Abstract
Fresnel lenses allow the concentration of sunlight that can be employed in different thermal unitary operations or endothermic chemical transformations. A system with Fresnel lenses should also take into account vessel or reactor surface thermal losses (reflection, convection and emission), as well as the thermal energy required to keep the vessel or reactor structure warm. In this paper, a numerical and experimental analysis indicated that the solar radiation incident on the lens, the Fresnel lens area and the specimen mass can be represented by a grouping called Heating Factor (31 ≤ Ψ (W/kg) ≤ 3347). The Heating Factor (Ψ) was strongly correlated with the maximum temperature conductive specimens could reach when inserted at the focal point of a Fresnel Lens. Equilibrium Temperatures were predicted by a physical-mathematical model and validated by experimental tests. The Fresnel lens system has been shown to be able of providing Equilibrium Temperatures from 345 to 1600 K for specimens with Heating Times between 3 and 85 min and Initial Thermal Rates from 1.16 to 312.00 K/min. Numerical-experimental analyses also showed that the heating dynamic was strongly influenced by the nature of the materials that constituted the specimens (specific mass and the specific heat).
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Abbreviations
- a :
-
parameter adjusted for Equilibrium Temperature Eq. (K kgm/Wm).
- a c :
-
gravitational acceleration (m/s2).
- a i :
-
linear effects (i = 1..3) of variables on Equilibrium Temperature (K).
- A ij :
-
nonlinear effects (i,j = 1..3) of variables on Equilibrium Temperature (K).
- a S :
-
surface area of specimen (m2).
- A L :
-
Fresnel lens useful area (m2).
- b :
-
parameter adjusted for Heating Time Equation (min).
- b i :
-
linear effects (i = 1..3) of variables on Heating Time (min).
- B ij :
-
nonlinear effects (i, j = 1..3) of variables on Heating Time (min).
- c i :
-
linear effects (i = 1..3) of variables on the Initial Thermal Rate (K/min).
- C ij :
-
nonlinear effects (i, j = 1..3) of variables on the Initial Thermal Rate (K/min).
- c PF :
-
specific heat of the fluid (J/kg K).
- c PS :
-
specific heat of the specimen (J/kg K).
- D :
-
sphere diameter (m).
- f :
-
parameter adjusted for Initial Thermal Rate Eq. (K kgg/min Wg).
- F S → ∞ :
-
form factor between specimen and environment (−).
- g :
-
parameter adjusted for Initial Thermal Rate Equation (−).
- G :
-
incident solar radiation on the top of the Fresnel lens (W/m2).
- h :
-
convective heat transfer coefficients (W/m2K).
- H :
-
height of the aluminum frame experimental unit (m).
- k F :
-
fluid thermal conductivity (W/m K).
- k S :
-
specimen thermal conductivity (W/m K).
- ℓ :
-
Fresnel lens focal length (m).
- L :
-
Fresnel lens length (m).
- m :
-
set parameter for Equilibrium Temperature Equation (−).
- n :
-
set parameter for Heating Time Equation (kg/W).
- M :
-
specimen mass (kg).
- N :
-
counter for possible combinations of Ψ (−).
- Nu :
-
Nusselt number (−).
- p :
-
significance index of adjusted parameters (−).
- Pr :
-
Prandtl number (−).
- q 0 :
-
initial thermal rate of specimens (K/min).
- q c :
-
thermal convection heat loss rate of the specimen (J/s).
- q e :
-
thermal radiation heat loss rate of the specimen (J/s).
- q i :
-
heat rate incident on the specimen (J/s).
- q r :
-
heat rate reflected by specimen (J/s).
- Ra :
-
Rayleigh number (−).
- t :
-
time (min).
- T :
-
instantaneous specimen temperature (K).
- T E :
-
steady-state specimen Equilibrium Temperature (K).
- T F :
-
melting temperature of specimen material (K).
- t H :
-
specimen Heating Time to reach steady state (min).
- T ∞ :
-
ambient temperature (K).
- VS :
-
specimen volume (m3).
- W :
-
Fresnel lens width (m).
- X 1 :
-
coded Fresnel lens area (−).
- X 2 :
-
coded specimen mass (−).
- X 3 :
-
incident solar radiation coded on Fresnel lens (−).
- α :
-
surface absorptivity of the specimen (−).
- α F :
-
thermal diffusivity of fluid (m2/s).
- β :
-
coefficient of thermal expansion of fluid (K−1).
- δ:
-
relative deviation between predicted values and experimentally observed values (−).
- ε :
-
surface emissivity of the specimen (−).
- η :
-
Average Equilibrium Temperatures of each specimen (K).
- λ :
-
Average Heating Times of each specimen (min).
- μF :
-
dynamic viscosity of the fluid (kg/m s).
- ρ :
-
surface reflectivity of the specimen (−).
- ρ F :
-
density of the fluid (kg/m3).
- ρ S :
-
density of the specimen (kg/m3).
- σ :
-
Stefan-Boltzmann Constant (W/m2K4).
- τ :
-
transmissivity of specimen (−).
- τ L :
-
transmissivity of Fresnel lens (−).
- ν F :
-
kinematic viscosity of the fluid (m2/s).
- φ:
-
Average Initial Thermal Rates of each specimen (K/min).
- Ψ :
-
Heating Factor (W/kg).
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The authors would like to thank FAPEMIG (Universal/APQ/01758-17) and the Laboratory for Separation and Sustainable Energy (LASER/FEQUI/UFU) for the financial resources.
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D’Arc de Fátima Palhares, D., Araújo, B.S.A., de Faria, É.V. et al. Numerical-experimental evaluation of FRESNEL lens heating dynamics. Heat Mass Transfer 56, 3147–3166 (2020). https://doi.org/10.1007/s00231-020-02924-8
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DOI: https://doi.org/10.1007/s00231-020-02924-8