Baffle selection.pdf

February 10, 2019 | Author: maruthigabbita | Category: Heat Exchanger, Heat Transfer, Vacuum Tube, Fluid Dynamics, Nozzle
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Heat Transfer

Selecting Baffles for Shell-and-Tube Heat Excha Exchangers ngers Salem Bouhairie

Heat Transfer Research, Inc.

Baffles play a crucial role in regulating shellside fluid flow and improving heat transfer between shellside and tubeside process fluids. Here’s Here’s how to choose the correct baffle to meet process requirements.

T

he rst step in specifying a shell-and-tube heat exchanger is selecting the right shell, which was discussed in a previous CEP  article  article (1 (1). The next step is determining the most effective bafe arrangement. Shell-and-tube heat exchangers employ bafes to trans port heat heat to to or from from tubesi tubeside de process process uids by directi directing ng the the shellside uid ow. The increased structural support that  bafes  bafes provide provide is is integral integral to to tube stability stability,, as they they minimi minimize ze  both tube tube saggin sagging g due to structu structural ral weight weight and vibrat vibration ion due due to cyclic ow forces. However, bafes improve heat transfer at the expense of increased total pressure drop. Bafes come in a range of shapes and sizes, the most common of which is the segmental bafe. The Tubular Exchanger Manufacturers Association, Inc. (TEMA) provides design guidelines for segmental bafes. Other, non-TEMAtype bafes include helical, disc-and-donut, and grid bafes. This article summarizes the performance characteristics of the different types of bafes and offers guidance on choosing effective bafes for shell-and-tube heat exchanger design.

Segmental baffle configurations Segmental bafes, often referred to simply as TEMA  bafes,  bafes, are circular circular plates plates with one or or more more segments segments removed to allow the shellside uid to ow through an open area, or window. To To prevent bundle ow bypass, sealing strips may be placed in notches along the edges of segmental  bafes.  bafes. Bafes Bafes may may also have holes through through which which steel steel tie-rods can pass to provide increased structural support. TEMA bafes can be single- or multi-segmental, or tube support plates. Tube support plates are used in the no-tubesin-window (NTIW) design to ensure that all bafes support every tube, eliminating tubes with long unsupported spans. Copyright © 2012 American Institute of Chemical Engineers (AIChE)

Figure 1 shows the most common types of TEMA bafes. Bafe spacing, cut, and orientation are key characteristics of TEMA bafe designs. Single-segmental bafes are bafes  are used in many industrial heat exchangers because of their suitability for a wide range of applications. They operate well in single-phase processes, and crossow heat transfer (across the tubes) is greater than the longitudinal heat transfer (through the windows). In addition, they are relatively easy to fabricate, so they are less expensive than other types of bafes. However, single-segmental bafes may not be effective with very viscous uids, where improperly mixed ow,  bypass,  bypass, and and leaka leakage ge strea streams ms reduc reducee the the efcie efciency ncy of heat heat transfer. Furthermore, this conguration generates an undesir-

Single-Segmental Highest Pressure Drop, ΔPS

Double-Segmental ΔPD ≈ 0.33Δ 0.33ΔPS – 0.5Δ 0.5ΔPS

Support Plate

Triple-Segmental 0.25ΔPS – 0.33Δ 0.33ΔPS ΔPT  ≈ 0.25Δ

Baffle

No-Tubes-In-Window Wide Spacing

In exchangers with TEMA baffle types, smaller windows result in higher pressure drops. p Figure 1.

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Center Baffle

Wing Baffles

The window flow areas around the center and wing baffles in a double-segmental baffle arrangement should be roughly equal.

Center Baffle (First Baffle Group)

Support Plates (Second Baffle Group)

Wing Baffles (Third Baffle Group)

p Figure 2.

In exchangers with triple-segmental baffles, larger window areas are responsible for lower total pressure drops. p Figure 3.

ably high pressure drop, especially with high-velocity ows.  Double-segmental bafes split the ow so that it passes around center bafes and between wing bafes (Figure 2). In general, the center and wing bafes overlap by two to four tube rows. The window ow area outside the center bafe should generally equal the window ow area between the wing bafes. Pressure drop is one-third to one-half that in a shell with single-segmental bafes. However, this results in lower crossow heat transfer — 60–90% of the heat transfer with single-segmental bafes at the same spacing and cut and the same total owrate. Triple-segmental bafes have lower longitudinal-ow and crossow velocities (whereas double-segmental bafes have only lower crossow velocities) for a given bafe spacing. Triple-segmental bafes produce roughly one-fourth to one-third the pressure drop of single-segmental bafes in a comparably sized unit, and have heat-transfer rates that are as much as one-half lower (2). Triple-segmental bafes typically consist of three distinct bafe groups that create the equivalent of two double-segmental streams in parallel (Figure 3).  No-tubes-in-window (NTIW) congurations provide sup port for all of the tubes to mitigate tube vibration in the window zone. Tube support plates are placed between widely spaced bafes. Because tubes cannot occupy the window spaces, larger shells are required to accommodate a specied tube count; this can be expensive for units operating at high shellside pressures. The lack of tubes in the window reduces  pressure drop, while added support plates enhance crossow. This results in better conversion of pressure drop to heat transfer than in exchangers with single-segmental bafes. The relative reduction in pressure drop depends on bafe cut, and the relative increase in heat transfer depends on the number of support plates added.

the potential for ow-induced vibration. The bafe spacing should be set such that the free-ow areas through the windows and across the tube bank are roughly equal. TEMA standards specify that the minimum spacing  between segmental bafes should be the larger of one-fth of the shell inside diameter or 51 mm (3). Spacing that is too small will result in higher pressure drop and poor bundle ow penetration — i.e., it increases the axial ow inertia through the outer leakage areas between the bafe and shell. Small bafe spacing also makes it difcult to mechanically clean the outsides of the tubes. Maximum spacing between segmental bafes (with tubes in window) should equal one-half the maximum unsupported span length. To enhance end-zone ow control and distribution, the bafes near the shell inlet and outlet should be located as close as practical to the shell nozzle. The distance between the rst and second bafes should not  be less than the central bafe spacing, as shellside ow tends to accelerate in the end zones. The optimum ratio of bafe spacing to shell inside diameter that results in the highest conversion of pressure drop to heat transfer is generally between 0.3 and 0.6 (4).

Baffle cut

Bafe spacing is the longitudinal distance between bafes. It controls the amount of effective heat transfer derived from the pressure drop within each compartment and affects

Bafe cut is the ratio of the bafe window height to the shell inside diameter. If the bafe cut is too small, the ow will jet through the window area and ow unevenly through the bafe compartment (Figure 4, left). If the bafe cut is too large, the ow will short-cut close to the bafe edge and avoid cross-mixing within the bafe compartment (Figure 4, right). A bafe cut that is either too large or too small can increase the potential for fouling in the shell. In both cases, recirculation zones of poorly mixed ow cause thermal maldistribution that reduces heat transfer. To divert as much heat-carrying ow across the tube bundle as  possible, adjacent bafes should overlap by at least one tube row. This requires a bafe cut that is less than one-half of the shell inside diameter.

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Copyright © 2012 American Institute of Chemical Engineers (AIChE)

Baffle spacing 

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Nozzle Axis

If the baffle cut is too small (left) or too l arge (right), fouling can occur in the shaded areas due to uneven flow distribution. p Figure 4.

Parallel-Cut Baffle

Perpendicular-Cut Baffle

Inclined-Cut Baffle

Baffle orientation is referenced with respect to the nozzle axis, and can be parallel, perpendicular, or inclined. p Figure 6.

12 m/s (39.4 ft/s) d 

Window  hw

Baffle Cut =  hw / d 

p Figure 5.

The optimum baffle cut is 25% of the shell inside diameter.

Optimum bafe cuts are typically 25% of the shell inside diameter (Figure 5). However, for a single-segmental  bafe conguration with low-pressure gas ows, a 40–45%  bafe cut is common to limit pressure drop. For NTIW congurations, a 15% bafe cut is most common. The ratio of the window velocity to crossow velocity should be less than 3:1 for effective ow distribution.

Parallel

Perpendicular

p Figure 7. Although

preferred for certain shellside fluids, parallel-cut single-segmental baffles can cause uneven flow in the inlet and outlet regions.

Baffle orientation The orientation of TEMA bafes is particularly important for horizontal shell-and-tube heat exchangers, especially near the inlet and outlet nozzles. Bafe cuts for segmental bafes may be parallel or perpendicular to the nozzle axis, or inclined, as shown in Figure 6. The best  bafe orientation depends on the bafe and shell type. Single-segmental bafes. For single-phase service, single-segmental bafes with a perpendicular bafe-cut orientation in an E- or J-shell are preferred to improve ow distribution in the inlet and outlet regions. With vertical inlet or outlet nozzles, parallel-cut bafes are preferred if the shellside process uid condenses and needs a means of drainage. Parallel-cut bafes should also be used when the shellside uid has the potential for particulate fouling, and in multipass F-, G-, or H-type shells to facilitate ow distribution. (For an introduction to shell types, see Ref. 1.) However, parallel-cut bafes have the potential for signicant ow and temperature maldistribution in the end zones, which can induce local tube vibration and reduce the effective heat-

Copyright © 2012 American Institute of Chemical Engineers (AIChE)

transfer rate in the inlet and outlet bafe spaces. Figure 7, obtained via computational uid dynamics (CFD) modeling, illustrates this phenomenon.  Double-segmental bafes. To distribute ow effectively in the inlet region with double-segmental bafes, a center  bafe with a parallel-cut orientation is generally selected as the rst bafe. The parallel bafe cut reduces the accumulation of deposits from high-fouling shellside uids. It is good  practice to locate the rst bafe under the nozzle, where high owrates can cause tube vibration. The rst bafe is often shaped like a T to provide intermediate tube support where bundle entrance velocities have high kinetic energy (Figure 8, top). If perpendicular-cut double-segmental bafes are used with single inlet and outlet nozzles, thermally ineffective areas will form in the end zones (Figure 8, middle). Better end-zone distribution can be achieved with two inlet and two outlet nozzles, plus wing bafes in the end zones to maintain ow symmetry upon entry and exit (Figure 8,

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Heat Transfer

to benet from added seal strips to block  bypass, as the strips only increase pressure drop. Helical bafes can be continuous spiral assemblies. However, these are not common Intermediate Vibration Support  because they are difcult (and expensive) to Perpendicular Cut (End View) fabricate. Instead, most helical-bafed heat exchangers use bafes that are inclined at an angle from a transverse plane perpendicular Ineffective Region to the shell axis (Figures 9 and 10). These quadrant bafes (each of which occupies Perpendicular Cut (End View) one-fourth of the shell cross-section) touch each other at crossover points that dene a cross-fraction. The bafe cross-fraction is the ratio of the distance from the center of the shell to the crossover point divided by the shell radius (Figure 10). p Figure 8. Double-segmental baffle configurations should use a T-shaped first plate with a Helical bafes can cross near their parallel-cut orientation. Perpendicular-cut orientation should be used only with double i nlet midpoint (a cross-fraction of 50%), tip-toand outlet nozzles. tip (a cross-fraction of 100%), or at a point  bottom). In effect, the performance of perpendicular-cut within this range. Depending on user and fabricator preferdouble-segmental bafes depends on the number ences, the cross-fraction selected may range from 20% to of nozzles. 100%. Reducing the cross-fraction (increasing the overlap) Triple-segmental bafes. The triple-segmental bafe enhances tube support and protects against vibration, but at set shown in Figure 3 has ve different components and is the expense of increased pressure drop. In general, helicalone of several possible arrangements. Other designs, which are not discussed here, have six pieces or three pieces. The  permutations complicate the determination of bafe orientation, particularly in the inlet and outlet zones. Orientation of triple-segemental bafes has not been studied extensively, and general guidelines have not been developed. T-Baffle (End View)

Parallel Cut (End View)

Non-TEMA baffle types Most non-TEMA-type bafes usually produce lower  pressure drops and have better ow and heat-transfer distri butions. The improvements stem from the bafes generating crossow through swirling, maximizing longitudinal ow, or increasing symmetrical ow and heat-transfer distribution. Helical, disc-and-donut, and grid bafes are the most common non-TEMA-type bafes.

Helical baffles promote swirling, which helps to reduce bypass and stagnant flow. p Figure 9.

 r 

B

Baffle Crossover Points

B

 r co

C

C

Helical baffles

 Ø S

Helical bafes promote swirling ow, which helps to alleviate bypass and stagnant ow areas that can occur with conventional segmental bafes. They are effective for lowto high-viscosity uids, and they are commonly used in oil-renery and refrigeration applications. Heat exchangers with helical bafes may experience less shellside fouling than exchangers with segmental bafes. Helical bafes are subject to bundle-to-shell bypass at very high mass owrates. Unlike segmental bafes, helical bafes do not seem 30

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 A



D

D

(End View)

(Elevation View)

Cross-fraction =  r co /  r   r  = shell radius  r co = radial distance from shell axis to baffle crossover point  Ø S= baffle angle relative to transverse plane through shell

Helical quadrant baffles touch at crossover points, which define the cross-fraction. p Figure 10.

Copyright © 2012 American Institute of Chemical Engineers (AIChE)

Spiral Crossflow

Bypass Flow Outside Tube Bundle Radially Expanding Crossflow around Disc Baffle

Longitudinal Flow within Tube Bundle

Y

Radially Contracting Crossflow through Donut Baffle

 X Z

Disc-and-donut baffles distribute flow in a radially symmetric manner. p Figure 12.

Flow Angle

Z

Z

Baffle Angle

The flow through a helical-baffled exchanger includes spiral crossflow, longitudinal flow, and bypass flow. p Figure 11.

 bafed exchangers have less potential for tube vibration  because the tubes are well supported by the quadrant bafes. Helical bafes come in single- or double-helix congurations. Many industrial applications use 12-deg. to 15-deg. angled bafes. Larger bafe angles result in lower pressure drop and increased longitudinal ow relative to crossow. Some studies have reported that bafe angles of 25 deg. to 40 deg. produce optimal conversion of pressure drop to heat transfer (5). The quadrant bafes induce ow that combines spiral crossow, longitudinal ow, and bypass ow (Figure 11). In reality, this ow is far from an ideal helix — it undergoes fewer revolutions than the number of bafe revolutions through the length of the exchanger. The design of these  bafes requires knowledge of both the bafe angle and the actual ow angle (i.e., the direction of the resulting vector of the three principal ow velocity components (x, y, and z, or axial, radial, and tangential), relative to a plane transverse to the exchanger axis).

Disc-and-donut baffles Disc-and-donut bafes generate radially symmetric ow in both the crossow and longitudinal ow directions — the ow expands around the disc bafe and contracts through the donut bafe (Figure 12). A step change in both pressure drop and temperature occurs between consecutive pairs of disc bafes and donut bafes. The main thermally effective crossow stream can occupy up to 80% of a bafe compartment, minimizing the  bypass ow around the outer tubes (6). The driving forces for bypass and leakage streams in an exchanger with disc-

Copyright © 2012 American Institute of Chemical Engineers (AIChE)

and-donut bafes are smaller than those in exchangers with segmental bafes. Disc-and-donut bafes are often installed in NTIW arrangements. Radial tube layouts are preferred over conventional triangular or square layouts, because the resulting radial ow distribution produces uniform heat transfer throughout the tube bundle cross-section. Disc-and-donut bafes are most effective in shellside vapor environments, and are commonly selected for gas-gas applications where vibration can be a problem.

Grid baffles Grid bafes are metal lattices that generate primarily longitudinal ow. They produce low pressure drops, which results in high heat-transfer-to-pressure-drop ratios and  protects against tube vibration. In addition, shellside ow distribution is uniform, which is particularly important for shellside vaporization because it eliminates vapor pockets that can cause pitting of tubes and bafes (7). The most common generic grid bafe designs are rodtype bafes and strip bafes. Each grid type has a characteristic bafe ow-contraction ratio, which is dened as the free ow area through the bafe divided by the free ow area through the bundle between bafes. This parameter ranges from zero to one, with practical values of about 0.2 for high contraction and 0.7 for low contraction. The grid  bafes act as strainers on the bundle free-ow area, locally contracting and accelerating the heat-carrying ow longitudinally along the tubes. The higher the contraction ( i.e., the lower the contraction ratio), the higher the pressure drop. An exchanger design with a low contraction ratio, therefore, requires more pumping power than one with a high contraction ratio.  Rod-type bafes are used in such applications as overhead condensers, gas coolers and heaters, feed and efuent exchangers, and kettle reboilers. They consist of rods laid out in a grid pattern that provide a supporting structure for the heat exchanger tubes and basic structural rigidity. The

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Heat Transfer

Y  X

Y Z

 X

p Figure 13.

Rod-type baffles support the tubes and provide structural

rigidity. Segmental Baffle

2 Rod-Type Baffles per Baffle Space

Rod-type baffles may be combined with segmental baffles for better tube support. p Figure 14.

longitudinal ow friction effectively generates heat transfer, especially in exchangers with long tubes. Rod-type bafes are made by welding round rods to a supporting ring (Figure 13), which also serves as a seal to prevent leakage ows. The rods are often located after every second tube row, with consecutive bafes assembled at 90-deg. angles. Thus, they are generally limited to square tube layouts. It is possible to corrugate the rods to support a triangular tube layout (known as a triangular-grid bafe). Triangulargrid bafes permit higher tube densities, produce higher turbulence, and generate higher heat transfer. However, mechanical cleaning of the tubes is more difcult due to limited access lanes. Therefore, triangular layouts are appropriate for shellside services that use chemical cleaning. In the bundle shown in Figure 13, four longitudinal tie bars are placed around the supporting ring to hold the  bafes in place and maintain the proper bafe spacing. Rods with as small a diameter as possible are preferred, to  permit a higher tube density and hence higher heat-transfer rate. The bafe contraction ratio for rod-type bafes is about 0.55–0.65 (7). Some industrial applications benet from combining rod-type bafes with segmental bafes. Figure 14 shows two rod-type bafes tted within the space between single-segmental bafes. This bafe combination provides increased tube support for vibration protection, without 32

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Z

Strip baffles have lower baffle contraction ratios and higher pressure drops than rod-type baffles. p Figure 15.

increasing pressure drop signicantly. Strip bafes (Figure 15) are grid bafes formed from at strips that are placed in a crisscross pattern, with a strip after every tube row in both directions. The overall structure is welded to a ring for rigidity and ease of assembly. The strips are notched to lock the tubes in place. Figure 15 shows square-layout strip bafes. Strip  bafes can also accommodate 30-deg. triangular layouts. For a given tube pitch ratio (i.e., the spacing between tubes divided by the tube outside diameter), 30-deg. layouts have the highest critical velocities prior to uidelastic instability, so tube vibration potential is minimized. With a bafe contraction ratio of approximately 0.2–0.25, strip bafes produce higher pressure drops per  bafe than rod-type bafes (7).

Closing thoughts Bafing is the most crucial shellside consideration in shell-and-tube heat exchanger design, because bafes regulate shellside uid ow and improve heat transfer while offering signicant tube support. Although TEMA bafes are easier to fabricate, they usually have higher pressure drops than non-TEMA-type bafes. It is equally important to consider how bafe selection affects other shellside  parameters, such as tube pitch ratio, tube layout pattern, tube size, shell type, and shell diameter. A basic understanding of the various bafe types and their advantages and disadvantages (Table 1) is essential to choosing an effective CEP  bafe conguration. SALEM BOUHAIRIE is a research engineer at Heat Transfer Research, Inc. (HTRI) (Email: [email protected]), where he conducts computational fluid dynamics (CFD) simulations and physical experiments for projects and contracts. He teaches workshops on heat exchanger vibration analysis and conducts webinars on heat exchanger design. Prior to joining HTRI, he worked at Northwest Hydraulic Consultants in Edmonton, Alberta, Canada, where he conducted hydraulic structure modeling investigations and river hydrology assessments. He has delivered presentations on his work in Canada, the U.S., Brazil, Thailand, and Korea, and has published research in the  Journal of Fluid Mechanics and the Journal of Hydro-environment Research. Bouhairie earned his BEng, MEng, and PhD in civil engineering from McGill Univ. in Montreal, Quebec, Canada.

Copyright © 2012 American Institute of Chemical Engineers (AIChE)

Table 1. Each baffle type has advantages and disadvantages that make it suitable for different applications. Baffle Type

Single-Segmental   s   e    fl    f   a    B Double-Segmental   e   p   y    T Triple-Segmental      A    M    E    T No-Tubes-in-Window

Advantages

Disadvantages/Limitations

Highest potential heat-transfer rates

Highest potential pressure drop

Easiest to fabricate

Cannot be used for very viscous fluids

Least expensive Lower pressure drop than with single-segmental baffles

Lower heat-transfer rates than with singlesegmental baffles

Lower pressure drop than with double-segmental baffles

Lower heat-transfer rates than with doublesegmental baffles

 All tubes are supported, eliminating tube vibration

Requires a smaller tube bundle and/or larger shell; a larger shell makes this configuration more expensive

Configuration

Higher conversion of pressure drop to shellside heat transfer than single-segmental baffles

Helical

Less shellside fouling Moderate heat-transfer rates and pressure drops Minimizes or eliminates areas of stagnant flow Minimizes or eliminates tube vibration

Disc-and-Donut   s   e    fl    f   a    B   e   p   y    T      A    M    E    T     n   o    N

Radially symmetric flow distribution

Significant bundle-to-shell bypass at high mass flowrates More expensive than traditional double-segmental baffles

Minimizes bypass flow Same pressure drop as with double-segmental baffles, with better heat transfer Well suited for gas-gas applications

Grid

Difficult fabrication, design methods are not standardized

Preferred radial tube layout requires a lesscommon fabrication method than triangular and square layouts In a r adial tube layout, the angular gaps between tubes near the shell are larger than those between tubes near the center; this requires the addition of an improvised, nonradial ( e.g., triangular or rotated square) layout between the radial tube rows

Provides tube support Uniform flow distribution

Relatively low heat-transfer rates, unless the tubes are long

Relatively low pressure drops

Specific tube layouts are required

High conversion ratio of pressure drop to heat transfer

Literature Cited 1.

Lestina, T. G., “Selecting a Heat Exchanger Shell,” Chem. Eng.  Progress, 107 (6), pp. 34–38 (June 2011).

2.

Green, D. W., and R. H. Perry,  “Heat-Transfer Equipment” in “Perry’s Chemical Engineers’ Handbook,” 8th ed., McGraw-Hill,  New York, NY (2008).

3.

Tubular Exchanger Manufacturers Association,  “Standards of the Tubular Exchanger Manufacturers Association,” 9th ed., TEMA, New York, NY (2007).

4.

Mukerjee, R.,  “Don’t Let Bafing Bafe You,” Chem. Eng.  Progress, 92 (4), pp. 72–79 (Apr. 1996).

5.

Lutcha, J., and J. Nemcansky, “Performance Improvement of Tubular Heat Exchangers by Helical Bafes,” Trans. IChemE., 68 (Part A), pp. 263–270 (1990).

6.

Taborek, J.,  “Pressure Drop to Heat Transfer Conversion in Shell-and-Tube Heat Exchangers with Disk-and-Donut Bafes,” AIChE Spring Meeting, New Orleans, LA (2004).

7.

Taborek, J.,  “Longitudinal Flow in Tube Bundles with Grid Bafes,” in “Heat Exchanger Design Handbook — Part 3, Thermal and Hydraulic Design of Heat Exchangers, Section 3.3.12,” Begell House, New York, NY (1998).

Copyright © 2012 American Institute of Chemical Engineers (AIChE)

Further Reading Bell, K. J., and A. C. Mueller,  “Wolverine Engineering Data Book II,” available at www.wlv.com/products/databook/databook.pdf, Wolverine Tube, Inc., Decatur, AL (2001). Hewitt, G. F., et al., “Process Heat Transfer,” CRC Press, Boca Raton, FL (1994). Hewitt, G. F., ed.,  “Heat Exchanger Design Handbook,” Begell House, New York, NY (1998). Kakac, S., and H. Liu,  “Heat Exchangers: Selection, Rating, and Thermal Design,” 2nd ed., CRC Press, Boca Raton, FL (2002). Kern, D., “Process Heat Transfer,” McGraw-Hill, New York, NY (1950). Rohsenow, W., et al., “Handbook of Heat Transfer,” 3rd ed., McGraw-Hill, New York, NY (1998). Serth, R. W.,  “Process Heat Transfer: Principles and Applications,” Elsevier, New York, NY (2007). Thome, J. R., “Wolverine Engineering Data Book III,” available at www.wlv.com/products/databook/db3/DataBookIII.pdf, Wolverine Tube, Inc., Decatur, AL (2004–2010). Webb, R., “Principles of Enhanced Heat Transfer,” 2nd ed., John Wiley & Sons, Inc., Hoboken, NJ (2005).

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