Abstract:
Majority of the present solar thermal systems are constructed using surface
absorption-based absorbers, wherein solar energy is first absorbed by a selectively coated
solid surface and then transferred to a working fluid through conduction and convection
heat transfer. Selective coatings have high absorptivity across the incident solar energy
spectrum (0.3 µm - 2.5 µm) while simultaneously having low emissivity in the midinfrared
region (2.5 µm - 10 µm). These characteristics make selective coatings quite
suitable for harnessing solar thermal energy. However, during such a process an inherent
thermal barrier is present in the form of conduction and convection resistances between
the absorbing surface and the working fluid. As a result, conversion of solar energy into
thermal energy of the working fluid is not a very efficient process in surface absorptionbased
solar thermal systems. This problem becomes more pronounced in the case of
concentrating solar collectors as the flux that must be transferred across this barrier
increases. In this case, excessively high surface temperatures can develop relative to fluid
temperature. Since radiative losses are proportional to the fourth power of the surface
temperature, high surface temperatures lead to excessively high radiative heat losses and
stringent material requirements. This problem can be reduced by allowing the incident
solar radiation to interact directly with the working fluid without heating any other
structures within the receiver.
Although typical heat transfer fluids are transparent in significant portion of solar
spectrum, dispersing trace amounts of nanoparticles can significantly enhance the solar
irradiance absorption capability of these basefluids. Excellent stability (relative to
micron-particle suspensions) coupled with high solar energy absorption capability make
nanoparticle dispersions (popularly known as 'nanofluids') suitable for solar thermal
applications. Moreover, the fact that the optical properties of metallic and semiconductor
nanoparticles are dependent on their shape, size, and the surrounding dielectric media
makes them easily usable for engineering highly solar selective nanoparticle dispersions
at very low volume fractions. Furthermore, critical analysis of the previous studies
relevant to nanofluid-based solar thermal systems reveals that these novel solar thermal
systems hold huge potential and warrant further exploration. The present study is an attempt to understand the optical behavior of nanoparticle
dispersions and investigate the key heat transfer mechanisms involved in the volumetric
absorption solar thermal systems employing these nanoparticle dispersions. Firstly, an
attempt has been made to model optical properties of nanoparticle dispersions. It has been
found that optical properties of metallic nanoparticles can be calculated from that of the
corresponding bulk values after incorporating intrinsic size effects in the classical Drude
model. Opposed to nanospheres, nanospheroids have optical signatures which are
characteristic of particle shape and size. Thus anisotropic geometries are far more
optically tunable as compared to their isotropic counterparts. Next, a detailed heat transfer
model was developed for cylindrical volumetric receiver (simulating a linear parabolic
trough) employing nanoparticle dispersion as the working fluid. Furthermore, it was
demonstrated that it is possible to make these volumetric receivers ‘solar selective’
through usage of heat mirrors. This exercise reveals that there is a definite improvement
in terms of thermal efficiency in the case of the nanofluid-based volumetric receivers
relative to their surface absorption-based counterparts. The modeling results being
encouraging paved the way to carry out experimental demonstrations of laboratory scale
solar thermal systems. As a first step in this direction, an attempt was made to identify the
optimal nanoparticle-basefluid pair for solar thermal systems. For this optical
characterization of various basefluids and nanoparticle dispersions was carried out using
UV-VIS and FT-IR spectrophotometers. This exercise confirmed that most of the
common basefluids are nearly transparent in most part of the short wavelength region
(0.2 µm - 1.5 µm) and highly absorbing in long wavelength region (2.5 µm - 25 µm).
Hence, as such these basefluids alone are not good enough for harnessing solar energy
and definitely some additives need to be added to make them good solar absorbers.
Furthermore, it was found that addition of nanoparticles to the basefluid significantly
enhanced the solar irradiance absorption capability. Rate of increase of solar weighted
absorptivity with increase in mass fraction of nanoparticles was found to be highest in the
case of amorphous carbon. Now that optimum nanoparticle material was identified, next
step was to test these nanoparticle dispersions for their heat transfer behavior. For this
purpose a proof-of-concept experiment was carried out. In this experiment, nanoparticle
dispersion (amorphous carbon nanoparticles in ethylene glycol) was employed as the
working fluid in the volumetric absorption system. Furthermore, in the same
configuration, pure liquid (ethylene glycol) was placed in contact with a selectively
coated (TiNOX) copper substrate to test the baseline surface absorption system. It was found that under similar operating conditions, higher average stagnation temperatures are
achievable if the electromagnetic radiation is allowed to directly interact with the bulk of
the fluid (which is the case in a volumetric absorption system), compared to the
conventional surface absorption system. Moreover, the performance of the volumetric
absorption system was found to be sensitive to the amount (mass fraction) of the
nanoparticles dispersed - which, in the limit, approached surface absorption at very high
mass fractions. Furthermore, the spatial temperature distribution was found to be
consistent with the underlying theory of volumetric absorption.
Based on the optical characterization and heat transfer analysis of nanofluid-based
volumetric absorption solar thermal systems it can be concluded that these systems
promise enormous potential in harnessing solar energy. Anisotropic metal nanoparticles
and broad absorption carbon nanoparticles are most suitable for harnessing solar thermal
energy. For high temperature operating conditions, heat mirrors should be employed to
curb radiative losses. As a whole there is a definite relevance of these nanofluid-based
solar thermal systems and further research into these systems is warranted.