Presentation is loading. Please wait.

Presentation is loading. Please wait.

Lecture 314/10/06. Thermodynamics: study of energy and transformations Energy Kinetic energy Potential Energy.

Similar presentations


Presentation on theme: "Lecture 314/10/06. Thermodynamics: study of energy and transformations Energy Kinetic energy Potential Energy."— Presentation transcript:

1 Lecture 314/10/06

2 Thermodynamics: study of energy and transformations Energy Kinetic energy Potential Energy

3 Units 1 calorie (cal) 1 calorie (cal) = 4.184 Joule (J) Calorie (Cal)

4 1 st Law of Thermodynamics Law of conservation of energy Energy in the universe is conserved System vs. surroundings vs. universe Internal energy

5 Specific heat capacity (C) Quantity of energy to increase the temperature of 1 gram of a substance by 1 degree C (liquid water)= 4.184 J/g·K C (ice)= 2.06 J/g·K C (steam)= 1.84 J/g·K C (aluminum)= 0.902 J/g·K Molar heat capacity Quantity of energy that must be transferred to increase the temperature of 1 mole of a substance by 1 °C

6 Specific heat capacity (C) q = Cm∆T

7 Heat transfer q gained + q lost = 0 q gained = - q lost 55.0 g of iron at 99.8°C is plunged into 225 g of water at 21°C. What is the final temperature? C (iron) = 0.451 J/g-K

8 Example 59.8 J are required to change the temperature of 25.0 g of ethylene glycol by 1 K. What is the specific heat capacity of ethylene glycol?

9 Does drinking ice water cause you to lose weight? Does drinking ice cold coke?

10 Changes in state Temperature stays the same during changes of state Gas/Vapor Liquid Solid ENERGY q = mass x constant q = moles x constant

11 Change of state constant??? Depends on two things: Identity of substance Which states are changing

12 Solid/Liquid Heat of fusion Solid  Liquid Endothermic ice  Water (333 J/g or 6 KJ/mol) Heat of crystallization Liquid  Solid Exothermic Water  ice (- 333 J/g or - 6 KJ/mol)

13 Liquid/Gas Heat of vaporization Liquid  Gas Endothermic water  water vapor (40.7 KJ/mol) Heat of condensation Gas  Liquid Exothermic vapor  Water (- 40.7 KJ/mol)

14 Solid/Gas Heat of sublimation Solid  Gas Endothermic Heat of deposition Gas  Solid Exothermic

15 What is the minimum amount of ice at 0 °C that must be added to a 340 mL of water to cool it from 20.5°C to 0°C? q water + q ice = 0 C water m water ∆T water + m ice ∆H fus = 0 (4.184 J/K-g)(340 g)(0°C - 20.5°C) + (333 J/g)m ice = 0 m ice = 87.6 g

16 A rainstorm deposits 2.5 x 10 10 kg of rain. Calculate the quantity of thermal energy in joules transferred when this much rain forms. (∆H vap = - 44 KJ/mol) Exothermic or endothermic? q = 2.5 x 10 10 Kg x (10 3 g/kg) x (1 mol/18 g) x -44 KJ/mol q = -6.1 x 10 13 KJ Exothermic

17 1 st Law of Thermodynamics revisited ∆E = q + w Change in Energy content heat work

18 work (w) = - F x d w = - (P x A) x d w = - P∆V if ∆V = 0, then no work

19 State function property of a system whose value depends on the final and initial states, but not the path driving to Mt Washington route taken vs. altitude change ∆E is a state function q and w are not

20 Change in Enthalpy (∆H or q p ) equals the heat gained or lost at constant pressure ∆E = q p + w ∆E = ∆H + (-P∆V) ∆H = ∆E + P∆V

21 ∆E vs. ∆H Reactions that don’t involve gases 2KOH (aq) + H 2 SO 4 (aw)  K 2 SO 4 (aq) + 2H 2 O (l) ∆V ≈ 0, so ∆E ≈ ∆H Reactions in which the moles of gas does not change N 2 (g) + O 2 (g)  2NO (g) ∆V = 0, so ∆E = ∆H Reactions in which the moles of gas does change 2H 2 (g) + O 2 (g)  2H 2 O (g) ∆V > 0, but often P∆V << ∆H, thus ∆E ≈ ∆H

22 Enthalpy is an extensive property Magnitude is proportional to amount of reactants consumed H 2 (g) + ½ O 2 (g)  H 2 O (g) ∆H = -241.8 KJ 2H 2 (g) + O 2 (g)  2H 2 O (g) ∆H = -483.6 KJ Enthalpy change for a reaction is equal in magnitude (but opposite in sign) for a reverse reaction H 2 (g) + ½ O 2 (g)  H 2 O (g) ∆H = -241.8 KJ H 2 O (g)  H 2 (g) + ½ O 2 (g) ∆H = 241.8 KJ Enthalpy change for a reaction depends on the state of reactants and products H 2 O (l)  H 2 O (g) ∆H = 88 KJ

23 Constant pressure calorimetry (cofee cup calorimetry) heat lost = heat gained Measure change in temperature of water 10 g of Cu at 188 °C is added to 150 mL of water in a cofee cup calorimeter and the temperature of water changes from 25 °C to 26 °C. Determine the specific heat capacity of copper.

24 Bomb calorimetry Mainly for combustion experiments ∆V = 0 q rxn + q bomb + q water = 0 Often combine q bomb + q water into 1 calorimeter term with q cal = C cal ∆T combustion chamber

25 Bomb calorimeter math K & T: q rxn + q bomb + q water = 0 q rxn + C bomb ∆T + C water m water ∆T = 0 In the lab: q rxn + q calorimeter = 0 q calorimeter = q bomb + q water q rxn + C calorimeter ∆T = 0 empirically determined same value On the exam

26 Bond enthalpies

27 Enthalpies of formation

28 Hess’ Law

29 Example A hot plate is used to heat two 50-mL beakers at the same constant rate. One beaker contains 20.0 grams of graphite (C=0.79 J/g-K) and one contains 10 grams of ethanol (2.46 J/g-K). Which has a higher temperature after 3 minutes of heating?

30 Standard heat of reaction (∆H° rxn ) Same standard conditions as before: 1 atm for gas 1 M for aqueous solutions 298 K For pure substance – usually the most stable form of the substance at those conditions

31 Standard heat of formation (∆H° f ) Enthalpy change for the formation of a substance from its elements at standard state Na(s) + ½ Cl 2 (g)  NaCl (s) ∆H° f = -411.1 kJ Three points An element in its standard state has a ∆H° f = 0 ∆H° f = 0 for Na(s), but ∆H° f = 107.8 KJ/mol for Na(g) Most compounds have a negative ∆H° f formation reaction is not necessarily the one done in lab

32 Using ∆H° f to get ∆H° rxn 2 ways to look at the problem Calculate ∆H° rxn for: C 3 H 8 (g) + 5 O 2  3 CO 2 (g) + 4 H 2 O (l) Given: 3 C(s) + 4 H 2 (g)  C 3 H 8 (g) ∆H° f = -103.85 KJ/mol C(s) + O 2 (g)  CO 2 (g) ∆H° f = -393.5 KJ/mol O 2 (g) + 2 H 2 (g)  2H 2 O (l) ∆H° f = -285.8 KJ/mol

33 Using Hess’s Law and ∆H° f to get ∆H° rxn 1 st way: Hess’s Law C 3 H 8 (g) + 5 O 2  3 CO 2 (g) + 4 H 2 O (l) ∆H° rxn = ∆H 1 + ∆H 2 + ∆H 3 Reverse 1 st equation: C 3 H 8 (g)  3 C(s) + 4 H 2 (g) ∆H 1 = - ∆H° f = 103.85 KJ Multiply 2 nd equation by 3: 3C(s) + 3O 2 (g)  3CO 2 (g) ∆H 2 = 3x∆H° f = -1180.5 KJ Multiply 3 rd equation by 2: 2O 2 (g) + 4 H 2 (g)  4H 2 O (l) ∆H 2 = 2x∆H° f = -571.6 KJ ∆H° rxn = (103.85 KJ) + (-1180.5 KJ) + (-571.6 KJ) ∆H° rxn = -1648.25 KJ

34 Using ∆H° f to get ∆H° rxn 2 nd way C 3 H 8 (g) + 5 O 2  3 CO 2 (g) + 4 H 2 O (l) ∆H° rxn = Σn ∆H° f (products) - Σn ∆H° f (reactants) ∆H° rxn = [3x(-393.5 KJ/mol) + 2x(-285.8 KJ/mol)] – [(-103.85 KJ/mol) + 0] ∆H° rxn = [-1752.1 KJ] – [-103.85 KJ] ∆H° rxn = -1648.25 KJ

35 Spontaneity Some thought that ∆H could predict spontaneity Exothermic – spontaneous Endothermic – non-spontaneous Sounds great BUT some things spontaneous at ∆H > 0 Melting Dissolution Expansion of a gas into a vacuum Heat transfer Clearly enthalpy not the whole story

36 Entropy (Measurement of disorder) Related to number of microstates S = klnW ∆S universe = ∆S system + ∆S surroundings 2 nd Law of Thermodynamics Entropy of the universe increases with spontaneous reactions Reversible reactions ∆S universe = ∆S system + ∆S surroundings = 0 Can be restored to the original state by exactly reversing the change Each step is at equilibrium Irreversible reaction ∆S universe = ∆S system + ∆S surroundings > 0 Original state can not be restored by reversing path spontaneous

37 3 rd Law of thermodynamics S = O at O K S° - entropy gained by converting it from a perfect crystal at 0 K to standard state conditions ∆S° = ΣS°(products) - ΣS°(reactants)


Download ppt "Lecture 314/10/06. Thermodynamics: study of energy and transformations Energy Kinetic energy Potential Energy."

Similar presentations


Ads by Google