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Thermochemistry Chapter 6. 2 Copyright © by Houghton Mifflin Company. All rights reserved. Thermochemistry Thermodynamics is the science of the relationship.

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Presentation on theme: "Thermochemistry Chapter 6. 2 Copyright © by Houghton Mifflin Company. All rights reserved. Thermochemistry Thermodynamics is the science of the relationship."— Presentation transcript:

1 Thermochemistry Chapter 6

2 2 Copyright © by Houghton Mifflin Company. All rights reserved. Thermochemistry Thermodynamics is the science of the relationship between heat and other forms of energy. Thermochemistry is the study of the quantity of heat absorbed or evolved by chemical reactions.

3 Chapter 63 Copyright © by Houghton Mifflin Company. All rights reserved. Energy Energy is defined as the capacity to move matter. Energy can be in many forms: Radiant Energy - Electromagnetic radiation. Thermal Energy - Associated with random motion of a molecule or atom. Chemical Energy - Energy stored within the structural limits of a molecule or atom.

4 Chapter 64 Copyright © by Houghton Mifflin Company. All rights reserved. Energy There are three broad concepts of energy: Kinetic Energy is the energy associated with an object by virtue of its motion. Potential Energy is the energy an object has by virtue of its position in a field of force. Internal Energy is the sum of the kinetic and potential energies of the particles making up a substance. We will look at each of these in detail.

5 Chapter 65 Copyright © by Houghton Mifflin Company. All rights reserved. Energy Kinetic Energy: An object of mass m and speed or velocity v has kinetic energy E k equal to This shows that the kinetic energy of an object depends on both its mass and its speed.

6 Chapter 66 Copyright © by Houghton Mifflin Company. All rights reserved. A Problem to Consider Consider the kinetic energy of a person whose mass is 130 lb (59.0 kg) traveling in a car at 60 mph (26.8 m/s). The SI unit of energy, kg. m 2 /s 2, is given the name Joule.

7 Chapter 67 Copyright © by Houghton Mifflin Company. All rights reserved. Energy Potential Energy: This energy depends on the “position” (such as height) in a “field of force” (such as gravity). For example, water of a given mass m at the top of a dam is at a relatively high “position” h in the “gravitational field” g of the earth.

8 Chapter 68 Copyright © by Houghton Mifflin Company. All rights reserved. A Problem to Consider Consider the potential energy of 1000 lb of water (453.6 kg) at the top of a 300 foot dam (91.44 m).

9 Chapter 69 Copyright © by Houghton Mifflin Company. All rights reserved. Energy Internal Energy is the energy of the particles making up a substance. The total energy of a system is the sum of its kinetic energy, potential energy, and internal energy, U.

10 Chapter 610 Copyright © by Houghton Mifflin Company. All rights reserved. Energy The Law of Conservation of Energy: Energy may be converted from one form to another, but the total quantities of energy remain constant.

11 Chapter 611 Copyright © by Houghton Mifflin Company. All rights reserved. Heat of Reaction In chemical reactions, heat is often transferred from the “system” to its “surroundings,” or vice versa. The substance or mixture of substances under study in which a change occurs is called the thermodynamic system (or simply system.) The surroundings are everything in the vicinity of the thermodynamic system.

12 Chapter 612 Copyright © by Houghton Mifflin Company. All rights reserved. Heat of Reaction Heat is defined as the energy that flows into or out of a system because of a difference in temperature between the system and its surroundings. Heat flows from a region of higher temperature to one of lower temperature; once the temperatures become equal, heat flow stops.

13 Chapter 613 Copyright © by Houghton Mifflin Company. All rights reserved. Heat of Reaction Heat is denoted by the symbol q. The sign of q is positive if heat is absorbed by the system. The sign of q is negative if heat is evolved by the system. Heat of Reaction is the value of q required to return a system to the given temperature at the completion of the reaction.

14 Chapter 614 Copyright © by Houghton Mifflin Company. All rights reserved. Heat of Reaction An exothermic process is a chemical reaction or physical change in which heat is evolved (q is negative). An endothermic process is a chemical reaction or physical change in which heat is absorbed (q is positive).

15 Chapter 615 Copyright © by Houghton Mifflin Company. All rights reserved. Heat of Reaction Exothermicity “out of” a system  q < 0 Endothermicity “into” a system  q > 0 Energy System Surroundings Energy System Surroundings

16 Chapter 616 Copyright © by Houghton Mifflin Company. All rights reserved. Enthalpy and Enthalpy Change The heat absorbed or evolved by a reaction depends on the conditions under which it occurs. Usually, a reaction takes place in an open vessel, and therefore at the constant pressure of the atmosphere. The heat of this type of reaction is denoted q p, the heat at constant pressure.

17 Chapter 617 Copyright © by Houghton Mifflin Company. All rights reserved. An extensive property is one that depends on the quantity of substance. Enthalpy is a state function, a property of a system that depends only on its present state and is independent of any previous history of the system. Enthalpy and Enthalpy Change Enthalpy, denoted H, is an extensive property of a substance that can be used to obtain the heat absorbed or evolved in a chemical reaction.

18 Chapter 618 Copyright © by Houghton Mifflin Company. All rights reserved. Enthalpy and Enthalpy Change The change in enthalpy for a reaction at a given temperature and pressure (called the enthalpy of reaction) is obtained by subtracting the enthalpy of the reactants from the enthalpy of the products.

19 Chapter 619 Copyright © by Houghton Mifflin Company. All rights reserved. Enthalpy and Enthalpy Change The change in enthalpy is equal to the heat of reaction at constant pressure. This represents the entire change in internal energy (  U) minus any expansion “work” done by the system.

20 Chapter 620 Copyright © by Houghton Mifflin Company. All rights reserved. The internal energy of a system, U, is precisely defined as the heat at constant pressure plus the work done by the system: In chemical systems, work is defined as a change in volume at a given pressure, that is: Enthalpy and Enthalpy Change Enthalpy and Internal Energy

21 Chapter 621 Copyright © by Houghton Mifflin Company. All rights reserved. So  H is essentially the heat obtained or absorbed by a reaction in an open vessel where the work portion of  U is unmeasured. Enthalpy and Enthalpy Change Since the heat at constant pressure, q p, represents  H, then

22 Chapter 622 Copyright © by Houghton Mifflin Company. All rights reserved. Thermochemical Equations A thermochemical equation is the chemical equation for a reaction (including phase labels) in which the equation is given a molar interpretation, and the enthalpy of reaction for these molar amounts is written directly after the equation.

23 Chapter 623 Copyright © by Houghton Mifflin Company. All rights reserved. Thermochemical Equations In a thermochemical equation it is important to note phase labels because the enthalpy change,  H, depends on the phase of the substances.

24 Chapter 624 Copyright © by Houghton Mifflin Company. All rights reserved. The following are two important rules for manipulating thermochemical equations: Thermochemical Equations When a thermochemical equation is multiplied by any factor, the value of  H for the new equation is obtained by multiplying the  H in the original equation by that same factor. When a chemical equation is reversed, the value of  H is reversed in sign.

25 Chapter 625 Copyright © by Houghton Mifflin Company. All rights reserved. Applying Stoichiometry and Heats of Reactions Consider the reaction of methane, CH 4, burning in the presence of oxygen at constant pressure. Given the following equation, how much heat could be obtained by the combustion of 10.0 grams CH 4 ?

26 Chapter 626 Copyright © by Houghton Mifflin Company. All rights reserved. To see how heats of reactions are measured, we must look at the heat required to raise the temperature of a substance, because a thermochemical measurement is based on the relationship between heat and temperature change. Measuring Heats of Reaction The heat required to raise the temperature of a substance is its heat capacity.

27 Chapter 627 Copyright © by Houghton Mifflin Company. All rights reserved. The heat capacity, C, of a sample of substance is the quantity of heat required to raise the temperature of the sample of substance one degree Celsius. Changing the temperature of the sample requires heat equal to: Measuring Heats of Reaction Heat Capacity and Specific Heat

28 Chapter 628 Copyright © by Houghton Mifflin Company. All rights reserved. A Problem to Consider Suppose a piece of iron requires 6.70 J of heat to raise its temperature by one degree Celsius. The quantity of heat required to raise the temperature of the piece of iron from 25.0 o C to 35.0 o C is:

29 Chapter 629 Copyright © by Houghton Mifflin Company. All rights reserved. Measuring Heats of Reaction Heat capacities are also compared for one gram amounts of substances. The specific heat capacity (or “specific heat”) is the heat required to raise the temperature of one gram of a substance by one degree Celsius. To find the heat required you must multiply the specific heat, s, of the substance times its mass in grams, m, and the temperature change,  T.

30 Chapter 630 Copyright © by Houghton Mifflin Company. All rights reserved. A Problem to Consider Calculate the heat absorbed when the temperature of 15.0 grams of water is raised from 20.0 o C to 50.0 o C. (The specific heat of water is 4.184 J/g.o C.)

31 Chapter 631 Copyright © by Houghton Mifflin Company. All rights reserved. Heats of Reaction: Calorimetry A calorimeter is a device used to measure the heat absorbed or evolved during a physical or chemical change. (see Figure 6.11)(see Figure 6.11) The heat absorbed by the calorimeter and its contents is the negative of the heat of reaction.

32 Chapter 632 Copyright © by Houghton Mifflin Company. All rights reserved. A Problem to Consider When 23.6 grams of calcium chloride, CaCl 2, was dissolved in water in a calorimeter, the temperature rose from 25.0 o C to 38.7 o C. If the heat capacity of the solution and the calorimeter is 1258 J/ o C, what is the enthalpy change per mole of calcium chloride?

33 Chapter 633 Copyright © by Houghton Mifflin Company. All rights reserved. Heats of Reaction: Calorimetry First, let us calculate the heat absorbed by the calorimeter. Now we must calculate the heat per mole of calcium chloride.

34 Chapter 634 Copyright © by Houghton Mifflin Company. All rights reserved. Heats of Reaction: Calorimetry Calcium chloride has a molecular mass of 111.1 g, so Now we can calculate the heat per mole of calcium chloride.

35 Chapter 635 Copyright © by Houghton Mifflin Company. All rights reserved. Hess’s law of heat summation states that for a chemical equation that can be written as the sum of two or more steps, the enthalpy change for the overall equation is the sum of the enthalpy changes for the individual steps. Hess’s Law

36 Chapter 636 Copyright © by Houghton Mifflin Company. All rights reserved. For example, suppose you are given the following data: Hess’s Law Could you use these data to obtain the enthalpy change for the following reaction?

37 Chapter 637 Copyright © by Houghton Mifflin Company. All rights reserved. If we multiply the first equation by 2 and reverse the second equation, they will sum together to become the third. Hess’s Law

38 Chapter 638 Copyright © by Houghton Mifflin Company. All rights reserved. Standard Enthalpies of Formation The term standard state refers to the standard thermodynamic conditions chosen for substances when listing or comparing thermodynamic data: 1 atmosphere pressure and the specified temperature (usually 25 o C). The enthalpy change for a reaction in which reactants are in their standard states is denoted  H o (“delta H zero” or “delta H naught”).

39 Chapter 639 Copyright © by Houghton Mifflin Company. All rights reserved. Standard Enthalpies of Formation The standard enthalpy of formation of a substance, denoted  H f o, is the enthalpy change for the formation of one mole of a substance in its standard state from its component elements in their standard state. Note that the standard enthalpy of formation for a pure element in its standard state is zero.

40 Chapter 640 Copyright © by Houghton Mifflin Company. All rights reserved. Standard Enthalpies of Formation The law of summation of heats of formation states that the enthalpy of a reaction is equal to the total formation energy of the products minus that of the reactants..  is the mathematical symbol meaning “the sum of”, and m and n are the coefficients of the substances in the chemical equation.

41 Chapter 641 Copyright © by Houghton Mifflin Company. All rights reserved. A Problem to Consider Large quantities of ammonia are used to prepare nitric acid according to the following equation: What is the standard enthalpy change for this reaction? Use Table 6.2 for data.

42 Chapter 642 Copyright © by Houghton Mifflin Company. All rights reserved. A Problem to Consider You record the values of  H f o under the formulas in the equation, multiplying them by the coefficients in the equation. You can calculate  H o by subtracting the values for the reactants from the values for the products.

43 Chapter 643 Copyright © by Houghton Mifflin Company. All rights reserved. A Problem to Consider Using the summation law: Be careful of arithmetic signs as they are a likely source of mistakes.

44 Chapter 644 Copyright © by Houghton Mifflin Company. All rights reserved. Fuels A fuel is any substance that is burned to provide heat or other forms of energy. In this section we will look at: Foods as fuels Fossil fuels Coal gasification and liquefaction

45 Chapter 645 Copyright © by Houghton Mifflin Company. All rights reserved. Fuels Food fills three needs of the body: It supplies substances for the growth and repair of tissue. It supplies substances for the synthesis of compounds used in the regulation of body processes. It supplies energy. About 80% of the energy we need is for heat. The rest is used for muscular action and other body processes

46 Chapter 646 Copyright © by Houghton Mifflin Company. All rights reserved. Fuels A typical carbohydrate food, glucose (C 6 H 12 O 6 ) undergoes combustion according to the following equation. One gram of glucose yields 15.6 kJ (3.73 kcal) when burned.

47 Chapter 647 Copyright © by Houghton Mifflin Company. All rights reserved. Fuels A representative fat is glyceryl trimyristate, C 45 H 86 O 6. The equation for its combustion is: One gram of fat yields 38.5 kJ (9.20 kcal) when burned. Note that fat contains more than twice the fuel per gram than carbohydrates contain.

48 Chapter 648 Copyright © by Houghton Mifflin Company. All rights reserved. Fuels Fossil fuels account for nearly 90% of the energy usage in the United States. Anthracite, or hard coal, the oldest variety of coal, contains about 80% carbon. Bituminous coal, a younger variety of coal, contains 45% to 65% carbon. Fuel values of coal are measured in BTUs (British Thermal Units). A typical value for coal is 13,200 BTU/lb. 1 BTU = 1054 kJ

49 Chapter 649 Copyright © by Houghton Mifflin Company. All rights reserved. Fuels Natural gas and petroleum account for nearly three-quarters of the fossil fuels consumed per year. Purified natural gas is primarily methane, CH 4, but also contains small quantities of ethane, C 2 H 6, propane, C 3 H 8, and butane, C 4 H 10. We would expect the fuel value of natural gas to be close to that for the combustion of methane.

50 Chapter 650 Copyright © by Houghton Mifflin Company. All rights reserved. Fuels Petroleum is a very complicated mixture of compounds. Gasoline, obtained from petroleum, contains many different hydrocarbons, one of which is octane, C 8 H 18. This value of  H o is equivalent to 44.4 kJ/gram.

51 Chapter 651 Copyright © by Houghton Mifflin Company. All rights reserved. Fuels With supplies of petroleum estimated to be 80% depleted by the year 2030, the gasification of coal has become a possible alternative. First, coal is converted to carbon monoxide using steam. The carbon monoxide can then be used to produce a variety of other fuels, such as methane.

52 Chapter 652 Copyright © by Houghton Mifflin Company. All rights reserved. Operational Skills Calculating kinetic energy. Writing thermochemical equations. Manipulating thermochemical equations. Calculating the heat of reaction from the stoichiometry. Relating heat and specific heat. Calculating  H from calorimetric data. Applying Hess’s law. Calculating the enthalpy of reaction from standard enthalpies of formation.

53 Chapter 653 Copyright © by Houghton Mifflin Company. All rights reserved. Figure 6.11: Coffee-cup calorimeter. Return to Slide 31


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