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If there is no experimental data available, are there any other methods of estimating thermochemical data? Group Additivity ab initio calculations molecular.

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Presentation on theme: "If there is no experimental data available, are there any other methods of estimating thermochemical data? Group Additivity ab initio calculations molecular."— Presentation transcript:

1 If there is no experimental data available, are there any other methods of estimating thermochemical data? Group Additivity ab initio calculations molecular mechanics calculations

2 Reasons for the Development of Estimation Techniques 1. To provide a value for the property when no experimental values are available 2. To provide a means of distinguishing between two or more discordant experimental values. 3. The parameters generated by the estimation technique may provide a handle to measure or understand some molecular property that can not be measured directly. 4. As a diagnostic tool to identify and sometimes quantify unusual interactions.

3 Question: Can thermochemical properties be subdivided into small increments so that the total molecular property in question can be calculated from the sum of its parts? 1. How small can the increments be? 2. Are these group increments interchangable so that they can be used to calculate similar properties of distinctively different molecules? 3. What properties are subject to this treatment?

4 Some Thermochemical properties that have been modeled by group additivity 1. Molecular weight 2. Atomic weight 3. Enthalpy of formation 4. Entropy of formation 4. Enthalpy of vaporization 5. Total phase change entropy 6. Heat capacity 7. Vapor pressure

5 Bond additivity 1. Bond Additivity: An assignment of a value associated with each type of bond. Group additivity 2. Values are associated with a series of atom combinations is various structural environments.

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7 Butane C 3 H 8  H f (298) = 8 C-H + 2C-C  H f (298) = [8(-3.83) + 2(2.73)]4.184 = -105.4 kJ mol -1  H f (298) expt = -104.6 kJ mol -1 Bond Additivity

8 Butadiene CH 2 =CH-CH=CH 2  H f (298) = 6 C d -H + C d -C  H f (298) = [6(3.2) + 6.7]*4.184 = 109.4 kJ mol -1  H f (298) expt = 110 kJ mol -1 Bond Additivity

9 Styrene  H f (298) = 5  -H +  -C +3 C d -H  H f (298) = 4.184[5(3.25) + 7.25 + 3(3.2)]  H f (298) = 138.5 kJ mol -1  H f (298) expt = 147.9 kJ mol -1 Bond Additivity

10 Benson’s Group Additivity Values are assigned to groups based on their constitution and on their neighboring environment

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12 Styrene  H f (298) = 5 C B -(H) + C B -(C d ) + C d -(C d )(H)+ C d -(H 2 )  H f (298) = 4.184[5(3.3) + 5.68 + 6.78 + 6.26]  H f (298) = 147.4 kJ mol -1  H f (298) expt = 147.9 kJ mol -1 Group Additivity

13 Butane  H f (298) = 2 C-(H) 3 (C) + 2 C-(H) 2 (C) 2  H f (298) = 4.184[2(-10.2) +2(-4.93)]  H f (298) = -126.6  H f (298)expt = -125.5

14 Group Additivity Cyclobutane  H f (298) = 4 C-(H) 2 (C) 2  H f (298) = 4.184[4(-4.93)] = -82.5  H f (298) expt = 28.4  H f (298) = -82.5-28.4 = -111 kJ mol -1 CH 2 CH 2 -CH 2 CH 2 CH 2 CH 2 - vs | | CH 2 CH 2  H f (298) = strain energy in cyclobutane

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16 Cp(g) Calculation of heat capacity follows the same rules as enthalpy. What is the heat capacity of 2-methylhexane? Cp(g)(298) = 3 C-(H) 3 C+3 C-(H) 2 (C) 2 +C-(H)(C) 3 Cp(g)(298) = 4.184[3(6.19) + 3(5.5) +4.54] Cp(g)(298) = 165.7 J mol -1 K -1

17 Entropy: (S (298) (g) The calculation of entropy follows the same rules as for enthalpy and heat capacity but has two additional corrections. Correction terms: (1) symmetry (-Rln  ) (2) mixing (-R  i n i ln(n i )) where n i refers to the mol fraction and  is the symmetry number. The symmetry number is the number of identical structures that can be obtained by a symmetry operation such as rotation.

18 What is the entropy of 2-methylhexane? S (298) (g) = 3 C-(H) 3 C+3 C-(H) 2 (C) 2 +C-(H)(C) 3 + corrections S (298) (g) = 4.184[3(30.41)+3(9.42)-12.07] + corrections S (298) (g) = 449.4 corrections = -3Rln(3) =-27.4 S (298) (g) = 449.4 - 27.4 = 422 J mol -1 K -1 S (298) (l) expt = 314.6, 315.1, 323.3 S (298) (g)

19 S (298) (g) = S (298) (l) + Cp(l)lnT B /298) +  H v /T B +Cp(g)ln(298/T B ) S (298) (l) = S (298) (g) - [Cp(l)lnT B /298) +  H v /T B +Cp(g)ln(298/T B )] S (298) (l) = 422 -[222.9ln(363/298)+34900/363+165.7ln(298/363)] S (298) (l) = 314.6 J mol -1 K -1 S (298) (l) expt = 314.6, 315.1, 323.3 S (298) (l) T B =363 K; Cp(l)=222.9J mol -1 K -1 ;  H v = 34.9 J mol -1 K -1

20 What is the entropy of 3-methylhexane? S (298) (g) = 3 C-(H) 3 C+3 C-(H) 2 (C) 2 +C-(H)(C) 3 + corrections S (298) (g) = 4.184[3(30.41)+3(9.42)-12.07] + corrections S (298) (g) = 449.4 corrections = -3Rln(3) =-27.4; +Rln(2) S (298) (g) = 449.4 - 27.4 +5.76 = 427 J mol -1 K -1 S (298) (l) expt = 309.6

21 S (298) (l) T B =364 K; Cp(l)=216.7J mol -1 K -1 ;  H v = 35.1 J mol -1 K -1 S (298) (g) = S (298) (l) + Cp(l)lnT B /298) +  H v /T B +Cp(g)ln(298/T B ) S (298) (l) = S (298) (g) - [Cp(l)lnT B /298) +  H v /T B +Cp(g)ln(298/T B )] S (298) (l) = 427 -[216.7ln(364/298)+35100/364+165.7ln(298/364)] S (298) (l) = 320.4 J mol -1 K -1 S (298) (l) expt = 309.6 J mol -1 K -1

22 What is the enthalpy of formation of 3-methylhexane?  H f (298)(g) = 3 C-(H) 3 C+3 C-(H) 2 (C) 2 +C-(H)(C) 3 + corrections  H f (298)(g) = 4.184[3(-10.2)+3(-4.93)-1.9] + corrections  H f (298)(g) = -197.9 + corrections correction = 0.8*4.184  H f (298)(g) = -194.5 kJ mol -1  H f (298)(g) expt = -191.3  1.3

23 1 gauche interaction

24 Summary on Using Benson Group Values 1. Identify the groups:  H f, Cp, S 2. Add non-bonded interactions:  H f, Cp, S 3. Add symmetry and chirality considerations: S


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