4
Chemical Engineering, Heat Engineering and Energy-Saving 87 УДК 621.5:519.6 A. А. Аndrizhievskiy, D. Sc. (Engineering), professor (BSTU); A. G. Trifonov, D. Sc. (Engineering), professor (BSTU). COMPUTER METHODS OF THE ANALYSIS OF THERMO-TECHNICAL CHARACTERISTICS OF HEAT EXCHANGER-COOLER OF THE “PIPE-IN-PIPE” TYPE In the given work we describe the results of the application of modern computational tools to ana- lyze the thermal performance of the heat exchanger of the “pipe in pipe” type in which in the inner tube refrigerant is circulating – a 50% aqueous solution of propylene glycol, and in the ring backlash – the coolant (water). Thus, on the heat exchange surfaces of pipes variable (both in time and length) layers of deposits of organic and inorganic origin. This article discusses only the deposits on the surfaces in contact with the coolant. Introduction. The heat exchangers of the “pipe in pipe” type are widely used in various in- dustries, particularly in food industry as heat ex- changers, coolers for various purposes. This may be explained not only by the relative simplicity of the design of these heat exchangers, but also the possibility of creating a reliable algorithm for the regulation of their regime parameters. However, such algorithms should take into account the dy- namics of a wide range of interconnected both thermal and hydraulic characteristics of the heat transfer surfaces and help reduce energy costs for the maintenance of heat exchangers. Currently, to analyze the heat transfer cha- racteristics of the heat exchangers computer me- thods are increasingly used. An example of this approach is the work [1], which describes the application of Simulink package according with the system MATLAB applied to the problems of modeling and optimization of heat-mass transfer processes. Formulation of the research problem. The procedure of constructing computational do- mains and the method of solution of non- stationary multidimensional conservation equa- tions on the basis of formalized templates of software package COMSOL Multiphysics and the finite element method embedded in this package are adopted in this research. The counterflow heat exchanger of the “pipe in pipe” type in which the refrigerant – 50% aqueous solution of propylene glycol is circulating in the inner pipe, and the coolant (water) [2, 3] in the annular gap, was chosen as the research object, based on the formalized templates of software package COM- SOL Multiphysics. The variable (both in time and in length) layers of deposits of organic and inorganic origin may be present on the surfaces of the heat transfer pipes. In this model experiment, the following as- sumptions are accepted: – deposits occur only on the heat exchange sur- faces in the annular gap in contact with the coolant (50% aqueous solution of propylene glycol), they are identical both in thickness and composition; – on the surface of the pipe with the coolant (water) deposit formation does not occur; – thickness of the sediments is considered as a parameter, the time-varying discrete or linearly (quasistationary) from 0 to 5 mm; – nature of deposits is seen in 2 versions: bio- fouling (thermal conductivity – 0.6 W/mK); salt toughness and corrosion products (thermal conduc- tivity – 1.2W/mK). The above assumptions allow us to consider the axisymmetric problem in the setting of pa- rameters of the heat exchanger. Fig. 1 shows an example of the calculated geometric pattern, composed on the assumptions made and the geometric characteristics of the heat exchanger, the outer radius of the outer pipe – 28 mm; the outer radius of the inner pipe – 12.5 mm; thick- ness of the pipe – 3 mm. Deposit thickness – 0, 1, 2, 3 and 4 mm. Results of the research. The computational experiment was carried out in the framework of the formal calculation pattern COMSOL Multiphysics based on the non-stationary conservation equations with the assignment of the corresponding con- stants, correlating factors, closure relations, as well as boundary and initial conditions. This series of computational experiments was conducted with the following parameters: maxi- mum speed of working bodies of the inner pipe and the annular gap is 0.1 m/s; inlet temperature, refrigerant and coolant are respectively 353 and 293 K; output pressure equal to 10,350 Pa. The graphical presentation of research results is illustrated in Fig. 2–5 on a series of computa- tional experiments for the case of discrete time changing the thickness of deposits. The task to determine the maximum flow rate of cooling water from the cooling conditions re- quired for its 4 о C with the predetermined limit val- ues for the pressure drop along the side of the chilled water and sediment values respectively equal to 0.6 MPa and 4 mm was considered at the first stage of the research. These limitations are related to the maximum allowable energy costs for pumping coolant.

A. Аndrizhievskiy A. G. Trifonov COMPUTER METHODS OF THE

  • Upload
    others

  • View
    4

  • Download
    0

Embed Size (px)

Citation preview

Chemical Engineering, Heat Engineering and Energy-Saving 87

УДК 621.5:519.6

A. А. Аndrizhievskiy, D. Sc. (Engineering), professor (BSTU); A. G. Trifonov, D. Sc. (Engineering), professor (BSTU).

COMPUTER METHODS OF THE ANALYSIS OF THERMO-TECHNICAL CHARACTERISTICS OF HEAT EXCHANGER-COOLER OF THE “PIPE-IN-PIPE” TYPE

In the given work we describe the results of the application of modern computational tools to ana-lyze the thermal performance of the heat exchanger of the “pipe in pipe” type in which in the inner tube refrigerant is circulating – a 50% aqueous solution of propylene glycol, and in the ring backlash – the coolant (water). Thus, on the heat exchange surfaces of pipes variable (both in time and length) layers of deposits of organic and inorganic origin. This article discusses only the deposits on the surfaces in contact with the coolant.

Introduction. The heat exchangers of the “pipe in pipe” type are widely used in various in-dustries, particularly in food industry as heat ex-changers, coolers for various purposes. This may be explained not only by the relative simplicity of the design of these heat exchangers, but also the possibility of creating a reliable algorithm for the regulation of their regime parameters. However, such algorithms should take into account the dy-namics of a wide range of interconnected both thermal and hydraulic characteristics of the heat transfer surfaces and help reduce energy costs for the maintenance of heat exchangers.

Currently, to analyze the heat transfer cha-racteristics of the heat exchangers computer me-thods are increasingly used. An example of this approach is the work [1], which describes the application of Simulink package according with the system MATLAB applied to the problems of modeling and optimization of heat-mass transfer processes.

Formulation of the research problem. The procedure of constructing computational do-mains and the method of solution of non-stationary multidimensional conservation equa-tions on the basis of formalized templates of software package COMSOL Multiphysics and the finite element method embedded in this package are adopted in this research. The counterflow heat exchanger of the “pipe in pipe” type in which the refrigerant – 50% aqueous solution of propylene glycol is circulating in the inner pipe, and the coolant (water) [2, 3] in the annular gap, was chosen as the research object, based on the formalized templates of software package COM-SOL Multiphysics. The variable (both in time and in length) layers of deposits of organic and inorganic origin may be present on the surfaces of the heat transfer pipes.

In this model experiment, the following as-sumptions are accepted:

– deposits occur only on the heat exchange sur-faces in the annular gap in contact with the coolant (50% aqueous solution of propylene glycol), they are identical both in thickness and composition;

– on the surface of the pipe with the coolant (water) deposit formation does not occur;

– thickness of the sediments is considered as a parameter, the time-varying discrete or linearly (quasistationary) from 0 to 5 mm;

– nature of deposits is seen in 2 versions: bio-fouling (thermal conductivity – 0.6 W/mK); salt toughness and corrosion products (thermal conduc-tivity – 1.2W/mK).

The above assumptions allow us to consider the axisymmetric problem in the setting of pa-rameters of the heat exchanger. Fig. 1 shows an example of the calculated geometric pattern, composed on the assumptions made and the geometric characteristics of the heat exchanger, the outer radius of the outer pipe – 28 mm; the outer radius of the inner pipe – 12.5 mm; thick-ness of the pipe – 3 mm. Deposit thickness – 0, 1, 2, 3 and 4 mm.

Results of the research. The computational experiment was carried out in the framework of the formal calculation pattern COMSOL Multiphysics based on the non-stationary conservation equations with the assignment of the corresponding con-stants, correlating factors, closure relations, as well as boundary and initial conditions.

This series of computational experiments was conducted with the following parameters: maxi-mum speed of working bodies of the inner pipe and the annular gap is 0.1 m/s; inlet temperature, refrigerant and coolant are respectively 353 and 293 K; output pressure equal to 10,350 Pa.

The graphical presentation of research results is illustrated in Fig. 2–5 on a series of computa-tional experiments for the case of discrete time changing the thickness of deposits.

The task to determine the maximum flow rate of cooling water from the cooling conditions re-quired for its 4оC with the predetermined limit val-ues for the pressure drop along the side of the chilled water and sediment values respectively equal to 0.6 MPa and 4 mm was considered at the first stage of the research. These limitations are related to the maximum allowable energy costs for pumping coolant.

88 ISSN 1683-0377. Proceedings of BSTU. 2014. No. 3. Chemistry and Technology of Inorganic Substances

а b

Fig. 1. The geometric calculation template of the exchanger-cooler: а – diagram of a heat exchanger with deposits;

b – finite element partition of a computational domain

As this computational experiment showed, un-der the above restrictions the limit water flow is ≈0,012 m3/h.

Fig. 2 shows the profiles of the dynamic para-meters of the heat exchanger of the propylene gly-col and the temperature gradient in the cross sec-tion of the heat exchanger for the initial portion and at a predetermined cooling water flow.

As might be expected, the thermal resistance of the heat transfer wall proportionally decreases with a decrease in the deposits values. Respec-tively, the required heat removal is provided at a lower flow of propylene glycol, which in its turn requires a lower pressure drop and capacity of its pumping.

On the other hand, the nature of curve 3 in Fig. 2 shows that the dependence of the thermal resis-tance and thus the thermal efficiency of the heat exchanger on the operation time has an asymptotic nature with access to a quasi-stationary regime. These results lead to a preliminary conclusion about the ineffectiveness of the intensification of

the process of heat transfer outside this area and the need to clean the surface of the heat transfer from the sediments. More detailed and well founded conclusions can be made after the consid-eration of the dynamics and sediment profile and optimization of thermal-hydraulic parameters of the heat exchanger.

Fig. 3 and 4 show the cross sections of the temperatures in different sections of the heat ex-changer. The nature of the given profiles indicates, firstly, the presence of the maximum thermal resis-tance of the heat exchanger in the central part (at the largest deposits) and, secondly, its sharp in-crease in its sediment ≈4 mm.

One of the factors affecting the efficiency of the cooling process in this heat exchanger can be thermo-physical properties of sediments and coo-lant. The character of the influence of these para-meters on the efficiency of the cooling water is illustrated in Fig. 5, which shows the profiles of the temperatures of heat carriers from the coolant and the cooling medium and coolant.

Refrigerant

Coolant

Layers of sediments

Refrigerant

Coolant

Layers of sediments

Refrigerant

1 meter

Layers of sediments

C

F

a

1

alcointhintr

gym

27

27

27

27

27

27

27

d,

Chem

Fig.

oncon

1 –

in t

Alongooleng this pndicrans

Ty-sa

mody

21.81.61.41.2

10.80.60.40.2

0

77.0

76.5

76.0

75.5

75.0

74.5

74.00

, mm

mic

. 2. o

n thensta

pre

Fthe

o

As g thed ltherprocatesfer Thisavinyna

2 8 6 4 2 1 8 6 4 2 0

0

5

0

5

0

5

0 .000

m

al E

Chaon the thiant f

dssur3 –

Fig.heaf de

follhe liqurmafile

es thsur

s reng ami

0

00 0

G, m

Eng

angihe sicknflowdiffere d

– ave

. 3. at exepos

lowlen

uid ial re tenhe irfacesulalg

ic p

0.00

m3/h

inee

ing side nessw (0erendroperag

in

Croxchasits

ws frngthis c

resisnds initice, alt algoritara

3

1

050

h

erin

theof p

s of .012

nce p (Δge ten the

oss sangesize

fromh ofconcstanto iallyandllowthm

ame

2

0.01

ng,

parpropthe 2 m(4°C

)PΔempe he

secter aed:

m Fif thcavnce a liy m

d subws um oters

2

100

Hea

rampylesed

m3/h)C) o; 2 –peraeat tr

tionat a h1, 2

ig. he

ve inof

neamorebseus tf ths of

δ, m

0.0

at E

meterene dime) anon t– voaturerans

ns ofheig2, 3,

5, thea

n nathe

ar pe ef

equeto ohe rf the

mm

0150

Engi

rs oglyent

nd a the wolume grsfer

f theght o, 4 –

the at eature hrofifficentlofferegue he

3 m

0 0.0

inee

f thycol (δ),con

watemetrradir wa

e teof 0– 0,

temexchre. Wheat file, cienly –er thulateat

0200

erin

he hedep

, whnstaner sric fent

all

mpe0.5 m1, 2

mpehanWit

trawh

nt us– its he tionexc

1

4

0 0.

ng a

eat pendhile nt t

side:flow(∇

eratm in2, 4

eratungerth thansfhichse oscaoptn ofchan

.025

and

excdingensemp:

w ra)T

turen thmm

urer frhe ifer h in of tarcitimaf thnge

,T∇

5

50 0

Ene

hang surinpera

ate (

e ca

m

proomincrsurits

the ity.al ehe ter.

К/м

35

30

25

20

15

10

50

05

0.030

ergy

nger

ng atur

G);

ase

ofilm th

reasrfacturhea

enerther

м

50

00

50

00

50

00

0

1234

00

y-Sa

r

e

lehes-cernat

r-r-

1 2 3 4

avin

1

ng

(vaexc

o

F

1, 1(

1.glycoe

cont

3,0

278

277

276

275

2740

2

27

2

27

2

27

2

27

2

27

2

Fariatchanof d

se

Fig.

′ – b(coe2 W

ycoleffic

ofnduthe v3′ –

0.56

00

274

275

276

277

2788

7

6

5

40

0

279

78.5

278

77.5

277

76.5

276

75.5

275

74.5

2740

Fig.tion nge

depoecti

. 5. fro

basieffic

W/(ml – 0cienf prctivvisc– thW/

0.005

0.01

0

. 4. ran

r (vositsions

Proom t

aic vacienm · K0.01

nt ofropyvity cosiherm/(m

0.010

1

1

0.

0.1

Depnge varias (vas at

an

ofilethe and aria

nt ofK),15 (mf sedylencoety o

mal c· K

0.015

1

3

.02

0.2

pen274ationariaa he

nd 0

es ofcoocoo

ant wf thethe mPadim

ne glefficof prcon

K), th

0.020

2

0.

2 0

den4–27n ra

ationeigh.75

f theoledolanwithermvis

a · sment

lycocienropyduche v

0,0

0.0250

2

.03

0.3

nce o78 Kangen ranht ofm (

e ted ment (ch the

mal cscoss); 2– 0

ol –nt ofylen

ctivivisco038

40.03

4

0.4 Len

of teK) oe 0–ngef 0.2(upp

empeediucurve sedcondity 2, 2

0.56 0.0

f sedne gity cositmP

4

4

0.5ngth

empover–0.0e 0–425 mper

eratum (ves 1dimductcoe

2′ – W/

015 mdimglyccoefy of

Pa ·

1

3

5 0h, m

perar the03 m4 mm (lpro

ture(cur1′, 2

mentstivit

efficthe

/(m mP

ment ol –fficif prs

1′

0.6 m

aturee ra

m) onmm) loweofile

e of rves2′, 3s of ty o

cienterma· Ka · s– 0

– 0.0ient ropy

2

2

2

0.7

e prdiusn thfor er p)

heas 1, 23′): f thicof set of al c

K), ts); t0.56 038 of

ylen

2′

2

0.

rofils ofhe th

theprofi

at ca2, 3

cknedimf proond

the vtherm

W/mP

sedne gl

1

3′

1

8 0

les f thehicke crofile)

arrie3)

ess mentopylductviscmal/(m Pa · imelyco

1

0.9

8

e heknesoss

ers

1 mt – lenetivitcositl · Ks);

ent –ol –

00

1

89

at ss

mm

e ty ty

K), –

0

90 ISSN 1683-0377. Proceedings of BSTU. 2014. No. 3. Chemistry and Technology of Inorganic Substances

Conclusion. The models and computer pro-grams for calculating the thermal characteristics of the heat exchanger-cooler of the "pipe in pipe" type with regard to deposits on the heat transfer surfaces in relation to food industry devices based on propylene glycol were developed.

1. 1. The solution of the complete system of equations taking into account the conservation of thermal energy on the heat transfer surface al-lowed excluding the calculation of the heat transfer coefficients from the model. This ap-proach is most appropriate when calculating the heat exchangers with considerably varying thickness of deposits.

2. As a result of the computational experiments the influence of deposits on the thermal perfor-mance of heat exchange equipment in the food in-dustry by using propylene glycol as the coolant was determined.

3. The results obtained can be used to optimize the timing of cleaning equipment at the enterprises exploiting heat exchangers and the development of optimal power saving algorithms to regulate their thermal parameters.

References 1. Андрижиевский А. А. Веремеева О. Н.,

Трифонов А. Г. Использование программного пакета MATLAB для оптимизации теплооб-менника «труба в трубе» // Exponenta.pro. Ма-тематика в приложениях. 2004. № 1 (5).

2. Генель Л. С., Галкин М. Л. Микробиоло-гическая безопасность систем охлаждения и кондиционирования воздуха // Холодильная техника. 2009. № 2. С. 3–7.

3. Галкин М. Л. Биообрастание как фактор снижения эффективности теплообмена. // Хо-лодильная техника. 2011. № 5. С. 2–8.

Received 05.03.2014