Recap: Introduction 12/1/2015. EVE 402 Air Pollution Generation and Control. Adsorption

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EVE 402 Air Pollution Generation and Control Chapter #6 Lectures Adsorption Recap: Solubility: the extent of absorption into the bulk liquid after the gas has diffused through the interface An internal process (gas-liquid equilibrium) Henry s Law: p i = k H C i Adsorption: an external process (gas-solid equilibrium mostly) Relationship between amount adsorbed and amount still in gas are non-linear Introduction Adsorption: the taking up of a gas (or liquid or dissolved substance) on the surface of a solid or a liquid Liquid surface adsorption is insignificant, though Certain finely divided solids (GAC, silica gel) have extremely large surface areas available and adsorb large quantities of material Adsorbent: the adsorbing solid Adsorbate: the adsorbed gas 1

Introduction Types of Adsorption Physical Consists of attracting gas molecules by van der Waals or electrostatic forces Result is a weak bonding of gas molecules to the solid Process is exothermic Adsorbent is cleaned (rather easily) by either applying heat to or reducing pressure in the adsorption vessel(s) Types of Adsorption (2) Chemical (chemisorption) Involves a chemical reaction and bonding of the adsorbate and the adsorbent Bonds are much stronger than for physical adsorption Not easily reversible (i.e., difficult to clean adsorbent) As a result, if recovery of the adsorbate is desirable, chemisorption is not feasible 2

Schematic Industrial Adsorption Towers The capacity of an adsorbent for a specific gas or vapor is often presented as an isotherm 3

Adsorption Isotherms A point on an isotherm represents the mass of adsorbate per unit mass of adsorbent at a specific temperature One of the best known adsorption models is the Langmuir isotherm: P a = 1 + k 2 P, where k 1 k 1 P = partial pressure of the adsorbate a = mass of adsorbate adsorbed per unit mass of adsorbent k 1, k 2 = constants Adsorption Isotherms (2) Re-arranging the equation: a = k 1P k 2 P + 1 At very low adsorbate partial pressure: a = k 1 P At high partial pressure: a = k 1P k 2 P = k 1 k 2 Adsorption Isotherms (3) Hence, over a narrow, intermediate range of partial pressure: a = k P n where k = constant n = constant (with a value between 0 and 1) This equation is called the Freundlich isotherm 4

Example Problem The data given below are for the adsorption of CO on charcoal at 273 K. Determine the isotherm that fits the data and give the constants of the equation using the given units. P (kpa) 13.3 26.7 40.0 53.3 66.7 80.0 93.3 a (kg/kg) 0.150 0.122 0.094 0.059 0.045 0.038 0.033 Adsorbents: Activated Carbon By far, the most frequently used adsorbent activated dehydration and oxidation steps impart increased surface area Any carbonaceous material can be activated Coconut shells, wood, bone, coal, etc. Ideal material is porous, with a uniform pore distribution Surface area: 600-1400 m 2 /g Adsorbents: Others Activated alumina Surface area: 300 m 2 /g Major applications Drying gas streams Solvent recovery Silica gel Used for over 50 years Surface area: 320 m 2 /g Major application is gas drying 5

Fixed Bed Adsorption: Description During gas flow through the bed, an active adsorption zone (AZ) moves through the bed Behind (above) the AZ, adsorbent is saturated In front of (below) the AZ, absorbent is clean The length of the AZ determines the minimum depth of the adsorbent bed At some point, there is very little clean carbon and the gas breaks through the bed Fixed Bed Adsorption: Schematic Adsorbent above red line (AZ) is saturated Adsorbent below AZ is clean inlet conc. Plot is called a breakthrough curve At this corresponding time, gas has broken through adsorbent outlet conc. Pressure Drop In the absence of measured pressure loss data, the pressure drop across the bed can be estimated with the following empirical relationship: Pg c ε 3 d p ρ g D(1 ε)g 2 = 150(1 ε)μ + 1.75 d p G where ΔP = pressure drop [lb f /ft 2 ] g c = gravitational constant = 4.17 x 10 8 lb m -ft/lb f -hr 2 ε = void fraction [ft 3 voids/ft 3 packed bed] d p = particle diameter [ft] ρ g = gas density [lb m /ft 3 ] D = bed depth [ft] G = gas superficial mass flux [lb m /hr-ft 2 ] μ = gas viscosity [lb m /hr-ft] 6

Pressure Drop A simpler empirical relationship, published by Union Carbide, is as follows: P = 0.37D V 1.56 100 where ΔP = bed pressure drop [in H 2 O] D = bed depth [in] V = superficial gas velocity [ft/min] 7