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33
International Journal on Integrated Education
e-ISSN : 2620 3502
p-ISSN : 2615 3785
Volume 3, Issue IX, September 2020 |
Mathematikal model of calclation parabola-cylindirical
solar hot water systems of industrial enterprises
SULAYMONOV HUSANBOY MANNOPOVICH
Ferghana Polytechnic Institute.
ERGASHEV SIROJIDDIN FAYAZOVICH .
Ferghana Polytechnic Institute.
MAMADIEVA DILXUMOR TOLIBJONOVNA
Ferghana Polytechnic Institute.
Abstract
The article analyzes a mathematical model for calculating solar parabola cylindrical hot water systems
for industrial and municipal enterprises. The formulas for determining heat losses associated with
radiant and convective heat exchange, as well as useful heat energy and efficiency of solar parabola-
cylindrical systems for obtaining heat for industrial purposes are given.
Keywords: Solar radiation, energy, temperature, heat supply, process steam, productivity, battery, hot
water, thermal energy, electricity, optical losses, heat losses, hot water supply, energy balance, industry
1. INTRODUCTION
Most solar parabola-cylindrical hot water systems for industrial and municipal enterprises
operate according to the thermal model shown in Fig.1 and consist of the following main components:
parabola-cylindrical collectors, accumulator tank, circulation pumps and hot water supply doubler 1, 2,
4, 5, 6. The system is provided with hot water with a temperature of 60÷100°C.
The hot water supply system is made according to a single-circuit scheme, i.e. the heated water
in parabola-cylindrical collectors enters the hot water storage tank. Water from the Central water supply
network enters the lower part of the battery tank, and hot water for technological processes are taken
from the upper part of the tank. The system is protected from freezing by draining water from the
collectors.
2. MAIN PART
When the water temperature falls below the required operating temperature for the
technological process,
т
г
Т the DT doubler is turned on; this will warm up the water coming from the
storage tank.
The system works as follows. Circulation of water through parabola-cylindrical collectors
occurs if the equilibrium temperature 
Т the absorbing surface of the heat receiver is higher than the
temperature Б
Т at the bottom of the battery tank by the amount of Т
 due to the temperature
difference in the main pipelines of this circuit
34
International Journal on Integrated Education
e-ISSN : 2620 3502
p-ISSN : 2615 3785
Volume 3, Issue IX, September 2020 |
Т
Т
Т Б 



(1) Hot water is extracted from the upper part of the battery tank by the flow rate r
m to places
where water is collected. From Fig.2 it can be seen that the consumption r
m defined as
follows:
Т
Г
r m
m  при
Т
Г
Б Т
Т 
and from the equality
  Т
Г
Р
Т
Г
в
х
Р
r
Т
Г
Б
Р
r Т
С
т
С
m
m
Т
С
m 






 .
.
 (2)
determine
 
 
в
х
Б
в
х
Т
Г
Т
r
r
Т
Т
Т
Т
m
т
.
.



при
Т
Г
Б Т
Т  (3)
where:
Т
Г
Т ,
Т
r
m - water temperature and flow rate determined by the process load schedule;
в
х
Т . - the temperature of the feed water provided from a Central water supply network.
In the description of the mathematical model parabola-cylindrical hot
Fig. 1 Thermal models of parabola-cylindrical installations for the production of hot water
(a), steam (b) and water lifting (C).
Fig. 2. Scheme for determining r
m
35
International Journal on Integrated Education
e-ISSN : 2620 3502
p-ISSN : 2615 3785
Volume 3, Issue IX, September 2020 |
the following assumptions were made: neglect the uneven distribution of solar energy flow between
collectors; do not take into account heat loss from the surface of connecting pipelines; based on the
results of preliminary calculations, neglect the temperature gradient along the perimeter and heat loss by
thermal conductivity to the supporting elements of the heat receiver design. These assumptions make it
possible to significantly simplify the mathematical model of the system, and consider parabolocylindric
collectors as a single collector.
To consider the energy balance over time, the estimated period of operation of the system is divided into
N equal parts in increments 
 , for each i
 point in time
 
N
i ,...
2
,
1
 at the beginning of the step,
the thermal balance of each system element is considered. In this case, the main dependencies used for
calculating each component of the system at a time i
 and the functional relationship between the
elements are shown below.
Unit parabola-cylindrical collectors. To determine the useful heat
пк
пол
Q , the collector energy balance
equation is used for the energy received from the parabolocylindric collectors in the storage tank,
expressed in terms of the equilibrium temperature of the absorbing surface of the receiver 
Т and
temperature Б
Т at the bottom of the tank
 
Б
L
R
пк
пол Т
Т
C
U
F
F
Q 



 
1
3 (4)
Equilibrium temperature 
Т the absorption surface of the receiver is determined by the formula [7]
,
L
зап
О
О
О
U
С
К
Е
Т
Т







(5)
where: зап
К -coefficient that takes into account dust on the mirror surface of the hub.
When calculating the flow density of direct solar radiation, the main methods used are the orientation of
collectors rotating around a horizontal North-South or East-West axis.
Heat losses associated with partial boiling and evaporation of water are determined by the formula [7]
 
Б
и
Р
к
пк
пол
пот
исп Т
Т
С
т
Q
Q 



.
(6)
where: и
Т - boiling point of water;
к
т - water consumption in the system circuit.
The flow rate of evaporated water is determined by a well-known formula 8:
r
Q
т u
и /
 . (7)
Taking into account (7) the water temperature at the outlet of the heat receiver is determined by the
formula:
 
Р
к
пот
исп
Б
вых
к
С
т
Q
Qппо
Т
Т



(8)
At the end time of the estimated period of operation of the system, the following values are determined
that characterize the balance of water heating energy in parabola-cylindrical collectors:
1. The Sum of the incident (direct component) of solar radiation
 
пад
Q
on the collector surface
perpendicular to the rays:
   
3
3
1
10

 




 
F
E
Q oi
I
N
пад
. (9)
2. Total solar energy
 
пог
Q
absorbed in the collector's heat sink:
   
3
3
1
10

 





 
о
oi
I
N
пог F
E
Q
. (10)
36
International Journal on Integrated Education
e-ISSN : 2620 3502
p-ISSN : 2615 3785
Volume 3, Issue IX, September 2020 |
3. The total optical loss in parabola-cilindrical collectors
     



 пог
пад
пот
опт Q
Q
Q
. (11)
4. Solar energy
  н
ц
пог
Q . water absorbed during the operation of the circulation pump through the
collector. Value
  н
ц
пог
Q . defined using equation (11) when the condition is met
Т
Т
Т Б 


 .
5. Total amount of heat
 Б
пк
пол
Q  coming into the storage tank of parabola-cilindrical collectors
     
 
3
1
3
1
10
10 



 









 
 Б
вых
к
Р
u
k
N
i
пк
полi
N
i
Б
пк
пол Т
Т
С
m
m
Q
Q
(19)
6. Heat losses in the collector heat sink
  с
т
нв
пот
теп
Q
.
caused by the impossibility of heat removal by the
heat carrier of the absorbed solar radiation under the condition
Т
Т
Т Б 



        н
ц
пог
пог
пог
тс
нв
пот
теп Q
Q
Q
Q .


 
 (20)
7. The total heat loss
 
пот
теп
Q
taking into account heat loss
 и
пот
теп
Q partially evaporated water at
the rate of mu
      
  3
.
.
1
10

 





 
с
т
i
нв
пот
теп
Б
u
Р
ui
N
i
пот
теп Q
Т
Т
С
m
Q
(21)
8. Heat losses in the collector during operation of the pump:
       
 

 пот
теп
Б
пк
пол
н
ц
пог
н
ц
пот
теп Q
Q
Q
Q .
.
(22)
The tank is a heat accumulator. To simplify the mathematical model of the heat storage tank, we write
down the heat balance equation without taking into account stratification and heat loss from the tank
surface 7, 8, 9.:
      
Б
в
х
u
r
Б
вых
к
Р
u
k
Б
Р
Б Т
T
m
т
Т
Т
С
m
m
d
dT
С
F
М 






 .
3
 (23)
where: Б
М - mass of water in the accumulator tank per 1 m2 of the aperture area of the parabola-
cylindrical collector, kg/m2
Integrating equation (23) according to the Euler model, we determine the temperatures 1

Бi
Т water at
the end of the time step:
     
 
Бi
в
х
ui
ri
Бi
ki
u
k
Б
i
Б
Бi Т
T
m
m
T
T
m
m
F
M
T
T 








 .
3
.
1

(24)
Backup hot water supply. Total amount of energy
 
Д
Q
the water consumed for preheating by the
backup in the load loop to the temperature
Т
Г
Т during the estimated period of operation of the system, it
is determined by the formula:
   
 
3
1
10








 
Бi
Т
Г
Р
T
Гi
N
i
Д Т
Т
С
m
Q
(25)
Hot water supply load loop. Total amount of energy
 
н
Q
the load that is diverted to the consumer
with the water flow rate is determined by the following equation:
37
International Journal on Integrated Education
e-ISSN : 2620 3502
p-ISSN : 2615 3785
Volume 3, Issue IX, September 2020 |
   
    э
сут
н
N
i
в
х
Т
Г
Р
Т
Г
н N
Q
Т
Т
С
m
Q 






 



1
3
. 10

(
26)
where:
 сут
н
Q
- daily heat load of hot water supply, kWh / day;
э
N - the number of days of operation of the system during the period of operation, day / year
In addition, at the end time, the total amount of solar heat received by the load from the system and
provided by the use of solar energy is determined.
   
 









N
i
в
х
Б
Р
r
c Т
Т
С
m
Q
1
3
. 10

(27)
3. CONCLUSION
Thus, according to the above formulas, the energy indicators of solar parabola-cylindrical hot water
systems of industrial and municipal enterprises can be determined
REFERENCES
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(1st ed.). Nairobi: University of Nairobi.
Adhiambo, L. (2012). Factors Affecting the Effectiveness of Donner Funded Projects in Akerland.
Journal Of Community Psychology, 6(28), 353-362.
Armitage, J. (2003). The Institutional Origins of Dynamic Capabilities in Multinational
Enterprises, Industrial and Corporate Change.
Batti, R. (2014). Challenges Facing Local NGOs in Resource Mobilization. Humanities and Social
Sciences, 2 (3), 57 - 64.
Bollinger, A. and Smith, R. (2001). Managing organizational knowledge as a strategic asset.
Journal of Knowledge Management, 5(1), pp. 8-18. https://doi.org/10.1108/13673270110384365
Chappel(2005).Art and Wellbeing.Sydney, Austrlia: Australia council of arts.
Cohen, W.M., Nelson, R.R. and Walsh, J.P. (2002). Links and Impacts: The Influence of Public
Research on Industrial R&D. Management Science, 48(1), pp. 1–23.
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Crosby, P. B. (1989) Let’s talk quality. New York: McGraw-Hill.
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https://doi.org/10.1287/opre.39.1.5
Dill, D. and & Vught, F. (2010) National Innovation and the Academic Research Enterprise.
Baltimore, MD: John Hopkins University Press.
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International Journal on Integrated Education
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p-ISSN : 2615 3785
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Etzkowitz, H. (2003). Innovation in Innovation: The Triple Helix of University-Industry-
Government Relations. The Social Science Information, 42(3), pp. 293-337.
https://doi.org/10.1177/05390184030423002
Gimenez-Espin JA, Jiménez-Jiménez D, Martínez-Costa M (2013). Organizational culture for total
quality management. Total Quality Management& Business Excellence;24(5–6):678–692.
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Abbet Publishers Limited
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organization culture and performance”, International Journal of Operation & Production
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Mathematikal model of calclation parabola-cylindirical solar hot water systems of industrial enterprises

  • 1. 33 International Journal on Integrated Education e-ISSN : 2620 3502 p-ISSN : 2615 3785 Volume 3, Issue IX, September 2020 | Mathematikal model of calclation parabola-cylindirical solar hot water systems of industrial enterprises SULAYMONOV HUSANBOY MANNOPOVICH Ferghana Polytechnic Institute. ERGASHEV SIROJIDDIN FAYAZOVICH . Ferghana Polytechnic Institute. MAMADIEVA DILXUMOR TOLIBJONOVNA Ferghana Polytechnic Institute. Abstract The article analyzes a mathematical model for calculating solar parabola cylindrical hot water systems for industrial and municipal enterprises. The formulas for determining heat losses associated with radiant and convective heat exchange, as well as useful heat energy and efficiency of solar parabola- cylindrical systems for obtaining heat for industrial purposes are given. Keywords: Solar radiation, energy, temperature, heat supply, process steam, productivity, battery, hot water, thermal energy, electricity, optical losses, heat losses, hot water supply, energy balance, industry 1. INTRODUCTION Most solar parabola-cylindrical hot water systems for industrial and municipal enterprises operate according to the thermal model shown in Fig.1 and consist of the following main components: parabola-cylindrical collectors, accumulator tank, circulation pumps and hot water supply doubler 1, 2, 4, 5, 6. The system is provided with hot water with a temperature of 60÷100°C. The hot water supply system is made according to a single-circuit scheme, i.e. the heated water in parabola-cylindrical collectors enters the hot water storage tank. Water from the Central water supply network enters the lower part of the battery tank, and hot water for technological processes are taken from the upper part of the tank. The system is protected from freezing by draining water from the collectors. 2. MAIN PART When the water temperature falls below the required operating temperature for the technological process, т г Т the DT doubler is turned on; this will warm up the water coming from the storage tank. The system works as follows. Circulation of water through parabola-cylindrical collectors occurs if the equilibrium temperature  Т the absorbing surface of the heat receiver is higher than the temperature Б Т at the bottom of the battery tank by the amount of Т  due to the temperature difference in the main pipelines of this circuit
  • 2. 34 International Journal on Integrated Education e-ISSN : 2620 3502 p-ISSN : 2615 3785 Volume 3, Issue IX, September 2020 | Т Т Т Б     (1) Hot water is extracted from the upper part of the battery tank by the flow rate r m to places where water is collected. From Fig.2 it can be seen that the consumption r m defined as follows: Т Г r m m  при Т Г Б Т Т  and from the equality   Т Г Р Т Г в х Р r Т Г Б Р r Т С т С m m Т С m         . .  (2) determine     в х Б в х Т Г Т r r Т Т Т Т m т . .    при Т Г Б Т Т  (3) where: Т Г Т , Т r m - water temperature and flow rate determined by the process load schedule; в х Т . - the temperature of the feed water provided from a Central water supply network. In the description of the mathematical model parabola-cylindrical hot Fig. 1 Thermal models of parabola-cylindrical installations for the production of hot water (a), steam (b) and water lifting (C). Fig. 2. Scheme for determining r m
  • 3. 35 International Journal on Integrated Education e-ISSN : 2620 3502 p-ISSN : 2615 3785 Volume 3, Issue IX, September 2020 | the following assumptions were made: neglect the uneven distribution of solar energy flow between collectors; do not take into account heat loss from the surface of connecting pipelines; based on the results of preliminary calculations, neglect the temperature gradient along the perimeter and heat loss by thermal conductivity to the supporting elements of the heat receiver design. These assumptions make it possible to significantly simplify the mathematical model of the system, and consider parabolocylindric collectors as a single collector. To consider the energy balance over time, the estimated period of operation of the system is divided into N equal parts in increments   , for each i  point in time   N i ,... 2 , 1  at the beginning of the step, the thermal balance of each system element is considered. In this case, the main dependencies used for calculating each component of the system at a time i  and the functional relationship between the elements are shown below. Unit parabola-cylindrical collectors. To determine the useful heat пк пол Q , the collector energy balance equation is used for the energy received from the parabolocylindric collectors in the storage tank, expressed in terms of the equilibrium temperature of the absorbing surface of the receiver  Т and temperature Б Т at the bottom of the tank   Б L R пк пол Т Т C U F F Q       1 3 (4) Equilibrium temperature  Т the absorption surface of the receiver is determined by the formula [7] , L зап О О О U С К Е Т Т        (5) where: зап К -coefficient that takes into account dust on the mirror surface of the hub. When calculating the flow density of direct solar radiation, the main methods used are the orientation of collectors rotating around a horizontal North-South or East-West axis. Heat losses associated with partial boiling and evaporation of water are determined by the formula [7]   Б и Р к пк пол пот исп Т Т С т Q Q     . (6) where: и Т - boiling point of water; к т - water consumption in the system circuit. The flow rate of evaporated water is determined by a well-known formula 8: r Q т u и /  . (7) Taking into account (7) the water temperature at the outlet of the heat receiver is determined by the formula:   Р к пот исп Б вых к С т Q Qппо Т Т    (8) At the end time of the estimated period of operation of the system, the following values are determined that characterize the balance of water heating energy in parabola-cylindrical collectors: 1. The Sum of the incident (direct component) of solar radiation   пад Q on the collector surface perpendicular to the rays:     3 3 1 10          F E Q oi I N пад . (9) 2. Total solar energy   пог Q absorbed in the collector's heat sink:     3 3 1 10           о oi I N пог F E Q . (10)
  • 4. 36 International Journal on Integrated Education e-ISSN : 2620 3502 p-ISSN : 2615 3785 Volume 3, Issue IX, September 2020 | 3. The total optical loss in parabola-cilindrical collectors           пог пад пот опт Q Q Q . (11) 4. Solar energy   н ц пог Q . water absorbed during the operation of the circulation pump through the collector. Value   н ц пог Q . defined using equation (11) when the condition is met Т Т Т Б     . 5. Total amount of heat  Б пк пол Q  coming into the storage tank of parabola-cilindrical collectors         3 1 3 1 10 10                   Б вых к Р u k N i пк полi N i Б пк пол Т Т С m m Q Q (19) 6. Heat losses in the collector heat sink   с т нв пот теп Q . caused by the impossibility of heat removal by the heat carrier of the absorbed solar radiation under the condition Т Т Т Б             н ц пог пог пог тс нв пот теп Q Q Q Q .      (20) 7. The total heat loss   пот теп Q taking into account heat loss  и пот теп Q partially evaporated water at the rate of mu          3 . . 1 10           с т i нв пот теп Б u Р ui N i пот теп Q Т Т С m Q (21) 8. Heat losses in the collector during operation of the pump:             пот теп Б пк пол н ц пог н ц пот теп Q Q Q Q . . (22) The tank is a heat accumulator. To simplify the mathematical model of the heat storage tank, we write down the heat balance equation without taking into account stratification and heat loss from the tank surface 7, 8, 9.:        Б в х u r Б вых к Р u k Б Р Б Т T m т Т Т С m m d dT С F М         . 3  (23) where: Б М - mass of water in the accumulator tank per 1 m2 of the aperture area of the parabola- cylindrical collector, kg/m2 Integrating equation (23) according to the Euler model, we determine the temperatures 1  Бi Т water at the end of the time step:         Бi в х ui ri Бi ki u k Б i Б Бi Т T m m T T m m F M T T           . 3 . 1  (24) Backup hot water supply. Total amount of energy   Д Q the water consumed for preheating by the backup in the load loop to the temperature Т Г Т during the estimated period of operation of the system, it is determined by the formula:       3 1 10           Бi Т Г Р T Гi N i Д Т Т С m Q (25) Hot water supply load loop. Total amount of energy   н Q the load that is diverted to the consumer with the water flow rate is determined by the following equation:
  • 5. 37 International Journal on Integrated Education e-ISSN : 2620 3502 p-ISSN : 2615 3785 Volume 3, Issue IX, September 2020 |         э сут н N i в х Т Г Р Т Г н N Q Т Т С m Q             1 3 . 10  ( 26) where:  сут н Q - daily heat load of hot water supply, kWh / day; э N - the number of days of operation of the system during the period of operation, day / year In addition, at the end time, the total amount of solar heat received by the load from the system and provided by the use of solar energy is determined.                N i в х Б Р r c Т Т С m Q 1 3 . 10  (27) 3. CONCLUSION Thus, according to the above formulas, the energy indicators of solar parabola-cylindrical hot water systems of industrial and municipal enterprises can be determined REFERENCES Ababa, C. (2013). Factors influencing sustainability of rural community water projects in Kenya (1st ed.). Nairobi: University of Nairobi. Adhiambo, L. (2012). Factors Affecting the Effectiveness of Donner Funded Projects in Akerland. Journal Of Community Psychology, 6(28), 353-362. Armitage, J. (2003). The Institutional Origins of Dynamic Capabilities in Multinational Enterprises, Industrial and Corporate Change. Batti, R. (2014). Challenges Facing Local NGOs in Resource Mobilization. Humanities and Social Sciences, 2 (3), 57 - 64. Bollinger, A. and Smith, R. (2001). Managing organizational knowledge as a strategic asset. Journal of Knowledge Management, 5(1), pp. 8-18. https://doi.org/10.1108/13673270110384365 Chappel(2005).Art and Wellbeing.Sydney, Austrlia: Australia council of arts. Cohen, W.M., Nelson, R.R. and Walsh, J.P. (2002). Links and Impacts: The Influence of Public Research on Industrial R&D. Management Science, 48(1), pp. 1–23. Cochran, W. G. (1963). Sampling Techniques, 2nd Ed., New York: John Wiley and Sons, Inc. Crosby, P. B. (1989) Let’s talk quality. New York: McGraw-Hill. Cyert, R.M. (1991). Knowledge and Economic Development. Operations Research, 39(1), pp. 5–8. https://doi.org/10.1287/opre.39.1.5 Dill, D. and & Vught, F. (2010) National Innovation and the Academic Research Enterprise. Baltimore, MD: John Hopkins University Press.
  • 6. 38 International Journal on Integrated Education e-ISSN : 2620 3502 p-ISSN : 2615 3785 Volume 3, Issue IX, September 2020 | Etzkowitz, H. (2003). Innovation in Innovation: The Triple Helix of University-Industry- Government Relations. The Social Science Information, 42(3), pp. 293-337. https://doi.org/10.1177/05390184030423002 Gimenez-Espin JA, Jiménez-Jiménez D, Martínez-Costa M (2013). Organizational culture for total quality management. Total Quality Management& Business Excellence;24(5–6):678–692. Githinji, C. (2013). Factors affecting sustainability of community based projects in Kitui County, Kenya. Nairobi: Kenyatta University. Lee, Y., (2011). University-Industry Collaboration on Technology Transfer: Views from the Ivory Tower. Policy Study Journal, 26, 69-84. Mavoko, M. (2013). Resource mobilization for NGOs in the developing. London: Adonis and Abbet Publishers Limited Muijs, D. (2010). Doing quantitative research in education with SPSS. Sage. multidimensional organization culture and performance”, International Journal of Operation & Production Management, Vol. 31, No. 7, pp. 712-735. Mulwa, F. (2010). Demystifying Participatory Community Development (Revised edition). Nairobi.: Pauline's Publications Africa. Prajogo, D.I. and McDermott, C.M. (2011), “The relationship between Psychometrical, vol.16, no. 3, pp. 297-334. Saunders, M., Lewis, P., & Thornhill, A. (2009) Research Methods for Business Students (5th. ed., pp. 318-359). Harlow: Pearson Education. Scot, S. (2004). Variation in Spinoff Activities Across Institutions. In Academic Entrepreneurship: University Spinoffs and Wealth Creation. Edward Elgar Publishing. Smith, K. M., Machalaba, C. C., Seifman, R., Feferholtz, Y., & Karesh, W. B. (2019). Infectious disease and economics: The case for considering multi-sectoral impacts. One Health, 7, 100080. World Health Organization [WHO] (2020b). Coronavirus disease 2019 (COVID-19) Situation Report – 46. https://www.who.int/docs/default-source/coronaviruse/situationreports/20200306- sitrep-46-covid 19.pdf?sfvrsn=96b04adf_2 Zu, X., Robbins, T. L., & Fredendall, L. D. (2010). Mapping the critical links between organizational culture and TQM/Six Sigma practices. International Journal of Production