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Thermochemistry

Thermochemistry. Chapter 6. Overview. Introduce the nature of energy and the general topics related to energy problems. Familiarize with the experimental procedures for measuring heats of reactions. Hess’s law and its applications based on enthalpies.

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Thermochemistry

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  1. Thermochemistry Chapter 6

  2. Overview • Introduce the nature of energy and the general topics related to energy problems. • Familiarize with the experimental procedures for measuring heats of reactions. • Hess’s law and its applications based on enthalpies. • Read the present and new sources of energy.

  3. Energyis the capacity to do work or produce heat • Thermal energy is the energy associated with the random motion of atoms and molecules • Chemical energy is the energy stored within the bonds of chemical substances • Nuclear energy is the energy stored within the collection of neutrons and protons in the atom • Electrical energy is the energy associated with the flow of electrons • Potential energy is the energy available by virtue of an object’s position

  4. Law of Conservation of Energy Energy can be converted from one form to another but can neither be created nor destroyed. (Euniverse is constant)

  5. The Two Types of Energy Potential:due to position or composition - can be converted to work (water before falling from dam, gasoline, etc.) Kinetic:due to motion of the object (water falling and doing work , gasoline burning and driving engine, etc.) KE = 1/2 mv2 (m = mass, v = velocity)

  6. Figure 6.1: (a) In the initial positions, ball A has a higher potential energy than ball B. (b) After A has rolled down the hill, the potential energy lost by A has been converted to random motions of the components of the hill (frictional heating) and to the increase in the potential energy of B.

  7. Total Energy = (PE)A + (KE)B + frictional heat

  8. Energy is a State Function Depends only on the present state of the system - not how it arrived there. It is independent of pathway. Internal Energy or Total Energy DE, Enthalpy DH, V, P, T are State Functions Heat and Work are not state functions

  9. Thermodynamics State functions are properties that are determined by the state of the system, regardless of how that condition was achieved. energy , pressure, volume, temperature Potential energy of hiker 1 and hiker 2 is the same even though they took different paths.

  10. Temperature v. Heat Temperature reflects random motionsof particles, therefore related to kinetic energy of the system. Heat involves a transfer of energybetween 2 objects due to a temperature difference

  11. Temperature = Thermal Energy 900C 400C Energy Changes in Chemical Reactions Heat is the transfer of thermal energy between two bodies that are at different temperatures. Temperature is a measure of the thermal energy. greater thermal energy

  12. Thermochemistry is the study of heat change in chemical reactions. SURROUNDINGS SYSTEM The system is the specific part of the universe that is of interest in the study. open closed isolated Exchange: mass & energy energy nothing

  13. System and Surroundings System: That on which we focus attention Surroundings: Everything else in the universe Universe = System + Surroundings

  14. Exo and Endothermic Heat exchange accompanies chemical reactions. Exothermic: Heat flows out of the system (to the surroundings). Endothermic: Heat flows into the system (from the surroundings).

  15. 2H2(g) + O2(g) 2H2O (l) + energy H2O (g) H2O (l) + energy energy + 2HgO (s) 2Hg (l) + O2(g) energy + H2O (s) H2O (l) Exothermic process is any process that gives off heat – transfers thermal energy from the system to the surroundings. PE stored in chemical bonds are the source of chemical energy. Energy lost by system = Energy gained by surrounding Endothermic process is any process in which heat has to be supplied to the system from the surroundings.

  16. Exothermic versus endothermic.

  17. The study of energy and its conversion is called thermodynamics. The law of conservation of energy is called First Law of Thermodynamics.

  18. First Law First Law of Thermodynamics: The energy of the universe is constant.

  19. Mathematical Definition of the First Law E = q+ w E = change in system’s internal energy q = heat w = work

  20. Figure 6.4: (a) The piston, moving a distance ∆h against a pressure P, does work on the surroundings. (b) Since the volume of a cylinder is the area of the base times its height, the change in volume of the gas is given by ∆h x A = V. Expansion

  21. Work work = force distance since pressure = force / area, work = pressure  volume wsystem = PV

  22. Enthalpy Enthalpy = H = E + PV E = HPV H = E + PV At constant pressure, qP = E + PV, where qP = H at constant pressure H = energy flow as heat (at constant pressure) E, H, P, V are state functions

  23. At constant pressure where PV work is allowed the change in enthalpy DH is equal to the energy flow as heat (q or Q).

  24. Signs Convention • Heat Flowing to the system from surrounding (heating) : DE <0, q or DH <0 • Heat Flowing from the system to the surrounding (cooling) : DE >0, q or DH >0 • Work done by the system on the surrounding : W > 0 (-) • Work done on the system by the surrounding : W < 0 (+)

  25. DH = -890.4 kJ CH4(g) + 2O2(g) CO2(g) + 2H2O (l) Thermochemical Equations Is DH negative or positive? System gives off heat Exothermic DH < 0 890.4 kJ are released for every 1 mole of methane that is combusted at 250C and 1 atm.

  26. Enthalpy (H) is used to quantify the heat flow into or out of a system in a process that occurs at constant pressure. DH = H (products) – H (reactants) DH = heat given off or absorbed during a reaction at constant pressure Hproducts > Hreactants Hproducts < Hreactants DH < 0 DH > 0

  27. Heat Capacity

  28. The specific heat (s) of a substance is the amount of heat (q) required to raise the temperature of one gram of the substance by one degree Celsius. The heat capacity (C) of a substance is the amount of heat (q) required to raise the temperature of a given quantity (m) of the substance by one degree Celsius. C = ms Heat (q) absorbed or released: q = msDt q = CDt Dt = tfinal - tinitial

  29. How much heat is given off when an 869 g iron bar cools from 940C to 50C? s of Fe = 0.444 J/g •0C Dt = tfinal – tinitial = 50C – 940C = -890C q = msDt = 869 g x 0.444 J/g •0C x –890C = -34,000 J

  30. Some Heat Exchange Terms specific heat capacity heat capacity per gram = J/°C g or J/K g molar heat capacity heat capacity per mole = J/°C mol or J/K mol

  31. Calorimetry • The device used experimentally to determine the heat from chemical reaction is called a calorimeter. • Calorimetry is the science to measure heat changes and it is based on the temperature change. • Heat capacity is a measure of the body or system ability to absorb heat.

  32. Two Types of Calorimeters • Constant Volume Calorimeter • Constant Pressure Calorimeter

  33. Constant-Pressure or Coffee Cup Calorimetry May be used to determine many Heats such as heat of solution, neutralization (acid-base), etc. qlost = - qgained qrxn = - (qwater + qcalorimeter) qwater = msDt qcal = Ccal Dt Reaction at Constant P DH = qrxn

  34. DH = qrxn Constant-Volume Calorimetry DE = q + W W = -pDV = 0 DE = qV qsys = qwater + qbomb + qrxn qsys = 0 qrxn = - (qwater + qbomb) qwater = msDt qbomb = CbombDt Reaction at Constant V DH~qrxn No heat enters or leaves!

  35. The enthalpy of solution (DHsoln) is the heat generated or absorbed when a certain amount of solute dissolves in a certain amount of solvent. DHsoln = Hsoln - Hcomponents Which substance(s) could be used for melting ice? Which substance(s) could be used for a cold pack?

  36. The Solution Process for NaCl DHsoln = Step 1 + Step 2 = 788 – 784 = 4 kJ/mol

  37. Sample Exercise Calculate the energy per gram for burning 1.50g of CH4 in a constant-volume calorimeter (S=11.3 KJ/0C) where Dt = 7.30C.. Energy released = m x s x Dt = 1.50 x 11.3x103 x 7.3 = 83 KJ per 1.50g of CH4 83 Energy released per g = = 1.50 55 KJ/g

  38. 2H2O (s) 2H2O (l) H2O (s) H2O (l) H2O (l) H2O (s) DH = -6.01 kJ DH = 6.01 kJ DH = 2 x 6.01= 12.0 kJ Thermochemical Equations • The stoichiometric coefficients always refer to the number of moles of a substance • If you reverse a reaction, the sign of DH changes • If you multiply both sides of the equation by a factor n, then DH must change by the same factor n.

  39. How much heat is evolved when 266 g of white phosphorus (P4) burn in air? P4(s) + 5O2(g) P4O10(s)DH = -3013 kJ H2O (l) H2O (g) H2O (s) H2O (l) DH = 6.01 kJ DH = 44.0 kJ Thermochemical Equations • The physical states of all reactants and products must be specified in thermochemical equations. 1 mol P4 123.9g -3013 kJ Q = -6470 kJ 266g Q

  40. Hess’s Law Reactants  Products The change in enthalpy is the samewhether the reaction takes place in one step or a series of steps.

  41. Establish an arbitrary scale with the standard enthalpy of formation (DH0) as a reference point for all enthalpy expressions. f Because there is no way to measure the absolute value of the enthalpy of a substance, must I measure the enthalpy change for every reaction of interest?

  42. Standard enthalpy of formation (DH0f) is the heat change that results when one mole of a compound is formed from its elements at a pressure of 1 atm. Example CO2(g) is formed from C(s) and O2(g) C(s) + O2(g) CO2(g) DH0f

  43. DH0 (O2) = 0 DH0 (O3) = 142 kJ/mol DH0 (C, graphite) = 0 DH0 (C, diamond) = 1.90 kJ/mol f f f f The standard enthalpy of formation of any element in its most stable form is zero.

  44. Then Apply Hess’s Law

  45. Standard States Compound • For a gas, pressure is exactly 1 atmosphere. • For a solution, concentration is exactly 1 molar. • Pure substance (liquid or solid), it is the pure liquid or solid. Element • The form [N2(g), K(s)] in which it exists at 1 atm and 25°C.

  46. Keep in mind the following concepts.

  47. Change in Enthalpy Can be calculated from enthalpies of formation of reactants and products. Hrxn° = npHf(products) nrHf(reactants)

  48. The standard enthalpy of reaction (DH0 ) is the enthalpy of a reaction carried out at 1 atm. rxn aA + bB cC + dD - [ + ] [ + ] = - S S = DH0 DH0 rxn rxn mDH0 (reactants) dDH0 (D) nDH0 (products) cDH0 (C) aDH0 (A) bDH0 (B) f f f f f f Hess’s Law: When reactants are converted to products, the change in enthalpy is the same whether the reaction takes place in one step or in a series of steps. (Enthalpy is a state function. It doesn’t matter how you get there, only where you start and end.)

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