1 10/10/2011 Chem 105 Mon 10 Oct 2011 Announcements 1. Blackboard gradebook is combined for both 105 sections. For Keller (JWK) students, the entries labeled FH (Fenton Heirtzler) should be blank . 2. OWL reminder. All OWL sections that are due or past due may be worked on at any time. If a catastrophe happened and you could not complete an OWL section, GO AHEAD and work on it. 1. 2. 3. 4. Chapt 5: Thermochemistry: Kinds of energy Heat flow and heat measurement Specific heat and heat capacity Heating/cooling curves 2 10/10/2011 Chapt 5: Energy and Chemical Reactions Kinetic energy = motion Thermal energy - atoms vibrating or moving in gas, liquid, or even solid (slightly) Mechanical energy - macroscopic motion (baseball, car moving etc) Electrical energy – electrons moving in a wire (current) Sound energy - (really just #1) 3 10/10/2011 Chapt 6: Energy and Chemical Reactions Potential Energy = stored energy Chemical - Energy stored in compounds that can be released by a chemical reaction Electrostatic – separation of + and – charges released as charges come closer to each other. Gravitational – separation of macroscopic bodies 4 10/10/2011 Conservation of energy Physicists give us the First Law of Thermodynamics: “Total energy of the universe is constant”. For the rest of us, we know that energy is not “lost” - it flows from one form to another. sound Thermal energy Mechanical energy of flying parts Mechanical energy of speeding car 5 10/10/2011 Conservation of energy sound Thermal energy Mechanical energy of speaker parts electrical energy chemical energy of battery 6 10/10/2011 Conservation of energy electrical energy A hand-cranked version of this device was used in 1820 by James Joule to define the “Joule” energy unit. Mechanical energy of stirrer thermal energy of water (increased water temperature) 7 10/10/2011 Quantitative definitions 1 calorie (cal) = amount of energy required to raise the temperature of 1.00 g water by 1.00 °C. 1 kilocalorie (kcal) = amount of energy required to raise the temperature of 1.00 kg water by 1.00 °C. 1 calorie (cal) = 4.184 joule (J) The exact conversion of electrical to thermal energy was determined in the stirred-water experiment: 1 kilocalorie (kcal) = 4.184 kilojoule (kJ) 1 kJ = 0.2778 watt-hour (No need to memorize these numbers; they are in text and on exam reference sheets) 8 10/10/2011 Heat flows from higher temperature body to a lower temperature body by conduction. Warm object At high temps, atoms vibrate faster with larger amplitudes At thermal equilibrium, atomic motions the same & temps are equal. Cool object Motion is transferred to atoms in adjacent body. Heat flow 9 10/10/2011 Heat transfer by conduction animation (This works similarly for gases, liquids, or solids.) 10 10/10/2011 DEFINE q = heat transferred to an object - positive for heat gained - negative for heat lost Tinitial Tinitial Initial state Heat flow q Final state Tfinal Tf < Ti q<0 Tfinal Tf > Ti q>0 11 10/10/2011 q =Heat transferred to object (joules) “Joules per gram per Kelvin” Specific heat capacity (joule/gram ·K) q = m x C x (Tf – Ti) You DO need to remember this equation. Mass of the body (solid, liquid, or gas) (g) Final temperature (K or °C) Initial temperature (K or °C) q = m x C x (Tf – Ti) J g J J K g o oC gK g C 12 10/10/2011 Say we have a beaker of warm water 144 g water at 55.5 °C … and a 29.5-g sample of metal was taken from a boiling water bath and was placed in the first beaker of water. 13 10/10/2011 What will be the SIGN of qwater? 142 1. + 13 2. 1 4 2 3 3. Don’t know 1 1 14 27 40 53 66 79 92 105 118 131 144 157 170 183 196 2 3 4 5 6 7 8 9 10 11 12 13 10/10/2011 14 Answer = 1. + q is defined as “the heat that flows INTO an object”. If a hot object is placed in the water, then heat flows from the one with higher temperature to the one with lower temp. I.e. q > 0 for water. 15 10/10/2011 We can use temperature changes and the known specific heat capacity of water to identify the metal. 144 g water at 55.5 °C A 29.5-g metal block was taken from boiling water bath. Final temp = 57.8 °C For water: Tf – Ti = 57.8-55.5 °C = +2.3°C For metal: Tf – Ti = 57.8-100.0 °C = -42.2°C 16 10/10/2011 Perhaps this metal is magnesium. Note that the data allow calculation of specific heat to only 2 sig figs. q w m w C w ΔTw 144 g 4.184 J o o x 57.8 C 55.5 C o g C q w 1385.7 J Heat flow into water Heat flow into metal J/g-°C Mg 1.03 Al 0.897 Co 0.695 Fe 0.449 Cu 0.385 Au 0.129 We can solve for Cm We know these.. q m q w m m C m ΔTw - qw 1385.7J Cm m m ΔTw 29.5g 57.8o C 100.0o C Cm 1.113 J 1.1 J o o g C g C 17 10/10/2011 Heating/Cooling Curves Includes heat flow during phase changes: Evaporation (l g) Condensation (g l) Melting (s l) Freezing (l s) [Sublimation (s g) (chem 106)] 10/10/2011 18 Melting requires added heat. Changes of state occur at constant temperature. 10/10/2011 19 In boiling water, the vapor phase in bubbles of vapor is in equilibrium with the surrounding liquid phase. 20 10/10/2011 H2O (s) -----> H2O (l) ΔH = +5.99 kJ ΔHfus = +5.99 kJ/mol (“molar heat of fusion) = +333 J/g (“mass heat of fusion”) q = (mass)(heat of fusion) = mΔHfus 10/10/2011 Heating Curve for Water 21 22 10/10/2011 What quantity of heat is required to melt 500. g of ice at 0 oC, and heat the water to vapor at 100 oC? Given data: Heat of fusion of ice = 333 J/g Specific heat of water = 4.2 J/g•K Heat of vaporization = 2260 J/g +333 J/g +2260 J/g 23 10/10/2011 What quantity of heat is required to melt 500. g of ice (at 0 oC) and convert the water to vapor at 100 oC? q = (500. g)(333 J/g) = 1.67x 105 J 2.To warm water from 0oC to100 oC q = (500. g)(4.184 J/g•K)(100- 0)K = 2.092 x 105 J Temperature 1. To melt ice 100° 0° 3. To evaporate water at 100 oC q = (500. g)(2260 J/g) = 1.130 x 106 J 4. Total heat = sum = 1.506 x 106 J = 1.51 x 103 kJ Heat added 24 10/10/2011 One clicker question on heating/cooling curve 25 10/10/2011 Identify the line segment on the following diagram that would require the heat of vaporization and specific heat of liquid to calculate an energy change. Within this segment, you would need to use the specific heat capacity of WATER VAPOR. 42% 29% Within this segment, you would need to use ONLY the heat of vaporization of water, because there is NO temperature change. ... tF tA ... se gm en tD ... ne Li Li ne se gm en tG ... Li ne se gm en ... tE se gm en ne 5. Li 4. 13% 2% se gm en 3. 13% ne 2. Line segment E-F-G Line segment G-H-J Line segment D-E-F Line segment A-B-C Line segment F-G-H Li 1. 26 10/10/2011 OWL: Ch 5- 3b Homework: Phase Change Energetics 27 10/10/2011 Typical heating/cooling curve Evaporate Temp 2270 °C --> Condense 560 °C --> 232 °C --> 211 °C --> <Freeze Melt-> Heat flow in 28 10/10/2011 q = mCΔT=25.9 g x 0.243 J/g°C x -328°C q = -2064.3 J q = m ΔHfus = 25.9 g x 59.60 J/g Temp 560 °C --> 232 °C --> Freeze q = -1543.6 J (negative „cause its freezing) q = mCΔT=25.9 g x 0.2260 J/g°C x -21°C 211 °C --> q = -122.9 J Heat flow in qtot = - 3730 J 29 10/10/2011 Arrgghhh! - 3730 Don‟t forget to calculate “kJ” if it asks for it. “Removed” takes care of the sign of q. “q” IS negative, but “heat removed” cannot be negative. 30 10/10/2011 The End
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