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Double-Pipe & Hairpin Heat Exchanger Sizer

Rate and size double-pipe & hairpin heat exchangers (TEMA Hairpin). Calculate pure counter-current LMTD (Ft=1.0), annular hydraulics, longitudinal fin efficiency, and series/parallel banks.


⚡ Industrial Presets:

1. Hot Side Stream Specifications

2. Cold Side Stream Specifications

3. Pipe Dimensions & Longitudinal Fins

4. Hairpin Modular Bank Arrangement

Double-Pipe & Hairpin Heat Exchanger Rating Results

TEMA Section 9 / ASME Section VIII Div 1 Pure Counter-Current Hairpin Sizer
SUCCESS
DYNAMIC HAIRPIN CAD STUDIO TEMA Section 9 / Longitudinal Fin Annular Hydraulic Profile
Hairpins: 8 (Series: 8) Fins: 24 (Hf = 12.7 mm) Ft = 1.00 (Counterflow)
INNER TUBE (COLD / TUBE STREAM) INNER TUBE (COLD / TUBE STREAM) U-BEND HOOD Hot In (Annulus) Hot Out (Annulus) Cold In (Tube) Cold Out (Tube) Leg Length = 6.10 m CROSS SECTION Tube Shell ID: 77.9 mm Tube OD: 48.3 mm Fins: 24 (12.7 mm) η_fin: 88.5% Ao/Ai: 4.85x
Surface Overdesign Margin
+12.4%
0% (Pinch) Target: +10% to +25% +50% (Excess)
Longitudinal Fin Efficiency (η_fin)
88.5%
50% Target: ≥ 75-85% 100%
Max Circuit ΔP Budget
0.64 bar
0.0 bar Limit: ≤ 1.0 bar 1.5 bar
Heat Duty (Q)
-- kW
Req Area: -- m²
Dirty Overall U
-- W/m²·K
Clean U: -- W/m²·K
Hairpin Sections
-- Sections
--
Stream ΔP (Hot / Cold)
-- / -- bar
Hairpin Loop Losses

1. Thermal Rating & Counterflow Balance

Total Transferred Duty (Q)-- kW (-- MW)
Log Mean Temp Diff (LMTD)-- °C
Counterflow Correction (Ft)1.000 (Pure Counter-Current)
Effective MTD (ΔTm)-- °C
Temperature Cross StatusNone
Terminal Temperature Approach (ΔT)-- °C
Clean Overall Coeff (Uclean)-- W/m²·K
Dirty Overall Coeff (Udirty)-- W/m²·K
Outside Area Required / Installed-- / -- m²
Overdesign Surface Margin-- %

2. Pipe & Longitudinal Fin Geometry

Outer Shell Pipe Inside Diameter-- mm
Inner Tube Outside / Inside Diameter-- / -- mm
Inner Tubes per Hairpin-- (--)
Fin Construction Type--
Number of Longitudinal Fins-- fins
Fin Height / Thickness-- mm / -- mm
Fin Efficiency (η_fin)-- %
Weighted Surface Efficiency (η_o)-- %
Surface Extension Ratio (Ao / Abare)-- ×
Annular Thermal Equivalent Dia (De)-- mm

3. Annular & Inner Tube Hydraulics

Hydraulic MetricInner TubeAnnular Space
Assigned Process Stream----
Flow Velocity (v)-- m/s-- m/s
Reynolds Number (Re)----
Prandtl Number (Pr)----
Nusselt Number (Nu)----
Convective Coeff (Film)-- W/m²·K-- W/m²·K
Effective Coeff (η_o · h)-- W/m²·K-- W/m²·K
Frictional ΔP-- bar-- bar
Return Bends / Loop ΔP-- bar-- bar
Total Circuit ΔP-- bar-- bar

4. Modular Bank & Mechanical Limits

Hairpins in Series per Bank-- sections
Number of Parallel Banks-- bank(s)
Total Installed Hairpins-- sections
Min Hairpins Required for Duty-- sections
Nominal Leg Length-- m
Effective Length per Hairpin (2 legs)-- m
Total Circuit Tubing Length-- m
Surface Area per Hairpin-- m²
Design Pressure Rating-- barg
Hydrostatic Test Pressure (1.43x)-- barg

AI Engineering Diagnostics & TEMA Hairpin Verification


📐 Engineering Formula & Specification Sheet

Double-Pipe & Hairpin Heat Exchanger Sizer: Sizing Methodology & Engineering Basis

Rate and size double-pipe & hairpin heat exchangers (TEMA Hairpin). Calculate pure counter-current LMTD (Ft=1.0), annular hydraulics, longitudinal fin efficie

📐 Reviewed by: ChemProCal Engineering Editorial Team
🗓️ Standards: ASME / API / GPSA / ISA
⏱️ Format: Quick Reference Spec Sheet

1. Calculation Scope & Governing Equations

This rating sheet provides sizing and thermal-hydraulic verification for double-pipe and hairpin heat exchangers in accordance with TEMA (10th Edition, Section 9) and ASME Section VIII Division 1.

$$Q = \dot{m}_h C_{p,h} (T_{h,in} - T_{h,out}) = \dot{m}_c C_{p,c} (T_{c,out} - T_{c,in})$$
$$\text{LMTD} = \frac{\Delta T_1 - \Delta T_2}{\ln(\Delta T_1 / \Delta T_2)}, \quad \Delta T_1 = T_{h,in} - T_{c,out}, \quad \Delta T_2 = T_{h,out} - T_{c,in}, \quad F_t = 1.000$$
$$A_{\text{req}} = \frac{Q}{U_o \cdot \text{LMTD}}, \quad N_{\text{hairpins}} = \left\lceil \frac{A_{\text{req}}}{A_{\text{hairpin}}} \right\rceil$$
$$\frac{1}{U_o} = \frac{1}{\eta_o h_{ann}} + R_{f,ann} + \frac{d_o \ln(d_o / d_i)}{2 k_w} + \left(R_{f,tube} + \frac{1}{h_{tube}}\right) \frac{A_o}{A_i}$$
$$m = \sqrt{\frac{2 h_{ann}}{k_f t_f}}, \quad \eta_f = \frac{\tanh(m H_f)}{m H_f}, \quad \eta_o = 1 - \frac{A_f}{A_o}(1 - \eta_f)$$
$$D_{h,hyd} = \frac{4 A_{ann}}{P_{w,hyd}} = \frac{4 A_{ann}}{\pi D_i + \pi d_o + 2 N_f H_f}, \quad D_{e,th} = \frac{4 A_{ann}}{\pi d_o + 2 N_f H_f}$$
$$\Delta P = \left(4 f \frac{L_{tot}}{D_h} + K_{bend} N_{bends}\right) \left(\frac{\rho v^2}{2}\right)$$

2. Standard Parameters & TEMA Design Criteria

Service / Fluid Type Typical Overall U ($W/m^2\cdot K$) Recommended Fin & Velocity Limits
Heavy Fuel Oil (HFO) Preheater $80 - 220\text{ W/m}^2\cdot\text{K}$ Longitudinal fins ($N_f = 24 - 36$); $v_{ann} = 0.6 - 1.2\text{ m/s}$; prevents asphalt deposition.
High-Pressure Gas-Gas Interchanger $150 - 350\text{ W/m}^2\cdot\text{K}$ Deep temperature cross ($T_{c,out} > T_{h,out}$); bare or low fins; $v = 8 - 18\text{ m/s}$.
Reactor Jacket Booster (Water/Glycol) $600 - 1,400\text{ W/m}^2\cdot\text{K}$ Bare inner tube ($N_f = 0$); $v = 1.2 - 2.2\text{ m/s}$; low hydraulic pressure loss ($\le 0.35\text{ bar}$).
LMTD Correction Factor ($F_t$) $1.000$ (Exact) Pure counter-current flow eliminates temperature cross instability; no shell-series penalty.

3. Engineering Assumptions & Boundary Limits

  • Pure Counterflow Rigor: Assumes counter-current flow along all straight runs and 180° return bends, enforcing $F_t = 1.000$.
  • Hydraulic vs Thermal Separation: Annular pressure drop is governed by total wetted perimeter ($D_{h,hyd}$), while convective heat transfer is evaluated using heat-transfer wetted perimeter ($D_{e,th}$) per Kern (1950).
  • Fin Heat Transfer: Longitudinal fins are assumed to be continuous welded or integral with carbon or stainless steel inner tubes, with 100 percent bond conductance.
  • Differential Thermal Expansion: Return bend floating hood allows independent expansion of the inner tube without requiring bellows or expansion joints.

📚 ChemProCal Knowledge Base

Need Complete Mathematical Derivations & Industrial Case Studies? Explore our in-depth engineering textbook guide: Double-Pipe & Hairpin Heat Exchanger Sizing: TEMA Standards & Counter-Current Design Guide.

Read Full Theory Guide →
Peer Review & Engineering Accuracy

This specification sheet and its mathematical formulations adhere to internationally recognized process codes (TEMA Section 9, ASME Section VIII Division 1, and API 660). Sizing parameters and default design allowances are cross-referenced with empirical industry design practices.

📚 ChemProCal Knowledge Base

Need Complete Mathematical Derivations & Industrial Case Studies?

Explore our in-depth engineering textbook guide: Double-Pipe & Hairpin Heat Exchanger Sizing: TEMA Standards & Counter-Current Design Guide. Features step-by-step manual hand calculations, thermodynamic proofs, and commercial simulator benchmarks.

Read Full Theory Guide →
Peer Review & Engineering Accuracy

This specification sheet and its mathematical formulations adhere to internationally recognized process codes (ASME, API, GPSA, TEMA, and ISA). Sizing parameters and default design allowances are cross-referenced with empirical industry design practices.

About This Tool

Thermodynamics & Hairpin Exchanger Rating: Pure Counterflow, Finned Annulus Dynamics & Modular Sizing

Principles of Double-Pipe & Hairpin Heat Exchangers (TEMA Section 9)

Double-pipe and hairpin heat exchangers are specialized industrial heat transfer units constructed from two concentric pipes or tubes joined at one end by a 180° return bend. Unlike multipass shell-and-tube exchangers which suffer from cross-flow inefficiency and complex baffle arrangements, hairpin exchangers direct fluid through continuous, uninterrupted annular and inner-tube flow passages.

Governed by TEMA Section 9, hairpin exchangers excel in high-pressure processing (> 100 bar), services with severe temperature crosses, and low thermal duties (Q < 500 kW) where conventional shell-and-tube units would operate at unacceptably low fluid velocities with heavy fouling tendencies.

Pure Counter-Current Flow & Immunity to Temperature Crosses

In standard multipass shell-and-tube exchangers (such as TEMA 1-2 or 2-4 designs), portions of the tube fluid flow in parallel (co-currently) with the shell fluid. This reduces the effective mean temperature difference, requiring the application of an LMTD correction factor (Ft < 1.0). When the cold fluid outlet temperature rises above the hot fluid outlet temperature (a temperature cross), the Ft factor drops catastrophically below 0.80, forcing engineers to split the service into multiple shells in series.

In hairpin heat exchangers, because the two streams flow in opposite directions along every linear metre of tubing, flow is purely counter-current. The LMTD correction factor is identically:

$$F_t = 1.000$$

This allows double-pipe hairpins to operate with extreme temperature crosses effortlessly without thermal pinch penalties or multi-shell multiplication.

Longitudinal Finned Tubes & Fin Surface Efficiency Dynamics

When one fluid exhibits a significantly lower heat transfer coefficient than the other (such as viscous heavy fuel oil or low-pressure gases flowing against high-pressure steam or water, where h_tube / h_annulus > 2.5), the outer annular film controls the overall heat transfer rate.

To overcome this bottleneck, continuous longitudinal fins are welded to the outer diameter of the inner tube, expanding the outer surface area by up to 10 to 15 times. Because heat conduction along the fin thickness creates a temperature gradient, fin efficiency is calculated via:

$$m = \sqrt{\frac{2 h_{ann}}{k_f \cdot t_f}}, \quad \eta_f = \frac{\tanh(m \cdot H_f)}{m \cdot H_f}$$

The weighted overall surface efficiency (ηo) accounts for both the finned area and the unfinned bare root area to establish true dirty thermal resistance.

Annulus Fluid Dynamics: Hydraulic vs. Thermal Equivalent Diameters

In the annular space between the inner tube and the outer pipe, fluid friction occurs across both outer and inner walls (plus all fin surfaces), while heat transfer occurs solely across the inner tube assembly. TEMA Section 9 and Kern (1950) separate these into two distinct equivalent diameters:

  • Hydraulic Diameter ($D_{h,hyd}$): Based on total wetted friction perimeter. Used to calculate the Reynolds number and Darcy-Weisbach friction factor for annular pressure drop: $$D_{h,hyd} = \frac{4 A_{ann}}{\pi D_i + \pi d_o + 2 N_f H_f}$$
  • Thermal Diameter ($D_{e,th}$): Based strictly on the heat-transfer transmitting perimeter. Used to evaluate the Nusselt number and film coefficient ($h_{ann}$): $$D_{e,th} = \frac{4 A_{ann}}{\pi d_o + 2 N_f H_f}$$

Step-by-Step Worked Example: Heavy Fuel Oil Hairpin Preheater Rating

Scenario: Size a hairpin exchanger to heat $18,000\text{ kg/h}$ of Heavy Fuel Oil from $50^\circ\text{C}$ to $110^\circ\text{C}$ using hot thermal oil entering at $180^\circ\text{C}$ and cooling to $140^\circ\text{C}$.

  1. Thermal Duty ($Q$):
    $$Q = \dot{m} \cdot Cp \cdot \Delta T = \frac{18,000}{3600} \times 2.15 \times (110 - 50) = 645.0\text{ kW}$$
  2. Pure Counter-Current LMTD:
    $$\Delta T_1 = 180 - 110 = 70.0^\circ\text{C}, \quad \Delta T_2 = 140 - 50 = 90.0^\circ\text{C}$$
    $$\text{LMTD} = \frac{70 - 90}{\ln(70 / 90)} = 79.58^\circ\text{C}, \quad F_t = 1.000$$
  3. Hairpin Specification:
    Outer pipe: 4" Sch 40 ($D_i = 102.3\text{ mm}$), Inner tube: 2" Sch 40 ($d_o = 60.3\text{ mm}$) with 24 carbon steel longitudinal fins ($H_f = 12.7\text{ mm}, t_f = 0.89\text{ mm}$), nominal leg length $6.0\text{ m}$.
  4. Coefficients & Fin Efficiency:
    $h_{ann} = 145\text{ W/m}^2\cdot\text{K}$, $m = 80.7\text{ m}^{-1}$, $\eta_f = 75.3\%$, $\eta_o = 82.1\%$, giving $U_o = 112\text{ W/m}^2\cdot\text{K}$.
  5. Bank Sizing:
    $A_{required} = 72.3\text{ m}^2$. Each hairpin provides $18.8\text{ m}^2$. Sizing yields 4 Hairpins in Series ($A_{installed} = 75.2\text{ m}^2$, overdesign margin $+4.0\%$).

Frequently Asked Questions

Why are double-pipe hairpin exchangers immune to temperature cross limitations?

In a double-pipe or multitube hairpin exchanger, the tube-side and annulus-side fluids flow in pure counter-current directions along every millimetre of active pipe length. Unlike multipass shell-and-tube exchangers where co-current passes degrade the effective temperature driving force (resulting in Ft < 0.80 and pinch warnings), hairpin exchangers have an Ft factor identically equal to 1.000. This enables them to easily handle cases where the cold fluid outlet temperature is hotter than the hot fluid outlet temperature.

When should I choose longitudinal finned inner tubes over bare tubes?

Longitudinal fins should be specified whenever the fluid in the annular space has a significantly lower convective heat transfer coefficient than the tube-side fluid (typically when h_tube / h_annulus > 2.5). Common examples include viscous heavy oils, lubricating oils, and low-pressure gases flowing against steam, thermal oil, or cooling water. The fins expand the outer surface area by a factor of 10 to 15, drastically reducing the overall physical length and number of hairpin sections required.

What is the difference between hydraulic diameter (Dh) and thermal diameter (De)?

In an annular passage, fluid friction occurs along the outer pipe inner wall, inner tube outer wall, and all fin surfaces. The hydraulic diameter (Dh = 4*A_ann / Pw_total) is based on the total wetted friction perimeter and is used to calculate the Reynolds number and Darcy friction factor for pressure drop. However, heat transfer only occurs across the inner tube and fin surfaces. The thermal equivalent diameter (De = 4*A_ann / Pw_heat) considers only the heat-transmitting perimeter and is used to compute the Nusselt number and convective film coefficient (Kern 1950).

How do I decide whether to arrange hairpins in series or parallel?

An all-series arrangement maximizes fluid velocity, creating higher convective film coefficients and higher overall U-values, which minimizes required surface area. However, series arrangement results in cumulative pressure drops across all legs. When the available pressure drop is limited (e.g., <= 0.7 bar), splitting the flow into parallel branches cuts the mass flow per branch in half and reduces the pressure drop by approximately a factor of 4, at the trade-off of slightly reduced film coefficients.

What are the typical pressure and size limits for double-pipe exchangers compared to shell-and-tube?

Because double-pipe exchangers use standard small-diameter piping (typically 2 to 6 inch shells) rather than large-diameter rolled vessel shells, their wall thickness provides immense mechanical strength. Double-pipes routinely operate at pressures from 100 bar up to 350 bar (1,500 to 5,000 psi) without requiring massive high-pressure flanges. They are ideal for duties below 500 kW or surface areas under 100 m²; beyond 150 to 200 m², standard shell-and-tube exchangers become more economically compact.

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