Adsorption Isotherms

Interactive visualization of adsorption isotherms - Explore Langmuir, Freundlich, BET, and Henry's law isotherms with adjustable parameters

Isotherm Model

Adsorption Isotherm q vs C

Isotherm Current Point

Linearized Plot

Current Values

Concentration C 0.00 mol/L
Adsorption Amount q 0.00 mg/g
Dimensionless C/C₀ 0.00
Current Isotherm Langmuir

Isotherm Equation

q = q_max × (K_L × C) / (1 + K_L × C)

Isotherm Parameters

Langmuir Parameters

Common Parameters

Display Options

Quick Presets

Adsorption Mechanism

Adsorption Types

Physical Adsorption Van der Waals forces, low heat (10-40 kJ/mol), reversible
Chemical Adsorption Chemical bonding, high heat (40-800 kJ/mol), specific

IUPAC Isotherm Types

Type I

Langmuir (Microporous)

Monolayer adsorption, microporous materials, reaches plateau at low P/P₀

Type II

Non-porous / Macroporous

Multilayer adsorption, non-porous materials, follows BET theory

Type III

Weak Adsorbate-Adsorbent

Weak interaction, multilayer formation without monolayer completion

Type IV

Mesoporous with Hysteresis

Mesoporous materials, capillary condensation, adsorption-desorption hysteresis

Type V

Weak Interaction, Mesoporous

Weak interaction with mesoporous structure, similar to Type III with hysteresis

Type VI

Layer-by-Layer Stepwise

Uniform non-porous surfaces, stepwise multilayer formation

Applications of Adsorption

🫧

Separation Processes

Gas purification, mixture separation, solvent recovery, drying processes

💧

Water Treatment

Removal of organic pollutants, heavy metals, color, odor from wastewater

⚗️

Heterogeneous Catalysis

Surface reactions, active sites, catalyst characterization, reaction optimization

🌬️

Gas Storage

Hydrogen storage, natural gas storage, carbon capture, methane adsorption

🧪

Surface Characterization

BET surface area, pore size distribution, surface chemistry analysis

💊

Pharmaceuticals

Drug delivery systems, purification, chromatography, formulation stability

What are Adsorption Isotherms?

Adsorption isotherms describe the equilibrium relationship between the amount of adsorbate adsorbed on a solid surface (adsorbent) and the concentration (or pressure) of the adsorbate in the fluid phase at constant temperature. The word "isotherm" means "constant temperature," reflecting that these measurements are performed at fixed temperatures. Adsorption isotherms are fundamental to understanding surface chemistry, characterizing porous materials, designing separation processes, and optimizing catalytic systems. Different isotherm models (Langmuir, Freundlich, BET, Henry's law) describe different adsorption mechanisms and material types, from monolayer coverage on uniform surfaces to multilayer formation in porous materials.

Langmuir Isotherm

The Langmuir isotherm, developed by Irving Langmuir in 1918, assumes monolayer adsorption on a homogeneous surface with a finite number of identical sites. The key assumptions are: (1) All adsorption sites are equivalent and have the same affinity for the adsorbate; (2) Each site can hold only one adsorbate molecule (monolayer coverage); (3) No lateral interaction between adsorbed molecules; (4) Adsorption is reversible and reaches dynamic equilibrium. The Langmuir equation is q = q_max × (K_L × C)/(1 + K_L × C), where q_max is the maximum adsorption capacity (monolayer coverage) and K_L is the Langmuir constant related to binding affinity. At low concentrations, it reduces to Henry's law (q = q_max × K_L × C); at high concentrations, it approaches saturation (q = q_max). The linearized form (C/q vs C) gives a straight line with slope 1/q_max and intercept 1/(q_max × K_L). The Langmuir isotherm is widely used for chemisorption and monolayer physisorption on uniform surfaces.

Freundlich Isotherm

The Freundlich isotherm is an empirical model developed by Herbert Freundlich in 1909, describing multilayer adsorption on heterogeneous surfaces. Unlike Langmuir, it does not assume monolayer coverage or a saturation limit. The equation is q = K_F × C^(1/n), where K_F is the Freundlich constant indicating adsorption capacity, and n is the intensity parameter indicating adsorption favorability. When n > 1, adsorption is favorable; when n < 1, adsorption is unfavorable. The linearized form (log q vs log C) gives a straight line with slope 1/n and intercept log K_F. The Freundlich model is particularly useful for describing adsorption on heterogeneous surfaces with sites of different energies, intermediate concentration ranges, and systems where multilayer adsorption occurs. However, it fails at very low concentrations (doesn't reduce to Henry's law) and very high concentrations (doesn't predict saturation). It is commonly applied to adsorption from solution, especially on activated carbon and natural materials.

BET Isotherm (Brunauer-Emmett-Teller)

The BET theory, developed by Brunauer, Emmett, and Teller in 1938, extends the Langmuir theory to multilayer adsorption. It assumes that the first layer adsorbs with a heat of adsorption E₁, while subsequent layers adsorb with a heat equal to the heat of liquefaction E_L (weaker, similar to condensation). The BET equation is q = q_max × (K_B × C/C₀)/[(1 - C/C₀) × (1 + (K_B - 1) × C/C₀)], where C is relative concentration (P/P₀) and K_B is the BET constant related to the energy difference between first and subsequent layers. When K_B >> 1 (strong first-layer adsorption), it approximates Langmuir behavior. The linearized BET plot [C/(q × (C_max - C)) vs C/P₀] allows determination of monolayer capacity q_max and BET constant K_B. The BET isotherm is the standard method for measuring surface area of porous materials (BET surface area) and describes Type II and Type IV isotherms well. It applies to non-porous and mesoporous materials where multilayer adsorption occurs before pore filling. Limitations include inapplicability to microporous materials (Type I) and failure at high relative pressures where capillary condensation dominates.

Henry's Law Isotherm

Henry's law describes the linear relationship between adsorbed amount and concentration at very low concentrations or pressures where the surface coverage is minimal (θ << 1). The equation is simply q = K_H × C, where K_H is the Henry's law constant representing the partition coefficient between the adsorbed and fluid phases. This linear behavior occurs when adsorbate-adsorbate interactions are negligible and each adsorption site acts independently. Henry's law is the limiting behavior of both Langmuir and Freundlich isotherms at very low concentrations. It is particularly important for describing trace component adsorption, gas solubility in liquids, and the initial portion of adsorption isotherms. Deviation from linearity indicates the onset of either site saturation (Langmuir behavior) or adsorbate-adsorbate interactions/multilayer formation (Freundlich or BET behavior). Henry's law constants are fundamental parameters in environmental engineering for predicting partitioning and transport of contaminants.

IUPAC Isotherm Classification

The IUPAC classification system categorizes adsorption isotherms into six types based on their shape and the underlying adsorption mechanism. Type I (Langmuir) shows monolayer saturation at low relative pressures, characteristic of microporous materials (< 2 nm pores) where pore filling occurs rather than surface coverage. Type II displays multilayer formation on non-porous or macroporous materials, following BET theory. Type III shows weak adsorbate-adsorbent interactions where multilayer formation begins before monolayer completion. Type IV is characteristic of mesoporous materials (2-50 nm) showing capillary condensation and hysteresis between adsorption and desorption branches. Type V combines weak interactions with mesoporous structure. Type VI represents stepwise layer-by-layer adsorption on highly uniform non-porous surfaces. Understanding isotherm types helps identify pore structure, adsorption mechanism, and select appropriate models for data analysis.

Adsorption-Desorption Hysteresis

Hysteresis occurs when the adsorption and desorption branches of an isotherm do not coincide, creating a loop. This phenomenon is characteristic of mesoporous materials (Type IV isotherms) and is caused by capillary condensation. During adsorption, condensation occurs at the equilibrium vapor pressure of the concave meniscus (Kelvin equation). During desorption, evaporation requires different meniscus curvature, occurring at a different pressure. Hysteresis loop shapes (H1, H2, H3, H4 types) provide information about pore geometry: H1 - cylindrical pores with uniform size; H2 - ink-bottle pores with narrow necks; H3 - slit-shaped pores; H4 - narrow slit pores. Hysteresis also indicates irreversible adsorption processes, pore network effects, and can be used to characterize pore size distribution. The absence of hysteresis (Types I, II, III, V) indicates either non-porous materials, microporous materials without mesopores, or reversible adsorption without capillary condensation.

Practical Applications in Detail

Activated carbon adsorption: Activated carbon is the most widely used adsorbent due to its high surface area (500-1500 m²/g) and porous structure. It removes organic contaminants from water and air through physisorption. The adsorption capacity depends on pore size distribution, surface chemistry, and adsorbate properties. Zeolite molecular sieves: Zeolites are crystalline aluminosilicates with uniform micropores (3-10 Å). They selectively adsorb molecules based on size and shape (molecular sieving) and are used in gas separation, drying, and catalysis. Silica gel: Amorphous silicon dioxide with high surface area and surface silanol groups, used as a desiccant and chromatographic stationary phase. Gas storage: Adsorbed natural gas (ANG) technology uses porous carbons or MOFs to store methane at lower pressures than compressed natural gas (CNG), improving safety and reducing costs. Carbon capture: Adsorption of CO₂ from flue gas using solid sorbents (amine-functionalized materials, MOFs) is a key technology for reducing greenhouse gas emissions.

Surface Characterization Techniques

BET surface area analysis: The standard method for measuring surface area uses N₂ adsorption at 77 K. The BET equation applied to the linear region (relative pressure 0.05-0.30) gives monolayer capacity, which is converted to surface area using the cross-sectional area of N₂ (0.162 nm²). Pore size distribution: Derived from adsorption isotherms using methods such as BJH (Barrett-Joyner-Halenda) for mesopores, DFT (Density Functional Theory) for micropores, and t-plot for micropore volume. Surface chemistry: Boehm titration, FTIR, XPS analyze surface functional groups that affect adsorption capacity and selectivity. Heat of adsorption: Calorimetric measurements or isosteric heat calculated from isotherms at different temperatures (Clausius-Clapeyron equation) provide information on adsorption strength and heterogeneity. In situ characterization: Techniques such as in situ IR, XRD, and NMR reveal adsorption mechanisms, molecular orientation, and structural changes during adsorption.