|
|
| Line 1: |
Line 1: |
| {{Redirect|Permeate|the milk product|Milk permeate}}
| | Alyson Meagher is the title her mothers and fathers gave her but she doesn't like when people use her full name. Office supervising is exactly where her primary income comes from but she's already utilized for an additional one. Her family lives in Ohio. It's not a common factor but what I like doing is to climb but I don't have the time recently.<br><br>my blog; [http://breenq.com/index.php?do=/profile-1144/info/ psychic chat online] |
| | |
| In [[physics]] and [[engineering]], '''permeation''' (also called '''imbuing''') is the penetration of a permeate (such as a [[liquid]], [[gas]], or [[vapor]]) through a solid. It is directly related to the concentration gradient of the permeate, a material's [[intrinsic permeability]], and the materials' [[Mass diffusivity]]. Permeation is modeled by equations such as [[Fick's laws of diffusion]], and can be measured using tools such as a [[minipermeameter]].
| |
| | |
| == Description ==
| |
| | |
| The process of permeation involves the diffusion of molecules, called the permeant, through a membrane or interface. Permeation works through diffusion; the permeant will move from high concentration to low concentration across the interface. A material can be semipermeable, with the presence of a [[semipermeable membrane]]. Only molecules or ions with certain properties will be able to diffuse across such a membrane. This is a very important mechanism in biology where fluids inside a blood vessel need to be regulated and controlled. Permeation can occur through most materials including metals, ceramics and polymers. However, the permeability of metals is much lower than that of ceramics and polymers due to their crystal structure and porosity.
| |
|
| |
| Permeation is something that must be regarded highly in various polymer applications, due to their high permeability. Permeability depends on the temperature of the interaction as well as the characteristics of both the polymer and the permeant component. Through the process of [[sorption]], molecules of the permeant can be either absorbed or adsorbed at the interface. The permeation of a material can be measured through numerous methods that quantify the permeability of a substance through a specific material.
| |
| | |
| Permeability is measured in units of area, commonly meters squared. It can be measured in a darcy or millidarcy popularized by [[Henry Darcy]]. They are not official SI units, however they are widely used. The permeability coefficient can be calculated in Barrers. Standard SI units for temperature, time, distance and pressure are used for the gasses and diffusion coefficients used to calculate permeability.
| |
| | |
| == Related terms ==
| |
| * Permeant: The substance or species, ion, molecules permeating through the solid.
| |
| * Semipermeability: Property of a material to be permeable only for some substances and not for others.
| |
| * Permeation measurement: Method for the quantification of the permeability of a material for a specific substance.
| |
| | |
| == History ==
| |
| | |
| === Abbé Jean-Antoine Nollet (physicist, 1700–1770) ===
| |
| [[Jean-Antoine Nollet|Nollet]] tried to seal wine containers with a [[pig's bladder]] and stored them under water. After a while the bladder bulged outwards. He noticed the high pressure that discharged after he pierced the bladder. Curious, he did the experiment the other way round: he filled the container with water and stored it in wine. The result was a bulging inwards of the bladder. His notes about this experiment are the first scientific mention of permeation (later it would be called semipermeability).
| |
| | |
| === Thomas Graham (chemist, 1805–1869) ===
| |
| [[Thomas Graham (chemist)|Graham]] experimentally proved the dependency of gas [[diffusion]] on [[molecular weight]], which is now known as [[Graham's law]].
| |
| | |
| === Richard Barrer (1910–1996) ===
| |
| Barrer developed the modern [[Barrer]] measurement technique, and first used scientific methods for measuring permeation rates.
| |
| | |
| == Permeation in everyday life ==
| |
| | |
| * [[Packaging]]: The permeability of the package (materials, seals, closures, etc.) needs to be matched with the sensitivity of the package contents and the specified [[shelf life]]. Some packages must have nearly [[hermetic seal]]s while others can (and sometimes must) be selectively permeable. Knowledge about the exact permeation rates is therefore essential.
| |
| [[File:Fuel cell still.gif|thumbnail|Fuel Cell Configuration]]
| |
| * [[Tires]]: Air pressure in tires should decrease as slowly as possible. A good tire is one that allows the least amount of gas to escape. Permeation will occur over time with the tires, so it is best to know the permeability of the material that will make up the tire with the desired gas to make the most efficient tires.
| |
| * Insulating material: Water vapour permeation of insulating material is important as well as for submarine cables to protect the conductor from corrosion.
| |
| * [[Fuel cell]]s: Automobiles are equipped with Polymer Electrolyte Membrane (PEM) fuel cells to convert hydrogen fuel and oxygen found in the atmosphere to produce electricity. However, these cells only produce around 1.16 volts of electricity. In order to power a vehicle, multiple cells are arranged into a stack. A stack's power output depends on both the number and the size of the individual fuel cells.
| |
| * Thermoplastic and Thermosetting Piping: Pipes intended to transport water under high pressure can be considered as failed when there is a detectable permeation of water through the pipe wall to the outer surface of the pipe.
| |
| * Medical Uses: Permeation can also be seen in the medical field in drug delivery. Drug patches made up of polymer material contain a chemical reservoir that is loaded beyond its solubility, and then transferred to the body through contact. In order for the chemical to release itself into the body, it must permeate and diffuse through the polymer membrane, according to the concentration gradient. Due to the over solubility of the reservoir, transport of the drug follows the burst and lag mechanism. There is a high transfer rate of the drug when the patch makes contact with the skin, but as time increases a concentration gradient is established, meaning delivery of the drug settles to a constant rate. This is crucial in drug delivery and is used in cases such as the Ocusert System.
| |
| | |
| == Permeation measurement ==
| |
| | |
| [[image:Permeation sweep gas.gif|thumb|Permeation measurement with sweep gas]]
| |
| | |
| The permeation of [[films]] and membranes can be measured with any gas or liquid. One method uses a central module which is separated by the test film: the testing gas is fed on the one side of the cell and the permeated gas is carried to the detector by a sweep gas. The diagram on the right shows a testing cell for films, normally made from metals like [[stainless steel]]. The photo shows a testing cell for pipes made from glass, similar to a [[Liebig condenser]]. The testing medium (liquid or gas) is situated in the inner white pipe and the permeate is collected in the space between the pipe and the glass wall. It is transported by a sweep gas (connected to the upper and lower joint) to an analysing device.
| |
| | |
| Permeation can also be measured through intermittent contact. This method involves taking a sample of the test chemical and placing it on the surface of the material whose permeability is being observed while adding or removing specific amounts of the test chemical. After a known amount of time, the material is analyzed to find the concentration of the test chemical present throughout its structure. Along with the amount of time the chemical was on the material and the analysis of the test material, one can determine the cumulative permeation of the test chemical.
| |
| | |
| The following table gives examples of the calculated permeability coefficient of certain gases through a silicone membrane.
| |
| | |
| {| class="wikitable"
| |
| |-
| |
| ! Gas Name !! Formula !! Silicone Permeability Coefficient (Barrer)*
| |
| |-
| |
| | Oxygen || <math>O_2</math> || 600
| |
| |-
| |
| | Hydrogen || <math>H_2</math> || 650
| |
| |-
| |
| | Carbon Dioxide || <math>CO_2</math> || 3250
| |
| |-
| |
| | Methanol || <math>CH_3OH</math> || 13900
| |
| |-
| |
| | Water || <math>H_2O</math> || 36000
| |
| |}
| |
| *1 Barrer = 10-10 cm3 (STP)· cm /cm2 · s · cm-Hg
| |
| Unless otherwise noted, permeabilities are measured and reported at 25C (RTP) and not (STP)
| |
| From: THIN SILICONE MEMBRANES-THEIR PERMEATION PROPERTIES AND SOME APPLICATIONS
| |
| Annals of the New York Academy of Sciences, vol. 146, issue 1 Materials in, pp. 119–137
| |
| W. L. Robb
| |
| | |
| == Approximation using Fick's First law==
| |
| | |
| The flux or flow of mass of the permeate through the solid can be modeled by [[Fick's_laws_of_diffusion#Fick.27s_first_law|Fick's first law]].
| |
| | |
| :<math>\bigg. J = - D \frac{\partial \phi}{\partial x} \bigg. </math>
| |
| | |
| This equation can be modified to a very simple forumula that can be used in basic problems to approximate permeation through a membrane.
| |
| | |
| :<math>\bigg. J = - D \frac{(C_2 - C_1)}{\delta} \bigg. </math>
| |
| | |
| where
| |
| * <math> J</math> is the "diffusion flux"
| |
| | |
| * <math>\, D</math> is the diffusion coefficient or [[mass diffusivity]]
| |
| | |
| * <math>C</math> is the concentration of the permeate
| |
| | |
| * <math>\, \delta </math> is the thickness of the membrane
| |
| | |
| We can introduce <math> S</math> into this equation, which represents the sorption equilibrium parameter, which is the constant of proportionality between pressure (<math>p</math>) and <math>C</math>. This relationship can be represented as <math>C=Sp</math>.
| |
| | |
| :<math>\bigg. J = - D \frac{S(p_2 - p_1)}{\delta} \bigg. </math>
| |
| | |
| The diffusion coefficient can be combined with the sorption equilibrium parameter to get the final form of the equation, where <math>P</math> is the permeability of the membrane. The relationship being <math> P = SD</math>
| |
| | |
| :<math>\bigg. J = -\frac{P(p_2 - p_1)}{\delta} \bigg. </math>
| |
| | |
| ==Solubility of a gas in a metal==
| |
| In practical applications when looking at gases permeating metals, there is a way to relate gas pressure to concentration. Many gases exist as diatomic molecules when in the gaseous phase, but when permeating metals they exist in their singular ionic form. [[Sieverts' law]] states that the solubility of a gas, in the form of a diatomic molecule, in metal is proportional to the square root of the partial pressure of the gas.
| |
| | |
| The flux can be approximated in this case by the equation:
| |
| | |
| :<math>\bigg. J = - D \frac{(S_1 - S_2)}{\delta} \bigg. </math>
| |
| | |
| We can introduce <math> K</math> into this equation, which represents the [[Sieverts' law|reaction equilibrium constant]]. From the relationship <math>S = {K \sqrt{p_N}}</math>.
| |
| | |
| :<math>\bigg. J = - D \frac{K(\sqrt{p_1} - \sqrt{p_2})}{\delta} \bigg. </math>
| |
| | |
| The diffusion coefficient can be combined with the reaction equilibrium constant to get the final form of the equation, where <math>P</math> is the permeability of the membrane. The relationship being <math> P = KD</math>
| |
| | |
| :<math>\bigg. J = - \frac{P(\sqrt{p_1} - \sqrt{p_2})}{\delta} \bigg. </math>
| |
| | |
| ==See also==
| |
| {{portal|Underwater diving}}
| |
| * [[Moisture vapor transmission rate]]
| |
| * [[Oxygen transmission rate]]
| |
| * [[Carbon dioxide transmission rate]]
| |
| * [[Hermetic seal]]
| |
| * [[Milk permeate]]
| |
| | |
| == External links ==
| |
| * [http://www.composite-agency.com/messages/3875.html Diffusion Coefficient of Gas, Liquid & Vapour in Polymers]
| |
| | |
| ==Further reading== | |
| * Yam, K. L., "Encyclopedia of Packaging Technology", John Wiley & Sons, 2009, ISBN 978-0-470-08704-6
| |
| * Massey,L K, "Permeability Properties of Plastics and Elastomers", 2003, Andrew Publishing, ISBN 978-1-884207-97-6
| |
| * ASTM F1249 Standard Test Method for Water Vapor Transmission Rate Through Plastic Film and Sheeting Using a Modulated Infrared Sensor
| |
| * ASTM E398 Standard Test Method for Water Vapor Transmission Rate of Sheet Materials Using Dynamic Relative Humidity Measurement
| |
| * ASTM F2298 Standard Test Methods for Water Vapor Diffusion Resistance and Air Flow Resistance of Clothing Materials Using the Dynamic Moisture Permeation Cell
| |
| * F2622 Standard Test Method for Oxygen Gas Transmission Rate Through Plastic Film and Sheeting Using Various Sensors
| |
| *F1383: Standard Test Method for Permeation of Liquids and Gases through Protective Clothing Materials under Conditions of Intermittent Contact.
| |
| *THIN SILICONE MEMBRANES-THEIR PERMEATION PROPERTIES AND SOME APPLICATIONS Annals of the New York Academy of Sciences, vol. 146, issue 1 Materials in, pp. 119–137 W. L. Robb
| |
| *Pharmaceutical Systems for Drug Delivery, David Jones; Chien YW. 2nd ed. New York: Marcel Dekker, Inc; 1992. Novel drug delivery systems.
| |
| *O.V. Malykh, A.Yu. Golub, V.V. Teplyakov, Polymeric membrane materials: New aspects of empirical approaches to prediction of gas permeability parameters in relation to permanent gases, linear lower hydrocarbons and some toxic gases, Advances in Colloid and Interface Science, Volume 164, Issues 1–2, 11 May 2011, Pages 89–99, ISSN 0001-8686, 10.1016/j.cis.2010.10.004.
| |
| (http://www.sciencedirect.com/science/article/pii/S0001868610001910)
| |
| Keywords: Prediction of gas/hydrocarbons membrane separation; Toxic gas permeability; Structure/diffusivity relations
| |
| | |
| {{Diving medicine, physiology and physics}}
| |
| | |
| [[Category:Physical quantities]]
| |
| [[Category:Packaging]]
| |
| [[Category:Underwater diving physics]]
| |