Introduction & Context

The convective mass-transfer coefficient \(k_c\) quantifies how fast a species is transported between an interface and a moving fluid. In process engineering it is the key parameter that links the driving force (concentration or partial-pressure difference) to the evaporation or absorption rate. Typical applications include:

  • Design of cooling towers, humidifiers and de-humidifiers
  • Prediction of drying rates for solids and sprays
  • Sizing of gas-scrubbing and stripping columns
  • Estimation of volatile losses from storage tanks or spills

Because direct measurement of interfacial concentration is difficult, the coefficient is usually inferred from the measurable partial-pressure difference and the ideal-gas law. The sheet below shows the standard conversion route from partial pressures to mass flux.

Methodology & Formulas

  1. Convert temperature to absolute scale
    \[T(\text{K})=T(^\circ\text{C})+273.15\]
  2. Evaluate the driving force
    Partial-pressure difference: \[\Delta p=p_{\text{sat}}-p_{\infty}\] Ideal-gas concentration difference (mass basis): \[\Delta C=\frac{\Delta p\cdot M}{R_u\,T}\] where \(M\) = molar mass of the evaporating species \(R_u\) = universal gas constant (kPa m3 kmol-1 K-1)
  3. Compute the mass flux
    Instantaneous flux: \[J=k_c\,\Delta C\] Hourly flux (if required): \[J_{\text{h}}=J\cdot 3600\]
Regime guidance for \(k_c\) selection
Flow regime Reynolds number based on length \(L\) Typical correlation form
Laminar \(\text{Re}_L \le 2\times10^5\) \(\text{Sh}=0.664\,\text{Re}_L^{1/2}\,\text{Sc}^{1/3}\)
Turbulent \(\text{Re}_L \ge 5\times10^5\) \(\text{Sh}=0.037\,\text{Re}_L^{4/5}\,\text{Sc}^{1/3}\)

The Sherwood number \(\text{Sh}=k_c\,L/\mathcal{D}_{AB}\) and the Schmidt number \(\text{Sc}=\nu/\mathcal{D}_{AB}\) link the coefficient to the diffusion coefficient \(\mathcal{D}_{AB}\) and kinematic viscosity \(\nu\). Once \(\text{Sh}\) is known, \(k_c\) follows directly.