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Temperature and Heat Energy: capacity to do work Kinetic energy (associated with motion) • Thermal, atoms, molecules, and ions are in motion – all matter has thermal energy • Mechanical, moving tennis ball, automobiles • Electrical, e − moving through a conductor • Sound, corresponds to compression and expansion of the space between molecules Potential energy (results from object’s position) • Gravitational, possessed by a ball held above floor • Electrostatic, associated with the separation of two dissimilar electrical charges • Chemical, burning coal ⇒ heat ⇒ work Thermodynamics: part of chemistry that deals with the energy changes involved in chemical rxns and changes in the physical state of substances. Thermochemistry: branch of Thermodynamics that deals with the evolution or absorption of energy as heat in chemical processes Work: w = F ⋅ d (recall F = ma) and the units of work are: kg m s −2 m = kg m2 s −2 Units of energy: Joule (J): kg m2 s −2 Calorie (cal): energy required to raise the temperature of 1.0 g of water by 1oC (from 14.5 to 15.5 oC) 1 cal = 4.184 J and 1 J = 0.2390 cal 1 kJ = 1000 J Nutritional calorie (Cal): energy available from food (1 Cal = 1000 cal) • The temperature of an object is a measure of its heat content and of its ability to transfer heat. We measure temperature by thermometers. HEAT IS NOT THE SAME AS TEMPERATURE! The more thermal energy a substance has, the greater the motion of atoms and molecules. 1 System: object or collection of objects under study Surroundings: everything outside the system can exchange energy with the system Thermal equilibrium: associated with directionality of heat transfer Calorimetry: measures flow of heat across boundaries Heat Capacity: measures the ability of the substance to pick up heat Heat capacity under constant pressure, Cp equals the amount of heat required to raise the q temperature of a system by 1oC (1 K) under constant pressure C P = (J K-1) ∆T CP q = ⇒ q = nc p ∆T (units: J K-1 mol-1) Molar hat capacity: cP = n n∆T Heat capacity under constant volume, Cv cP (J K-1 kg-1) q = mcs ∆T , m so cP = Mcs the molar heat capacity equals its specific heat capacity multiplied by its molar mass. Specific heat capacity: cs = Heat Transfer The quantity of heat transferred from or to an object depends on a) the quantity of material b) the size of temperature change c) the identity of the material gaining or losing heat See Table 10.1 How to find the temperature at thermal equilibrium amt of heat gained by the cooler body = amt of heat lost by the warmer body ∆ means: final - initial ∆T = + q = + heat transferred from surroundings to system ∆T = - q = - heat transferred from system to surroundings The heat content changes within a given system is zero. q1 + q2 + q3 + .... = 0 2 Example 55.0 g of a hot metal at 98.8oC is immersed in a beaker containing 225.0 g of cool water at 21.0oC. The final temperature is 23.1oC. Find the specific heat capacity of the metal and using Table 10.1 identify the metal. qwater + qmetal = 0 assuming no loss in the surroundings cs , water mH 2O (T f − Ti ) + cs , metal mmetal (T f − Ti ) = 0 (4.184 J K-1 g-1)(225.0 g)(296.3 – 294.2)K + cs ,metal (55.0 g)(296.3 – 371.95)K -1 -1 c s ,metal =0.469 J K g Fe is the closest in Table 10.1 Example Calculate the minimum amt of heat required to raise the temperature of 45 kg of granite by 15.0 K The heat absorbed by the granite is: q = mcs ∆T = ( 45 x103 g )(0.82 JK −1 g −1 )(15.0 K ) = 5.5 x105 J = 550kJ This is the minimum heat lost to surroundings as the rock heats up Now, Calculate the temperature change of 45.0 kg of water if it stores the same amt of thermal energy as the 45 kg of granite q 5.5 x105 J ∆T = = = 2.9 K cs m ( 4.184 JK −1 g −1 )( 45 x103 g ) Calorimeters Containers that have an interior space thermally insulated from the surroundings and a means to measure the temperature in the interior. The idea is to measure the temperature at thermal equilibrium among well-defined systems on the inside while preventing heat flow to or from outside q = CCAL ∆T part absorbs CCAL is the calorimeter constant and it tells us how much heat the interior Combustion (bomb) calorimeter confines the rxn into a fixed volume 3 Example A stryrofoam cup calorimeter is filled with 150.0 g of water at room temperature. Adding 1312 J of heat to the contents raises the interior temperature by 1.93 K. Calculate the calorimeter constant. Assume that the calorimeter does not leak heat. qwater + qCAL = 1312 J cs , water mH 2O ∆T + CCAL ∆T = 1312 J (4.184JK -1g -1)(150.0g)(1.93K)+CCAL(1.93K)=1312 J, and CCAL =52.2 JK-1 Now we dissolve some LiCl in the 150.0 g of water contained in the same calorimeter and we observe a temperature rise by 3.46 K. Calculate the amt of heat evolved in the dissolution of LiCl if the heat capacity and mass of LiCl are the same as of water. qsolution + qCAL + qrxn = 0 msolutioncs ,solution ∆T + CCAL ∆T + qrxn = 0 (150.0 g)(4.184 JK-1g-1)(3.46K) + (52.2 JK-1)(3.46K) + qrxn = 0 qrxn = - 2352 J, the dissolution rxn absorbs - 2352 J and the heat that evolves is the opposite of it, the reverse of absorbing it, + 2352 J EXAMPLE A manufacturer claims that its new dietetic dessert has fewer than 10 Calories per serving. To test the claim a chemist at the Department of Consumer Affairs places one serving in a bomb calorimeter and burns it in oxygen. The heat capacity of the calorimeter is 8.151 kJ K-1. The temperature increases 4.937oC. Is the manufacturer’s claim correct? qsample + qCAL = 0 ⇒ qCAL = − qsample qCAL = (8.151 kJ K-1)(4.937K)=40.24 kJ The heat released upon burning is gained by the calorimeter 10 Calories = (10 kcal)(4.184 kJ/kcal) = 41.84 kJ because 1 Calorie = 1 kcal 4 And 41.84 kJ > 40.24 kJ and the manufacturer is honest!!! EXAMPLE A chemist burns 0.865 g. of graphite in a new bomb calorimeter and CO2 is formed. If T increases 2.613 K and 393.5 kJ of heat is released per mole of graphite, what is the heat capacity of the calorimeter? qsample + qCAL = 0 (0.865g )( 1molC )( −393.5kJmol −1 ) + (2.613K )CCAL = 0 12.0 gC CCAL = 10.85kJK −1 Enthalpy The heat content of a substance under constant pressure, ∆H = qP. It is a state property. ∆H= Hf - Hi Enthalpy of a rxn is the change in enthalpy when a chemical rxn occurs ∆H= Hproducts – Hreactants CH4 (g) + 2 O2 (g) → CO2 (g) + 2 H2O (l) ∆Hrxn = qp < 0 exothermic N2 (g) + O2 (g) → 2 NO2 (g) ∆Hrxn = qp > 0 endothermic Enthalpies of rxn are written in association with a balanced equation CO (g) + ½ O2 (g) → CO2 (g) ∆Hrxn = - 283 kJ mol-1 2 CO (g) + O2 (g) → 2 CO2 (g) ∆Hrxn = - 566 kJ mol-1 EXAMPLE The major source of aluminum in the world is bauxite (mostly aluminum oxide). Its thermal decomposition can be represented by Al2O3 (s) → 2Al (s) + 3/2 O2 (g) ∆H rxn = 1676 kJ. How many grams of Al can be formed when 1.000 x 103 kJ of heat is transferred? (1.000 x 103 kJ) x (2 mol Al/1676 kJ)(26.98 g Al/1 mol Al) = 32.20 g Al Changes in State (Phase diagrams) Common phase transitions involve a transfer of heat between system and surroundings at constant temperature and pressure. 5 GAS Condensation Vaporization Sublimation Deposition LIQUID Fusion to m.p. Freezing SOLID EXAMPLE Heating of 500.0 g of water from -50oC to 200oC (Heat of fusion: 333 J/g, heat of vaporization: 2256 J/g). How much is needed for this process to occur? Step 1: warm water from -50oC to 0oC (cs of ice = 2.06 J K-1 g-1) q1 = cs,ice mice ∆T = (2.06 J K-1 g-1)(500.0 g)(273.15 – 223.15)K = 5.15 x 104 J Step 2: melt ice at 0oC q2 = (500.0 g)(333 J g-1) = 1.67 x 105 J Step 3: provide heat to raise the temperature of water from 0oC to 100oC q3 = cs , water mH 2O ∆T = (4.184 J K-1 g-1)(500.0 g)(373.15-273.15)K = 1.13 x 105 J Step 4: provide heat to evaporate water at 100oC q4 = (500.0 g)(2256 J g-1) = 1.13 x 106 J Step 5: raise the temperature of steam from 100oC to 200oC q5 = cs , steammwater ∆T = (1.92 J g-1)(500.0 g)(473.15-373.15)K = 9.60 x 104 J qTOTAL = q1 + q2 + q3 + q4 + q5 = 1.60 x 106 J = 1600 kJ 6 Determining the heat of a reaction You place 50.0 mL of 0.500 M NaOH in a coffee-cup calorimeter at 25.00oC and carefully add 25.0 mL of 0.500 M HCl, also at 25.00oC. After stirring, the final temperature is 27.21oC. Calculate qsoln (in J) and ∆Hrxn (in kJ/mol). (Assume the total volume is the sum of the individual volumes and that the final solution has the same density and specific heat capacity as water: d = 1.00 g/mL and c = 4.184 J/g K) 1. We find the mass of the solution msoln = (25.0 mL + 50.0 mL)(1.00 g/mL) = 75.0 g 2. We find ∆Tsoln, ∆Tsoln = 27.21oC - 25.00oC = 2.21 oC = 2.21K 3. Now we find qsoln qso ln = mso ln cs , so ln ∆Tso ln = (75.0 g )(4.184 JK −1 g −1 )(2.21K ) = 693J 4. Now we find ∆Hrxn We have a neutralization rxn HCl + NaOH → NaCl + H2O Let us write the net ionic equation: H+ (aq) + OH − (aq) → H2O (l) We find the moles of reactants and products n H + = (0.500mol / L)(0.0250L) = 0.0125 nOH − = (0.500mol / L)(0.050L) = 0.0250 ∴ H+ is the limiting reactant and only 0.0125 mol of H2O will be formed. The heat gained by water was lost from the rxn: qsoln = - qrxn ⇒ qrxn = - 693 J ∆H rxn = qrxn 1kJ − 693J 1kJ x = x = −55.4kJmol −1 molH 2O 1000 J 0.0125 1000 J ↑(to get the units requested) ENTHALPY CHANGES ACCOMPANY CHEMICAL REACTIONS 7 Summary of the relationship between amount (mol) of substance and the heat (kJ) transferred during a reaction. 8