logging in or signing up gpcatkins06 Christo Download Post to : URL : Related Presentations : Share Add to Flag Embed Email Send to Blogs and Networks Add to Channel Uploaded from authorPOINTLite Insert YouTube videos in PowerPont slides with aS Desktop Copy embed code: (To copy code, click on the text box) Embed: URL: Thumbnail: WordPress Embed Customize Embed The presentation is successfully added In Your Favorites. Views: 285 Category: Education License: All Rights Reserved Like it (0) Dislike it (0) Added: January 04, 2008 This Presentation is Public Favorites: 0 Presentation Description No description available. Comments Posting comment... By: maan75 (19 month(s) ago) Thank you Saving..... Post Reply Close Saving..... Edit Comment Close Premium member Presentation Transcript The properties of mixtures: The properties of mixtures Yongsik Lee March 2005Thermodynamic description of mixtures: Thermodynamic description of mixtures Yongsik LeePartial molar properties: Partial molar properties Definition Contribution (per mole) that a substance makes to an overall property of a mixture Example Partial molar volume (VJ) Partial molar Gibbs energy (GJ)Partial molar volume: Partial molar volume Example : VJ Water/ethanol mixture What is the total volume of a mixture of 50.0 g of ethanol and 50.0 g of water at 25โ? 1 mol of water + pure water = 18 cm3 1 mol of water + pure ethanol = ?Partial molar volume (VJ): Partial molar volume (VJ) Water/ethanol mixture VJ V = nAVA + nBVB 1 mol of water + pure water = 18 cm3 1 mol of water + pure EtOH = 14 cm3 2.77 mol water + 1.09 mol EtOH Mole fraction X EtOH = 0.282 Partial molar Gibbs energy: Partial molar Gibbs energy Contribution of J to the total Gibbs energy of a mixture G = nAGA + nBGB Chemical potential (ฮผ) Partial molar Gibbs energy G = nAฮผ A + nBฮผ BVariation of chemical potential: Variation of chemical potential For a perfect gas, G(Pf)-G(Pi)=nRT ln(Pf/Pi) Gm(Pf) = Gm(Pi) + RT ln(Pf/Pi) Set Pf=P and Pi=P°(the standard pressure, 1 bar) Gm(P) = Gm(P°) + RT ln(P/P°) For a mixture of perfect gases, Gm(P) = Gm(P°) + RT ln(P/P°) ฮผJ = ฮผJ° + RT ln(PJ/P°) ฮผJ = ฮผJ° + RT lnPJ ฮผJ° = Standard chemical potential of the gas JSpontaneous mixing: Spontaneous mixing All gases mix spontaneously Gibbs energy of mixing (ฮGmix) < 0 nA, p, T nB, p, T nA+ nB, p, TGibbs energy of mixing: Gibbs energy of mixing ฮGmix = Gf - Gi Gi = nAฮผ A + nBฮผ B = nA(ฮผA° + RT ln p) + nB(ฮผB° + RT ln p) Gf= nA(ฮผA° + RT ln xAp) + nB(ฮผB° + RT ln xBp) consider partial pressure for A and B ฮGmix = nA(RT ln xA) + nB(RT ln xB) = nRT[xAln xA + xBln xB] (ฮGmix) < 0Entropy of mixing: Entropy of mixing ฮGmix = nRT[xAln xA + xBln xB] With ฮG = ฮH - T ฮS ฮH =0 then ฮSmix = -nR[xAln xA + xBln xB] The increase in entropy of the system is the driving force of the mixing!Raoultโs law: Raoultโs law Chemical potential of a solute Partial vapor pressure(pJ) of each component in the mixture Francois Raoult (1830-1901)Raoultโs Law: Raoultโs Law pJ = xJpJ* The partial vapor pressure of a substance(pJ) in a mixture is proportional to its mole fraction(xJ) in the solution and its vapor pressure when pure(pJ*) Limiting law ([J]โ0)Molecular origin of Raoultโs law: Molecular origin of Raoultโs lawIdeal solution: Ideal solution Definition A hypothetical solution That obeys Raoultโs law throughout the composition range from pure A to pure B No mixture is perfectly ideal! (deviations)Real solution vs. ideal solution: Real solution vs. ideal solutionIdeal dilute solution: Ideal dilute solution Henryโs law pB=xBKB KB= Henryโs law constant Only at low [B] Ideal-dilute solution Solute B obeys HenryโsReal solution: Real solution Activity(aJ) = effective concentration ฮผJ = ฮผJ° + RT ln aJ Always true at any concentration For ideal solution, aJ = xJ For ideal-dilute solution, aA = ฮณAxA, aB = ฮณB[B], Activity coefficient ฮณA โ1 as xA โ1 ; ฮณB โ1 as [B] โ0 For a pure liquid or solid, a=1 Colligative properties: Colligative properties Yongsik LeeColligative properties: Colligative properties Definition โDepending on the collectionโ Depending on the number not the nature Chemical potential equilibrium Examples Boiling point, freezing point modification Osmosis, osmotic pressureModification of bp and fp: Modification of bp and fpCondition of solute: Condition of solute ์ฉ์ง์ ์กฐ๊ฑด Solute is not volatile No concentration to the vapor phase Solute does not dissolve in solid solvent ฮTb = Kb b(B) Ebullioscopic constant ฮTf = Kf b(B) Cryoscopic constantosmosis: osmosisOsmotic Pressure: Macromolecule is uncharged Macromolecule can not pass through the membrane Solvent flows from right to left, diluting the macromolecular solโn As the dilution takes place, the solutionn vol. increases and the level in the capillary rises Osmotic PressureOsmotic pressure: Osmotic pressureosmosis: osmosis movement of a solvent through a semipermeable membran (๋ฐํฌ๋ง) into a solution of higher solute concentration to equalize the concentrations of solute on the two sides of the membrane Osmotic pressure (ฮ )Jacobus H. van 't Hoff (1852-1911) Nobel Prize 1901: Jacobus H. van 't Hoff (1852-1911) Nobel Prize 1901 The first nobel prize in chemistryVanโt Hoff equation: Vanโt Hoff equation At Equilibrium ฮผ(solvent in the solution, p+ฮ ) = ฮผ(pure solvent, p) Vanโt Hoff equation ฮผ*(pure solvent, p)= ฮผ(xA solvent, p+ฮ ) ฮผ*(pure solvent, p)= ฮผ*(p+ฮ ) + RT ln xA ฮผ*(pure solvent, p)= ฮผ*(p) + VAฮp + RT ln xA 0 = VAฮp + RT ln xA VAฮ = RTxB Useful for Molecular weight determination Macromolecules โ MALDIVanโt Hoff Coefficient: Vanโt Hoff Coefficient Vanโt Hoff ๊ณ์(i) ์ฉ์ก์ ์๋ ์ ์์ ๋ชฐ ์์ ์ฉ์ก์ ๋ น์ ์๋ ์ฉ์ง์ ๋ชฐ ์ ๋น์จ ์ค์ ๊ฐ๊ณผ ์ด๋ก ๊ฐ์ด ๋ค๋ฅธ ์ด์ ์ด์จ๋ค์ด ์ด์จ์์ผ๋ก ํ๋ ์ ํ๋์ด ํฐ ์ด์จ์ ๊ฒฝ์ฐ ๋๋๋ฌ์ง๋ค ฮT = imKPhase diagrams of mixtures: Phase diagrams of mixtures Yongsik Lee 2005. 4. 7Phase Diagram: Phase Diagram ๋ฌผ์ง์ ์์ ์ด๋(phase diagram) ๋ฌผ์ง์ ์จ๋๋ฅผ ์ผ์ ํ๊ฒ ํ๊ณ ์๋ ฅ์ ๋ณํ์ํค๋ฉด ์ด๋ค ํน์ ํ ์๋ ฅ์์ ๋ฌผ์ง์ ๋ ์ ์ฌ์ด์ ์ ์ด(phase transition)๊ฐ ์ผ์ด๋๊ฒ ๋๋ค. ์ด ๊ณผ์ ์ ๋ง์ ๋ค๋ฅธ ์จ๋์์ ๋ํ์ดํ๋ฉด ํํ๊ณก์ ์ด ์์ฑ๋๋ค. ์์ ์ด๋์ ๊ตฌ์ฑ ๊ฐ๋ก์ถ์ ์จ๋, ์ธ๋ก์ถ์ ์๋ ฅ์ ํ์ํ๊ณ ์ฃผ์ด์ง ์จ๋์ ์๋ ฅ์์ ๊ฐ์ฅ ์์ ๋ ์์ ํ์ํ๋ค.Mixtures of volatile liquids: Mixtures of volatile liquids Temp(T)-composition(xA) diagram Vapor in equilibrium is also a mixture of two Composition is different (tie line) Tie line A line joining two phases that are in equilibrium with each otherFractional distillation: Fractional distillationDistiller: Distiller ์ ์ ๋ณดํต ์ ์กฐ๋ฐฉ๋ฒ์ ๋ฐ๋ผ ์ธ ๊ฐ์ง๋ก ๋ถ๋ฅ๋๋ค. ์์กฐ์ฃผ ์ฆ๋ฅ์ฃผ ์ฌ์ ์ฃผ(ํผ์ฑ์ฃผ) ์์กฐ์ฃผ(้้ ้ )- ๋ฐํจ์ฃผ ๊ณผ์ค์ด๋ ๊ณก๋ฅ ๋ฑ์ ํจ์ ๋ ๋น๋ถ์ด๋ ๋ น๋ง์ ํจ๋ชจ์ ์์ฉ์ ์ํด ๋ฐํจ ์์ฝ์ฌ๋ถ์ด ๋น๊ต์ ๋ฎ์ ๋ณ์ง๋๊ธฐ ์ฌ์ด ๋จ์ ์ด ์์ผ๋ฉฐ, ์๋ฃ ์ฑ๋ถ์์ ์ค๋ ํน์ ์ ํฅ๊ธฐ์ ๋ถ๋๋ฌ์ด ๋ง์ด ์๋ค. ๋ง๊ฑธ๋ฆฌ, ๊ณผ์ค์ฃผ(ํฌ๋์ฃผ, ์ฌ๊ณผ์ฃผ ๋ฑ), ๋งฅ์ฃผ, ์ฒญ์ฃผ ์ฆ๋ฅ์ฃผ: ์ฆ๋ฅ์ฃผ ์ฆ๋ฅ์ฃผ(่ธๆบ้ ) ์์กฐ์ฃผ๋ฅผ ๋ค์ ์ฆ๋ฅํ๋ฏ๋ก์จ ์์ฝ์ฌ๋ถ์ด ๋น๊ต์ ๋์ผ๋ฉฐ ์ฆ๋ฅ๊ณผ์ ์์ ๋ถ์๋ฌผ์ ๋๋ถ๋ถ ์ ๊ฑฐํ๋ค. ๋ง์๊ณ ๋ํ ์์กฐ์ฃผ์ ๋นํด ์์ทจ๊ฐ ๋ํ ๊ฒ๋ ์ด๋๋ฌธ์ด๋ค. ์์ธ์ ์ฆ๋ฅํ ๋ธ๋๋, ๊ณก์ฃผ๋ฅผ ์ฆ๋ฅํ ์์ฃผ, ๋ณด๋์นด, ๊ณ ๋์ฃผ, ๋งฅ์ฃผ๋ฅผ ์ฆ๋ฅํ ์์คํค, ์ฌํ์์์ฃผ๋ฅผ ์ฆ๋ฅํ ๋ผ ๋ฑ์ด ์ฆ๋ฅ์ฃผ์ ์ํ๋ฉฐ ์ด๋ฐ์๋ ์ ์ธ์ฅ์ฃผ๋ฅผ ์ฆ๋ฅํ ๋ฐํฌ๋ผ ๋ฐ์๋ฅผ ๋ค ์ ์๋ค. ์ฆ๋ฅ์ฃผ๋ ์์กฐ์ฃผ์ ๋ฌ๋ฆฌ ์ค๋ ๋ฌต์ผ๋ฉด ๋ฌต์์๋ก ์ฃผ์ง์ด ์ข์์ง๋ค. ์ฌ์ ์ฃผ(ๅ่ฃฝ้ ) ์์กฐ์ฃผ๋ ์ฆ๋ฅ์ฃผ ๋ฑ์ ๊ณผ์ค, ํฅ๋ฃ, ๊ฐ๋ฏธ๋ฃ, ์ฝ์ด ๋ฐ์๋ฅผ ์ฒจ๊ฐํ์ฌ ์นจ์ถ ๋๋ ์ฆ๋ฅํ์ฌ ๋ง๋ ์ ์ ๋งํ๋ค. ํผ์ฑ์ฃผ(ๆททๆ้ )๋ผ๊ณ ๋ ํ๋ ์ด ์ฃผ๋ฅ๋ ๊ฐ๋ฏธ(็ๅณ) ๋ฐ ํผ์ ์ฌ๋ฃ์์ ์ค๋ ๋ ํนํ ํฅ๊ธฐ๊ฐ ์๋ ๊ฒ์ด ํน์ง์ด๋ค. ์ฌ์ ์ฃผ๋ฅ์ ์ํ๋ ์ ๋ก๋ ๋งค์ค์ฃผ, ์ธ์ผ์ฃผ, ์ค๊ฐํผ์ฃผ ๋ฑ์ ๋ค ์ ์๋ค.Oil refining: Oil refiningazeotrope: azeotropeSlide38: Azeotrope Greek words for โboiling without changingโ No furthur separation by distillation High-boiling azeotrope HCl/water mixture 80%wt, boils at 108.6โ Low-boiling azeotrope EtOH/water 4%wt, boils at 78โLiquid-liquid phase diagrams: Liquid-liquid phase diagramsIodine in heptane/water: Iodine in heptane/water The two layers are then mixed by "vigorously flicking" the test tube with the fingers of the right hand. The purple color is the formation of I2 I2 is more soluble in heptane than water. http://www.sfu.ca/chemistry/students/courses/chem110-111/techniques/hept_iodine.htmPartially miscible liquids: Partially miscible liquids Partially miscible Do not mix together in all proportions Consists of two liquid phases Nitrobenzene/hexane Use lever ruleLever rule: Lever rule Lever rule Mixture of xA (Amount of phase of aโ)(lโ) = (amount of phase of aโ)(aโ)Critical solution temperature: Critical solution temperature Upper critical solution temperature (Tuc) Upper limit of temperature at which phase separation occurs Fully miscible when T> Tuc Because of thermal motion of molecules Gibbs energy of mixing is negative Lower c. s. Temperature(Tlc) Two components are more miscible because they form a weak complexWater(A) & 2-methyl-1-propanol(B): Water(A) & 2-methyl-1-propanol(B)Liquid-solid phase diagrams: Liquid-solid phase diagrams A system of Two metals (alloy) At xA = a1, molten liquid composition Liquid + A (pure solid) B richer solution b3 + pure solid A At xA = e, almost pure A + almost pure BEutectic composition: Eutectic composition Melting without change of composition Melting at the lowest temperature Solidifies at a single definite temperature Without gradually unloading one or other of the components from the liquid Microcrystal mixtures Example Solder 67 wt% Sn + 33 wt% Pb (Te = 183โ)Thermal analysis for eutectic point: Thermal analysis for eutectic pointUltrapurity and controlled impurity: Ultrapurity and controlled impurity Nine nine pure = 99.9999999%Wafer stepper for lithography: Wafer stepper for lithographyIngot pulling: Ingot pulling The base material for silicon is a sand. The sand is melted and refined to a high level of purity. An ingot is drawn from molten pure silicon in a crucible. This ingot starts by dipping a seed crystal in the melt and pulling it back at a controlled speed and temperature profile. The resulting cylindrical ingot has the single crystal structure required to manufacture active devices.Zone refining: Zone refiningexercises: exercises 6-4, 6-5, 6-16, 6-18, 6-27References: References http://www.whfreeman.com/ECHEM/INDEX.HTML http://www.schaft.org/eri/people.html http://cwx.prenhall.com/bookbind/pubbooks/hillchem3/medialib/media_portfolio/17.html Hillโs general chemistry http://www.personal.psu.edu/ruc114/egee101.html Oil refining http://www.theodoregray.com/PeriodicTable/Elements/Solid/index.s7.html Various elements http://www.ami.ac.uk/courses/ami4019_bim/u02/index.asp Wafer processingReferences: References http://fox.rollins.edu/~tlairson/ecom/ E-commerce lecture http://www.fbh-berlin.de/english/pres/pres_3.html stepperCreative Commons: Creative Commons Attribution-NonCommercial-ShareAlike 2.0 You are free: to copy, distribute, display, and perform the work to make derivative works Under the following conditions: Attribution. 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Edit Comment Close Premium member Presentation Transcript The properties of mixtures: The properties of mixtures Yongsik Lee March 2005Thermodynamic description of mixtures: Thermodynamic description of mixtures Yongsik LeePartial molar properties: Partial molar properties Definition Contribution (per mole) that a substance makes to an overall property of a mixture Example Partial molar volume (VJ) Partial molar Gibbs energy (GJ)Partial molar volume: Partial molar volume Example : VJ Water/ethanol mixture What is the total volume of a mixture of 50.0 g of ethanol and 50.0 g of water at 25โ? 1 mol of water + pure water = 18 cm3 1 mol of water + pure ethanol = ?Partial molar volume (VJ): Partial molar volume (VJ) Water/ethanol mixture VJ V = nAVA + nBVB 1 mol of water + pure water = 18 cm3 1 mol of water + pure EtOH = 14 cm3 2.77 mol water + 1.09 mol EtOH Mole fraction X EtOH = 0.282 Partial molar Gibbs energy: Partial molar Gibbs energy Contribution of J to the total Gibbs energy of a mixture G = nAGA + nBGB Chemical potential (ฮผ) Partial molar Gibbs energy G = nAฮผ A + nBฮผ BVariation of chemical potential: Variation of chemical potential For a perfect gas, G(Pf)-G(Pi)=nRT ln(Pf/Pi) Gm(Pf) = Gm(Pi) + RT ln(Pf/Pi) Set Pf=P and Pi=P°(the standard pressure, 1 bar) Gm(P) = Gm(P°) + RT ln(P/P°) For a mixture of perfect gases, Gm(P) = Gm(P°) + RT ln(P/P°) ฮผJ = ฮผJ° + RT ln(PJ/P°) ฮผJ = ฮผJ° + RT lnPJ ฮผJ° = Standard chemical potential of the gas JSpontaneous mixing: Spontaneous mixing All gases mix spontaneously Gibbs energy of mixing (ฮGmix) < 0 nA, p, T nB, p, T nA+ nB, p, TGibbs energy of mixing: Gibbs energy of mixing ฮGmix = Gf - Gi Gi = nAฮผ A + nBฮผ B = nA(ฮผA° + RT ln p) + nB(ฮผB° + RT ln p) Gf= nA(ฮผA° + RT ln xAp) + nB(ฮผB° + RT ln xBp) consider partial pressure for A and B ฮGmix = nA(RT ln xA) + nB(RT ln xB) = nRT[xAln xA + xBln xB] (ฮGmix) < 0Entropy of mixing: Entropy of mixing ฮGmix = nRT[xAln xA + xBln xB] With ฮG = ฮH - T ฮS ฮH =0 then ฮSmix = -nR[xAln xA + xBln xB] The increase in entropy of the system is the driving force of the mixing!Raoultโs law: Raoultโs law Chemical potential of a solute Partial vapor pressure(pJ) of each component in the mixture Francois Raoult (1830-1901)Raoultโs Law: Raoultโs Law pJ = xJpJ* The partial vapor pressure of a substance(pJ) in a mixture is proportional to its mole fraction(xJ) in the solution and its vapor pressure when pure(pJ*) Limiting law ([J]โ0)Molecular origin of Raoultโs law: Molecular origin of Raoultโs lawIdeal solution: Ideal solution Definition A hypothetical solution That obeys Raoultโs law throughout the composition range from pure A to pure B No mixture is perfectly ideal! (deviations)Real solution vs. ideal solution: Real solution vs. ideal solutionIdeal dilute solution: Ideal dilute solution Henryโs law pB=xBKB KB= Henryโs law constant Only at low [B] Ideal-dilute solution Solute B obeys HenryโsReal solution: Real solution Activity(aJ) = effective concentration ฮผJ = ฮผJ° + RT ln aJ Always true at any concentration For ideal solution, aJ = xJ For ideal-dilute solution, aA = ฮณAxA, aB = ฮณB[B], Activity coefficient ฮณA โ1 as xA โ1 ; ฮณB โ1 as [B] โ0 For a pure liquid or solid, a=1 Colligative properties: Colligative properties Yongsik LeeColligative properties: Colligative properties Definition โDepending on the collectionโ Depending on the number not the nature Chemical potential equilibrium Examples Boiling point, freezing point modification Osmosis, osmotic pressureModification of bp and fp: Modification of bp and fpCondition of solute: Condition of solute ์ฉ์ง์ ์กฐ๊ฑด Solute is not volatile No concentration to the vapor phase Solute does not dissolve in solid solvent ฮTb = Kb b(B) Ebullioscopic constant ฮTf = Kf b(B) Cryoscopic constantosmosis: osmosisOsmotic Pressure: Macromolecule is uncharged Macromolecule can not pass through the membrane Solvent flows from right to left, diluting the macromolecular solโn As the dilution takes place, the solutionn vol. increases and the level in the capillary rises Osmotic PressureOsmotic pressure: Osmotic pressureosmosis: osmosis movement of a solvent through a semipermeable membran (๋ฐํฌ๋ง) into a solution of higher solute concentration to equalize the concentrations of solute on the two sides of the membrane Osmotic pressure (ฮ )Jacobus H. van 't Hoff (1852-1911) Nobel Prize 1901: Jacobus H. van 't Hoff (1852-1911) Nobel Prize 1901 The first nobel prize in chemistryVanโt Hoff equation: Vanโt Hoff equation At Equilibrium ฮผ(solvent in the solution, p+ฮ ) = ฮผ(pure solvent, p) Vanโt Hoff equation ฮผ*(pure solvent, p)= ฮผ(xA solvent, p+ฮ ) ฮผ*(pure solvent, p)= ฮผ*(p+ฮ ) + RT ln xA ฮผ*(pure solvent, p)= ฮผ*(p) + VAฮp + RT ln xA 0 = VAฮp + RT ln xA VAฮ = RTxB Useful for Molecular weight determination Macromolecules โ MALDIVanโt Hoff Coefficient: Vanโt Hoff Coefficient Vanโt Hoff ๊ณ์(i) ์ฉ์ก์ ์๋ ์ ์์ ๋ชฐ ์์ ์ฉ์ก์ ๋ น์ ์๋ ์ฉ์ง์ ๋ชฐ ์ ๋น์จ ์ค์ ๊ฐ๊ณผ ์ด๋ก ๊ฐ์ด ๋ค๋ฅธ ์ด์ ์ด์จ๋ค์ด ์ด์จ์์ผ๋ก ํ๋ ์ ํ๋์ด ํฐ ์ด์จ์ ๊ฒฝ์ฐ ๋๋๋ฌ์ง๋ค ฮT = imKPhase diagrams of mixtures: Phase diagrams of mixtures Yongsik Lee 2005. 4. 7Phase Diagram: Phase Diagram ๋ฌผ์ง์ ์์ ์ด๋(phase diagram) ๋ฌผ์ง์ ์จ๋๋ฅผ ์ผ์ ํ๊ฒ ํ๊ณ ์๋ ฅ์ ๋ณํ์ํค๋ฉด ์ด๋ค ํน์ ํ ์๋ ฅ์์ ๋ฌผ์ง์ ๋ ์ ์ฌ์ด์ ์ ์ด(phase transition)๊ฐ ์ผ์ด๋๊ฒ ๋๋ค. ์ด ๊ณผ์ ์ ๋ง์ ๋ค๋ฅธ ์จ๋์์ ๋ํ์ดํ๋ฉด ํํ๊ณก์ ์ด ์์ฑ๋๋ค. ์์ ์ด๋์ ๊ตฌ์ฑ ๊ฐ๋ก์ถ์ ์จ๋, ์ธ๋ก์ถ์ ์๋ ฅ์ ํ์ํ๊ณ ์ฃผ์ด์ง ์จ๋์ ์๋ ฅ์์ ๊ฐ์ฅ ์์ ๋ ์์ ํ์ํ๋ค.Mixtures of volatile liquids: Mixtures of volatile liquids Temp(T)-composition(xA) diagram Vapor in equilibrium is also a mixture of two Composition is different (tie line) Tie line A line joining two phases that are in equilibrium with each otherFractional distillation: Fractional distillationDistiller: Distiller ์ ์ ๋ณดํต ์ ์กฐ๋ฐฉ๋ฒ์ ๋ฐ๋ผ ์ธ ๊ฐ์ง๋ก ๋ถ๋ฅ๋๋ค. ์์กฐ์ฃผ ์ฆ๋ฅ์ฃผ ์ฌ์ ์ฃผ(ํผ์ฑ์ฃผ) ์์กฐ์ฃผ(้้ ้ )- ๋ฐํจ์ฃผ ๊ณผ์ค์ด๋ ๊ณก๋ฅ ๋ฑ์ ํจ์ ๋ ๋น๋ถ์ด๋ ๋ น๋ง์ ํจ๋ชจ์ ์์ฉ์ ์ํด ๋ฐํจ ์์ฝ์ฌ๋ถ์ด ๋น๊ต์ ๋ฎ์ ๋ณ์ง๋๊ธฐ ์ฌ์ด ๋จ์ ์ด ์์ผ๋ฉฐ, ์๋ฃ ์ฑ๋ถ์์ ์ค๋ ํน์ ์ ํฅ๊ธฐ์ ๋ถ๋๋ฌ์ด ๋ง์ด ์๋ค. ๋ง๊ฑธ๋ฆฌ, ๊ณผ์ค์ฃผ(ํฌ๋์ฃผ, ์ฌ๊ณผ์ฃผ ๋ฑ), ๋งฅ์ฃผ, ์ฒญ์ฃผ ์ฆ๋ฅ์ฃผ: ์ฆ๋ฅ์ฃผ ์ฆ๋ฅ์ฃผ(่ธๆบ้ ) ์์กฐ์ฃผ๋ฅผ ๋ค์ ์ฆ๋ฅํ๋ฏ๋ก์จ ์์ฝ์ฌ๋ถ์ด ๋น๊ต์ ๋์ผ๋ฉฐ ์ฆ๋ฅ๊ณผ์ ์์ ๋ถ์๋ฌผ์ ๋๋ถ๋ถ ์ ๊ฑฐํ๋ค. ๋ง์๊ณ ๋ํ ์์กฐ์ฃผ์ ๋นํด ์์ทจ๊ฐ ๋ํ ๊ฒ๋ ์ด๋๋ฌธ์ด๋ค. ์์ธ์ ์ฆ๋ฅํ ๋ธ๋๋, ๊ณก์ฃผ๋ฅผ ์ฆ๋ฅํ ์์ฃผ, ๋ณด๋์นด, ๊ณ ๋์ฃผ, ๋งฅ์ฃผ๋ฅผ ์ฆ๋ฅํ ์์คํค, ์ฌํ์์์ฃผ๋ฅผ ์ฆ๋ฅํ ๋ผ ๋ฑ์ด ์ฆ๋ฅ์ฃผ์ ์ํ๋ฉฐ ์ด๋ฐ์๋ ์ ์ธ์ฅ์ฃผ๋ฅผ ์ฆ๋ฅํ ๋ฐํฌ๋ผ ๋ฐ์๋ฅผ ๋ค ์ ์๋ค. ์ฆ๋ฅ์ฃผ๋ ์์กฐ์ฃผ์ ๋ฌ๋ฆฌ ์ค๋ ๋ฌต์ผ๋ฉด ๋ฌต์์๋ก ์ฃผ์ง์ด ์ข์์ง๋ค. ์ฌ์ ์ฃผ(ๅ่ฃฝ้ ) ์์กฐ์ฃผ๋ ์ฆ๋ฅ์ฃผ ๋ฑ์ ๊ณผ์ค, ํฅ๋ฃ, ๊ฐ๋ฏธ๋ฃ, ์ฝ์ด ๋ฐ์๋ฅผ ์ฒจ๊ฐํ์ฌ ์นจ์ถ ๋๋ ์ฆ๋ฅํ์ฌ ๋ง๋ ์ ์ ๋งํ๋ค. ํผ์ฑ์ฃผ(ๆททๆ้ )๋ผ๊ณ ๋ ํ๋ ์ด ์ฃผ๋ฅ๋ ๊ฐ๋ฏธ(็ๅณ) ๋ฐ ํผ์ ์ฌ๋ฃ์์ ์ค๋ ๋ ํนํ ํฅ๊ธฐ๊ฐ ์๋ ๊ฒ์ด ํน์ง์ด๋ค. ์ฌ์ ์ฃผ๋ฅ์ ์ํ๋ ์ ๋ก๋ ๋งค์ค์ฃผ, ์ธ์ผ์ฃผ, ์ค๊ฐํผ์ฃผ ๋ฑ์ ๋ค ์ ์๋ค.Oil refining: Oil refiningazeotrope: azeotropeSlide38: Azeotrope Greek words for โboiling without changingโ No furthur separation by distillation High-boiling azeotrope HCl/water mixture 80%wt, boils at 108.6โ Low-boiling azeotrope EtOH/water 4%wt, boils at 78โLiquid-liquid phase diagrams: Liquid-liquid phase diagramsIodine in heptane/water: Iodine in heptane/water The two layers are then mixed by "vigorously flicking" the test tube with the fingers of the right hand. The purple color is the formation of I2 I2 is more soluble in heptane than water. http://www.sfu.ca/chemistry/students/courses/chem110-111/techniques/hept_iodine.htmPartially miscible liquids: Partially miscible liquids Partially miscible Do not mix together in all proportions Consists of two liquid phases Nitrobenzene/hexane Use lever ruleLever rule: Lever rule Lever rule Mixture of xA (Amount of phase of aโ)(lโ) = (amount of phase of aโ)(aโ)Critical solution temperature: Critical solution temperature Upper critical solution temperature (Tuc) Upper limit of temperature at which phase separation occurs Fully miscible when T> Tuc Because of thermal motion of molecules Gibbs energy of mixing is negative Lower c. s. Temperature(Tlc) Two components are more miscible because they form a weak complexWater(A) & 2-methyl-1-propanol(B): Water(A) & 2-methyl-1-propanol(B)Liquid-solid phase diagrams: Liquid-solid phase diagrams A system of Two metals (alloy) At xA = a1, molten liquid composition Liquid + A (pure solid) B richer solution b3 + pure solid A At xA = e, almost pure A + almost pure BEutectic composition: Eutectic composition Melting without change of composition Melting at the lowest temperature Solidifies at a single definite temperature Without gradually unloading one or other of the components from the liquid Microcrystal mixtures Example Solder 67 wt% Sn + 33 wt% Pb (Te = 183โ)Thermal analysis for eutectic point: Thermal analysis for eutectic pointUltrapurity and controlled impurity: Ultrapurity and controlled impurity Nine nine pure = 99.9999999%Wafer stepper for lithography: Wafer stepper for lithographyIngot pulling: Ingot pulling The base material for silicon is a sand. The sand is melted and refined to a high level of purity. An ingot is drawn from molten pure silicon in a crucible. This ingot starts by dipping a seed crystal in the melt and pulling it back at a controlled speed and temperature profile. The resulting cylindrical ingot has the single crystal structure required to manufacture active devices.Zone refining: Zone refiningexercises: exercises 6-4, 6-5, 6-16, 6-18, 6-27References: References http://www.whfreeman.com/ECHEM/INDEX.HTML http://www.schaft.org/eri/people.html http://cwx.prenhall.com/bookbind/pubbooks/hillchem3/medialib/media_portfolio/17.html Hillโs general chemistry http://www.personal.psu.edu/ruc114/egee101.html Oil refining http://www.theodoregray.com/PeriodicTable/Elements/Solid/index.s7.html Various elements http://www.ami.ac.uk/courses/ami4019_bim/u02/index.asp Wafer processingReferences: References http://fox.rollins.edu/~tlairson/ecom/ E-commerce lecture http://www.fbh-berlin.de/english/pres/pres_3.html stepperCreative Commons: Creative Commons Attribution-NonCommercial-ShareAlike 2.0 You are free: to copy, distribute, display, and perform the work to make derivative works Under the following conditions: Attribution. 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