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10.4 Continuous Contact Methods, Membrane Separations, and Evaporative Operations

Key Takeaways

  • Continuous contact height is Z=HTU×NTUZ = \text{HTU} \times \text{NTU}, where HTU measures packing efficiency and, for dilute systems with straight operating/equilibrium lines, NTU (NOGN_{OG}) is computed from the log-mean concentration driving force ΔyLM\Delta y_{LM}.

  • Reverse osmosis water flux is Jw=A(ΔP−Δπ)J_w = A(\Delta P - \Delta \pi), where osmotic pressure is given by the van 't Hoff equation π=iCRT\pi = i C R T.

  • Gas permeation flux depends on gas partial pressure difference, and selectivity is the ratio of species permeabilities (αij=PM,i/PM,j\alpha_{ij} = P_{M,i} / P_{M,j}).

  • In ultrafiltration, concentration polarization forms a gel layer at high pressures, leading to pressure-independent flux modeled by the gel-polarization equation.

  • For humidification operations the humidity ratio ω=0.622 pv/(P−pv)\omega = 0.622 \, p_v/(P - p_v) and relative humidity ϕ=pv/psat(TDB)\phi = p_v/p_{\text{sat}}(T_{DB}) define moist-air state on the psychrometric chart, while evaporator mass balance FxF=LxLF x_F = L x_L and energy balance FH^F+Qs=VH^V+LH^LF\hat{H}_F + Q_s = V\hat{H}_V + L\hat{H}_L drive single- and multiple-effect evaporator design.

Last updated: July 2026

10.4 Continuous Contact Methods and Membrane Separations

While trayed columns represent stage-wise contact, many separation processes utilize continuous contact, such as packed columns. Additionally, membrane separations have become essential unit operations in water purification and gas separation. The FE Chemical exam covers packed column design equations (HTU, NTU, HETP) and membrane performance calculations (flux, rejection, and selectivity).

Packed Column Design (Continuous Contact)

In packed columns, liquid and gas contact each other continuously along the height of the column rather than on discrete trays. The total height of the packing (ZZ) required for a separation is determined by:

Z=HTU×NTUZ = \text{HTU} \times \text{NTU}

Where:

  • HTU (Height of a Transfer Unit): Characterizes the mass transfer efficiency of the packing material. A smaller HTU value indicates a more efficient packing.
  • NTU (Number of Transfer Units): Represents the difficulty of the separation, determined by the change in concentration relative to the average driving force.

Gas-Phase Transfer Units

When design is based on gas-phase resistance:

Z=HOG×NOGZ = H_{OG} \times N_{OG}

The Height of an Overall Gas Transfer Unit (HOGH_{OG}) is defined as:

HOG=G′KyaPH_{OG} = \frac{G'}{K_y a P}

Where:

  • G′G' is the molar gas flux per unit area (kmol/(m2⋅s)\text{kmol}/(\text{m}^2\cdot\text{s})).
  • KyaK_y a is the overall gas-phase volumetric mass transfer coefficient (kmol/(m3⋅s⋅Δy)\text{kmol}/(\text{m}^3\cdot\text{s}\cdot\Delta y)).
  • PP is the total operating pressure.

The Number of Overall Gas Transfer Units (NOGN_{OG}) is given by:

NOG=∫y2y1dyy−y∗N_{OG} = \int_{y_2}^{y_1} \frac{dy}{y - y^*}

For dilute systems where both the operating line and the equilibrium line (y∗=mxy^* = m x) are straight, this integrates to:

NOG=y1−y2ΔyLMN_{OG} = \frac{y_1 - y_2}{\Delta y_{LM}}

Where the log-mean concentration driving force (ΔyLM\Delta y_{LM}) is:

ΔyLM=(y1−y1∗)−(y2−y2∗)ln⁡(y1−y1∗y2−y2∗)\Delta y_{LM} = \frac{(y_1 - y_1^*) - (y_2 - y_2^*)}{\ln\left(\frac{y_1 - y_1^*}{y_2 - y_2^*}\right)}

Where y1∗=mx1y_1^* = m x_1 and y2∗=mx2y_2^* = m x_2 are the vapor compositions in equilibrium with the liquid at the bottom and top of the column, respectively.

HETP (Height Equivalent to a Theoretical Plate)

HETP is an empirical parameter used to relate packed column height to the number of equivalent theoretical stages (NstagesN_{\text{stages}}):

Z=Nstages×HETPZ = N_{\text{stages}} \times \text{HETP}

For dilute systems, HETP is related to HOGH_{OG} by the absorption factor A=L/(mG)A = L / (m G):

HETP=HOGln⁡(1/A)(1/A)−1\text{HETP} = H_{OG} \frac{\ln(1/A)}{(1/A) - 1}

Membrane Separations

Membrane processes use a semi-permeable barrier to separate components based on size, charge, or solubility differences.

Reverse Osmosis (RO)

RO is a pressure-driven membrane process used primarily for water purification and desalination. The membrane allows water to pass while rejecting salts.

Water Flux (JwJ_w)

The volumetric or mass flux of water through the membrane depends on the net pressure driving force:

Jw=A(ΔP−Δπ)J_w = A (\Delta P - \Delta \pi)

Where:

  • JwJ_w is the water flux (kg/(m2⋅s)\text{kg}/(\text{m}^2\cdot\text{s}) or L/(m2⋅h)\text{L}/(\text{m}^2\cdot\text{h})).
  • AA is the water permeability coefficient of the membrane.
  • ΔP=Pfeed−Ppermeate\Delta P = P_{\text{feed}} - P_{\text{permeate}} is the transmembrane hydraulic pressure difference.
  • Δπ=πfeed−πpermeate\Delta \pi = \pi_{\text{feed}} - \pi_{\text{permeate}} is the transmembrane osmotic pressure difference.

Osmotic Pressure (π\pi)

Osmotic pressure is estimated using the van 't Hoff equation:

π=iCRT\pi = i C R T

Where ii is the van 't Hoff factor (number of ions formed by the solute, e.g., 2 for NaCl\text{NaCl}, 1 for glucose), CC is molar concentration (mol/L\text{mol/L}), RR is the gas constant, and TT is absolute temperature.

Solute Flux (JsJ_s) and Rejection (RR)

The transport of solute is driven solely by concentration difference:

Js=B(Cf−Cp)J_s = B (C_f - C_p)

Where BB is the solute permeability coefficient, and Cf,CpC_f, C_p are the solute concentrations in the feed and permeate, respectively. The solute rejection (RR) is defined as:

R=1−CpCfR = 1 - \frac{C_p}{C_f}

Gas Permeation

Gas permeation separates gas mixtures based on differences in their rate of permeation through a polymer membrane. The flux of component ii is:

Ji=PM,il(pf,i−pp,i)J_i = \frac{P_{M,i}}{l} (p_{f,i} - p_{p,i})

Where PM,iP_{M,i} is the membrane permeability of component ii, ll is the membrane thickness, and pf,i,pp,ip_{f,i}, p_{p,i} are the partial pressures of component ii in the feed and permeate streams. The membrane selectivity (αij\alpha_{ij}) is the ratio of permeabilities:

αij=PM,iPM,j\alpha_{ij} = \frac{P_{M,i}}{P_{M,j}}

Ultrafiltration (UF)

UF separates macromolecular solutes. Due to the high molecular weight of these solutes, osmotic pressure is negligible. However, at high operating pressures, a concentrated solute layer forms on the membrane surface, creating a gel layer. This phenomenon is known as concentration polarization.

Under gel-limited conditions, the flux becomes independent of pressure and is described by the gel-polarization model:

Jv=kcln⁡(Cg−CpCb−Cp)J_v = k_c \ln\left(\frac{C_g - C_p}{C_b - C_p}\right)

Where JvJ_v is the volumetric flux, kck_c is the mass transfer coefficient, CgC_g is the gel layer concentration at the membrane surface, CbC_b is the bulk solute concentration, and CpC_p is the permeate concentration.


Worked Example: Reverse Osmosis Performance

Problem: A reverse osmosis system desalines water containing 0.15 M NaCl0.15\text{ M}\text{ NaCl} at 298 K298\text{ K}. The feed pressure is 50.0 bar50.0\text{ bar} (5000 kPa5000\text{ kPa}), and the permeate side is at atmospheric pressure (1.0 bar1.0\text{ bar} or 100 kPa100\text{ kPa}). The water permeability coefficient of the membrane is A=2.0×10−6 kg/(m2⋅s⋅kPa)A = 2.0 \times 10^{-6}\text{ kg}/(\text{m}^2\cdot\text{s}\cdot\text{kPa}). Assume the membrane achieves 99%99\% salt rejection (R=0.99R = 0.99). The gas constant is R=8.314 kPa⋅L/(mol⋅K)R = 8.314\text{ kPa}\cdot\text{L}/(\text{mol}\cdot\text{K}), and the van 't Hoff factor for NaCl\text{NaCl} is i=2.0i = 2.0.

  1. Calculate the osmotic pressure of the feed solution (πf\pi_f).
  2. Calculate the osmotic pressure of the permeate solution (πp\pi_p).
  3. Calculate the water flux (JwJ_w) in kg/(m2⋅s)\text{kg}/(\text{m}^2\cdot\text{s}).

Solution:

  1. Compute the feed osmotic pressure:
πf=iCfRT=(2.0)(0.15 mol/L)(8.314 kPa⋅L/(mol⋅K))(298 K)\pi_f = i C_f R T = (2.0) (0.15\text{ mol/L}) (8.314\text{ kPa}\cdot\text{L}/(\text{mol}\cdot\text{K})) (298\text{ K}) πf=0.30×8.314×298=743.27 kPa≈7.43 bar\pi_f = 0.30 \times 8.314 \times 298 = 743.27\text{ kPa} \approx 7.43\text{ bar}
  1. Determine the permeate concentration using the rejection:
R=1−CpCf  ⟹  Cp=Cf(1−R)=0.15×(1−0.99)=0.0015 MR = 1 - \frac{C_p}{C_f} \implies C_p = C_f (1 - R) = 0.15 \times (1 - 0.99) = 0.0015\text{ M}

Compute the permeate osmotic pressure:

πp=iCpRT=(2.0)(0.0015)(8.314)(298)=7.43 kPa≈0.07 bar\pi_p = i C_p R T = (2.0) (0.0015) (8.314) (298) = 7.43\text{ kPa} \approx 0.07\text{ bar}
  1. Calculate the net osmotic pressure difference:
Δπ=πf−πp=743.27−7.43=735.84 kPa\Delta \pi = \pi_f - \pi_p = 743.27 - 7.43 = 735.84\text{ kPa}

Calculate the net hydraulic pressure difference:

ΔP=Pf−Pp=5000−100=4900 kPa\Delta P = P_f - P_p = 5000 - 100 = 4900\text{ kPa}
  1. Compute the water flux:
Jw=A(ΔP−Δπ)=(2.0×10−6 kg/(m2⋅s⋅kPa))(4900−735.84 kPa)J_w = A (\Delta P - \Delta \pi) = (2.0 \times 10^{-6}\text{ kg}/(\text{m}^2\cdot\text{s}\cdot\text{kPa})) (4900 - 735.84\text{ kPa}) Jw=2.0×10−6×4164.16=8.33×10−3 kg/(m2⋅s)J_w = 2.0 \times 10^{-6} \times 4164.16 = 8.33 \times 10^{-3}\text{ kg}/(\text{m}^2\cdot\text{s})

The water flux is 8.33×10−3 kg/(m2⋅s)8.33 \times 10^{-3}\text{ kg}/(\text{m}^2\cdot\text{s}).


Humidification, Drying, and Evaporation

These operations use vaporization and gas-phase contact to remove water or solvent from a process stream. They are grouped in the NCEES FE Chemical Mass Transfer and Separation knowledge area because the same mass-transfer coefficients and equilibrium relationships drive them.

Psychrometrics and Humidification

Psychrometrics describes the thermodynamic properties of moist air. Key definitions shown on the FE Reference Handbook psychrometric chart are:

  • Dry-bulb temperature (TDBT_{DB}): Air temperature measured by a standard thermometer.
  • Wet-bulb temperature (TWBT_{WB}): The temperature reached by evaporative cooling when air flows over a water-saturated wick. It approximates the temperature of liquid water in an adiabatic saturator.
  • Dew point (TDPT_{DP}): The temperature at which air becomes saturated and water just begins to condense.
  • Humidity ratio (ω\omega): The mass of water vapor per mass of dry air. For ideal gases: ω=0.622 pv/(P−pv)\omega = 0.622 \, p_v / (P - p_v), where pvp_v is the partial pressure of water vapor and PP is total pressure.
  • Relative humidity (ϕ\phi): The ratio of actual water vapor pressure to the saturation vapor pressure at the same dry-bulb temperature: ϕ=pv/psat(TDB)\phi = p_v / p_{\text{sat}}(T_{DB}).

An adiabatic humidification process (such as a cooling tower or air washer) follows the constant-enthalpy adiabatic saturation line on the psychrometric chart. In a cooling tower, warm process water is cooled by contact with ambient air; the water evaporates, removing its latent heat of vaporization from the remaining liquid. A cooling tower's approach is Twater,out−TWB,air,inT_{\text{water,out}} - T_{WB,\text{air,in}}, and its range is Twater,in−Twater,outT_{\text{water,in}} - T_{\text{water,out}}. Smaller approach indicates better tower performance but higher capital cost.

Drying Operations

Drying removes liquid (usually water) from a wet solid by vaporization. Drying proceeds in two periods:

  1. Constant-rate period: The solid surface stays saturated; drying rate is controlled by external heat and mass transfer. The rate is approximately Rc=h(TDB−TWB)/λR_c = h (T_{DB} - T_{WB}) / \lambda, where hh is the heat transfer coefficient and λ\lambda is the latent heat of vaporization.
  2. Falling-rate period: Surface unsaturation develops and the rate is controlled by internal moisture diffusion. The critical moisture content marks the transition between the two periods.

The total drying time is the sum of constant-rate and falling-rate contributions; the FE exam most often tests the constant-rate calculation, which reduces to a heat/mass transfer balance.

Evaporation

Evaporation is the concentration of a solution by vaporizing the solvent. A single-effect evaporator heats the feed with steam in a shell-and-tube heat exchanger; vapor leaves the top and concentrated liquor leaves the bottom. The mass balance is:

F=V+L,FxF=LxLF = V + L, \quad F x_F = L x_L

where FF is the feed, VV is the vapor, LL is the concentrated liquor, and xx are mass fractions of solute. The energy balance is:

FH^F+Qs=VH^V+LH^LF \hat{H}_F + Q_s = V \hat{H}_V + L \hat{H}_L

where QsQ_s is the heat supplied by steam. Multiple-effect evaporators reuse vapor from one effect as the heating steam for the next effect at lower pressure; the steam economy (kg vapor produced per kg steam consumed) approaches the number of effects for NN effects operating ideally.

Test Your Knowledge

A reverse osmosis membrane system is operating with a feed pressure of 50 bar and a feed osmotic pressure of 15 bar. The permeate side is at atmospheric pressure (1 bar) with negligible osmotic pressure. If the feed pressure is increased to 70 bar while keeping all other conditions constant, how will the water flux change?

A

It will increase by approximately 59%.

B

It will increase by approximately 40%.

C

It will remain unchanged because osmotic pressure limits the maximum flux.

D

It will double.

Test Your Knowledge

In a packed column separation process, under what condition is the Height Equivalent to a Theoretical Plate (HETP) exactly equal to the Height of an Overall Gas Transfer Unit (HOGH_{OG})?

A

When the column is operating at minimum reflux.

B

When the gas film resistance is completely negligible.

C

When the absorption factor, A=L/(mG)A = L/(mG), is exactly equal to 1.0.

D

When the system is highly concentrated, and the operating line is curved.

Test Your Knowledge

During the ultrafiltration of a protein solution, it is observed that increasing the transmembrane pressure beyond a certain point does not increase the permeate flux. What is the physical explanation for this phenomenon?

A

The membrane pores are completely blocked by irreversible chemical bonding with the protein solute.

B

A concentrated gel layer of solute forms on the membrane surface, creating a dynamic resistance that increases proportionally with pressure.

C

The osmotic pressure of the protein solution becomes equal to the applied transmembrane pressure.

D

The protein molecules undergo denaturation under high pressure, causing them to precipitate and block the permeate channel.

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