John C. Kotz Paul M. Treichel John Townsend http://academic.cengage.com/kotz Chapter 14 Solutions and Their Behavior John C. Kotz • State University of New York, College at Oneonta Important – Read Before Using Slides in Class Instructor: This PowerPoint presentation contains photos and figures from the text, as well as selected animations and videos. For animations and videos to run properly, we recommend that you run this PowerPoint presentation from the PowerLecture disc inserted in your computer. Also, for the mathematical symbols to display properly, you must install the supplied font called “Symb_chm,” supplied as a cross-platform TrueType font in the “Font_for_Lectures” folder in the "Media" folder on this disc. If you prefer to customize the presentation or run it without the PowerLecture disc inserted, the animations and videos will only run properly if you also copy the associated animation and video files for each chapter onto your computer. Follow these steps: 1. Go to the disc drive directory containing the PowerLecture disc, and then to the “Media” folder, and then to the “PowerPoint_Lectures” folder. 2. In the “PowerPoint_Lectures” folder, copy the entire chapter folder to your computer. Chapter folders are named “chapter1”, “chapter2”, etc. Each chapter folder contains the PowerPoint Lecture file as well as the animation and video files. For assistance with installing the fonts or copying the animations and video files, please visit our Technical Support at http://academic.cengage.com/support or call (800) 423-0563. Thank you. 3 Solutions Chapter 14 PLAY MOVIE Why does a raw egg swell or shrink when placed in different solutions? © 2009 Brooks/Cole - Cengage Some Definitions 4 A solution is a One constituent is usually HOMOGENEOUS mixture regarded as the SOLVENT of 2 or more substances and the others as SOLUTES. in a single phase. © 2009 Brooks/Cole - Cengage Definitions Solutions can be classified as saturated or unsaturated. A saturated solution contains the maximum quantity of solute that dissolves at that temperature. © 2009 Brooks/Cole - Cengage PLAY MOVIE 5 Definitions Solutions can be classified as unsaturated or saturated. A saturated solution contains the maximum quantity of solute that dissolves at that temperature. SUPERSATURATED SOLUTIONS contain more than is possible and are unstable. © 2009 Brooks/Cole - Cengage 6 PLAY MOVIE 7 Dissolving An Ionic Solid See Active Figure 14.9 © 2009 Brooks/Cole - Cengage Energetics of the Solution Process See Figure 14.8 © 2009 Brooks/Cole - Cengage 8 Energetics of the Solution Process PLAY MOVIE © 2009 Brooks/Cole - Cengage If the enthalpy of formation of the solution is more negative that that of the solvent and solute, the enthalpy of solution is negative. The solution process is exothermic! 9 10 Supersaturated Sodium Acetate PLAY MOVIE © 2009 Brooks/Cole - Cengage • One application of a supersaturated solution is the sodium acetate “heat pack.” • Sodium acetate has an ENDOthermic heat of solution. 11 Supersaturated Sodium Acetate Sodium acetate has an ENDOthermic heat of solution. NaCH3CO2 (s) + heat f Na+(aq) + CH3CO2-(aq) Therefore, formation of solid sodium acetate from its ions is EXOTHERMIC. Na+(aq) + CH3CO2-(aq) f NaCH3CO2 (s) + heat © 2009 Brooks/Cole - Cengage Colligative Properties On adding a solute to a solvent, the props. of the solvent are modified. • Vapor pressure decreases • Melting point decreases • Boiling point increases • Osmosis is possible (osmotic pressure) These changes are called COLLIGATIVE PROPERTIES. They depend only on the NUMBER of solute particles relative to solvent particles, not on the KIND of solute particles. © 2009 Brooks/Cole - Cengage 12 Concentration Units An IDEAL SOLUTION is one where the properties depend only on the concentration of solute. Need conc. units to tell us the number of solute particles per solvent particle. The unit “molarity” does not do this! © 2009 Brooks/Cole - Cengage 13 Concentration Units MOLE FRACTION, X For a mixture of A, B, and C mol A X A mol fraction A = mol A + mol B + mol C MOLALITY, m mol solute molality of solute (m) = kilograms solvent WEIGHT % = grams solute per 100 g solution © 2009 Brooks/Cole - Cengage 14 Calculating Concentrations Dissolve 62.1 g (1.00 mol) of ethylene glycol in 250. g of H2O. Calculate mol fraction, molality, and weight % of glycol. © 2009 Brooks/Cole - Cengage 15 Calculating Concentrations Dissolve 62.1 g (1.00 mol) of ethylene glycol in 250. g of H2O. Calculate X, m, and % of glycol. 250. g H2O = 13.9 mol 1.00 mol glycol Xglycol = 1.00 mol glycol + 13.9 mol H2O X glycol = 0.0672 © 2009 Brooks/Cole - Cengage 16 Calculating Concentrations Dissolve 62.1 g (1.00 mol) of ethylene glycol in 250. g of H2O. Calculate X, m, and % of glycol. Calculate molality 1.00 mol glycol conc (molality) = 4.00 molal 0.250 kg H2O Calculate weight % 62.1 g % glycol = x 100% = 19.9% 62.1 g + 250. g © 2009 Brooks/Cole - Cengage 17 Dissolving Gases & Henry’s Law PLAY MOVIE Gas solubility (mol/L) = kH · Pgas kH for O2 = 1.66 x 10-6 M/mmHg When Pgas drops, solubility drops. © 2009 Brooks/Cole - Cengage 18 Understanding Colligative Properties To understand colligative properties, study the LIQUID-VAPOR EQUILIBRIUM for a solution. © 2009 Brooks/Cole - Cengage 19 Understanding Colligative Properties To understand colligative properties, study the LIQUID-VAPOR EQUILIBRIUM for a solution. PLAY MOVIE © 2009 Brooks/Cole - Cengage PLAY MOVIE 20 Understanding Colligative Properties VP of H2O over a solution depends on the number of H2O molecules per solute molecule. Psolvent proportional to Xsolvent Psolvent = Xsolvent · Posolvent VP of solvent over solution = (Mol frac solvent)•(VP pure solvent) RAOULT’S LAW © 2009 Brooks/Cole - Cengage 21 Raoult’s Law An ideal solution is one that obeys Raoult’s law. PA = XA · PoA Because mole fraction of solvent, XA, is always less than 1, then PA is always less than PoA. The vapor pressure of solvent over a solution is always LOWERED! © 2009 Brooks/Cole - Cengage 22 Raoult’s Law Assume the solution containing 62.1 g of glycol in 250. g of water is ideal. What is the vapor pressure of water over the solution at 30 oC? (The VP of pure H2O is 31.8 mm Hg; see App. E.) Solution Xglycol = 0.0672 and so Xwater = ? Because Xglycol + Xwater = 1 Xwater = 1.000 - 0.0672 = 0.9328 Pwater = Xwater · Powater = (0.9382)(31.8 mm Hg) Pwater = 29.7 mm Hg © 2009 Brooks/Cole - Cengage 23 Raoult’s Law For a 2-component system where A is the solvent and B is the solute ∆PA = VP lowering = XBPoA VP lowering is proportional to mol frac solute! For very dilute solutions, ∆PA = K·molalityB where K is a proportionality constant. This helps explain changes in melting and boiling points. © 2009 Brooks/Cole - Cengage 24 Changes in Freezing and Boiling Points of Solvent VP Pure solvent 1 atm VP solvent after adding solute P BP solution BP pure solvent © 2009 Brooks/Cole - Cengage T See Figure 14.13 25 26 Vapor Pressure Lowering See Figure 14.13 © 2009 Brooks/Cole - Cengage The boiling point of a solution is higher than that of the pure solvent. PLAY MOVIE © 2009 Brooks/Cole - Cengage 27 Elevation of Boiling Point Elevation in BP = ∆TBP = KBP·m (where KBP is characteristic of solvent) VP Pure solvent 1 atm VP solvent after adding solute P BP solution BP pure solvent © 2009 Brooks/Cole - Cengage T 28 Change in Boiling Point Dissolve 62.1 g of glycol (1.00 mol) in 250. g of water. What is the BP of the solution? KBP = +0.512 oC/molal for water (see Table 14.3). Solution 1. Calculate solution molality = 4.00 m 2. ∆TBP = KBP · m ∆TBP = +0.512 oC/molal (4.00 molal) ∆TBP = +2.05 oC BP = 102.05 oC © 2009 Brooks/Cole - Cengage 29 Change in Freezing Point Pure water Ethylene glycol/water solution PLAY MOVIE PLAY MOVIE The freezing point of a solution is LOWER than that of the pure solvent. FP depression = ∆TFP = KFP·m © 2009 Brooks/Cole - Cengage 30 31 Lowering the Freezing Point Water with and without antifreeze © 2009 Brooks/Cole - Cengage When a solution freezes, the solid phase is pure water. The solution becomes more concentrated. Freezing Point Depression Calculate the FP of a 4.00 molal glycol/water solution. KFP = -1.86 oC/molal (Table 14.3) Solution ∆TFP = KFP · m = (-1.86 oC/molal)(4.00 m) ∆TFP = -7.44 oC Recall that ∆TBP = +2.05 ˚C for this solution. © 2009 Brooks/Cole - Cengage 32 Freezing Point Depression How much NaCl must be dissolved in 4.00 kg of water to lower FP to -10.00 oC?. Solution Calc. required molality ∆TFP = KFP · m -10.00 oC = (-1.86 oC/molal)(Conc) Conc = 5.38 molal © 2009 Brooks/Cole - Cengage 33 Freezing Point Depression How much NaCl must be dissolved in 4.00 kg of water to lower FP to -10.00 oC?. Solution Conc req’d = 5.38 molal This means we need 5.38 mol of dissolved particles per kg of solvent. Recognize that m represents the total concentration of all dissolved particles. Recall that 1 mol NaCl(aq) f 1 mol Na+(aq) + 1 mol Cl-(aq) © 2009 Brooks/Cole - Cengage 34 Freezing Point Depression How much NaCl must be dissolved in 4.00 kg of water to lower FP to -10.00 oC?. Solution Conc req’d = 5.38 molal We need 5.38 mol of dissolved particles per kg of solvent. NaCl(aq) f Na+(aq) + Cl-(aq) To get 5.38 mol/kg of particles we need 5.38 mol / 2 = 2.69 mol NaCl / kg 2.69 mol NaCl / kg f 157 g NaCl / kg (157 g NaCl / kg)(4.00 kg) = 629 g NaCl © 2009 Brooks/Cole - Cengage 35 36 Boiling Point Elevation and Freezing Point Depression ∆T = K·m·i A generally useful equation i = van’t Hoff factor = number of particles produced per formula unit. Compound Theoretical Value of i glycol 1 NaCl 2 CaCl2 3 © 2009 Brooks/Cole - Cengage 37 Osmosis PLAY MOVIE Dissolving the shell in vinegar © 2009 Brooks/Cole - Cengage Egg in pure water Egg in corn syrup Osmosis The semipermeable membrane allows only the movement of solvent molecules. Solvent molecules move from pure solvent to solution in an attempt to make both have the same concentration of solute. Driving force is entropy © 2009 Brooks/Cole - Cengage 38 39 Process of Osmosis © 2009 Brooks/Cole - Cengage Osmotic Pressure, ∏ Equilibrium is reached when pressure — the OSMOTIC PRESSURE, ∏ — produced by extra Osmotic pressure solution counterbalances pressure of solvent molecules moving thru the membrane. ∏ = cRT (c is conc. in mol/L) © 2009 Brooks/Cole - Cengage 40 Osmosis PLAY MOVIE © 2009 Brooks/Cole - Cengage 41 PLAY MOVIE Osmosis at the Particulate Level See Figure 14.17 © 2009 Brooks/Cole - Cengage 42 43 Osmosis • Osmosis of solvent from one solution to another can continue until the solutions are ISOTONIC — they have the same concentration. © 2009 Brooks/Cole - Cengage 44 Osmosis and Living Cells © 2009 Brooks/Cole - Cengage Reverse Osmosis Water Desalination Water desalination plant in Tampa © 2009 Brooks/Cole - Cengage 45 Osmosis Calculating a Molar Mass Dissolve 35.0 g of hemoglobin in enough water to make 1.00 L of solution. ∏ measured to be 10.0 mm Hg at 25 ˚C. Calc. molar mass of hemoglobin. Solution (a) Calc. ∏ in atmospheres ∏ = (10.0 mmHg)(1 atm / 760 mmHg) = 0.0132 atm (b) Calc. concentration © 2009 Brooks/Cole - Cengage 46 Osmosis Calculating a Molar Mass Dissolve 35.0 g of hemoglobin in enough water to make 1.00 L of solution. ∏ measured to be 10.0 mm Hg at 25 ˚C. Calc. molar mass of hemoglobin. Solution (b) Calc. concentration from ∏ = cRT 0.0132 atm Conc = (0.0821 Lįatm/Kįmol)(298K) (c) Conc = 5.39 x 10-4 mol/L Calc. molar mass Molar mass = 35.0 g / 5.39 x 10-4 mol/L Molar mass = 65,100 g/mol © 2009 Brooks/Cole - Cengage 47