The 2nd law of thermodynamics prohibits a 100%-efficient solar cellular. More
specifically, Carnot’s theorem pertains to photovoltaics and any other solar
power system, where the hot part of the “heat engine” may be the temperature of
the sun and also the cold side is the background temperature on earth. (This is
actually slightly oversimplified. ) In this way, for a system with sunshine
concentration (lenses and decorative mirrors and motors to follow sunlight as it
moves in the sky), the maximum efficiency is ~85%, and for a system that does
not monitor the sun, the maximum efficiency will be ~55%. (For details check in
with my calculations here. )
With an overcast day, tracking the sunlight doesn’t work, so ~55% is the
theoretical maximum.
Available today, the highest efficiency that money can buy is usually …
drumroll … ~35% for unconcentrated photovoltaics (PV) (e. g. Spectrolab), ~35%
for concentrated PV (e. g. Amonix), and ~35% for solar thermal (e. gary the
gadget guy. Ripasso).
By the way, in unconcentrated PV, there is currently an enormous gap between
the highest effectiveness that money can buy (~35% from Spectrolab, for ~$100,
000 for each square meter) and the maximum efficiency that is not insanely
costly (~20% silicon modules through SunPower SPWR +4. 35%). I expect that
difference to shrink dramatically within the next NXGPY +% 10-20 many years
thanks to Alta Devices, that already has a pilot collection creating affordable
~25%-efficient photo voltaic modules, and is moving in the direction of 30% or
even beyond. These types of cells will be light and versatile too! This is very
exciting. However I’m getting off-topic. The actual question is not primarily
regarding what’s affordable, but there is no benefits possible. How to explain
the actual gap between ~35% as well as the theoretical maximum?
For unconcentrated PV, the best cells (currently ~35%) have been creeping
towards theoretical maximum (~55%) for many years (see chart), and I anticipate
they will continue to do so. Really dont mean that they will literally
asymptotically approach closer and nearer to 55%; eventually there will be the
tradeoff where higher minimal efficiency (under standard examination conditions)
comes at the expense associated with lower real-world efficiency (which involves
working robustly below a variety of light and temperatures conditions). So there
is a roof for unconcentrated PV performance, and it’s somewhere between ~35% and
~55%, but Dont really know where.
For focused PV: In theory, PV tissues should get more and more efficient
because light concentration increases. Quite simply, if you double the light
strength, it should *more* than dual the electricity generation. That is why the
theoretical restrict for concentrated systems (~85%) is higher than
unconcentrated (~55%). However , there is a cost in order to concentration too:
(1) The contacts / mirrors are not ideal; (2) The solar mobile will get hotter,
which reduces its efficiency; (3) You are able to only get power from the light
coming directly from sunshine, not the diffuse glowing blue light from the rest
of the atmosphere, which accounts for at least 15% of the light, sometimes much
more. Thanks to those problems, the best centered PV system that money can buy
is definitely more-or-less equally efficient since the best unconcentrated
system that you can buy. Will that always be correct? Well, the nominal
assumptive limit is ~85%, however the only way to get which high is to
concentrate sun light to the maximum possible focus of 50, 000X. At a a lot more
realistic concentration like 1000X, the theoretical limit is actually ~75%.
Next, we take into account the 15% or more dissipates light, and we’re right
down to ~65%. After accounting with regard to imperfect lenses/mirrors and cell
phone heating, we are probably to a limit of 55-60%. Therefore I don’t think we
should assume a huge divergence between the greatest available concentrated PV
compared to unconcentrated PV. The productivity will be basically determined by
the particular PV cell, and the concentrator will have only a small impact on
the system-level efficiency.
The last main category is solar heating, which uses lenses as well as mirrors
and solar-tracking to be able to heat something really very hot, and then use
that to operate a heat engine. The particular highest-efficiency solar thermal
systems currently available are based on stirling engines and they are ~35%
efficient. A Stirling engine can already operate near the Carnot limit,
therefore presumably the primary way to improve efficiency of a solar thermal
product is to heat the thing to the next temperature. To get that hypothetical
~85% efficiency, you need to focus the sunlight by a factor of fifty, 000, and
heat the one thing to 2000C. This heat is insanely high: I believe that no one
knows how to create a long-lasting high-efficiency heat motor that can work at
such a warm. If you heat to “only” 1000C, the maximum efficiency falls to ~75%;
if you temperature to 600C - that is realistic in a solar stirling engine system
- then your maximum efficiency is ~65% (or ~55% including the lost 15% diffuse
light, since discussed above). That 57% figure is still way over a ~35% that has
been achieved up to now, so there seems to be lots of room for improvement when
the solar thermal industry continues to grow. However the 85% figure will never
occur, and even 70% is extremely not likely.
(For completeness, I should point out that there are solar power systems that
will don’t fit in any of the over categories, like thermophotonics and also
thermophotovoltaics. These are very early-stage ideas, and I don’t understand
enough about them to opinion. )
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