Heat Exchanger Fundamentals
Heat Transfer Rate
Overall Heat Transfer Rate:
\[q = UA \Delta T_m\]
- q = heat transfer rate (Btu/hr or W)
- U = overall heat transfer coefficient (Btu/hr·ft²·°F or W/m²·K)
- A = heat transfer surface area (ft² or m²)
- ΔTm = mean temperature difference (°F or K)
Heat Balance - Hot Fluid:
\[q = \dot{m}_h c_{p,h} (T_{h,in} - T_{h,out})\]
- ṁh = mass flow rate of hot fluid (lbm/hr or kg/s)
- cp,h = specific heat of hot fluid (Btu/lbm·°F or J/kg·K)
- Th,in = hot fluid inlet temperature (°F or K)
- Th,out = hot fluid outlet temperature (°F or K)
Heat Balance - Cold Fluid:
\[q = \dot{m}_c c_{p,c} (T_{c,out} - T_{c,in})\]
- ṁc = mass flow rate of cold fluid (lbm/hr or kg/s)
- cp,c = specific heat of cold fluid (Btu/lbm·°F or J/kg·K)
- Tc,in = cold fluid inlet temperature (°F or K)
- Tc,out = cold fluid outlet temperature (°F or K)
Heat Capacity Rate
Heat Capacity Rate:
\[C = \dot{m} c_p\]
- C = heat capacity rate (Btu/hr·°F or W/K)
- ṁ = mass flow rate (lbm/hr or kg/s)
- cp = specific heat (Btu/lbm·°F or J/kg·K)
Minimum and Maximum Heat Capacity Rates:
\[C_{min} = \min(C_h, C_c)\]
\[C_{max} = \max(C_h, C_c)\]
Heat Capacity Rate Ratio:
\[C_r = \frac{C_{min}}{C_{max}}\]
- Cr = heat capacity rate ratio (dimensionless)
- Range: 0 ≤ Cr ≤ 1
Log Mean Temperature Difference (LMTD) Method
Parallel Flow Heat Exchanger
Log Mean Temperature Difference:
\[\Delta T_{lm} = \frac{\Delta T_1 - \Delta T_2}{\ln(\Delta T_1 / \Delta T_2)}\]
- ΔTlm = log mean temperature difference (°F or K)
- ΔT₁ = temperature difference at one end (°F or K)
- ΔT₂ = temperature difference at the other end (°F or K)
For Parallel Flow:
\[\Delta T_1 = T_{h,in} - T_{c,in}\]
\[\Delta T_2 = T_{h,out} - T_{c,out}\]
Counterflow Heat Exchanger
For Counterflow:
\[\Delta T_1 = T_{h,in} - T_{c,out}\]
\[\Delta T_2 = T_{h,out} - T_{c,in}\]
Note: In counterflow, the cold outlet temperature can exceed the hot outlet temperature if Cc < Ch.
Correction Factor Method
Corrected LMTD for Complex Configurations:
\[\Delta T_m = F \Delta T_{lm,cf}\]
- F = LMTD correction factor (dimensionless)
- ΔTlm,cf = LMTD calculated for counterflow arrangement (°F or K)
Correction Factor Parameters:
\[P = \frac{T_{c,out} - T_{c,in}}{T_{h,in} - T_{c,in}}\]
\[R = \frac{T_{h,in} - T_{h,out}}{T_{c,out} - T_{c,in}}\]
- P = temperature effectiveness (dimensionless)
- R = heat capacity rate ratio = Cc/Ch (dimensionless)
- F values are obtained from charts based on P and R for different configurations (1-shell pass/2-tube pass, 2-shell pass/4-tube pass, crossflow, etc.)
Alternative Form:
\[R = \frac{\dot{m}_h c_{p,h}}{\dot{m}_c c_{p,c}}\]
Effectiveness-NTU Method
Heat Exchanger Effectiveness
Effectiveness Definition:
\[\varepsilon = \frac{q}{q_{max}}\]
- ε = heat exchanger effectiveness (dimensionless)
- q = actual heat transfer rate (Btu/hr or W)
- qmax = maximum possible heat transfer rate (Btu/hr or W)
Maximum Heat Transfer Rate:
\[q_{max} = C_{min}(T_{h,in} - T_{c,in})\]
Effectiveness in Terms of Temperatures (when Ch = Cmin):
\[\varepsilon = \frac{T_{h,in} - T_{h,out}}{T_{h,in} - T_{c,in}}\]
Effectiveness in Terms of Temperatures (when Cc = Cmin):
\[\varepsilon = \frac{T_{c,out} - T_{c,in}}{T_{h,in} - T_{c,in}}\]
Number of Transfer Units (NTU)
Number of Transfer Units:
\[NTU = \frac{UA}{C_{min}}\]
- NTU = number of transfer units (dimensionless)
- U = overall heat transfer coefficient (Btu/hr·ft²·°F or W/m²·K)
- A = heat transfer area (ft² or m²)
- Cmin = minimum heat capacity rate (Btu/hr·°F or W/K)
Effectiveness-NTU Relationships
Parallel Flow:
\[\varepsilon = \frac{1 - \exp[-NTU(1 + C_r)]}{1 + C_r}\]
Counterflow:
\[\varepsilon = \frac{1 - \exp[-NTU(1 - C_r)]}{1 - C_r \exp[-NTU(1 - C_r)]}\]
\[\varepsilon = \frac{NTU}{1 + NTU}\]
Shell-and-Tube (1-shell pass, 2,4,6... tube passes):
\[\varepsilon = 2\left\{1 + C_r + \sqrt{1 + C_r^2} \frac{1 + \exp[-NTU\sqrt{1 + C_r^2}]}{1 - \exp[-NTU\sqrt{1 + C_r^2}]}\right\}^{-1}\]
Crossflow (both fluids unmixed):
\[\varepsilon = 1 - \exp\left[\frac{NTU^{0.22}}{C_r}\left(\exp[-C_r \cdot NTU^{0.78}] - 1\right)\right]\]
Crossflow (Cmax mixed, Cmin unmixed):
\[\varepsilon = \frac{1}{C_r}\left[1 - \exp(-C_r(1 - \exp(-NTU)))\right]\]
Crossflow (Cmin mixed, Cmax unmixed):
\[\varepsilon = 1 - \exp\left[-\frac{1}{C_r}(1 - \exp(-C_r \cdot NTU))\right]\]
Special Case - Condensers and Evaporators (Cr = 0):
\[\varepsilon = 1 - \exp(-NTU)\]
- Valid for all flow configurations when one fluid undergoes phase change at constant temperature
Overall Heat Transfer Coefficient
Thermal Resistance Network
Overall Heat Transfer Coefficient (based on inside area):
\[\frac{1}{U_i A_i} = \frac{1}{h_i A_i} + \frac{\ln(r_o/r_i)}{2\pi k L} + \frac{1}{h_o A_o}\]
- Ui = overall heat transfer coefficient based on inside area (Btu/hr·ft²·°F or W/m²·K)
- Ai = inside surface area (ft² or m²)
- Ao = outside surface area (ft² or m²)
- hi = inside convection coefficient (Btu/hr·ft²·°F or W/m²·K)
- ho = outside convection coefficient (Btu/hr·ft²·°F or W/m²·K)
- ri = inside radius (ft or m)
- ro = outside radius (ft or m)
- k = thermal conductivity of tube wall (Btu/hr·ft·°F or W/m·K)
- L = tube length (ft or m)
Overall Heat Transfer Coefficient (based on outside area):
\[\frac{1}{U_o A_o} = \frac{1}{h_i A_i} + \frac{\ln(r_o/r_i)}{2\pi k L} + \frac{1}{h_o A_o}\]
Relationship between Ui and Uo:
\[U_i A_i = U_o A_o\]
Flat Plate Heat Exchanger
Overall Heat Transfer Coefficient (flat plate):
\[\frac{1}{U} = \frac{1}{h_1} + \frac{t}{k} + \frac{1}{h_2}\]
- U = overall heat transfer coefficient (Btu/hr·ft²·°F or W/m²·K)
- h₁, h₂ = convection coefficients on each side (Btu/hr·ft²·°F or W/m²·K)
- t = wall thickness (ft or m)
- k = thermal conductivity of wall (Btu/hr·ft·°F or W/m·K)
Fouling Resistance
Overall Heat Transfer Coefficient with Fouling:
\[\frac{1}{U} = \frac{1}{h_i} + R_{f,i} + \frac{t}{k} + R_{f,o} + \frac{1}{h_o}\]
- Rf,i = fouling factor on inside surface (hr·ft²·°F/Btu or m²·K/W)
- Rf,o = fouling factor on outside surface (hr·ft²·°F/Btu or m²·K/W)
For Cylindrical Tubes with Fouling:
\[\frac{1}{U_i A_i} = \frac{1}{h_i A_i} + \frac{R_{f,i}}{A_i} + \frac{\ln(r_o/r_i)}{2\pi k L} + \frac{R_{f,o}}{A_o} + \frac{1}{h_o A_o}\]
Heat Transfer Area
Total Heat Transfer Area (shell-and-tube):
\[A = N \pi D L\]
- N = number of tubes (dimensionless)
- D = tube diameter (ft or m)
- L = effective tube length (ft or m)
Inside Area of Tubes:
\[A_i = N \pi D_i L\]
Outside Area of Tubes:
\[A_o = N \pi D_o L\]
Actual Heat Transfer Rate
From Effectiveness Method:
\[q = \varepsilon C_{min} (T_{h,in} - T_{c,in})\]
From LMTD Method:
\[q = U A F \Delta T_{lm}\]
Shell-and-Tube Heat Exchangers
Tube-Side Flow
Tube-Side Velocity:
\[V_t = \frac{\dot{m}}{\rho n_p A_t N_t}\]
- Vt = tube-side velocity (ft/s or m/s)
- ṁ = mass flow rate (lbm/s or kg/s)
- ρ = fluid density (lbm/ft³ or kg/m³)
- np = number of tube passes (dimensionless)
- At = cross-sectional area per tube (ft² or m²)
- Nt = total number of tubes (dimensionless)
Cross-Sectional Area per Tube:
\[A_t = \frac{\pi D_i^2}{4}\]
Number of Tubes per Pass:
\[N_{tubes/pass} = \frac{N_t}{n_p}\]
Shell-Side Flow
Shell-Side Cross-Flow Area:
\[A_s = \frac{D_s B (P_T - D_o)}{P_T}\]
- As = shell-side cross-flow area (ft² or m²)
- Ds = shell inside diameter (ft or m)
- B = baffle spacing (ft or m)
- PT = tube pitch (ft or m)
- Do = tube outside diameter (ft or m)
Shell-Side Mass Velocity:
\[G_s = \frac{\dot{m}_s}{A_s}\]
- Gs = shell-side mass velocity (lbm/hr·ft² or kg/s·m²)
- ṁs = shell-side mass flow rate (lbm/hr or kg/s)
Pressure Drop in Heat Exchangers
Tube-Side Pressure Drop
Tube-Side Pressure Drop:
\[\Delta P_t = n_p \left(\frac{f L}{D_i} + 4n_p\right) \frac{\rho V_t^2}{2g_c}\]
- ΔPt = tube-side pressure drop (lbf/ft² or Pa)
- np = number of tube passes (dimensionless)
- f = Darcy friction factor (dimensionless)
- L = tube length (ft or m)
- Di = tube inside diameter (ft or m)
- ρ = fluid density (lbm/ft³ or kg/m³)
- Vt = tube velocity (ft/s or m/s)
- gc = gravitational constant (32.174 lbm·ft/lbf·s² or 1 kg·m/N·s²)
- The factor 4np accounts for entrance/exit losses and return losses
Simplified Form (US Customary):
\[\Delta P_t = \frac{f n_p L \rho V_t^2}{2 g_c D_i}\]
Shell-Side Pressure Drop
Shell-Side Pressure Drop:
\[\Delta P_s = \frac{f_s N_b D_s \rho V_s^2}{2 g_c D_e}\]
- ΔPs = shell-side pressure drop (lbf/ft² or Pa)
- fs = shell-side friction factor (dimensionless)
- Nb = number of baffles (dimensionless)
- Ds = shell inside diameter (ft or m)
- ρ = shell-side fluid density (lbm/ft³ or kg/m³)
- Vs = shell-side velocity (ft/s or m/s)
- De = equivalent diameter (ft or m)
Equivalent Diameter (square pitch):
\[D_e = \frac{4(P_T^2 - \pi D_o^2/4)}{\pi D_o}\]
Equivalent Diameter (triangular pitch):
\[D_e = \frac{4(0.5 P_T^2 \sin(60°) - \pi D_o^2/8)}{\pi D_o/2}\]
Heat Exchanger Selection and Design
Maximum Effectiveness Limits
Maximum Effectiveness for Parallel Flow:
\[\varepsilon_{max} = \frac{1}{1 + C_r}\]
Maximum Effectiveness for Counterflow:
- When Cr < 1: εmax = 1
- When Cr = 1: εmax approaches 1 as NTU → ∞
Temperature Approach
Minimum Temperature Approach (Counterflow):
\[\Delta T_{min} = T_{h,out} - T_{c,in}\]
or
\[\Delta T_{min} = T_{h,in} - T_{c,out}\]
- Whichever is smaller determines the closest approach
- Must be positive for practical heat exchangers
Heat Exchanger Sizing
Required Heat Transfer Area (LMTD Method):
\[A = \frac{q}{U F \Delta T_{lm}}\]
Required Heat Transfer Area (ε-NTU Method):
\[A = \frac{NTU \cdot C_{min}}{U}\]
Special Cases and Condensers/Evaporators
Condensers (Phase Change at Constant Temperature)
Heat Transfer Rate:
\[q = \dot{m} h_{fg}\]
- ṁ = condensate mass flow rate (lbm/hr or kg/s)
- hfg = latent heat of vaporization (Btu/lbm or J/kg)
Effectiveness:
\[\varepsilon = 1 - \exp(-NTU)\]
- Valid because Cr = 0 for phase change
LMTD for Condenser:
\[\Delta T_{lm} = \frac{(T_{sat} - T_{c,in}) - (T_{sat} - T_{c,out})}{\ln\left[\frac{T_{sat} - T_{c,in}}{T_{sat} - T_{c,out}}\right]}\]
- Tsat = saturation temperature of condensing fluid (°F or K)
Evaporators (Boiling at Constant Temperature)
Heat Transfer Rate:
\[q = \dot{m} h_{fg}\]
LMTD for Evaporator:
\[\Delta T_{lm} = \frac{(T_{h,in} - T_{sat}) - (T_{h,out} - T_{sat})}{\ln\left[\frac{T_{h,in} - T_{sat}}{T_{h,out} - T_{sat}}\right]}\]
Compact Heat Exchangers
Finned Surface Parameters
Total Surface Area:
\[A_{total} = A_{fin} + A_{base}\]
- Afin = total fin surface area (ft² or m²)
- Abase = exposed base surface area (ft² or m²)
Fin Efficiency:
\[\eta_f = \frac{\tanh(mL)}{mL}\]
- ηf = fin efficiency (dimensionless)
- m = fin parameter = √(hP/kAc) (1/ft or 1/m)
- L = fin length (ft or m)
- h = convection coefficient (Btu/hr·ft²·°F or W/m²·K)
- P = fin perimeter (ft or m)
- k = thermal conductivity of fin material (Btu/hr·ft·°F or W/m·K)
- Ac = fin cross-sectional area (ft² or m²)
Overall Surface Efficiency:
\[\eta_o = 1 - \frac{A_{fin}}{A_{total}}(1 - \eta_f)\]
- ηo = overall surface efficiency (dimensionless)
Modified Heat Transfer Coefficient:
\[h_{eff} = \eta_o h\]
Regenerative Heat Exchangers
Rotating Regenerator
Effectiveness:
\[\varepsilon = 1 - \exp\left[-\frac{1}{(1 + C_r)}\left(\frac{UA}{C_{min}}\right)\right]\]
- For balanced regenerators with equal heat capacity rates on both sides
Dimensionless Groups for Correlations
Reynolds Number
Reynolds Number:
\[Re = \frac{\rho V D}{\mu} = \frac{V D}{\nu}\]
- Re = Reynolds number (dimensionless)
- ρ = fluid density (lbm/ft³ or kg/m³)
- V = fluid velocity (ft/s or m/s)
- D = characteristic length (tube diameter) (ft or m)
- μ = dynamic viscosity (lbm/ft·s or Pa·s)
- ν = kinematic viscosity (ft²/s or m²/s)
Prandtl Number
Prandtl Number:
\[Pr = \frac{c_p \mu}{k} = \frac{\nu}{\alpha}\]
- Pr = Prandtl number (dimensionless)
- cp = specific heat (Btu/lbm·°F or J/kg·K)
- μ = dynamic viscosity (lbm/ft·s or Pa·s)
- k = thermal conductivity (Btu/hr·ft·°F or W/m·K)
- ν = kinematic viscosity (ft²/s or m²/s)
- α = thermal diffusivity (ft²/s or m²/s)
Nusselt Number
Nusselt Number:
\[Nu = \frac{hD}{k}\]
- Nu = Nusselt number (dimensionless)
- h = convection heat transfer coefficient (Btu/hr·ft²·°F or W/m²·K)
- D = characteristic length (ft or m)
- k = thermal conductivity of fluid (Btu/hr·ft·°F or W/m·K)
Heat Transfer Coefficient from Nusselt Number:
\[h = \frac{Nu \cdot k}{D}\]
Stanton Number
Stanton Number:
\[St = \frac{Nu}{Re \cdot Pr} = \frac{h}{\rho V c_p}\]
- St = Stanton number (dimensionless)
Common Heat Transfer Correlations
Tube-Side Correlations
Dittus-Boelter Equation (turbulent flow in tubes):
\[Nu = 0.023 Re^{0.8} Pr^n\]
- Valid for: Re > 10,000; 0.7 ≤ Pr ≤ 160; L/D > 10
- n = 0.4 for heating (Twall > Tbulk)
- n = 0.3 for cooling (Twall <>bulk)
Sieder-Tate Equation (turbulent flow with viscosity correction):
\[Nu = 0.027 Re^{0.8} Pr^{1/3} \left(\frac{\mu}{\mu_w}\right)^{0.14}\]
- Valid for: 0.7 ≤ Pr ≤ 16,700; Re > 10,000
- μ = viscosity at bulk temperature
- μw = viscosity at wall temperature
Gnielinski Equation (improved accuracy for turbulent flow):
\[Nu = \frac{(f/8)(Re - 1000)Pr}{1 + 12.7(f/8)^{0.5}(Pr^{2/3} - 1)}\]
- Valid for: 3000 ≤ Re ≤ 5×10⁶; 0.5 ≤ Pr ≤ 2000
- f = friction factor from Moody chart or Colebrook equation
Laminar Flow in Tubes (fully developed, constant wall temperature):
\[Nu = 3.66\]
Laminar Flow in Tubes (fully developed, constant heat flux):
\[Nu = 4.36\]
Shell-Side Correlations
Shell-Side Heat Transfer (simplified):
\[Nu = C Re^m Pr^{1/3}\]
- Constants C and m depend on tube arrangement and baffle configuration
- Typically: C ≈ 0.36, m ≈ 0.55 for crossflow over tube banks
Heat Exchanger Analysis Procedure Summary
LMTD Method (Rating Problem)
Procedure:
- Calculate heat transfer rate from energy balance: q = ṁhcp,hΔTh = ṁccp,cΔTc
- Determine outlet temperatures if not given
- Calculate ΔTlm for counterflow configuration
- Determine correction factor F from charts using P and R parameters
- Calculate corrected mean temperature difference: ΔTm = F·ΔTlm
- Solve for U or verify: q = UA·ΔTm
ε-NTU Method (Sizing Problem)
Procedure:
- Calculate heat capacity rates: Ch = ṁhcp,h, Cc = ṁccp,c
- Identify Cmin and Cmax
- Calculate Cr = Cmin/Cmax
- Calculate maximum possible heat transfer: qmax = Cmin(Th,in - Tc,in)
- Determine required effectiveness: ε = q/qmax
- Find NTU from ε-NTU relationship for the specific heat exchanger type
- Calculate required area: A = NTU·Cmin/U
Heat Exchanger Types and Configurations
Flow Arrangement Classification
- Parallel Flow: Both fluids enter at the same end and flow in the same direction
- Counterflow: Fluids enter at opposite ends and flow in opposite directions
- Crossflow: Fluids flow perpendicular to each other (mixed or unmixed)
- Shell-and-Tube: One fluid flows through tubes while the other flows through the shell around the tubes
- Plate Heat Exchanger: Thin corrugated plates create channels for fluid flow
Performance Comparison
Effectiveness Ranking (for same NTU and Cr):
- Counterflow > Crossflow (both unmixed) > Parallel flow
- Counterflow is most efficient for given heat transfer area
- Parallel flow has the lowest maximum effectiveness