ERT 209 HEAT AND MASS TRANSFER FOR BIOPROCESS ENGINEERING Heat Exchangers.

43
ERT 209 HEAT AND MASS TRANSFER FOR BIOPROCESS ENGINEERING Heat Exchangers

Transcript of ERT 209 HEAT AND MASS TRANSFER FOR BIOPROCESS ENGINEERING Heat Exchangers.

ERT 209HEAT AND MASS TRANSFER FOR

BIOPROCESS ENGINEERING

Heat Exchangers

Heat transfer equipments:

i) Heat exchangers

ii) Evaporators

iii) Dryers

iv) Agitated vessel

Topic Outline

• Types of heat exchangers

• Log Mean Temperature Different (LMTD)

• Correction Factor of LMTD

• Heat Exchanger Effectiveness

• Fouling Factors

• Design of heat exchanger

HEAT EXCHANGERS

• Types of heat exchangers:

1. Double pipe heat exchanger

2. Shell and tube exchanger

3. Plate-type exchanger

4. Crossflow exchanger

• The function of a heat exchanger is to increase the temperature of a cooler fluid and decrease that of a hotter fluid.

1. Double pipe heat exchanger

• The simplest configuration (Fig 1.1)

• One fluid flow through the inside pipe, and the second fluid flows through the annular space between the outside and the inside pipe.

• The fluid can be in co-current or countercurrent flow.

• Useful for small flow rates and when not more than 100 – 150 ft2 of surface is required.

Fig. 1.1 Double pipe heat exchanger

2. Shell and Tube Exchanger• The most important type of exchanger in use in oil

refineries and larger chemical processes and is suited for higher-pressure applications.

• Useful for larger flow rates as compared to double pipe heat exchanger.

• The simplest configuration: 1-1 counterflow exchanger (one shell pass and one tube pass) – refer to Figure 1.2.

• consists of a shell (a large pressure vessel) with a bundle of tubes inside it.

• One fluid runs through the tubes, and another fluid flows over the tubes (through the shell) to transfer heat between the two fluids.

• The cold fluid enters and flow inside through all the tubes in parallel in one pass

• The hot fluid enters at the other end and flow counterflow across the outside the tubes in the shell side.

• Cross-baffles – increase the shell side heat transfer coefficient

Fig 1.2 Shell and tube heat exchanger (1 shell pass and 1 tube passes (1-1 exchanger))

Fig 1.3 Shell and tube heat exchanger (1 shell pass and 2 tube passes (1-2 exchanger))

• The liquid on the tube side flows in two passes• The shell-side liquid flows in one pass• In the first pass of the tube side, the cold fluid is flowing

counterflow to the hot shell-side fluid• In the second pass of the tube side, the cold fluid flows in parallel

(co-current)

Fig 1.4 Shell and tube heat exchanger (2 shell pass and 4 tube passes (2-4 exchanger))

Fig. 1.5 Shell and tube heat exchanger

Fig. 1.6 Hellical baffle

3. Plate heat exchanger

• Use metal plates to transfer heat between two fluids• Consist of many corrugated stainless steel sheets separated by

polymer gaskets and clamped in a steel frame.• The corrugation induce turbulence for improve heat transfer• The space between plates is equal to the depth of the corrugations

(2 - 5 mm)• The plates are compressed in a rigid frame to create an

arrangement of parallel flow channels with alternating hot and cold fluids.

• Major advantage over a conventional heat exchanger in that the fluids are exposed to a much larger surface area because the fluids spread out over the plates.

Fig. 1.6 Plate heat exchanger

• A common device used to heat or cool a gas such as air • One of the fluids, which is a liquid, flows inside through the tubes,

and the exterior gas flows across the tube bundle by forced or sometimes natural convection.

4. Cross-flow exchanger

Fig. 1.7 Cross-flow heat exchangers: (a) one fluid mixed (gas) and one fluid unmixed; (b) both fluids unmixed.

• The fluid inside the tubes is considered to be unmixed, since it is confined and cannot mix with any other stream. • The gas flow outside the tubes is mixed, since it can move about freely between the tubes, and there will be a tendency for the gas temperature to equalize in the direction normal to the flow.• For the unmixed fluid inside the tubes, there will be a temperature gradient both parallel and normal to the direction of flow.

• A second type of cross-flow heat exchanger shown in Fig. 1.7(b) is typically used in air- conditioning and space-heating applications. •In this type the gas flows across a finned-tube bundle and is unmixed, since it is confined in separate flow channels between the fins as it passes over the tubes. The fluid in the tubes is unmixed.

Log Mean Temperature Difference (LMTD) Correlation Factors•For counter-current flow, LMTD for 1-1 exchanger with one shell pass and one tube pass is given by:

Where:

ΔTlm = log mean temperature difference

ΔT1 = T1 - t1

ΔT2 = T2 – t2

T1 = inlet shell-side fluid temperature

T2 = outlet shell-side fluid temperature

t1 = outlet tube-side temperature

t2 = inlet tube-side temperature

T1

t1

T2

t2

Temperature cross

----------------- Eq. (1)

ΔT1 ΔT2

2

1

21

lnTT

TTTlm

•For co-current flow, LMTD for 1-1 exchanger with one shell pass and one tube pass is given by:

Where:

ΔTlm = log mean temperature difference

ΔT1 = T1 - t1

ΔT2 = T2 - t2

T1 = inlet shell-side fluid temperature

T2 = outlet shell-side fluid temperature

t1 = inlet tube-side temperature

t2 = outlet tube-side temperature

T1

t1

T2

t2

Temperature cross

----------------- Eq. (2)

2

1

21

lnTT

TTTlm

ΔT1 ΔT2

Exercise 1

A reaction mixture having a cpm = 2.85 kJ/kg.K is flowing at a rate of 7260 kg/h and is to be cooled from 377.6 K to 344.3 K. Cooling water at 288.8 K is available and the flow rate is 4536 kg/h. The overall Uo is 653 W/m2.K.

a) For counterflow, calculate the outlet water temperature and the area Ao of the exchanger.

b) Repeat for cocurrent flow

Correction of LMTD in Multipass Exchanger• Multipass exchangers have more tube passes than shell passes.

• The LMTD as given in Eq (1 & 2) does not apply in this case and it is customary to define a correction factor, FT.

• The relationship between LMTD and FT is define as below:

Where is define as the correct mean temperature drop.

• The general equation for heat transfer across surface of an exchanger is:

lmTm TFT

mT

moomii TAUTAUq

---------------- Eq. (3)

----------------- Eq. (4)

• Figure 4.9-4 (Geankoplis, 4th ed.) shows the correction factor to LMTD for:

a) 1-2 and 1-4 exchangers

b) 2-4 exchangers

• Two dimensionless ratios are used as follows:

• Using the nomenclature of Eqs. (5 & 6), the of Eq. (1) can be written as:

cico

hohi

TT

TTZ

cihi

cico

TT

TTY

ciho

cohi

cihocohilm

TT

TT

TTTTT

ln

----------------- Eq. (5 & 6)

---------------- Eq. (7)

Figure 4.9-4(a) Correction factor to LMTD for 1-2 and 1-4 exchangers (Geankoplis, 4th ed.)

Figure 4.9-4(b) Correction factor to LMTD for 2-4 exchangers (Geankoplis, 4th ed.)

Example 1 Temperature Correction Factor for a Heat Exchanger

A 1-2 heat exchanger containing one shell pass and two tube passes heats 2.52 kg/s of water from 21.1 to 54.4 0C by using hot water under pressure entering at 115.6 and leaving at 48.9 0C. The outside surface area of the tubes in the exchanger is Ao = 9.30 m2.

a) Calculate the mean temperature different ΔTm in the exchanger and the overall heat transfer coefficient Uo.b) For the same temperatures but using a 2-4 exchanger, what would be the ΔTm?

Solution:The temperatures are as follows:Thi = 115.6 0C Tho = 48.9 0C Tci = 21.2 0CTco = 54.4 0C

Heat balance on the cold water, assume Cpm of water of 4187 J/kg.K and Tco – Tci = (54.4 – 21.1) 0C = 33.3 0C = 33.3 K

q = mCpm(Tco – Tci) = (2.52)(4187)(54.4 – 21.1) = 348 200 W

The log mean temperature difference using Eq. (1) is

Calculate the Z and Y values using Eq (5 & 6)

KCTlm 3.423.42

1.219.48

4.546.115ln

1.219.484.546.115

00.21.214.54

9.486.115

cico

hohi

TT

TTZ

352.01.216.115

1.214.54

cihi

cico

TT

TTY

From Figure 4.9-4(a), FT = 0.74

Using Eq. (3),

Rearranging Eq. (4) to solve for Uo and substituting the known values, we have

b) for 2-4 exchanger, refer to Fig. 4.9-4(b), FT = 0.94, Then,

Hence, in this case the 2-4 exchanger utilizes more of the available temperature driving force.

KCTFT mTm 3.313.31)3.42(74.0

F).bu/h.ft (211.K W/m1196)3.31)(30.9(

348200 o22

mo

o TA

qU

K 8.39C8.39)3.42(94.0 lmTm TFT

Heat Exchanger Effectiveness – NTU Method•The LMTD is used in equation if the inlet and outlet temperatures of the two fluids are known and can be determined by a heat balance.•The surface area can be determined if U is known. •However, when the temperature of the fluids leaving the exchanger are not known, the tedious trial-and-error procedure is necessary.•To solve these cases, a method called the heat exchanger effectiveness is used which does not involve any of the outlet temperatures.•The Effectiveness – NTU (Number of Transfer Unit) method is a procedure for evaluating the performance of heat exchangers if heat transfer area, A and construction details are known .

lmTUAq

•Heat balance for the cold (C ) and hot (H ) fluids is:

•Calling

, then CH > CC

•Designate CC as Cmin or minimum heat capacity.•If there is an infinite area available for heat transfer, TCo = THi , the effectiveness ε is

•If the hot fluid is the minimum fluid, THo = TCi , and

)(

)(

)(

)(

min

max

CiHi

HoHi

CiHiC

HoHiH

TTC

TTC

TTC

TTC

)(

)(

)(

)(

min

max

CiHi

CiCo

CiHiH

CiCoC

TTC

TTC

TTC

TTC

)()()()( CoCiCpHoHiHp TTmCTTmCq ----------- Eq. (8)

CCp

HHp

CmC

CmC

)(

)(

----------- Eq. (10)

----------- Eq. (9)

• In both equations the denominators are the same and the numerator gives the actual heat transfer:

• Note that Eq. (11) uses only inlet temperatures.

• For the case of a single-pass, counterflow exchanger, combining Eqs (9 & 10):

• We consider first the case when the cold fluid is the minimum fluid. Using the present nomenclature,

)( min CiHi TTCq

----------- Eq. (13)

----------- Eq. (12)

----------- Eq. (11)

)(

)(

)(

)(

minmin CiHi

CiCoC

CiHi

HoHiH

TTC

TTC

TTC

TTC

CoHi

CiHo

CoHiCiHoCiCoC

TT

TT

TTTTUATTCq

ln

•Combining Eq. (8) with the left side of Eq. (12) and solving for THi.

•Subtracting TCo from both sides,

•From Eq. (8) for Cmin = CC and Cmax = CH ,

•This can be rearranged to give the following:

)(11

)(1

CiCoCiCoCoCiCoHi TTTTTTTT

)(1

CiCoCiHi TTTT

----------- Eq. (14)

----------- Eq. (16)

----------- Eq. (15)

----------- Eq. (17)

)(max

minCiCoHiHo TT

C

CTT

)(max

minCiCoCiHiCiHo TT

C

CTTTT

•Substituting Eq. (14) into Eq. (17),

•Finally, substituting Eq. (15) and Eq. (18) into Eq. (13), rearranging, taking the antilog of both sides, and solving for ε,

•We define NTU as the number of transfer unit as follows:

•The same results would have been obtained if CH = Cmin

)(1

max

minCiCoCiCoCiHo TT

C

CTTTT

----------- Eq. (19)

----------- Eq. (18)

----------- Eq. (20)

max

min

minmax

min

max

min

min

1exp1

1exp1

CC

CUA

CC

CC

CUA

UA

NTUminC

•For parallel flow we obtain:

•Figure 4.9-7 (Geankoplis, 4th ed.) shows the heat exchanger effectiveness, ε for

a)counterflow exchanger – using Eq. (19)

b)parallel flow exchanger – using Eq. (21)

max

min

max

min

min

1

1exp1

CC

CC

CUA

----------- Eq. (21)

Figure 4.9-7 Heat exchanger effectiveness, ε:

a)counterflow exchanger; b)parallel flow exchanger (Geankoplis, 4th ed.)

Example 2 Effectiveness of heat exchanger

Water flowing at a rate of 0.667 kg/s enters a countercurrent heat exchanger at 308 K and is heated by an oil stream entering at 383 K at a rate of 2.85 kg/s (cp = 1.89 kJ/kg.K). The overall U = 300 W/m2.K and the area A = 15.0 m2. Calculate the heat transfer rate and the exit water temperature.

SolutionAssuming that the exit water temperature is about 370 K, the cp for water at an average temperature of (308 + 370)/2 = 339 K is 4.192 kJ/kg.K (Appendix A.2).

Then (mcp)H = CH = 2.85(1.89 x 103) = 5387 W/K and (mcp)C = CC = 0.667(4.192 x 103) = 2796 W/K = Cmin.

Since CC is the minimum, Cmin /Cmax = 2796 / 5387 = 0.519.

Using Eq. (20), NTU = UA/Cmin = 300 (15.0)/2796 = 1.607

Using Fig. 4.9-7(a) for a counterflow exchanger, ε = 0.71.

Substituting into Eq. (11)

q = ε Cmin (THi – TCi) = 0.71 (2796)(383 – 308) = 148 900 W

Using Eq. (8), q = 128 900 = 2796 (TCo – 308)

Solving TCo = 361.3 K

Fouling Factors and Typical Overall U Values• After a period of operation, the heat transfer surface for a heat

exchanger may become coated with various deposits present in the flow system, dirt, soot or the surface may become corroded as a result of the interaction between the fluids and the material used for construction of the heat exchanger.

• Biological growth such as algae can occur with cooling water in the biological industries.

• These deposits offer additional resistance to the flow of heat and reduce the overall heat transfer coefficient U.

• To avoid or lessen these fouling problems, chemical inhibitors are often added to minimize corrosion, salt deposition and algae growth.

• It is necessary to oversize an exchanger to allow for the reduction in performance during operation.

•The effect of fouling is allowed for in design by including the resistance of the fouling on the inside and outside of the tube in Eq. (22).

Where:hdi = fouling coefficient for inside of the tube (W/m2.K) hdo = fouling coefficient for outside of the tube (W/m2.K)

•Fouling coefficients or fouling factors must be obtained experimentally by determining the value of U for both clean and dirty conditions in the heat exchanger. The fouling factor, Rf is define as:

doo

i

oo

i

AA

iio

dii

i

hAA

hAA

AkArr

hh

U

lm 11

1----------- Eq. (22)

cleandirtyf UU

R11

----------- Eq. (23)

•Typical Fouling Coefficients is shown in Table 1 and the typical values of overall heat transfer coefficients are given in Table 2.

Table 1 Typical Fouling Coefficients

hd

(W/m2.K)

hd

(btu/h.ft2.0F)

Distilled and seawaterCity water

Muddy waterGases

Vaporizing liquidsVegetable and gas oils

113505680

1990-2840284028401990

20001000

350-500500500350

Table 2 Typical Values of Overall Heat Transfer Coefficient in Shell and Tube Exchanger

U (W/m2.K)

U (btu/h.ft2.0F)

Water to waterWater to brineWater to organic liquidsWater to condensing steamWater to gasolineWater to gas oilWater to vegetable oilGas oil to gas oilSteam to boiling waterWater to air (finned tube)Light organics to light organicsHeavy organics to heavy organics

1140 – 1700570 – 1140570 – 1140

1420 – 2270340 – 570140 – 340110 – 285110 – 285

1420 – 2270110 – 230230 – 42555 - 230

200 – 300100 – 200100 – 200250 – 40060 – 10025 – 6020 – 5020 – 50

250 – 40020 – 4040 – 7510 – 40

Design of a Shell and Tube ExchangersExample 3

Design an exchanger to sub-cool condensate from a methanol condenser from 950C to 400C. Flow rate of methanol 100,000 kg/h. Brackish water will be used as the coolant with a temperature rise from 250C to 400C. The U for Brackish water is 600 W/m2.0C

SolutionHeat capacity of methanol, cp = 2.84 kJ/kg0C

Heat water capacity, cp = 4.2 kJ/kg0C

kW 4340409584.23600

000,100loadHeat

Use one shell pass and two tube passes,

From Figure 4.9-4(a), FT = 0.85

kg/s 9.68)2540(2.4

4340flow water Cooling

C31

2540

4095ln

25404095

lmT

67.32540

4095

cico

hohi

TT

TTZ

21.02595

2540

cihi

cico

TT

TTY

CTFT mTm 26)31(85.0

Given, U = 600 W/m2.0CProvisional area,

Choose 20 mm o.d., 16 mm i.d., 4.83 m long tubes (3/4 inch x 16 ft), cupro-nickel.

Area of one tube

Number of tubes, Nt

As the shell-side fluid is relatively clean, use 1.25 triangular pitch.

(The constants, K1 = 0.249 and n1 = 2.207)

23

m 278)26)(600(

104340

mTU

qA

23 m 303.0)m 83.4)(m1020(2 DLjL

918m 303.0

m 278

tubeone of area

area lprovisiona2

2

Bundle diameter,

Use a split-ring floating head type.

The bundle diametrical clearance = 68 mm

Hence, shell diameter, Ds = 826 + 68 = 894 mm.

mm 826249.0

918 20

207.2/1/1

1

1

n

tob K

NdD