Direct conversion into electricity
Photovoltaics; conversion of solar photons into electrons that
flow down a semi-conductor.
Main problem is low efficiency (about 10%).
When photons strike a metal, their energy is used to liberate loosely
bound electrons and therefore induce a current.
Efficiency of this process depends upon the material
This is the principle behind Digital Cameras (all college graduates should know how
a digital camera works -- its a literacy test).
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?
1.11 eV corresponds to the energy that a photon of
wavelength 1.12 microns has.
77% of the energy from the sun is carried in photons
with wavelength less than this and therefore can move
a valence electron in silicon into the conducting band.
However, as silicon heats up, more frequent collisions
of atoms and carriers occur in the material. This causes the
internal resistance to increase and the overall ability to
carry a current decreases. Thus, as the temperature rises,
the efficiency of a silicon PV cell decreases .
You can not defeat this fundamental piece
of physics without paying an even larger energy cost in cooling.
Note that all measures of PV efficiency are made a 0 degrees C
when done in a lab. "Rated" efficiencies are usually done at a
standard temperature of 25 C.
In general:
efficiency is decreased by 0.5% for every 1 degree C incresae in Temperature
operating temperature of roof top PV array is usually 20-40 degrees C higher
than the air temperature.
ON a 100 degree F day, a PV will have an efficiency of only 2-3% (but this is compensated
for by abundant sunshine).
Real world performance of most systems, averaged anually, is 5-10%
Important Notes:
NanoSolar turns out to be lying; CIGS = copper indium gallium deselenide
We are limited in copper and sellenium
FSLR (First Solar): CdTe (cadmium telluride)
Cadmium is toxic and banned in many countries; The abundance of Tellerium is
15-30 times less than the abundance of Platinum
Thin film (amorphous silicon) is most abundant and most practical but has
the highest costs and somewhat low efficiency.
Crystalline silicon is the best but takes a long time to process.
What's unique about this class: We interrogate the real world!
Real World Production
Notes:
by 2011 Total installed worldwide capacity is now 16 GigaWatts (16,000 MegaWatts)
The World uses 2TW of net electricit now and by 2011 that will have increased to
abotu 2.4 TW (2400 Gigawatts)
Total installed capacity is thus 16/2400 = .007 (.7 %)
Now pick 2020 target: World uses 3 TW; Optimistic PV Growth Scenario (doubles every 2.5 years)
means that you get about 135 GW installed by year 2020 - in raw numbers this is good but as
part of the energy portfolio is still just 135/3000 which is less than 5%
Worse, however, is that is unlikely that this doubling time can be sustained due to ever
increasing material requirements
Bottom line: Conventional PV solar power is probably not scalable fast enough!
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).