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Research Article

Studies on hybrid solar collector with water driven solar tracking unit

, ORCID Icon, , ORCID Icon &
Pages 8108-8131 | Received 04 Dec 2023, Accepted 12 Jun 2024, Published online: 26 Jun 2024
 

ABSTRACT

The current solar concentrating collectors can be driven by water gravity without using a torque motor. It saves the electricity required to drive the large solar concentrating collectors. The objective of this study is to simulate and experimentally evaluate a novel hybrid system that combines photovoltaic and thermal technology with a hydro-powered solar tracking unit. The device consists of a hybrid solar collector, which is a multi-reflector compound parabolic collector (MRCPC), an evacuated tube receiver, photovoltaic (PV) panels, and a tracking system. The tracking mechanism attaches the tracking weights to both sides of a chain and sprocket. This hybrid collector rotates around its axis by adjusting the weight of the water in each of the monitoring weights. The system integrates a 12-volt direct current pump (operated by photovoltaic power) for tracking, with flow rate control. A mathematical model is developed and applied to determine the ideal tilt angle for a solar concentrating collector. The model was then used to compare the actual tilt angle and minimize errors in tracking. An experimental investigation used a flow rate of 0.8 LPM. The study achieved a mean tracking error of 2.05º, a maximum thermal efficiency of 43.65%, a maximum solar PV efficiency of 11.30%, and a maximum overall efficiency of 29.81%. An analytical method was developed to simulate the collector’s outlet temperature.

Notations

Acronyms=
MRCPC=

Multi-reflector compound parabolic collector

ETC=

Evacuated Tube Collector

CPC=

Compound Parabolic Collector

PV=

Photovoltaic

LPM=

Liters per minute

DC=

Direct current

PTC=

Parabolic Trough Collector

CG=

Center of gravity

MATLAB=

Matrix Laboratory

HTF=

Heat transfer fluid

Symbols=
WE=

Eastern tracking weight, kg

WW=

Western tracking weight, kg

WC=

Collector weight, kg

WCW=

Counterweight, kg

L=

Spring length at normal position, m

k=

Spring constant, N/m

r=

Radius of circle formed by the end of the spring

e=

Offset from the axis of rotation, m

D=

Diameter of sprocket, m

Dh=

Hydraulic diameter, m

PW=

Wetted perimeter, m

AC=

Net free flow area, m2

di=

Copper tube inner diameter

do=

Copper tube outer diameter

Di=

Evacuated tube inner diameter, m

Re=

Reynold’s number

m˙=

Mass flow rate

Pr=

Prandtl number

Nu=

Nusselt number

h=

Average heat transfer coefficient

Ib=

Average hourly beam radiation

rb=

Tilt factor for beam radiation

A=

Aperture area

W=

Upper aperture width

w=

Lower aperture width

f=

Height of focal point from bottom parabola

Ul=

Overall heat loss coefficient

FR=

Rate of heat removal

S=

Heat flux falling on the evacuated tube, W/m2

C=

Concentration ratio

ql=

Rate of heat loss

hw=

Convective heat transfer coefficient between the glass cover and surrounding air, W/m2

qu=

Useful heat gain rate for the absorber

Cp=

Specific heat

T1=

Temperature at the collector inlet

T2=

Temperature at the collector outlet

T3=

Temperature of storage tank

Greek Symbols=
ζ=

Spring angle with horizontal plane

β=

Collector tilt angle

χ=

Spring tilt angle

ρ=

Reflectivity

υ=

Kinematic viscosity

μ=

Dynamic viscosity

τ=

Transmissivity

α=

Absorptivity

σ=

Stefan-Boltzmann constant

δ=

Declination angle

ω=

Hour angle

φ=

Local Latitude

θ=

Incidence angle

γ=

Azimuth angle

η=

Efficiency

ψ=

Rim angle

ε=

Emissivity

Subscripts=
ref=

Reference

amb=

Ambient

fi=

Inlet fluid of collector

fo=

Outlet fluid of collector

gc=

Glass cover

amb=

Ambient

Acknowledgements

The authors acknowledge the project grant of the Department of Science and Technology (DST), New Delhi, India (DST/TMD/CERI/RES/2020/38(G)) under Applied Research Solar Stream.

Disclosure statement

No potential conflict of interest was reported by the author(s).

Additional information

Funding

The work was supported by the Department of Science and Technology, Ministry of Science and Technology, India [DST/TMD/CERI/RES/2020/38(G)].

Notes on contributors

Tangellapalli Srinivas

Dr. Tangellapalli Srinivas is a Professor in the Department of Mechanical Engineering at the Dr. B.R. Ambedkar National Institute of Technology in Jalandhar, Punjab, India. He received his PhD from JNT University College of Engineering and was a postdoctoral fellow at the University of Ontario Institute of Technology. Dr. Srinivas is the principal investigator for research projects funded by CSIR, SERB, SERB (IMPRINT), and DST. He has industrial consulting experience in solar thermal energy and thermal systems, has one granted patent, two copyrights, and published five patents. He has authored four books, three edited books, 15 book chapters, 125 journal publications, and 90 conference proceedings. Dr. Srinivas has supervised five Ph.D. students, 40 master’s theses, and 45 UG projects.

Aakash Kumar Nimesh

Aakash Kumar Nimesh is pursuing a PhD affiliated with the Department of Mechanical Engineering at Dr B.R. Ambedkar National Institute of Technology in Jalandhar, Punjab, India.

Shivam Tiwari

Shivam Tiwari is a postgraduate scholar from the Department of Mechanical Engineering, Dr B.R. Ambedkar National Institute of Technology, Jalandhar, Punjab, India.

Rajan Kumar

Dr. Rajan Kumar is an Assistant Professor in the Department of Mechanical Engineering at the Dr. B.R. Ambedkar National Institute of Technology, Jalandhar, Punjab, India. He is currently working on laminar micro-convection of gas and liquid with variations in fluid properties. His research interest includes micro-convective flow, micro-electronic cooling, and heat exchanger, numerical investigation of variation in thermophysical properties, and computational fluid dynamics.

Parmvir Singh

Parmvir Singh is pursuing a PhD affiliated with the Department of Mechanical Engineering at Dr B.R. Ambedkar National Institute of Technology in Jalandhar, Punjab, India.

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