What Are The Seebeck Effect And The Peltier Effect?

The Seebeck Effect and the Peltier Effect are the two major principles which govern the working of thermoelectric generators.

The Seebeck Effect and the Peltier Effect can be classified under the thermoelectric effect. Any thermoelectric effect involves the conversion of differences in temperatures into voltage differences. The Seebeck and Peltier Effects are different manifestations of the same physical process.

In some instances, they are linked and known as the Seebeck-Peltier Effect. The reason why these two effects are separated is due to their independent discoveries by two different individuals.

Let’s first look at the Seebeck Effect in detail.

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What Is The Seebeck Effect?

The Seebeck Effect was discovered by the Baltic German physicist Thomas Johann Seebeck. This phenomenon occurs when there is a temperature difference between two dissimilar conductors or semiconductors, which results in a voltage difference between them.

When heat is applied to one of the conductors or semiconductors, the electrons in the material become excited and start moving toward the cooler side of the two substances. If the two conductors are connected in a circuit, a direct current flows through it.

Seebeck Effect With A Simple-to-understand Example

The Seebeck Effect is like your brain telling your hand to pull away when it accidentally touches something hot. Imagine two different wires placed next to each other. When one wire gets heated, the energy (in the form of hot electrons) starts to jump around much more. Because the other wire is cooler, the agitated electrons start to move towards it.

Picture those electrons like a group of kids in a classroom. When the room gets hot (like when you turn the heater on), the kids (or electrons) get more active. They start to move around, trying to find a cooler spot to settle down.

Now, if you connect these two wires like a full loop (just imagine two ends of a jump rope), those moving electrons will start to flow around that loop. This flow is what we call electricity or direct current.

So, just by heating one wire and connecting both ends, we’ve created an electric current! That’s the Seebeck Effect.

The voltages produced by the Seebeck Effect are tiny. The range of the voltage produced is usually on the order of a few microvolts (one-millionth of a volt) per Kelvin of temperature difference at the junction. If the temperature difference is significant enough, some devices can produce a few millivolts (one-thousandth of a volt).

Several such devices can be connected in parallel to increase the maximum deliverable current. Such devices have been shown to provide a small-scale level of electrical power if a large temperature difference is maintained across the junctions.

The Seebeck Effect can help us calculate the electromotive field generated by a device. This can be done by using the Seebeck Coefficient. The Seebeck Coefficient of a material is the measure of the magnitude of the increased thermoelectric voltage in response to the temperature differences in a given material. Using the Electromotive force, we can also calculate the current density of the thermoelectric material. The relevant equations for this are as follows:

E_emf= -S∆T

J= σ(-∆V+E_emf)

Here, J signifies the current density, and σ  signifies the local conductivity of the conductor.

What Is The Peltier Effect?

The Peltier Effect was named after the French physicist Jean Charles Athanase Peltier, who discovered this phenomenon in 1834. The Peltier Effect is the presence of heating or cooling at an electrified junction of two different conductors. When a current is made to flow through a junction between two conductors, heat may be added or removed at the junction.

The Peltier Effect is like a special power that can make parts of an electrical circuit hot or cold. Think of it this way: two different types of metal wires are joined together. When you send electricity through that joining point, it can heat up or cool down that spot.

The Peltier heat generated at the junction per unit time is where ∏_A and ∏_B are the Peltier coefficients.

Q=(∏_A – ∏_B)I

Here, A and B signify the two ends of the conductors, while I is the electric current. The Peltier coefficients represent how much heat is carried per unit of charge. Since the charge must be continuous across a junction, the associated heat flow will discontinue if ∏_A  and ∏_B differ.

The Peltier Effect can be considered as the back-action counterpart to the Seebeck Effect. If a simple thermoelectric circuit is closed, the Seebeck Effect will drive a current, which in turn (by the Peltier effect) will always transfer heat from the hot to the cold junction.

A typical Peltier heat pump involves multiple junctions in series, through which a current is driven. Some junctions lose heat due to the Peltier Effect, while others gain heat. Thermoelectric heat pumps, as do thermoelectric cooling devices found in refrigerators, exploit this phenomenon.