in voltage, in $$V$$
$$\Delta T$$ is the change in temperature, in $$K$$ (although $$^{\circ}C$$ would also work)

Because of the negative sign in the above equation, a positive Seebeck coefficient will result in the higher temperature region having a lower voltage. Most Seebeck coefficients are small relative to $$1VK^{-1}$$ are written in units of $$uVK^{-1}$$.

Semiconductors also have Seebeck coefficients. In general, P-doped semiconductors have positive Seebeck coefficients and N-doped semiconductors have negative Seebeck coefficients. Most semiconductor Seebeck coefficients are much larger than those of metals. Intrinsic semiconductors have a Seebeck coefficient of $$0$$.

The Seebeck coefficient of some common metals and semiconductors, relative to Platinum, are shown in the below tables1:

Metals

MaterialSeebeck Coefficient ($$uVK^{-1}$$)
Copper6.5
Gold6.5
Lead4.0
Aluminium3.5
Platinum0 (by definition)
Sodium-2.0
Nickel-15
Constantan-35
Bismuth-72

Semiconductors

Notice how the coefficients are typically much higher than metals!

MaterialSeebeck Coefficient ($$uVK^{-1}$$)
Se900
Te500
Si440
Ge300
PbTe-180
$$Pb_{15}Ge_{37}Se_{58}$$-1990

## Authors

### Geoffrey Hunter

Dude making stuff.

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