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Modern Engineering Thermodynamics

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604 CHAPTER 15: Chemical <strong>Thermodynamics</strong><br />

WHAT IS THE STANDARD REFERENCE STATE?<br />

The standard reference state (SRS) is defined by the following temperature and pressure:<br />

SRS temperature = T° =25:0°C = 298 K = 77:0°F = 537 R<br />

SRS pressure = p° =0:100 MPa = 14:5 psia ≈ 1 atm<br />

Consequently, the specific internal energies of the elements at the SRS are always negative and computed from<br />

u° = − p°v°, wherep° =0:100 MPa and v° is the corresponding specific volume of the element in question. Thermodynamic<br />

properties at the standard reference state are always denoted by a superscript °.<br />

15.6 HEAT OF FORMATION<br />

When a reaction gives off or liberates heat, the reaction is said to be exothermic, and when it absorbs heat, it is<br />

said to be endothermic. Our sign convention for heat transport of energy requires that Q exothermic < 0whereas<br />

Q endothermic > 0. The heat of formation of a compound is the heat liberated or absorbed in the reaction when the<br />

compound is formed from the stable form of its elements at the standard reference state. For example, if the<br />

elements and the resulting compound are both at the standard reference state, then we can write<br />

<br />

Elements ðat the SRSÞ ! Compound ðat the SRSÞ+ q<br />

f<br />

° compound<br />

<br />

where q<br />

f<br />

° is the molar heat of formation of the compound at the standard reference state.<br />

compound<br />

In 1840, the Swiss chemist Germain Henri Hess (1802–1850) discovered that the total amount of heat liberated<br />

or absorbed during a chemical reaction is independent of the thermodynamic path followed by the reaction.<br />

This is known as Hess’s law or the law of constant heat sums. It allows us to determine heats of formation for compounds<br />

that cannot be synthesized directly from their elements.<br />

For example, the complete combustion of a hydrocarbon compound of the form C n H m in pure oxygen, wherein<br />

the reactants and the products are both maintained at the standard reference state, can be written as<br />

C n H m + aðO 2 Þ!nðCO 2 Þ + ðm/2ÞðH 2 OÞ + HHV CnH m<br />

where HHV is the higher heating value of the hydrocarbon (defined later, see Tables 15.2 and 15.3). We also<br />

have the following carbon dioxide and water formation reactions:<br />

and<br />

C + O 2 ! CO 2 − 393:5 MJ/kgmole CO 2<br />

H 2 + ð1/2ÞðO 2 Þ!H 2 O − 285:8 MJ/kgmole H 2 O<br />

Now Hess’s law states that the heats liberated or absorbed in these reactions are independent of the reaction<br />

path, so we can rearrange them as<br />

CO 2 ! C + O 2 + 393:5 MJ/kgmole CO 2<br />

WHAT IS HESS’S LAW?<br />

Using caloric theory, Henri Hess tried to extend Dalton’s interpretation of chemical reactions by attempting to find examples<br />

of the combination of caloric with chemical elements in simple mass ratios. He discovered that, for a given reaction,<br />

the total amount of caloric (heat) involved was always the same, independent of the number of intermediate steps contained<br />

within the reaction. Today, we know that this is really true only for aergonic, steady state, steady flow, open systems<br />

and for isobaric, closed systems where the heat of reaction equals the change in total enthalpy (because enthalpy is a point<br />

function and therefore independent of the actual chemical path taken by the reaction).

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