Solar Energy III

Photovoltaic Cells

Direct conversion into electricity Photovoltaics; conversion of solar photons into electrons that flow down a semi-conductor. Main problem is low efficiency (about 10%).

Photons into Electrons: PhotoVoltaic Devices

Charge Generation Photoelectric Effect

To make use of the photoelectric effect, we need material that is a good conductor of electricity and which can be manufactured in bulk at reasonable cost. This conditions strongly constrain the available choices. For most practical aspects, Silicon is the material of choice.

Silicon:

To begin with, we will consider a solid (like a semi-conductor) as any material in which the atoms are arranged in an ordered fashion. Such ordered is usually referred to as a crystal or a lattice. Let's consider the case of silicon.

Silicon has 14 electrons, but only the outer most 4 are available as "valence" electrons to help bond with other atoms.

In its solid form, each silicon atom normally shares one of its four valence electrons in a covalent bond with each of four neighboring silicon atoms. The solid thus consists of basic units of five silicon atoms: the original atom plus the four other atoms with which it shares valence electrons.

In two dimensions we can represent silicon as below

Each silicon atom shares its four valence electrons with valence electrons from four nearest neighbors, filling the shell to 8 electrons, and forming a stable, periodic structure.

Once the atoms have been arranged like this, the outer valence electrons are no longer strongly bound to the host atom. Therefore, in principle, thse outer electrons can easily be "freed" from the lattice and move through the material. The movement of electrons through material is a current.

The outer shells of all of the atoms blend together and form what is called a band. This band is called the conduction band . Electrons that are still bound in atoms are said to be in the valence band .

The difference in energy between these two bands is called the bandgap energy

For a solar energy application, we must find a material in which there is a good match between the band gap and the incoming energy spectrum of solar radiation.

Fortunately, silicon suffices and its very abundant and easily mined from the earth's crust.

Note: more exotic materials can be used to make a solar cell and make a more efficient one but none of those materials has any cost-effective mass production ability.

Schematic structure of energy bands in Silicon:

Hence, if a silicon atom receives at least 1.11 Electron Volts from some source, a valence electron will move to the conduction band. Once an electron is in the conduction band, the material can carry a current and the material is now a conductor.

So much energy is 1.11 Electron Volts?

Recently, a new dimension to this problem is being researched and developed Organic Solar Cells: (a.k.a. Light Harvesting devices)

In essence, the electronic properties of semiconductors (e.g. silicon) can now be mimicked by the use of organic materials, dyes, etc, as means or separating out electrons from the material.

Advantages:

  • Organic (dyes) are flexible and can be commercially produced at a far greater rate than silicon.

Disadvantages:

  • low efficiencies (about 3%) (hence more R&D needed to find the right material)
  • Organics decay - refresh times need to be long (years).
  • high quality control needed for mass production
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