Membrane Air Separation University of Illinois Membrane Air Separation In this lab two membranes are used to separate oxygen from nitrogen in air. The two separators are used in series and in parallel to see which set-up will result in the best separation. 1 Unit Operations ChE 382 Group 5 Damo, Duffy, Guerrero, Hsu, Kosak, Qamar, Tyska Spring 2011 4/19/2011 Membrane Air Separation University of Illinois Lab Prep Report Unit Operations II Lab 6 April 19th, 2011 Group 5 Andrew Duffy Daniyal Qamar Jeff Tyska Bernard Hsu Ryan Kosak Tomi Damo Alex Guerrero 2 Unit Operations ChE 382 Group 5 Damo, Duffy, Guerrero, Hsu, Kosak, Qamar, Tyska Spring 2011 4/19/2011 Membrane Air Separation University of Illinois Contents 1. Introduction ........................................................................................................................................... 4 2. Literature Review/Theory ..................................................................................................................... 5 3. Experimental ....................................................................................................................................... 10 3.1. Apparatus .................................................................................................................................... 10 3.2 Materials and Supplies ...................................................................................................................... 13 3.3 Experimental Procedure .............................................................................................................. 13 4. Anticipated Results ............................................................................................................................. 14 5. References ........................................................................................................................................... 16 6. Appendix I: Job Safety Analysis ......................................................................................................... 17 3 Unit Operations ChE 382 Group 5 Damo, Duffy, Guerrero, Hsu, Kosak, Qamar, Tyska Spring 2011 4/19/2011 Membrane Air Separation University of Illinois 1. Introduction The chemical industry relies heavily on the ability to separate streams into their constitute components. Distillation, desalination, and membrane separation are among a few of the methods used. This lab will demonstrate how membrane air separation can be used to achieve the separation of nitrogen and oxygen from an air feed stream. This method of gas separation has an industrial advantage of being moderately efficient yet inexpensive. In this system an air stream will be feed through two permeable polymetric membranes. Because oxygen and nitrogen each have different relative rates of diffusion through the membranes, oxygen will selectively be transported through them at a different rate than nitrogen. The membrane separators (Prism Separator Modules) consist of non-porous hollow fibers which form a semi-permeable barrier for which the gas molecules must pass through to reach the product stream. Oxygen is more permeable than nitrogen through the membranes thus oxygen molecules will pass through at a faster rate creating a product stream rich in oxygen. Four basic steps are involved in the movement of gas molecules through the membranes: adsorption on to the membrane surface, dissolution through the membrane, elution from membrane, and finally desorption from the membrane. The characteristic permeation rate of transfer of the two gases is a function of the molecules ability to dissolve and diffuse through the membranes. Fick’s Law of Diffusion and Henry’s Law will both be used to relate the diffusive flux with diffusivity and concentration with solubility and pressure respectively. Although oxygen and nitrogen pass through the membranes at different rates, both types of molecules are permeable. This means that high levels of separation cannot be achieved using this method. To determine the most efficient separation method the system will be run with the two 4 Unit Operations ChE 382 Group 5 Damo, Duffy, Guerrero, Hsu, Kosak, Qamar, Tyska Spring 2011 4/19/2011 Membrane Air Separation University of Illinois membranes arranged in both series and parallel, as well as differing pressures will be tested. Separation efficiency can then be determined by taking the ration of the permeation of the two gases. 2. Literature Review/Theory Microporous membranes essentially perform as sieves and allow small molecules to move through the pores while large molecules are blocked (Towler and Sinnot, 562). Membrane separation works on the basis of relative permeation rates of the components being separated. Each component transporting through the membrane has a permeation rate that is unique and is a function of the ability of the component to dissolve and diffuse through the membrane. The two main relationships for this separation are Fick’s Law (1) which relates diffusion and Henry’s Law (3) which relates solubility. The gas being separated in this experiment is dry air. This fluid is assumed to be an ideal binary perfect mixture of oxygen and nitrogen. The permeate in this experiment is oxygen whereas nitrogen is the retentate. The first relation to show the diffusive flux through the membrane is expressed by Fick’s Law in equation (1) below. π½π = π·π πΏ ∗ (πΆππ1 − πΆππ2 ) (1) Where: Ji = Flux of component i in mol/m2s Di = Diffusivity of component i in m2/s L = Thickness of membrane in meters Cin1 = Concentration of component i inside membrane wall on feed side in mol/m3 5 Unit Operations ChE 382 Group 5 Damo, Duffy, Guerrero, Hsu, Kosak, Qamar, Tyska Spring 2011 4/19/2011 Membrane Air Separation University of Illinois Cin2 = Concentration of component i outside the membrane wall on permeate side in mol/m3 The total flux of component i, Ji, can then be calculated. π½π = πππ π ππ΄ (2) Where: Qip = Volumetric flow rate of species i in the permeate in m3/s ρ = Density of permeate in mol/m3 A = Area of membrane, (in this case 2.7m2 per module) n = Number of modules used, (in this case 2) Using equation (1) and (2) the only unknown turns out to be the diffusivity of component i, Di, which can be solved for when the two equations are equated through the calculated flux of component i, Ji . From Henry’s Law. πΆππ = ππ ππ (3) Where: Cim = Concentration of component i inside the membrane wall in mol/m3 Si = Solubility constant for component i in the membrane in mol/m3Pa pi = Partial pressure of component i in the gas phase in Pa ( Pascal) 6 Unit Operations ChE 382 Group 5 Damo, Duffy, Guerrero, Hsu, Kosak, Qamar, Tyska Spring 2011 4/19/2011 Membrane Air Separation University of Illinois Permeation through the membrane is a function of diffusivity and solubility therefore: ππ = π·π ππ (4) Where: Pi = Component i membrane permeability in mol/m3sPa Di = Diffusivity of component i in m2/s Si = Solubility constant for component i in the membrane in mol/m3Pa Figure. 1. General values on the permeability of species through different membranes (Wankat, 545) The graph above shows permeability’s for oxygen and nitrogen through four types of membranes calculated at standard pressure and temperature. Using equation (3) and (4) along with the collected data allows the calculation of the solubility constant for component i in the membrane, Si. 7 Unit Operations ChE 382 Group 5 Damo, Duffy, Guerrero, Hsu, Kosak, Qamar, Tyska Spring 2011 4/19/2011 Membrane Air Separation University of Illinois Next the separation efficiency can be determined based off of different permeation rates of the gas components. π πΌππ = π π (5) π Where: αij = Separation factor Pi = Component i membrane permeability in mol/m3sPa An experimental separation factor is frequently used to quantify the separation of a binary system using mole fractions. ′ πΌππ =( π₯ππ π₯ππ π₯ππ ) (6) π₯ππ ′′ πΌππ =( π₯ππ π₯ππ π₯ππ ) (7) π₯ππ Where: α’ij = Separation factor based on the non-permeate composition α’’ij = Separation factor based on feed composition Next the recovery of oxygen and nitrogen can be determined. ππ πΆπ2π π2 π ππππ£πππ¦ = π π πΆπ2π (8) 8 Unit Operations ChE 382 Group 5 Damo, Duffy, Guerrero, Hsu, Kosak, Qamar, Tyska Spring 2011 4/19/2011 Membrane Air Separation University of Illinois π πΆ π2 π ππππ£πππ¦ = π π πΆπ2π π π2π (9) Where: Qp = Volumetric flow rate of permeate in m3/s Qf = Volumetric flow rate of feed in m3/s CO2f = Molar concentration of oxygen in feed in mol/m3 CO2p = Molar concentration of oxygen in permeate in mol/m3 CN2f = Molar concentration of nitrogen in feed in mol/m3 CN2r = Molar concentration of oxygen in permeate in mol/m3 Finally the stage cut can be determined which is the fractional amount of the total feed entering the membrane that passes through as the permeate. πππ΄πΊπΈπΆππ = π ππ π +ππ (10) Where: Qp = Volumetric flow rate of permeate in m3/s Qf = Volumetric flow rate of feed in m3/s 9 Unit Operations ChE 382 Group 5 Damo, Duffy, Guerrero, Hsu, Kosak, Qamar, Tyska Spring 2011 4/19/2011 Membrane Air Separation University of Illinois 3. Experimental 3.1. Apparatus Apparatus: The apparatus could be set up such that the membrane separators would operate in series or in parallel. The apparatus is shown on the next page. 10 Unit Operations ChE 382 Group 5 Damo, Duffy, Guerrero, Hsu, Kosak, Qamar, Tyska Spring 2011 4/19/2011 Membrane Air Separation 6 7 University of Illinois 4 8 12 11 9 3 10 1 14 2 5 15 13 16 11 Unit Operations ChE 382 Group 5 Damo, Duffy, Guerrero, Hsu, Kosak, Qamar, Tyska Spring 2011 4/19/2011 Membrane Air Separation Part No. 1 2 3 4 5 6 7 Apparatus Air Inlet to Apparatus Inlet Manometer Power Switch Membrane Air separators Oxygen outlet Pressure Reader 8 Pressure Transducer Flow Meters 9 Oxygen Sensor 10 Oxygen conc. reader 11 Valve A 12 Valve B 13 Valve C 14 Valve D 15 Manometer Air Tank Air tank 16 University of Illinois Use Make/Model - - Measures the pressure of the inlet air Turns apparatus On/Off Separates Oxygen from air ARO Outlet to the separated oxygen Reads the pressure into the apparatus, theoretically same pressure as 2 Turns pressure into an electrical signal to be read Reads the air flow across each of the membranes Measures the concentration of oxygen in outlet air Top: Measures oxygen rich stream Bottom: Measures Nitrogen rich stream Displays the concentration measured by 9 Control series/parallel flow through apparatus Parallel: Left Series: Right Control series/parallel flow through apparatus Parallel: Down Series: Up Control series/parallel flow through apparatus Parallel: Down Series: Up Control series/parallel flow through apparatus Parallel: Up Series: Up Measures air flow from air tank Holds compressed air Permea – Prism Alpha Model # PPA-22A0 OMEGA - Specification Error Max psig: 150 Max Temp: 200 F Max psig: 300 Max Temp: 150 F - ±1 psi ±1 psi - - TOP TRAK Sierra Instruments Model# 822-13-0VI Teledyne analytical instruments S/N# 719940 Max Psig: 150 Units: SLPM Range: 0-10 Class I-17 sensor ±.01 GB300 Rev 2 ±.01% - Range: 0 - 100 % O2 Response time: 90% of final value in less than 10 s - - - - - - - - - - US Gauge - - - ±1 psi - 12 Unit Operations ChE 382 Group 5 Damo, Duffy, Guerrero, Hsu, Kosak, Qamar, Tyska Spring 2011 4/19/2011 - Membrane Air Separation University of Illinois 3.2 Materials and Supplies Materials/Supplies Compressed Air Description Compressed air to see the effects of membrane separation Specifications - 3.3 Experimental Procedure Start Up Procedure: 1. Turn the power switch on the power strip (3) to the ON position to power up the flow meters (8), digital pressure reader (6), and oxygen analyzers (9). 2. Allow the oxygen analyzers several minutes to reach a steady reading. Also, the flow meters may need resetting if there has been a ground fault. 3. Open the valve (near 15) on the compressed air cylinder. Using the cylinder regulator, set outlet pressure to 140 psig. 4. Set the outlet of the second pressure regulator (near 2) to 100 psig. Do not let it exceed this pressure. 5. At this point the oxygen analyzers should read a percentage by volume of oxygen near 20.9% on the sensor display (10). If they do not, gently remove them and slowly wave them in the air until the sensor displays 20.9%. Parallel Configuration: 6. For a parallel configuration, position the valves as follows: turn valve A (11) to the left, valves B (12) and C (13) down, and valve D (14) up. 7. Allow system to reach steady state and collect data on both oxygen analyzers. 13 Unit Operations ChE 382 Group 5 Damo, Duffy, Guerrero, Hsu, Kosak, Qamar, Tyska Spring 2011 4/19/2011 Membrane Air Separation University of Illinois 8. Allow a few minutes between experimental runs for the system to reach a new steady state. 9. Repeat this procedure with various flow rates of air and various pressures (between 80-120 psig). Allow the system to reach steady state before resuming data collection on both oxygen analyzers. Series Configuration: 10. For a series configuration, position the valves as follows: turn valve A (11) to the right, and valves B (12), C (13), and D (14) up. Shut Down Procedure: 11. Close the valve on the compressed air tank completely. 12. Turn the power switch on the power strip (3) to the OFF position to turn off the flow meters (8), digital pressure reader (6), and oxygen analyzers (9). 13. Close the valve for the outlet of the second pressure regulator. 14. Clean up the surrounding experiment area. 4. Anticipated Results The procedure for running this experiment and changing the independent variables is very simple. The inlet pressures from the air-gas cylinder are varied and the separation method for the air can be run either in parallel or in series (separation cylinders). Because the purpose of this experiment is to determine the mass transfer coefficients, the numbers are difficult to anticipate without some sort of error. It can be anticipated however, that the separation of the 14 Unit Operations ChE 382 Group 5 Damo, Duffy, Guerrero, Hsu, Kosak, Qamar, Tyska Spring 2011 4/19/2011 Membrane Air Separation University of Illinois oxygen from nitrogen will be greater for the series configuration than for the parallel configuration. This is because the air will be passing through two different membranes, one after the other, rather than in parallel, the feed stream will be split and each stream will pass through the membranes only once, thus leading to lesser of separation as compared to the series configuration. While the configuration is one variable to be considered, pressure is a second variable that is to be considered as well. For higher inlet pressures, the amount of oxygen in the permeate stream will be greater and the amount of oxygen in the nonpermeate stream will be lower. Because the driving force for this process is pressure, when pressure increases, more nitrogen diffuses into the membrane. The results that can be anticipated from this laboratory are based off of the two independent variables for the experiment. Placing the membranes in a series configuration will lead to a greater separation of oxygen from nitrogen due to the fact that a single stream will pass through two membranes, while in parallel, the feed stream is split and two streams pass through only one membrane. The second independent variable is that of inlet pressure, where when inlet pressure is increased, the absorption of nitrogen and the concentration of oxygen in the permeate both increase. In order to achieve the highest separation of oxygen from nitrogen as possible, a series configuration with the highest allowable inlet pressure will be used. In order to achieve the lowest separation of oxygen from this laboratory, a parallel configuration with low inlet pressure will be used. 15 Unit Operations ChE 382 Group 5 Damo, Duffy, Guerrero, Hsu, Kosak, Qamar, Tyska Spring 2011 4/19/2011 Membrane Air Separation University of Illinois 5. References Bird, R. Byron, Warren E. Stewart, and Edwin N. Lightfoot. Transport Phenomena. New York: J. Wiley, 2007. Print. Sinnott, Ray, and Gavin Towler. Chemical Engineering Design. Amsterdam: Elsevier, 2009. Print. W.E. McCabe, J.C. Smith, and P. Harriott 2001. Unit Operations of Chemical Engineering, McGraw Hill, New York. 16 Unit Operations ChE 382 Group 5 Damo, Duffy, Guerrero, Hsu, Kosak, Qamar, Tyska Spring 2011 4/19/2011 Membrane Air Separation University of Illinois 6. Appendix I: Job Safety Analysis What is the purpose of this experiment? The purpose of this lab is to separate ambient air into two streams concentrated in its two major components; nitrogen and oxygen. This separation will be achieved using a semipermeable membrane in both a series and parallel setup. Data collected during this experiment will be used to calculate the mass transfer coefficient used in Fick’s law. This value can be used to determine how effective this apparatus is separating the two components. What are the hazards associated with the experiment? High pressure air will be used in this experiment along with sensitive electrical equipment. Concentrated oxygen streams will be created which may be dangerous to operators due to pure oxygen’s combustibility. How will the experiment be conducted in a safe manner? Eye protection will be worn at all times during this lab for protection from this apparatus and the neighboring ones. The pressurized air cylinder will be safely secured to the wall and all valves must be in proper working order. The apparatus must be inspected for any leaks or damaged piping, fittings, or valves. The main cylinder valve will be shut off when the experiment is not running. All electronic components will be checked for damage or exposed (un-insulated) wiring. 17 Unit Operations ChE 382 Group 5 Damo, Duffy, Guerrero, Hsu, Kosak, Qamar, Tyska Spring 2011 4/19/2011 Membrane Air Separation University of Illinois What safety controls are in place? The majority of this apparatus is cover with Plexiglas shielding to protect the operators. The pressurized air cylinder is equipped with a blowout valve in case the pressure inside the take becomes too great. Also, vents are built into the apparatus to exhaust excess pressure. Describe safe and unsafe ranges of operations. This system is rated to operate at a maximum pressure of 140 psig. Pressures above this can damage the membrane. Gas flow rates should be set to around 10−6 square meters/second. Higher flow rates can also damage the membrane used in this system. I have read relevant background material for the Unit Operations Laboratory entitled: Membrane Air Separation and understand the hazards associated with conducting this experiment. I have planned out my experimental work in accordance to standards and acceptable safety practices and will conduct all of my experimental work in a careful and safe manner. I will also be aware of my surroundings, my group members, and other lab students, and will look out for their safety as well. 18 Unit Operations ChE 382 Group 5 Damo, Duffy, Guerrero, Hsu, Kosak, Qamar, Tyska Spring 2011 4/19/2011 Membrane Air Separation University of Illinois Electronic Signatures: Bernard Hsu Daniyal Qamar Jeff Tyska Alex Guerrero Tomi Damo Ryan Kosak Andrew Duffy 19 Unit Operations ChE 382 Group 5 Damo, Duffy, Guerrero, Hsu, Kosak, Qamar, Tyska Spring 2011 4/19/2011