—‘w W 'K~erf.m- w.- FEASIBILITY STUDY OF THE UTILIZATION OF THERMAL DISCHARGES FOR THE REARING 0F CATFISH mesis for the Degree of M. S. MICHIGAN STATE UNIVERSITY LARRY PHILLIP WALKER 1975 oo' o -09 nv‘.owfl(-«cm-~flm ; ' ' IIIIIIIIIIIIIIIIIIIIIIIIIIIIIII JIIIIIIIIIIIIIIIIIIIIIIIIIIIIIIII.IIIIIIIIIII L 9 Jussss dig. 0C C) .52.. ' ABSTRACT (gjx FEASIBILITY STUDY OF THE UTILIZATION OF THERMAL DISCHARGES FOR THE REARING OF CATFISH BY Larry Phillip Walker The subject of utilization of waste heat from electric power plants in agriculture has recently received considerable attention. Several research groups are investigating the economical uses of thermal dis- charge under a variety of conditions. This study is an investigation of the use of thermal discharge for the production of catfish under Michigan conditions. This study explores the economic and environ- mental incentives for using thermal discharge for the rearing of catfish. It examines some of the constraints in the construction of a biological System which is dependent on the operation of a traditional industrial system. A computer model for catfish growth is developed. In addition, a turbulent mixed pond is modeled to pre- dict ambient temperature of the catfish environment in Larry Phillip Walker response to Michigan meteorological conditions. The two models are used to simulate the growth of catfish over one growing season. Approved . - C / — Major Professor 2: é_7§" Approved 15: {2 ma Department Chairman FEASIBILITY STUDY OF THE UTILIZATION OF THERMAL DISCHARGES FOR THE REARING OF CATFISH BY Larry Phillip Walker A THESIS Submitted to Michigan State University in partial fulfillment of the requirements for the degree of MASTER OF SCIENCE Department of Agricultural Engineering 1975 To Joe and Christina Fowlkes and Empherus Jeffery ii ACKNOWLEDGMENTS Every man must seek out his own predilection in life. In his never-ending search he will cross the path of many individuals whose encouragement and guidance shall enhance his perception of what lies ahead. In my journey I was fortunate to meet Dr. F. W. Bakker-Arkema. His wisdom, encouragement and friendship has helped me overcome some of the obstacles on this leg of the journey. I would also like to thank the faculty and staff of the Agricultural Engineering Department and countless others who have contributed to my personal and intellectual growth. Last, but not least, I would like to thank Consumer Power Company of Michigan and Detroit Edison for their financial support. iii LIST LIST LIST I. II. III. IV. V. VI. TABLE OF CONTENTS OF TABLES . . . . . . . . OF FIGURES . . . . . . . . OF SYMBOLS . . . . . . . . INTRODUCTION . . . . . . . FEASIBILITY EVALUATION . . . A. Historical Development . . B. Incentives . . . . . . C. System Constraints . . . D. Growth . . . . . . . E. Calculating Water Temperature MATHEMATICAL MODELS . . . . A. Growth Model . . . . . B. Pond Model . . . . . . RESULTS AND DISCUSSION . . . SUMMARY AND CONCLUSIONS . . . RECOMMENDATIONS . . . . . . REFERENCES . . . . . . . . . APPENDIX C O O C O O O O O 9 iv Page vi viii b NH OSI-‘mxlb 28 37 50 58 59 60 64 LIST OF TABLES Table Page 1. Estimated acreage devoted to catfish farming and value of production . . . . 5 2. Instantaneous relative growth rates and tests for differences (Tyler, 1972) . . 20 3. Details of weight gain, food consumption, and food conversion efficiency at . 100 days and 240 days (Tyler, 1972) . . 21 4. Water quality data during the 13-to-16 week period of catfish production (Andrews, 1971) . . . . . . . . . . . . 25 5. Meteorological condition, equilibrium temperature, thermal exchange coef- ficient, and heat input needed to maintain the pond at the specified temperature . . . . . . . . . . 51 LIST OF FIGURES Figure Page 1. Plot of catfish production from 1960 to 1975 in units of a million pounds . . . 6 2. Curves of average lengths of 40-day-old guppies in l/4 strength sea water at various temperatures (weatherley, 1972) . . . . . . . . . . . . 13 3. Gross efficiency of food conversion in relation to temperature and ration, drawn as isoPIeths overlying the growth curves (Brett, 1969) . . . . . 14 4. The relationship between environmental temperature and average percentage gain in 12 weeks of channel catfish finger- 1ings fed at three feeding rates (Andrews, 1972) . . . . . . . . . 16 5. The relationship between environmental temperature and food conversion ratio (9 feed/ 9 gain) for channel catfish fed at three feeding rates (Andrews, 1972) . . . . . . . . . . . . l7 6. Combined effects of temperature and photo- period on food conversion efficiency of channel catfish (Kilambi, 1971) . . . 19 7. The relations between stocking rates and average weight per fish for each water turnover rate (Andrews, 1971) . . . . 22 8. The relations between stocking rates and average biomass (grams per cubic foot) for three water exchange rates (Andrews, 1971) . . . . . . . . . 23 9. Relations between stocking rates and food conversion ratios (grams of feed per gram of gain) for three water turnover rates (Andrews, 1971) . . . . . . . 24 vi Figure Page 10. Catfish growth causal loop diagram . . . 31 11. Catfish growth block diagram . . . . . 32 12. Plot of growth with a growth rate that decreases exponentially . . . . . . 33 13. Flow chart of subroutine design to solve a system of 3 equations and 3 unknowns . . . . . . . . . . . 49 14. Graph of air temperature and deWpoint temperature over a 12 month period . . . 52 15. Plot of the thermal exchange coefficient over a 12 month period . . . . . . . 53 16. Heat input from power plant needed to maintain the fish pond at the optimal temperature for growth . . . . . . . 55 17. Growth of catfish at 4 percent feeding rate . . . . . . . . . . . . . 56 18. Growth of catfish at 6 percent feeding rate . . . . . . . . . . . . . 57 vii Har br 81' I'd t" 73 III Cl: 06 I-3 *3 LIST OF SYMBOLS absolute temperature, °R constant in Bowen ratio, in.-Hg-°F-l atmOSpheric vapor pressure, in. Hg saturation vapor pressure of water at the temperatures of the water surface, in. H9 a general function of wind velocity and surface phenomenon rate0 [w [—11] — K (a constant) (3) Observation and empirical data indicate that K is not a constant but decreases exponentially with age. Temperature strongly influences the growth rate of fish (Figures 2 and 3). The growth rate as a lENGTH (mm) I3 —I N d d 5 13 SEA WATER 1 ‘ 1 1 L 4 J 20 22 21 2o 28 30 32 tween/nuns PC) Figure 2. Curves of average lengths of 40- day-old guppies in 1/4 strength sea water at various temperatures. (Weatherley,1972) SPECIFIC GROWTH RATE - ‘l. WEIGHT IOoy l4 1 6.053 CONVEISION . ('I'C'CNCY-‘ . ............. ~ §-."~'-6-- . I. , ' “ 2‘ .0" cu: / ‘\ "15.-1:11» LETML TEMPERATURE o- .0 .0 .- a o -uo' t o -' ...--.'° I . e --n m" TEMPERATURE - C Figure 3. Gross efficiency of food conversion in relation to temperature and ration, drawn as isopleths overlying the growth curves (Brett et al., 1969). 15 function of temperature follows a parabolic-shape curve, which rises to an optimal temperature'and then begins to fall off. In Figure 3, each of the curves represents growth rate as a function of temperature at a different feeding rate. As mentioned earlier, the growth rate decreases with time resulting in a cor- responding flattening of the growth rate curves and approaching the minimum growth rate for aged fish (Brett et al., 1969). Several studies have been conducted on growth, digestion, and metabolism in channel catfish, but few quantitative data are available on the interaction between feeding rates, temperature, growth, food conversion and body composition (Andrews and Stickney, 1972). An examination of Figure 4 indicates that optimal growth of channel catfish occurs in the interval of 26-34°C. The maximum growth is achieved at a temperature of 30°C and a feeding rate of six percent. In Figure 5, the food conversion ratio is plotted against temperature. Again, the optimum ratio is obtained in the interval between 22 and 30°C. Swift (1964) and Brett et a1. (1969) observed similar growth response to temperature for the Windermen char and sockeye salmon. Kilambi et a1. (1971) investigated the influence of temperature and photOperiod on growth, food consumption, and conversion efficiency. It was observed that the 16 L FEEDING RATES 800 ‘ A 6 percent 0 4 percent -h . 2 percent 600 .. 2: H 3 .. E2 a: L) E3 .- n. 400 SI 13 4 200 " II 0 .., l 1 l J l r I U I I 18 22 26 30 34 TEMPERATURE (°C) Figure 4. - The relationship between environmental temperature and average percentage gain in 12 weeks of channel catfish fingerlinga fed at three feeding rates. Each point represents average values from duplicate aquaria each containing twenty fish. (Andrews, 1972) FOOD CONVERSION RATIO 12 10 17 FEEDING RATES .I_ ; 6 percent . 4 percent 0 2 percent L I I. c: n I l 18 22 26 30 34 TEMPERATURE Figure 5. The relationship between environmental temper- ature and food conversion ratio (9 feed/ 9 gain) for channel catfish fed at three feeding rates. Each point represents combined data from duplicate aquaria each containing twenty fish (Andrews et al., 1972). 18 combined effects of temperature and photoperiod on food consumption of channel catfish varied with time (Figure 6) . Tyler and Kilambi (1972) determined the instanta- neous relative growth rates of catfish (Table 2, page 20) and expressed them as regression coefficients of equation (1). In the first year Of the study, the fish under condi- tions 25°C—total darkness and 30°C-16 hour photoperiod had significantly larger growth rates in comparison to the other test groups. In the second year, the fish under 25°C-total darkness condition again showed the greatest growth followed by those under 30°C-8 hour conditions. The growth rates of catfish in the rest of the experi- ments were not significantly different. Andrews et a1. (1971) carried out a series of experiments on stocking rate and its influence on average weight per catfish (Figure 7, page 22), average biomass (Figure 8, page 23), and food conversion (Figure 9, page 24). It was found that an increased water exchange could offset the effect of an increased stocking rate. The high biomass and excellent survival rates show that channel catfish is well suited for high density culture. One problem of high population densities and temperatures is the growth of parasites and spread of diseases. The Tennessee Valley Authority (TVA, 1973) has provided a set of guidelines for disease control: ESTIMATED FOOD CONVERSION EFFICIENCY thONb O) 19 28C 32c 26C 280 -....._-,.,,_..,:._---_--__,. 32c "' ' 26c _-a .............. 32C """‘ 250 326 260 o ". -O '0 ’0 ’O u . - fl 9 “ O C .' 0" 0 I20 DAYS 90 DAYS 60 DAYS 30 DAYS IO HOURS I4 HOURS LIGHT Figure 6. Combined effects of temperature and photo- period on food conversion efficiency of channel cat- fish. 20 TABLE 2.--Instantaneous relative growth rates and tests for differences (Tyler, 1972). Instantaneous Relative Experimental Condition Growth Rate Year 1 25C-Tota1 darkness 0.08381 * 30C-16 hr. 0.06684 25C-l6 hr. 0.03445 20C-Total darkness 0.03418 30C-8 hr. 0.03949 20C-l6 hr. 0.01716 Year 2 25C-Tota1 darkness 0.02698 30C-8 hr. 0.01558 30C-Tota1 darkness 0.00724 25C—(1/2) 8 hr. 0.00640 30C-Total darkness 0.00576 25C-(1/2) 8 hr. 0.00528 25C-8 hr. 0.00495 25C-16 hr. 0.00327 25C-8 hr. 0.00143 20C-8 hr. 0.00123 20C-Tota1 darkness 0.00111 20C-16 hr. 0.00038 30C-16 hr. 0.00025 20C-8 hr. -0.00113 *The values underscored by the same line are not significatnly different. 21 00 00 HH00. 00.0 0.0 00.0 00.0 00.0 0 AN\H0100N 00 00 0000. 00.0 H.0H 00.H «0.00 00.0 01000 00 00 H000. 00.0 0.00 00.0 00.HH 00.0 .0.BIU0N 00 00 00H0. 00.0 0.H 00.0 00.0 00.0 .Q.BIUON 00 00 0000. 00.0 «.0 00.0 00.0 00.0 0H1000 00 00 maro. 00.0 0.0 00.0 00.0 00.0 .0.91000 00 00 H000. 00.0 0.0 00.0 0H.0 00.0 0H100~ 00 00 0000. 00.0 0.0 00.0 0H.0 00.0 01000 00 00 0000. 00.0 0.0 00.0 00.0 00.0 0aloom 00 00 0000. 00.0 H.0 H0.0 00.0 00.0 01000 0 ~00» NH 00 h0ha. 000a. 00.00 00.0H 0.00 00.0 00.N 00.0H 00.0 00.0 .0.9100~ mm 00 «N00. H000. NH.H0 00.0H 0.00 00.0 H0.0 00.0 00.0 00.0 .0.BIUON mm 00 0000. N000. 00.00 0H.0H 0.00 00.0 0~.H 00.0 00.0 0H.0 01000 mm 00 000a. 00HH. 00.50 00.0H 0.00 00.0 00.0 00.0H 00.0 00.0 0H1000 on 00 0000. 0000. 00.00 00.0H 0.00 «0.0 N0.H 00.0 00.0 00.0 0H100N 0H 00 05H0. N000. 00.00 00.0H 0.HH 00.H H0.0 00.0 00.0 00.0 0H100~ H Mme» Hmswm HaauflcH mwmn 0000 0000 mhma mama mwmn mama when 0000 00m 00H 000 00a 00H 000 00a 000 00a A00 .uz sowuwcsou pm 1335 Hmucmfiuwmxm game some 5 Ba swam sea 58 a £083 5 fine um £3.03 swam mo Hmnasz cwasmcou 0000 .ANNOH .HOEOHHM 0:0 Hmamav m>00 000 can mwmv 00H um mocmHOmem coflmuw>soo 000% 0:0 .cowumfismcoo UOOH .cflmm “£0003 mo maflmumall.0 Manda AVERAGE WEIGHT/ FISH (g) 400 300 200 100 22 HOURS / EXCHANGE -.r:-:.:- :._.3 ‘2‘ 1 2 \\\\\\‘ \\\\\\\\\\\\\ STOCKING RATE (FISH/CUBIC FOOT) Figure 7. - The relations between stocking rates and average weight per fish for each water turnover rate. Each bar re- presents the average of two replicate groups. Ckndrews et al., 1971) (S/Cubic foot) AVERAGE BIOMASS 1600 1200 800 400 23 HOURS/EXCHANGE . W 2 4 6 STOCKING RATE (FISH/CUBIC FOOT) Figure 8. The relations between stocking rates and average biomass (grams per cubic fOot) for three water exchange rates. Each bar represents the average values for two groups (Andrews et al., 1971). FOOD CONVERSION 3.0 2.5 2.0 24 WATER TURNOVER A 2.5 hours/Iurnovor . 8 hours/Iurnovor .I 0 I2 hours/turnover “——l A :- -I W'- 2 4 6 FISH / CUBIC FOOT Figure 9. Relations between stocking rates and food conversion ratios (grams of feed per gram gain) for three water turnover ratios. Each point represents the average of two replicate groups (Andrews et al., 1971). 25 .x0000 050800 :000xo u 000« 0.0 0 0.5 0.0 5.0 0.0 0.000 0.0 0 0.5 0.0 5.0 0.0 0.000 0.0 0 0.0 0.0 0.5 0.0 5.00 0.5 000 0.5 0.0 0.0 0 0.000 0.0 000 0.5 5.0 0.0 0 5.00 0.0 00 0.5 0.0 0.5 0 0.00 0.0 500 0.5 0.0 0.0 00 0.00 0.5 00 0.5 0.0 0.0 00 5.00 0.0 00 5.5 0.0 0.5 00 0.00 A5000 00>00 A0\0fiv A8000 0O>00 A5000 0O>00 A00>00050\mn5onv A000 O00x000 000000 h.000 000 0000EE¢ 0000xo 0509 0000£Oxm mm0EO0m 00000>¢ 00000>< 000HO>¢ 00000>¢ 0000300000 00000>¢ .x0nm0 ..00 pm mzmanmv 0000050000 0000000 00 000000 0003 00:00:00 000 000050 0000 0000050 0000311.0 00005 26 l. The major responsibility for disease prevention and control will fall on the facility operator. 2. A disease specialist should be available in case a problem arises when the facility operator needs assistance in handling. 3. A prestocking check of external para- sites at the site of the fingerling vendor should be conducted. 4. The facility operator must keep a day- to-day watch on the general condition of the fish. E. Calculating Water Temperature The literature on the response of water pond temperatures to meteorological and hydrodynamic influ- ences is extensive. Several models have been examined (Edinger et al., 1968; Linstrom and Boersma, 1973; Ding— man, 1972; Goodman and Tucker, 1970) to determine which one would be most apprOpriate for the present study to predict the temperature in a body of water. The various meteorological and hydrodynamic factors have to be exam- ined to determine which factors should be considered and which can be dropped, thereby simplifying substantially the complexity of the model. Hydrodynamic factors entering into the model can be quite complex, requiring specification of inlet and outlet geometry, water condition, geometry of the pond, and wind direction. In addition, the conserva- tion of mass and energy equations and the equation of 27 motion have to be solved in order to determine pre- cisely how the warm water travels through the pond, how it mixes and how much it is cooled in the process (Littleton, 1970). The flow in the pond can be assumed to be either turbulently mixed or slug flow without turbulent mixing. Slug flow is strongly influenced by the hydrodynamic behavior of the pond. Because the surface temperature is higher for the slug flow the cooling capacity is greater. This is due to the fact that evaporation, conduction and back radiation are greater at higher temperatures. In a turbulently mixed pond, the tempera- ture of the water is assumed to be approximately con- stant in a horizontal plane as a result of horizontal flow and mixing. II I . MATHEMATICAL MODELS A. Growth Model In the feasiability evaluation it was stated that the growth of catfish is not constant, but decreases exponentially with time. Exponential growth damped at an exponentially decreasing rate is charac- terized by a set of differential equations (Laird et al., 1965): 33.9 = —ow (4) aw(t) _ —3:E— - 3W(t) (5) where a is a constant and y is the proportional rate of growth (a function of t). The initial conditions are W(t) = W and Y = A at t = 0. The solutions of the differential equation become: “Y t I 3% = I -03t (6) A 0 28 29 ln [%} = —0t (7) Y = A Exp I-at] (8) agét) = yW(t) = W(t) A Exp [-at] (9) and W(t) t I 33%;; = I A Exp [-at]3t (10) W0 0 1 W(t) _ A t n W — - 5 Exp [-at] (11) 0 0 W(t) = W0 Exp [2’ I1 - Exp (-ont) I] (12) The growth rate can be derived by substituting equation (12) into equation (9): aw t A Bé ) = W0 A Exp {-at] Exp [5 Il ' EXP (”at)I] W0 A Exp [Ak] (l3) Explat + g-Exp (-at)] Equations (12) and (13) are in agreement with Medawar's (1945) laws of growth discussed in the section on feasibility evaluation. However, the effects of temperature T and population density P are not incor- porated into the model. As stated earlier, growth is 30 strongly influenced by temperature. Also, the effect of pOpulation density cannot be neglected. Figure 10 is a causal loop diagram of the variables considered to be significant for adequately modeling the growth of fish. Figure 11 is a block diagram of catfish growth, with the arrows representing the exogenous variable, temperature, the endogenous variable, pOpulation density and the desired output of growth rate K and growth W. Figures 10 and 11 are based on the experi- mental results of Andrews et a1. (1971), Kilambi et a1. (1971) and Tyler and Kilambi (1972). From the above results it can be concluded that the proportional rate of growth y is dependent on time t, population density P and temperature T: Y = Y(t. T. P) (14) The most practical approach to this problem would be to employ a nonlinear least-squares program using eqn (12) and fitting growth data at various times, pOpulation densities and temperature to this equation. Unfortu- nately, the necessary experimental data is not available. Therefore, the above technique cannot be employed, Fig- ure 12 is a graphical representation of equation (11). Another approach to the problem would be to assume that equation (4) represents the change of the 31 \ E... o“ ouamfim 52020 83 .328 5380 5:00 0.30 15500 ”mafia 0.: 0200 20.2.5000 32 A[ 5205 n a 9E u 2 a” auswfim Panama v.85 5380 5.58 ¢ [Iv so u a v_ Al . u H Al 2:52.58 up 33ch 563.5 33 maamaucuaomnu oomwmuowv umfi mum.“ nuaouw N 5.“: 533m no no: .2 85me we; o M 215M 3:» A 3» 23» <2|d 34 proportional rate of growth Y with time at constant temperature and population density: <11] _ -a — Y (15) at T P Applying the chain rule the following partial differen- tial equation is generated to replace eqn (4): .91. - .31. at (tITlP) '- The main obstacle preventing the utilization of eqn (16) are the terms LY ”LA: and Most fish biologists use a general exponential equation of the form: W(t) = w0 ekt (17) to determine the specific growth k at different tempera- tures. Also, BT/at is difficult to calculate and would require a complicated pond model and growth model for simulation on an hourly basis. This would be costly in computer time and storage. If it is assumed that aT/at 35 is zero because waste heat is being utilized to keep the pond at constant Optimal temperature, then the temperature influence on growth disappears and the remaining term is an incomplete model of growth. The term 8P/3t can be derived from some of the present available mathematical models observing that P is coupled in a feedback loop. However, the term 3Y/3P)t,T is impossible to obtain because of the lack of data. The lack of appropriate data severely hampered the development of a soPhisticated model for catfish growth. It is desirable to have growth rate data over a larger range of temperature to adequately assess the value of waste heat in catfish production. Data on population density would be beneficial in an effort to obtain more accuracy in the simulation of catfish growth. However, this endeavor is hampered by insuffi- cient data. It can also be argued that the effects of increased population can be offset by an increase in the water exchange rate. The dependence of the growth rate on time cannot be adequately explored because of lack of data. For this investigation a constant growth rate will be assumed, since the purpose is to assess the value of increasing the ambient temperature of the rearing pond. The final alternative is to employ a linear approximation of the growth rate at different 36 temperatures. Andrews and Stickney (1972) determined the average percent gain over a 12 week growing period, at five different temperatures: W(t) - W(t - Dt) Wo = percent gain. (18) Equation (18) is divided by the growing period (12 weeks or 84 days) to determine the average percent gain per day, _ Percent gain _ W(t) - W(t - At) k ‘ 84* ' wO At (19) where At = 1 day. Rewriting equation (19), the following expression for growth is derived: W(t) = W(t - At) + W k At (20) O The next step was to approximate percentage gain per day k as a function of temperature using an interpolating polynomial of the form: — n n-l O O . P(X) — an+1x + anX + + aZX + a1 (21) such that P(Xi) = f(Xi) for i = 0, l, 2, ..., n (22) 37 For this investigation, Tn + anTn-l + ~-- + a T + a k(T) = P(T) = a. 2 l n+1 (23) The above polynomial with the desired property is the LaGrange interpolation polynomial. Appendix 2 contains a Fortran prOgram for growth employing the above method. Equation (20) is a rough approximation of growth, yet it makes it possible to assess the impact of waste heat on catfish production. B. Pond Model There is more agreement on the optimum depth of the catfish rearing pond than there is on surface area among catfish producers. The recommended depth in the South is 0.9 to 1.81nand 1.8 to 3.0 m in the North (Bar- dach et al., 1972). Shallow ponds are desirable for cat- fish growth because it poses no problem for maintaining the oxygen requirement. With deep ponds there is the problem of an anaerobic environment at the bottom. When a shallow natural pond (that is, one which does not display a vertical temperature gradient) is subject to a constant climatic condition, the water will approach a steady state value known as the equilibrium temperature, T (Littleton, 1970). The E equilibrium temperature is the temperature that a body 38 of water reaches when the heat input and output to the pond are balanced. In searching the literature, several mathemati- cal models were encountered which predict the response of water temperature to meteorological conditions. Boersma and Rykbost (1973) developed a mathematical model of a system of open water basin which allows beneficial use of heated discharge from the thermal power station. Their model was based on the premise that the heat lossjj; controlled by the rate of heat loss at the air-water interface which varies as a function of windspeed and relative humidity. The main difficulty with this ana- lytical model is finding and implementing a solution to a nonlinear hyperbolic differential equation. Dingman (1972), using a set of equations to describe the heat exchange processes at the surface, produced curves of heat exchange rate versus (Tw - Ta), where Ta is the air temperature. These curves can be approximated by linear functions of wind speed, humidity, cloud covering, etc. The problem with this approach is that it requires vast amounts of data to obtain an accurate linear least—square regression approximation. The same problem is encountered with Sefchovich's (1970) model. Most of these models use an energy balance simi- lar to the one used by Edinger (1968) containing the following terms: :1: ar Hbr Hsr If 39 rate of long-wave atmospheric radiation; rate of conductive heat transfer; rate of evaporative heat transfer; net rate of heat exchange between the air and water surface; rate of absorbed radiation (the total net contribution to the energy of the pond); rate of reflected long-wave atmospheric radiation; rate of long-wave radiation from the water; rate of reflected radiation. the equilibrium temperature can be derived from the heat contributions, then the water surface temperature can be calculated from the following equa- tion (Edinger, 1968): where K(TS - Te) (24) thermal exchange coefficient, surface temperature, equilibrium temperature, and net rate of heat exchange surface (heat loss at the surface). For the purpose of this investigation, it will be assumed that HD is equal to the heat input from the power plant needed to elevate the temperature of the pond for optimal temperature for growth. Edinger (1968) 40 derived the following expression for the equilibrium temperature (Te): 660(AT)2T: + KTe = Hr - €0(AT)4 + K;g:°iA§;3 (clTa+er) (25) where K = thermal exchange coefficients, units Btu-day-l - ft_2 - "F‘-1 e = emissivity of water 0 = Stefan-Boltzman constant, Btu ft-z day-1 "R"4 AT = absolute temperature, -°R C1 = constant in Bowen ratio, -:h1.Hg °F-1 Ta = air temperature, °F Td = dew point temperature, °F Hr = absorbed radiation, Btu - ft.2 - day-l. The thermal exchange coefficient K has the following form (Edinger, 1968): K = 4eo(AT)3 + Lp(cl+s)f(u,¢) (26) where L = heat of vaporization of water, Btu/lb f(U,w) = a general function of wind velocity and surface phenomenon. B = (eS - ea)/(Te - Td) (27) 41 where atmospheric vapor pressure, in. Hg; saturation vapor pressure of water at (‘D II (D II the temperature of the water surface, in. H . 9 Wend and Wend (1973) derived the following expression for the general function of wind velocity and surface phenomenon: .00682 + .00682 - U (28) f(U: T) where U = wind velocity, miles per hour. To simplify equations (27) and (26) the following con- stants are defined: 02 = 6 so (AT)2 _ 4 C3 — 80 (AT) 3 C4 = 4 60 (AT) Placing the above constants into equations (25) and (26) yields c T 2 + KT = H - c + [K‘4EG‘AT’3 (c T +BT ) (29) 2 e e r 3 (C1 + B) 1 a d and K = C4 + Lp(cl + B) (30) The coefficients C1 and B are strongly dependent on the local meteorological condition. Michigan in 42 comparison to other states receives the smallest amount of the net radiation and has higher humidity. Edinger et a1. (1968) were able to approximate B, K, and Te from data they gathered from a previous investigation. In this investigation the lack of data requires an iteration scheme to compute three dependent variables. The problem is to solve a system of three equations [equations (29), (30) and (28)] and three unknowns. Newton's iteration scheme for a system of equations (Henrici, 1964) was employed to determine the equilibrium temperature and the thermal exchange coefficient. The first step in the Newton algorithm is to put equations (27), (29), and (30) in the following form: P(Te. B. K) = o (31) G(Ter BI K) = 0 (32) H(Tel B! K) = 0 (33) Thus, — 2 - P(Te, B, K) - CZTe + KTe Hr + C3 K - C4 (C—l+—B—)— (ClTa + BTd) = 0 (34) G(Te’ B. K) = c4 + Lo = o (54) as Equations (49) and (50) indicate that there is a dis- continuity at Te = Td. This problem can be eliminated by decreasing the increment as the equilibrium tempera- ture approaches the dew point temperature. Newton's method for solving a system of equa- tions is derived from the following equations: P(Te+6, 8+5, K+y) = 0 (55) G(Te+6, 8+6, K+Y) = 0 (56) H(Te+6, 8+8, K+y) = O (57) Using Taylor series expansion, equations (55), (56) and (57) become: P(Te+6, 8+3, K+y) F(Te,B,K) + FT (Te.B,K)6+FB(Te,B,K)e e + FK(Te.B,K)Y = 0 (58) G(Te+5, 8+6, K+Y) G(Te,B,K) + GT (Te,8,K)6-+G (Te,B,K)€ e + GK(Te,B,K)Y = 0 (59) 46 H(Te+6, 8+8, K+Y) = H(Te,B,K) + HT (Te,B,K)6 + HB(Te,B,K)e e + HK(T ,B,K)Y = 0 (60) e or -F(Te,B,K) FT (Te,B,K)5 + FB(Te,B,K)€ + FK(Te.B.K)Y (61) e -G(Te,B,K) = FTe(Te,B,K)6 + FB(Te,B,K)€ + FK(Te,B,K)Y (62) -H(Te.B.K) HT (Te.B.K)6 + HB(Te’B’K)€ + HK(Te,8.K)Y (63) e This yields a system of three simultaneous linear equa- tions with three equations with three unknowns. Applying Cramer's rule the following solutions are generated. -F FB FK -G GB GK 6 = -H HB HK (64) FTe FB FK GTe GB GK HTe HB HK 47 FT -F FK e G -G G Te K HTe -H HK s = (65) F F F Te 8 K G G G Te 8 K H H H Te 8 K F F -F Te GT G -G e HTe H -H Y = (66) F F F Te K GT G GK e H H H Te K or = [-F(GBHK-GKHB) - FB(-GHK+GKH) + FK(-GHB+G8H)] (67) D t... - - [FT ( GHK+HGK) + F(GT HK HT GK) + FK( GT H+GHT )] €= e e e e e D (68) [F (-HG +GH 48 - F (-GT H+GHT ) + FK(-G H +G H )1 ) Y = Te 8 B B e e Te 8 8 Te D (69) where D = F (G H -G H ) - F (G -G H ) + F (G H -G H ) Te 8 K K B 8 Te K Te K Te 8 8 Te (70) The final results are T8 = Te + (71) B = B + e (72) K = K + y (73) Figure 14 is a flow chart of this iteration. The time required for the convergence of the problem is 12 sec. on the MSU CDC 6500. 49 Guess-T v Calculate F,G,H, ETC. Calculate 5: EsY No Conver- Calculate Heat Load STOP Figure 13. Flow chart of subroutine design to solve a system of 3 equations and _3 unknowns. IV. RESULTS AND DISCUSSION The results of the water basin simulation are tabulated in Table 5. The simulation was implemented using average monthly weather conditions for Michigan (Table 5, columns 1 through 3). Columns 4 and 5 con- tain the equilibrium temperature and the thermal exchange coefficients. In the last three columns the heat input from the power plant needed to elevate the pond to the desired temperature TS is tabulated. The Optimal temperature is 86.0°F. It would have been desirable to simulate the response of the pond to heat input on a daily basis. However, this was hampered by insuffi- cient weather information. The three different surfaces were chosen to assess the heat load necessary to main- tain the pond at an optimal temperature for catfish production of 86.0°F. Figure 14 (page 52) is a plot of the air tem- perature and the calculated equilbrium temperature over the lZ-month period. The differences between the two range from 3.2°F in month 1 (January) to 9.6°F in month 7 (July). Figure 15 (page 53) is a plot of the thermal exchange coefficient K over a 12-month period. The values for K range from a minimum of 373.7 to 50 51 m.mmm- o.oasm~ o.ammm~ m.amm v.o~ o.- e.m m.o~ o.omema o.amm- o.~a~m~ H.oov ~.om o.Hm m.m o.mm e.mmmea «.momha m.ms>o~ H.4ov m.a¢ o.av m.o m.om m.HH-H H.0Hema m.o~oaa m.~s¢ o.mm o.~m N.» m.am o.mmooa o.mmsva «.momma m.ohm H.om o.mm e.m m.mo m.aoam m.emm~a n.5mmoa e.mam ~.Hm o.mm m.m m.os ~.ommoa H.mavqa c.4mHmH m.oam H.mm o.mm q.m ~.mo m.mmv~a o.emema m.mn¢ma «.mae n.mw o.o¢ m.n 0.0m h.mm~na m.pwmo~ m.vu~mm m.eae H.5m o.¢m m.m m.v¢ m.h~hma H.maqmm «.moamm >.mnm o.o~ o.e~ o.m «.mm e.om~m~ m.hmmm~ m.moem~ ~.omm s.na o.ma m.m e.- H.momm~ ~.mmoo~ «.mmsmm m.vnm e.ea o.ma m.m ~.- mom.mnume moo.omume mo~.mmuma s so .mmwe wmmmwww” . m. HOW Gm HOW cm HOW cm 0H. “aflom 30a wad”; mama... “Ha .ousuouomfiou powmwoomm onu um wcom onu Gwoucflofi ou cocoon usmcw woo: woo .ucowowm (moon omconoxo Hoauocu .ousuonomfiou Esflnnwawsvo .cowuwosoo HoowmoHouoouozll.m mqmfia TEMPERATURE 0F 75 65 55 45 35 25 15 52 A Air Temperature 0F U Equilbrium Temperature 0F MONTH Figure 14. Graph of air temperature and dewpoint temperature over a 12 month period. 10 11 12 THERMAL EXCHANGE COEFFICIENT - Btu-Day_1-ft-2-0F-1 x 10 6O 55 50 45 40 35 53 I I I I I I I I I I 1 1 2 3 4 5 6 7 8 9 10 11 12 MONTH Figure 15. Plot of the thermal exchange coefficient over a 12 month period. 54 2 1 570.8 Btu-day—l-ft— -°F- . The tabulated values for the thermal exchange coefficients are well within the bounds established by Edinger et a1. (1968) and Dingman (1972). Figure 16 is a graph of the heat input from the power plant needed to maintain the optimal temperature for growth. Table 5 and Figure 16 indicate that the maximum heat input needed to achieve the optimal temperature for the growth of catfish is 26,058 Btu-day-l-ft-2 or 1085 Btu-hr-l-ft-z. For a hundred acre pond this is 9 1 approximately 4.72 x 10 Btu-hr- . A 700 megawatt power plant produces thermal discharges of approxi- 9 Btu-hr-l. mately 4.72 x 10 The temperature generated by the pond model (Appendix 1) was used as input into the catfish growth model (Appendix 2) to assess the impact of waste heat on catfish production. Figures 17 and 18 are plots of the data generated by the linear catfish model (Appendix 2). Though this is a rough approximation of growth it can be seen that the use of waste heat does signifi- cantly enhance the growth of catfish. 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