Heat Exchanger NTU Effectiveness Reference
Reference-style context for the NTU/effectiveness method — common flow arrangements, typical ε–NTU relationships, dimensionless groups (NTU, C*), and how NTU concepts support preliminary heat exchanger checks. Not a design chart and not a calculator.
Caution
This is a reference for preliminary checks only.
The relationships on this page describe idealised flow arrangements with constant fluid properties and uniform flow distribution. They are useful for sanity-checking sizes, rating existing exchangers, and building intuition — they are not a substitute for a complete thermal-hydraulic rating or vendor design. There is no NTU calculator on ProcessConvert; the values here are reference relations, not an interactive chart.
Purpose
The NTU/effectiveness method expresses heat exchanger performance through two dimensionless groups — the number of transfer units NTU = UA / C_min and the capacity rate ratio C* = C_min / C_max — combined into an effectiveness ε = Q / Q_max. It is mathematically equivalent to the LMTD method but is often easier when outlet temperatures are unknown (typical of rating, off-design analysis, or checks against an existing exchanger). This reference summarises the dimensionless groups, the most common ε–NTU relations, and the boundaries within which they are useful.
Dimensionless variables
A measure of the exchanger's heat-transfer size relative to the smaller capacity stream. Higher NTU means a larger exchanger relative to the flow.
Ratio of the smaller stream capacity rate to the larger. C* = 1 means balanced flow; C* = 0 means one side is changing phase (condenser or evaporator).
Ratio of actual duty to the maximum thermodynamically possible duty for the given inlet temperatures and flow rates. Always between 0 and 1.
Typical ε–NTU relationships
| Flow arrangement | ε(NTU, C*) relation | C* = 1 limit |
|---|---|---|
Counter-current (single pass) Best effectiveness at a given NTU and C*; F = 1 in LMTD equivalent. | ε = (1 − exp(−NTU × (1 − C*))) / (1 − C* × exp(−NTU × (1 − C*))) | ε = NTU / (1 + NTU) |
Parallel-flow (co-current, single pass) Maximum effectiveness ≈ 0.5 even at very high NTU when C* = 1. | ε = (1 − exp(−NTU × (1 + C*))) / (1 + C*) | ε = (1 − exp(−2 × NTU)) / 2 |
Shell-and-tube, 1 shell – 2 tube passes Equivalent to LMTD × F correction; F-charts published for this arrangement. | ε = 2 × {(1 + C*) + (1 + C*²)^½ × (1 + exp(−NTU × (1 + C*²)^½)) / (1 − exp(−NTU × (1 + C*²)^½))}⁻¹ | Use the general relation with C* = 1 |
Cross-flow, both fluids unmixed Approximate correlation; vendor rating required for design. | ε ≈ 1 − exp{(1/C*) × NTU^0.22 × [exp(−C* × NTU^0.78) − 1]} (approximate) | Use chart or numerical solution |
Cross-flow, one fluid mixed, one unmixed Two sub-cases (mixed = C_min vs mixed = C_max) give different ε relations. | C_mixed = C_max: ε = (1/C*) × (1 − exp(−C* × (1 − exp(−NTU)))) | ε = 1 − exp(−(1 − exp(−NTU))) |
Phase change (condenser or evaporator) Independent of flow arrangement when C* = 0. | ε = 1 − exp(−NTU) | N/A — C* approaches 0 |
Relations summarised from standard heat transfer references (Incropera; Kays & London; Coulson & Richardson Vol. 6). Compact correlations for cross-flow arrangements are approximate; vendor rating uses tabulated charts or numerical solutions.
Practical guidance
- •Sizing job (terminal temperatures known): the LMTD method is usually faster. NTU is not required.
- •Rating job (area known, outlets unknown): NTU/effectiveness is the natural fit because it gives the outlet temperatures in one pass without iteration.
- •Off-design check: given the same exchanger at a new flow rate or inlet temperature, NTU lets you predict new outlets quickly.
- •Diminishing returns: for any C* > 0, effectiveness asymptotes well below 1. Doubling NTU from 4 to 8 typically gains only a few percent in ε.
- •Pure-condenser shortcut: when one side is condensing or evaporating, C* → 0 and ε = 1 − exp(−NTU) regardless of flow arrangement.
- •Balanced flow: at C* = 1 with counter-current flow, ε = NTU / (1 + NTU). For NTU = 4, ε ≈ 0.80; for NTU = 8, ε ≈ 0.89.
Units / dimensionless variables
- •NTU: dimensionless. Computed from U × A / C_min; U in W/(m²·K), A in m², C in W/K — or any consistent set.
- •C*: dimensionless. Bounded between 0 (one-sided phase change) and 1 (balanced flow).
- •ε: dimensionless. Bounded between 0 and 1.
- •C = ṁ × Cp: capacity rate in W/K or BTU/(h·°F).
- •Q_max: C_min × (T_h,in − T_c,in), in W or BTU/h.
Assumptions
- •Constant overall heat transfer coefficient U across the exchanger.
- •Constant specific heat capacity Cp for each stream (no large temperature ranges with strong Cp variation).
- •Steady-state operation; no heat losses to the environment.
- •Idealised flow arrangement matching the chosen ε–NTU relation (e.g., pure counter-current, true cross-flow with the assumed mixing).
- •Uniform flow distribution — no bypassing, maldistribution, or leakage.
- •Single-phase on each side (except in explicit phase-change cases where C* = 0 applies).
Boundaries and exclusions
- •This page does not include an interactive ε–NTU chart. The relations are listed for reference, not as a design tool.
- •Cross-flow correlations are approximations — production rating uses tabulated charts or numerical solutions.
- •Multi-pass shell-and-tube arrangements have arrangement-specific ε–NTU forms; mixing relations across arrangements gives wrong answers.
- •Phase-change behaviour (boiling, condensation, partial vaporisation) generally needs zone-by-zone treatment or specialised correlations.
- •Fouling, pressure drop, vibration, and mechanical design are not part of NTU/effectiveness — they belong to detailed rating and mechanical design.
- •No standards-grade design accuracy is implied — these relations are for preliminary checks.
How to use in calculations
- 01Identify which side is C_min — the stream with the lower ṁ × Cp. Compute C* = C_min / C_max.
- 02For a sizing job with all terminal temperatures known, prefer the LMTD route. Use the LMTD Calculator for ΔTₘ and the Heat Exchanger Area Calculator for A.
- 03For a rating job (area known, outlets unknown), compute NTU = U × A / C_min and pick the ε relation for the actual flow arrangement.
- 04Compute Q_max = C_min × (T_h,in − T_c,in) and Q = ε × Q_max.
- 05Back out the outlet temperatures: T_h,out = T_h,in − Q / C_h, T_c,out = T_c,in + Q / C_c.
- 06Cross-check the result against the LMTD method using the computed outlets — they should agree.
- 07For multi-pass or cross-flow arrangements outside the listed relations, use vendor rating software or the tabulated charts in Kays & London or Incropera.
Source / context notes
- •Kays & London, Compact Heat Exchangers — standard tabulated ε–NTU charts for all common flow arrangements.
- •Incropera, Bergman, Lavine, DeWitt, Fundamentals of Heat and Mass Transfer — textbook derivation of ε–NTU relations.
- •Coulson & Richardson's Chemical Engineering Volume 6, Chapter 12 — process-engineering treatment of LMTD and NTU.
- •Perry's Chemical Engineers' Handbook, Section 11 — summarised relations and worked examples.
The relations here are summarised for reference. Use the original sources or vendor rating software when chart-level accuracy matters.
Related guides
- Heat Exchanger SizingEngineering guide
- LMTD vs NTU Method: Which Heat Exchanger Sizing Method to UseEngineering guide
- Heat Exchanger Typical U-Values ReferenceEngineering reference
- Heat Exchanger Fouling Factors ReferenceEngineering reference
- Minimum Approach Temperature Reference for Heat ExchangersEngineering reference
- Heat Exchanger Design Margin ReferenceEngineering reference