Determination of heat losses of a concrete silo for sugar and a fan project

Similar documents
Principles of Food and Bioprocess Engineering (FS 231) Problems on Heat Transfer

TankExampleNov2016. Table of contents. Layout

Examination Heat Transfer

Simplified calculation of sugar juice evaporator and examples of its optimisation

Solar Flat Plate Thermal Collector

1. Nusselt number and Biot number are computed in a similar manner (=hd/k). What are the differences between them? When and why are each of them used?

MECHANISM BEHIND FREE /NATURAL CONVECTION

Circle one: School of Mechanical Engineering Purdue University ME315 Heat and Mass Transfer. Exam #2. April 3, 2014

Principles of Food and Bioprocess Engineering (FS 231) Exam 2 Part A -- Closed Book (50 points)

S.E. (Chemical) (Second Semester) EXAMINATION, 2011 HEAT TRANSFER (2008 PATTERN) Time : Three Hours Maximum Marks : 100

ECE309 INTRODUCTION TO THERMODYNAMICS & HEAT TRANSFER. 3 August 2004

True/False. Circle the correct answer. (1pt each, 7pts total) 3. Radiation doesn t occur in materials that are transparent such as gases.

Tutorial 1. Where Nu=(hl/k); Reynolds number Re=(Vlρ/µ) and Prandtl number Pr=(µCp/k)

Heat Transfer Convection

WTS Table of contents. Layout

Convection Workshop. Academic Resource Center

Empirical Co - Relations approach for solving problems of convection 10:06:43

Name: ME 315: Heat and Mass Transfer Spring 2008 EXAM 2 Tuesday, 18 March :00 to 8:00 PM

DESIGN OF A SHELL AND TUBE HEAT EXCHANGER

1 st Law Analysis of Control Volume (open system) Chapter 6

Examination Heat Transfer

Minhhung Doan, Thanhtrung Dang

8.1 Technically Feasible Design of a Heat Exchanger

Attempt ALL QUESTIONS IN SECTION A and ANY TWO QUESTIONS IN SECTION B Linear graph paper will be provided.

Experiment 1. Measurement of Thermal Conductivity of a Metal (Brass) Bar


ME 331 Homework Assignment #6

Comparison of syrup heating with perforated tubes or plate heat exchangers

Convection Heat Transfer. Introduction

ME 315 Final Examination Solution 8:00-10:00 AM Friday, May 8, 2009 CIRCLE YOUR DIVISION

Autumn 2005 THERMODYNAMICS. Time: 3 Hours

Ben Wolfe 11/3/14. Figure 1: Theoretical diagram showing the each step of heat loss.

SCWR Research in Korea. Yoon Y. Bae KAERI

Department of Mechanical Engineering, VTU, Basveshwar Engineering college, Bagalkot, Karnataka, India

S.E. (Chemical) (Second Semester) EXAMINATION, 2012 HEAT TRANSFER (2008 PATTERN) Time : Three Hours Maximum Marks : 100

SSRG International Journal of Mechanical Engineering ( SSRG IJME ) Volume 2 Issue 5 May 2015

Heat Transfer Predictions for Carbon Dioxide in Boiling Through Fundamental Modelling Implementing a Combination of Nusselt Number Correlations

PHYSICAL MECHANISM OF NATURAL CONVECTION

COVENANT UNIVERSITY NIGERIA TUTORIAL KIT OMEGA SEMESTER PROGRAMME: MECHANICAL ENGINEERING

Level 7 Post Graduate Diploma in Engineering Heat and mass transfer

Convection. forced convection when the flow is caused by external means, such as by a fan, a pump, or atmospheric winds.

University of Rome Tor Vergata

EXPERIMENTAL AND THEORETICAL ANALYSIS OF TRIPLE CONCENTRIC TUBE HEAT EXCHANGER

ELEC9712 High Voltage Systems. 1.2 Heat transfer from electrical equipment

CHME 302 CHEMICAL ENGINEERING LABOATORY-I EXPERIMENT 302-V FREE AND FORCED CONVECTION

Chapter 5. Mass and Energy Analysis of Control Volumes. by Asst. Prof. Dr.Woranee Paengjuntuek and Asst. Prof. Dr.Worarattana Pattaraprakorn

CONCENTRIC EXCHANGER TEST PROBLEMS

Conjugate heat transfer from an electronic module package cooled by air in a rectangular duct

PHYSICAL MECHANISM OF CONVECTION

Coolant. Circuits Chip

SHELL-AND-TUBE TEST PROBLEMS

Lectures on Applied Reactor Technology and Nuclear Power Safety. Lecture No 6

ME 315 Exam 3 8:00-9:00 PM Thursday, April 16, 2009 CIRCLE YOUR DIVISION

CHAPTER 5 CONVECTIVE HEAT TRANSFER COEFFICIENT

If there is convective heat transfer from outer surface to fluid maintained at T W.

HEAT TRANSFER BY CONVECTION. Dr. Şaziye Balku 1

Heat Transfer Coefficient Solver for a Triple Concentric-tube Heat Exchanger in Transition Regime

Phone: , For Educational Use. SOFTbank E-Book Center, Tehran. Fundamentals of Heat Transfer. René Reyes Mazzoco

Dishwasher. Heater. Homework Solutions ME Thermodynamics I Spring HW-1 (25 points)

XHDU Cassette type fan-coils for double/four pipe connections 1,98-14 kw HYDRONIC TERMINALS

Chapter 7: External Forced Convection. Dr Ali Jawarneh Department of Mechanical Engineering Hashemite University

TOPIC 2 [A] STEADY STATE HEAT CONDUCTION

HEAT TRANSFER AND FRICTION FACTOR CHARACTERISTICS OF COMPOUND TURBULATORS IN RECTANGULAR DUCTS OF SOLAR AIR HEATER

Q1 Give answers to all of the following questions (5 marks each):

PLATE TYPE HEAT EXCHANGER. To determine the overall heat transfer coefficient in a plate type heat exchanger at different hot fluid flow rate

Infrared measurements of heat transfer in jet impingement on concave wall applied to anti-icing

Analysis, Design and Fabrication of Forced Convection Apparatus

11. Advanced Radiation

MAE 598 Project #1 Jeremiah Dwight

Steps for design of Furnace/Fired Heater

Application of analogy of momentum and heat transfer at shell and tube condenser

c Dr. Md. Zahurul Haq (BUET) Thermodynamic Processes & Efficiency ME 6101 (2017) 2 / 25 T145 = Q + W cv + i h 2 = h (V2 1 V 2 2)

EXPERIMENTAL AND CFD ANALYSIS OF TURBULENT FLOW HEAT TRANSFER IN TUBULAR HEAT EXCHANGER

EXPERIMENTAL AND CFD ANALYSIS OF TURBULENT FLOW HEAT TRANSFER IN TUBULAR EXCHANGER

Mixing Process of Binary Polymer Particles in Different Type of Mixers

MYcsvtu Notes HEAT TRANSFER BY CONVECTION

Heat Tracing Basics. By: Homi R. Mullan 1

Countercurrent heat exchanger

SEM-2017(03HI MECHANICAL ENGINEERING. Paper II. Please read each of the following instructions carefully before attempting questions.

HEAT TRANSFER 1 INTRODUCTION AND BASIC CONCEPTS 5 2 CONDUCTION

Thermal engineering with QuickField

Chapter 5. Mass and Energy Analysis of Control Volumes

Heat processes. Heat exchange

TUBE BANKS TEST PROBLEMS

Chapter 1: 20, 23, 35, 41, 68, 71, 76, 77, 80, 85, 90, 101, 103 and 104.

Introduction to Heat Transfer

Overall Heat Transfer Coefficient

Introduction to Heat and Mass Transfer. Week 14

The Research of Heat Transfer Area for 55/19 Steam Generator

Exergy Analysis of Solar Air Collector Having W Shaped Artificial Roughness

EFFECT OF BAFFLES GEOMETRY ON HEAT TRANSFER ENHANCEMENT INSIDE CORRUGATED DUCT

Piping Systems and Flow Analysis (Chapter 3)

Axial profiles of heat transfer coefficients in a liquid film evaporator

Analysis of the Cooling Design in Electrical Transformer

PROBLEM 1.3. dt T1 T dx L 0.30 m

Vincent Barraud SOPREMA BASICS OF THERMAL INSULATION

SHRI RAMSWAROOP MEMORIAL COLLEGE OF ENGG. & MANAGEMENT B.Tech. [SEM V (ME-51, 52, 53, 54)] QUIZ TEST-1 (Session: )

Thermo-Hydraulic performance of Internal finned tube Automobile Radiator

2 Navier-Stokes Equations

Transcription:

Determination of heat losses of a concrete silo for sugar and a fan project VLP - Processing lines of food industry - example, 5/2000. Given data Silo diameter Height of a cylindrical part of silo Concrete wall thickness D = 36 m H = 33 m T = 0,32 m There are 225 holes (vertical tubes ) with diameter 00 mm and spacing 500 mm for silo s heat losses compensation in the wall. Tempering air flows upward through tubes (holes), maximal difference between inlet and outlet air temperatures is 4 C (28 C 24 C). The silo is insulated by a 00 mm thick polystyrene boards and sheathed by a mm thick Al plate. 00 0 φ 00 0 500 320 400 φ 00 surrounding air AL insulation concrete concrete sugar temper. air φ 36000 Silo s wall section t WC t WT t AIRφ =26 C sugar 25 /- ( 2) C t WAL t Wi t SUR = -5 Temperatures in the silo s wall Average sugar temperature in the silo is c. 25 C. A minimal temperature of surrounding air for calculation is 5 C (according Czech standards ČSN Heat losses of a concrete silo Print date: 04.03.03

06020 are for Pardubice 2 C, Chrudim 2 C). In a similar silo were in a tempering air system measured out pressure losses from 2500 to 3500 Pa. Considering considerably higher heat conductivity of concrete than for sugar and much higher than for the insulation we can suppose that the wall temperature in the wall axis and in a 50 mm distance are the same and are approximately equal to the tempering air temperature. From the same reason we suppose that the wall temperature is practically the same around the silo s perimeter (there is no effect of tubes (holes) spacing). Another data necessary for calculations: λ CON =,5 W/mK s CON = 0 mm λ IN = 0,036 W/mK ρ IN = 30 kg/m 3 s IN = 00 mm λ AL = 209 W/mK s AL = mm λ SUG = 0,46 W/mK ρ SUG = 770 kg/m 3 (sugar in bulk) Average tempering air temperature is t AIR = 26 C. According ČSN 730548 is a heat transfer coefficient on an outside vertical silo s wall α e = 5 W/m 2 K, according ČSN 730542 is in winter (winds) α e = 23 W/m 2 K. For our calculation we take into account the less advantageous value. The same value we will take for a silo s lid. The values are not important for our calculations, as we will see from following results. Heat transfer coefficient for heat transfer from the tempering air to the concrete wall of tubes is, according the following calculations, estimated to α i 76 W/m 2 K. If we do not know a number of tubes we have to estimate an overall heat transfer coefficient k and set the amount of tempering air and a heat flux q. Than we specify an air velocity and consequently α i and k values. Here is, in brief, state a result of the last iteration (number of tubes and their dimensions are given, amount of the tempering air is specified in the chapter 5.). Specification of the heat transfer coefficient from the tempering air to the tubes wall λ AIR = 0,065 W/mK ν AIR = 5,9*0-6 m 2 /s Pr AIR = 0,7 ρ AIR =,5 kg/m 3 Amount of the tempering air M AIR = 5,6 kg/s V AIR = M AIR /ρ AIR = 5,6 /,5 = 3,6 m 3 /s Tubes clear area f T = n * π * D 2 T / 4 = 225*π*0, 2 /4 =,77 m 2 Air velocity in tubes w AIR = V AIR / f T = 3,6 /,77 = 7,7 m/s Re = w AIR * D T / ν AIR = 7,7 * 0, / 5,9*0-6 = 48428 Nu = 0,023 * Re 0,8 * Pr 0,3 = 0,023 * 48428 0,8 * 0,7 0,3 = 6,2 α i = Nu * λ AIR / D T = 6,2 * 0,065 / 0, = 76 W/m 2 K Heat losses of a concrete silo 2 Print date: 04.03.03

2. Specification of overall heat transfer coefficient k = scon α λ i CON siz λ IZ s AL λ AL α e = 76 0, 0,0 0,00,5 0,036 209 23 = 0,32... W / m 2 K From the equation follows that for a heat loss is determinant the insulation (from 95,6 %). Exact of α e determination has weigh c. 64 times lower (from c.,5 %); as well as is low an effect of the exact tubes location and their spacing on a temperature field in the concrete wall including a determination of a calculated temperature layer (for the of 26 C) location. The effect of α i is only from 0,5 % and the concrete wall only from c. 2,3 %. Effect of Al sheathing is c. 580000 times lower. 3. Specific heat losses (specific heat flux through composite wall) q HL = k * (t AIR t SUR ) = 0,32 * (26 5) = 3, W/m 2 For a wet insulation (mineral wool) were q HL = 20-22 W/m 2. Silo s wall temperature calculations Inside surface of concrete tubes t WT = t AIR q / α i = 26,0-3,/76 = 25,8 C Outside surface of the concrete wall t WC = t WT q * s B / λ B = 25,8-3,*0,/,5 = 24,9 C Outside surface of the AL plate t WAL = t SUR q / α e = -5,0 3,/23 = -4,4 C Outside surface of the insulation t WIN = t WAL q * s AL / λ AL = -4,43,*0,00/209 = -4,4 C The calculations confirm our former presumptions about neglecting of the effect of different temperatures in the silo s wall. Simultaneously they show us the effect of separate layers of the silo s wall on the temperatures and consequently on the heat losses too. 4. Total heat losses of silo As a silo s floor is tempered separately we take into account only the surface of the cylindrical part and the lid (by reason of a simplification of the example we will calculate the lid as a circle, not as a conus). We will calculate with an outside silo s diameter (simplifying for worse conditions). Than the heat transfer area and the total silo s heat losses are A S = π * D S * H π * D S 2 / 4 = π * 36 * 33 π * 36 2 / 4 = 4750 m 2 Q HLT = q HL * A S = 3, * 4750 = 62320 W = 62,3 kw For an exact calculation of the conical silo s lid (height of the conus H = 9 m) is the area 37 m 2, the circle area is 08 m 2. The relative error is 0,5 %. But if we relate the error to the all silo s surface the relative error is only c.2,5 %. It is negligible. The calculation is shown only as an example what simplifications an engineer can do in practice and what are the errors and their effect to a result (for Heat losses of a concrete silo 3 Print date: 04.03.03

example an approximate calculation when we do not know an lid shape). 5. Calculation of heating air system 5.. Estimation of heating air quantity Required temperature difference between inlet and outlet air is 4 C. For the average temperature 26 C we set c AIR =,0 kj/kgk ρ AIR =,5 kg/m 3 Than is (Q AIR = Q HLT ) M AIR = Q AIR / (c AIR * t AIR ) = 62,3 / (,0 * 4) = 5,6 kg/s 5.2. Estimation of fan power requirement From a calculation of the tempering air system (piping, concrete tubes, channel distribution and collection, butterfly valves atc.) we can set that the total pressure losses in the system are c. p L = 3000 Pa p (Pa) Fan characteristic From a fan characteristic curves we set its efficiency η = 0,8 Theoretical fan input is η V(m 3 /s) φ of fan impeller P = M AIR * p L / (ρ AIR * η) = 5,6 * 3000 / (,5 * 0,8) = 50870 W P = 50,9 kw Theoretical electric motor input (power requirement) P M =,2 * P =,2 * 50,9 = 6 kw 5.3. Analysis The value of power requirement is comparable to the heat losses of the all silo. In the option (that was required by a customer) a total energy consumption was c. 62 kw of heat and 5 kw of electric energy. The option is not economical. It is possible to project among others 2 more economical solutions: Heat losses of a concrete silo 4 Print date: 04.03.03

Installation of an electric heating cables. Their input is equal to the heat losses. It is not possible to install the system of heating air incl. the fan with its high requirements for energy and an air heater (using steam or hot water). Permit a higher difference between the inlet and outlet air temperatures; it is the higher difference in the silo s wall temperatures Both variants are used in praxis. We will test the second variant (as it is more complicated). 6. Optimised solution When sugar enters to the silo it has temperature c. 28 C (the highest sugar layer). During the storage its temperature gradually decrease to c. 23-24 C nearly to a silo s bottom. Here is sugar removed for other processing. Original requirement for the sugar temperature in the silo was 25 /- ( - 2) C, it is from 24 to 26 C or from 23 to 27 C. A customer set the stronger limits in the setting. If we take into consideration the wider limit (the temperature of entering sugar is out the limit too) it is possible to admit the higher air temperature difference. In addition it is possible to turn down the air flow. It means from the upward to the downward flow. This change reduces the temperature difference between air and a corresponding sugar layer. The solution makes possible to increase difference between inlet and outlet air temperatures from 4 to 8 C. In the case the inlet air temperature is 32 C and the outlet one is 24 C. Temperatures in the silo are in the next table. Primary solution Proposed solution Air Sugar Air Sugar Top part of silo 24 C 28 C 32 C 28 C Middle part of silo 26 C 25 C 28 C 25 C Lower part of silo 28 C 23 C 24 C 23 C Average difference 3,3 C 2,7 C It follows that average differences between air and sugar temperatures in mentioned parts are for both solutions approximately the same. It follows that the solution does not cause problems with moisture migration in the stored sugar (and consequently its hardening). Analogous to the chapter 5., we carry out a new calculation of the tempering air system. In the middle part of the silo average values are considered. Regarding temperatures in the silo it is possible to lower air temperature (field experience, good temperature regulation). In the case the inlet air temperature would be c. 30 C, in the middle part c. 26 C and outlet air temp. c. 22 C. For the temperatures would be the heat losses the same like for the primary solution (the same average air temperature i.e. silo s surface temperature). From practice reasons we will calculate with higher temperatures (to see that it is necessary to recalculate Heat losses of a concrete silo 5 Print date: 04.03.03

heat losses). 7. Calculation for optimised option 7.. Specific heat losses As the average temperature is higher, the heat losses will be higher too. We suppose that the overall heat transfer coefficient will be the same (see note later). q HL = k * (t AIR t SUR ) = 0,32 * (28 5) = 3,8 W/m 2 7.2. Total heat losses of silo Q HLT = q HL * A S = 3,8 * 4750 = 65550 W = 65,6 kw = Q AIR 7.3. Estimation of heating air quantity In the case is the difference between inlet and outlet air temperatures 8 C. (32 24 C). For a medium air temperature 28 C we set Than is c AIR =,0 kj/kgk ρ AIR =,5 kg/m 3 M AIR = Q AIR / (c AIR * t AIR ) = 65,6 / (,0 * 8) = 8,2 kg/s 7.4. Estimation of fan power requirement The lower circulating heating air quantity the lower pressure loss. Approximately we can say that the loss will reduce in the proportion of squares of air quantities. Than the new pressure loss in the system is p L = 3000 * (8,2 / 5,6) 2 = 829 Pa again An efficiency of a new fan we set analogous to the chapter 5.2. For example η = 0,8 Theoretical fan input is P = M AIR * p L / (ρ AIR * η) = 8,2 * 829 / (,5 * 0,8) = 7389 W P = 7,4 kw Heat losses of a concrete silo 6 Print date: 04.03.03

Theoretical electric motor input (power requirement) is P M =,2 * P =,2 * 7,4 9 kw 7.5. Analysis From the calculations follows that the case makes possible to reduce the fan input from 50,9 kw to 7,4 kw (it is c. 6,8 times). As a price of heat in steam or hot water is much lower than a price of electric energy is the solution more economical than tempering with electric heating cables (even with depreciation of higher fixed assets fan, heat exchanger, regulating system, piping etc.). Approximate economical balance energy costs Cost of heat in steam for air heating Cost of electric energy for fan C HS = 333 Kč/GJ =,20 Kč/kWh C EE = 3,00 Kč/kWh Primary option costs per day N D = (Q HLT * C HS P * C EE ) * 24 = (62,3 *,2 50,9 * 3,00) * 24 = 5459 Kč/d Optimised option costs per day N D = (Q HLT * C HS P * C EE ) * 24 = (65,6 *,2 7,4 * 3,00) * 24 = 24 Kč/d Effects of optimised option N D = N D N D = 5459 24 = 3048 Kč/d Because for the optimised option was the amount of tempering air c. 5,6/8,2 =,9 times lower than for the primary option, it is in the same ratio lower the velocity in tubes. The result is the lower heat transfer coefficient. For,9 times lower velocity is Nusselt number (Nu ~ Re 0,8 ) or α i,9 0,8 =,7 times lower too. Because the overall heat transfer coefficient (and subsequently heat losses too) is affected by α i value only from about 0,5 %, its reducing by c. 4 % causes k value reducing only by c. 0,2 %. As the k value was during the calculations round down it is good for nothing to do a new calculations. Quality of insulation and its sheathing are decisive factors for the total heat losses. When rainwater runs into an insulation its thermal conductivity will be higher and consequently heat losses too (several times). Polystyrene or polyurethane boards are less sensitive than mineral wool. Heat losses of a concrete silo 7 Print date: 04.03.03