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MURDOCH RESEARCH REPOSITORY
This is the author’s final version of the work, as accepted for publication following peer review but without the publisher’s layout or pagination.
The definitive version is available at http://dx.doi.org/10.1021/es5038047
Altarawneh, M. and Dlugogorski, B.Z. (2014) Thermal decomposition of 1,2-bis-(2,4,6-tribromophenoxy)ethane
(BTBPE), a novel brominated flame retardant. Environmental Science & Technology, 48 (24). pp. 14335-14343.
http://researchrepository.murdoch.edu.au/24303/
Copyright: © 2014 American Chemical Society.
It is posted here for your personal use. No further distribution is permitted.
1
Thermal Decomposition of 1,2-bis-(2,4,6-tribromophenoxy)ethane 1
(BTBPE), a Novel Brominated Flame Retardant 2
3
Mohammednoor Altarawneh*†, Bogdan Z. Dlugogorski 4
5
School of Engineering and Information Technology 6
Murdoch University, Perth, Australia 7
8
*Corresponding Author: 9
Phone: (+61) 8 9360-7507 10
E-mail: [email protected] 11
12
† On leave from Chemical Engineering Department, Al-Hussein Bin 13
Talal University, Ma’an, Jordan 14
15
16
2
Abstract 17
18
1,2-bis-(2,4,6-tribromophenoxy)ethane (BTBPE) is currently one of the most commonly 19
applied novel brominated flame retardants. In this contribution, we analyse in detail the 20
mechanisms pertinent to its thermal decomposition in view of analogous experimental 21
findings. We demonstrate that a 1,3-hydrogen shift, leading to 2,4,6-tribromophenol (M9) 22
and 1,3,5-tribromo-2-(vinyloxy)benzene (M10) molecules, dominates direct scission of O-23
CH2 bonds up to a temperature of ~ 680 K. H atom abstraction from CH2 sites, followed 24
by a fission of a C-C bond, produce a 2,4,6-tribromophenoxy radical (M2) and a M10 25
molecule. Bimolecular condensation reactions involving M2, M9 and M10 generate 26
several congeners of brominated diphenyl ethers and their OH/OCHCH2 substituents, 27
which serve as direct precursors for the formation of polybrominated dibenzo-p-dioxins. 28
Reaction of M9 with a model compound of a hydrocarbon chain preferentially yields M2. 29
Strong adsorption energy of the latter on a radical site of a hydrocarbon chain suggests that 30
mechanisms such as Langmuir–Hinshelwood, Eley–Rideal and Diels-Alder might be 31
operating during the formation of PBDD/Fs from brominated flame retardants (BFRs). 32
Reactions of alkyl primary/secondary radicals and diradical with the BTBPE molecule 33
proceed via H abstraction from a –CH2- moiety. 34
35
36
3
1. Introduction 37
38
Brominated flame retardants (BFRs) represent a broad group of chemicals added to 39
polymeric components in numerous consumer products (such as electronic equipment and 40
furniture) to increase their fire resistance. So far, about 75 different BFRs have been 41
produced on a commercial scale.1 During the last few decades, technical mixtures of 42
polybrominated diphenyl ethers (PBDEs) were the most deployed BFRs. As a 43
consequence of serious environmental and health burdens, voluntary or strict bans have 44
discontinued production and usage of PBDEs.2 Currently, hexabromocyclododecane 45
(HBCD) and tetrabromobisphenol A (TBBA) are the two most deployed BFRs, where the 46
latter constitutes nearly 60 % of the world’s total production and usage of BFRs:1 47
48
49
50
Recent studies on HBCD and TBBA have linked them to mounting carcinogenic character 51
and have proved their behaviour as persistent organic pollutants (POPs).3 This has paved 52
the way for the development and the use of the next generation of BFRs, or the so-called 53
NBFRs.4 The term NBFRs refers to BFRs that are new to the market or recently detected 54
in the environment. The latest comprehensive report by the European Food Safety 55
HO OH
Br
Br
Br
Br
O
PBDEs TBBA
Br
Br
Br
Br
Br
Br
HBCD
O O
Br
Br
Br
Br
Br
Br
BTBPE
BrxBry
4
Authority has stressed a general lack of information on physical and chemical 56
characteristics, reactivity and stability of all NBFRs.5 This in turn has hindered attempts 57
to perform risk characterisation with regard to environmental and combustion behaviour, 58
overall persistence and bioaccumulative tendency of NBFRs.6 59
60
1,2-bis-(2,4,6-tribromophenoxy)ethane (BTBPE) represents one of the most deployed 61
NBFRs with a total production estimated at 16,710 tonnes as of 2001.4 BTBPE exhibits a 62
low potential for bioaccumulation and for long range atmospheric transport.7 As thermal 63
treatment and recycling activities represent mainstream strategies for disposal of materials 64
laden with BFRs,8 it is essential to describe precisely the decomposition behaviour of 65
NBFRs at elevated temperatures and interaction of these compounds with the polymeric 66
matrix. 67
68
The sole study on thermal decomposition of BTBPE was performed by Balabanovich et 69
al.9, who found that pyrolysis of BTBPE commences via concerted or radical-derived 70
rupture of one of its two ether linkages. Major decomposition products were reported to 71
be 2,4,6-tribromophenol and vinyl tribromophenol. Condensation reactions involving 72
bromophenols and their derived bromophenoxy radicals constitute the most significant 73
pathways for the formation of polybrominated dibenzo-p-dioxins (PBDDs) and 74
polybrominated dibenzofurans (PBDFs). A detailed quantitative account of the thermal 75
behaviour of BTBPE necessitates accurate thermochemical and kinetic parameters. 76
77
To this end, we report in this study the results of a theoretical investigation into thermal 78
decomposition of BTBPE and its bimolecular reactions with reactive radical species 79
present in the pyrolytic environment. As BFRs are typically deployed as immiscible 80
5
constituents in polymeric hydrocarbon materials, it is essential to investigate bimolecular 81
reactions stemming from the co-pyrolysis of BFRs with CxHy structural entities. For that 82
reason, we also study bimolecular reactions of the BTBPE molecule with alkyl radicals 83
and diradicals. These radicals typically arise as initial intermediates from pyrolysis of any 84
polymeric hydrocarbons such as polyethylene and polypropylene. Because the overall 85
decomposition of BTBPE is centred on the ether bridge, results provided in this study 86
should also assist in elucidating the decomposition chemistry of other NBFRs that contain 87
the ether functionality. 88
89
90
2. Computational methodology 91
92
Gaussian09 code10 facilitated calculations of all structures and energies at the theoretical 93
level of M062X/6-311+G(2d,p).11 M062X is a meta hybrid density functional theory 94
(DFT) method that has been shown to perform very well in predicting thermochemistry 95
and kinetics of organic systems. We have demonstrated in a recent study12 that, M062X-96
calculated energies vary only marginally (~ 1-2%) when deploying a significantly bigger 97
basis set on similar brominated systems. Computations of the intrinsic reaction 98
coordinates (IRC) confirm the nature of transition structures along their assigned pathways 99
and an isodesmic work reaction provides the standard enthalpy of formation of the BTBPE 100
molecule. Calculations of reaction rate constants are carried out via the “KiSThelp” 101
code.13 A one-dimensional Eckart functional afforded estimation of quantum tunnelling 102
corrections (i.e., transmission coefficients).14 Based on the accuracy margin of the 103
adapted methodology, we envisage maximum uncertainty limits in the calculated 104
activation energy (Ea) to be within ±3 kcal/mol.11 105
6
3. Results and discussion 106
107
3.1. Structure, enthalpy of formation and internal rotations 108
109
Figure 1 depicts optimised geometries of the BTBPE molecule. The BTBPE molecule 110
exhibits a C2 symmetry around the -H2C-CH2- bond. Ortho C-Br bonds are slightly 111
shortened by 0.003 Å in reference to the para C-Br bond. The structure of the BTBPE 112
molecule features the existence of two internal rotations centred on -O-CH2- and -H2C-113
CH2- bonds. Figure 2 portrays energy potentials for these two rotors. In calculations of 114
the potentials of these rotors, we performed partial optimisations by fixing the 115
corresponding dihedral angles and allowing the rest of the molecules to relax. Overall 116
barriers for rotations associated with -O-CH2- and -H2C-CH2- amount to 2.1 kcal/mol and 117
8.6 kcal/mol, respectively. The relatively shallow barriers for these rotors indicate the 118
establishment of an equilibrium state between the several accessible conformers of the 119
BTBPE molecule, especially at elevated temperatures. Weak interaction between ortho 120
bromine atoms and the -H2C-CH2- bridge causes the unsymmetrical shapes of the 121
potential of the -O-CH2- and -H2C-CH2- rotors. 122
123
To the best of our knowledge, present literature reports no value of the standard enthalpy 124
of formation ( 298o
f H∆ ) of the BTBPE molecule. For this reason, isodesmic reaction in 125
Scheme 1 serves to provide 298o
f H∆ for the title molecule: 126
127
7
128
129
Scheme 1 utilises accurate experimental values of 298o
f H∆ for reference species15 to yield 130
298o
f H∆ of the BTBPE molecule of 72.6 kcal/mol. Based on the estimates of errors in 131
298o
f H∆ for reference species, a value of ± 1.0 kcal/mol represents a lower uncertainty limit 132
inherent in the calculated 298o
f H∆ of BTBPE. 133
134
135
3.2. Unimolecular decomposition of the BTBPE molecule 136
137
Figure 3 illustrates all plausible initial pathways operating in the unimolecular 138
decomposition of the BTBPE molecule. Six out of the seven corridors proceed without 139
encountering an intrinsic reaction barrier. Direct scissions of aliphatic O-CH2, H2C-CH2 140
and O-phenyl bonds are endothermic by 66.0 kcal/mol, 88.0 kcal/mol and 101.0 kcal/mol, 141
correspondingly. We find that, the presence of phenyl rings in the BTBPE molecule 142
significantly reduces the bond dissociation enthalpy (BDH) of the O-CH2 bond in 143
reference to the corresponding linkage in the 1,2-dimethoxyethane molecule 144
(CH3O(CH2)2OCH3), i.e. 85.5 kcal/mol. Fissions of the aromatic para C-Br, C-H and 145
allylic C-H bonds demand endothermicity of 80.2 kcal/mol, 109.8 kcal/mol and 95.6 146
kcal/mol, in that order. Breakage of an ortho C-Br bond slightly overshoots that of para 147
C-Br bond by 0.6 kcal/mol. 148
O O
Br
Br
Br
Br
Br
Br + 6 + CH3-CH3 = O + 6 + CH3-(CH2)2-CH3
Scheme 1:
Br
8
A 1,3-hydrogen shift from a CH2 site to an O site occurs in a concerted mechanism via the 149
transition structure TS1. The barrier of TS1 amounts to 63.7 kcal/mol and the reaction is 150
endothermic by 10.4 kcal. Products from this channel comprise the two main species of 151
2,4,6-tribromophenol (M9) and 1,3,5-tribromo-2-(vinyloxy)benzene (M10) observed in 152
experiments. 153
154
In view of the enthalpic profile reported in Figure 3, two competing channels control the 155
overall self-decomposition of the BTBPE molecule, namely β O-CH2 bond fission (M1 + 156
M2) and a 1,3-hydrogen shift (M9 + M10). We estimate a rate constant in the high-157
pressure limit for the latter within the formalism of the conventional transition state 158
theory, fitting the Arrhenius rate expression in the temperature range of 400 K – 1500 K to 159
yield k(T(K))=1.86×1012exp(-26 900/T) s-1. As scission of the O-CH2 bond occurs 160
without encountering an intrinsic barrier, we apply the variational transition state theory 161
(VTST)16 to derive its corresponding rate constant. We find that, the VTS for this 162
reactions is located at a O····CH2 separation of 4.000 Å. This reaction coordinate also 163
corresponds to the longest O····CH2 separation at which the candidate VTS still holds one 164
and only one negative vibrational frequency. We fit the rate constant for this reaction to 165
expression of k(T(K)=3.79×1015exp(-30 800/T) s-1, in the same temperature interval. We 166
found that treating the torsions in the BTBPE molecule as hindered rotors (HRs) changes 167
marginally the calculated reaction rate constants. For example, treating the -O-CH2- and -168
H2C-CH2- torsions as HRs changes the estimated reaction rate constant for the BTBPE → 169
M9 + M10 channel at 1000 K by 3.1 %, in reference to treating these two rotors as 170
harmonic oscillators. This implies that, HR treatment induces negligible changes in the 171
kinetic and thermodynamic analyses. 172
9
Figure 4 depicts the branching ratios for the two competing channels as a function of 173
temperature. We observe that, the O-CH2 bond fission outpace that of the 1,3-hydrogen 174
transfer at ~ 680 K. At the temperature interval of the experimental study, i.e. 513 K – 175
613 K, and based on computed branching ratios in Figure 4, we anticipate that the major 176
product flux into M9 and M10 species arises from the 1,3-hydrogen transfer rather than 177
from fission of the O-CH2 linkage. Furthermore, the extremely facile C-C bond in the M1 178
intermediate (i.e., 1.4 kcal/mol) implies that, the sole fate of this radical entails the 179
formation of ethene molecule and 2,4,6-tribromophenoxy radical. A parallel pathway, 180
involving a C-H bond rupture and yielding the M10 molecule from the M1, should be 181
hindered owing to its endothermicity of 32.8 kcal/mol. Thus, little M10 would appear if 182
the O-CH2 fission were the predominant initial decomposition channel. 183
184
185
3.3. Secondary reactions of the BTBPE molecule 186
187
Thermal decomposition of BFRs typically proceeds in an environment that is rich in H and 188
Br atoms, with H atoms sourced from polymeric entities.17 Figure 5 depicts a series of 189
reactions initiated by Br and H atoms. Owing to a significant difference in BDH for 190
primary C-H and aromatic C-H bonds (95.6 kcal/mol and 109.8 kcal/mol), H and Br atoms 191
preferentially abstract alkylic H bonds via trivial activation enthalpies. These facile H 192
abstraction reactions produce the M7 radical. Rupture of a C-O bond in the M7 adduct 193
takes place through a modest enthalpic barrier of 14.5 kcal/mol (TS7) and produces the 194
main experimental product M10 and 2,4,6-tribromophenoxy radical (M2). The phenoxyl 195
O atom in the M2 radical could readily abstract an H from any RH species in the system to 196
form the M9 molecule. 197
10
Abundance of experimental evidence points out that nearly 50 % of the initial bromine 198
content in deployed BFRs transforms into HBr.18 While HBr represents an inert 199
bromination agent, it reacts with stable molecules. The middlemost pathway in Figure 5 200
illustrates that, the radical site in the M7 species can abstract a Br from hydrogen bromide 201
releasing an H atom and forming the M11 molecule. The enthalpic barrier of this pathway 202
amounts to 23.6 kcal/mol (TS6). Further decomposition of M11 follows analogous steps 203
illustrated for the parent BTBPE; i.e., competition between 1,3-hydrogen transfer reaction 204
and C-O bond fission. Most notably, Figure 5 depicts pathways initiated by HBr reactions 205
with the M7 radical that generate the major experimental product of ethylene bromide 206
(CH2CHBr). Reactions of Br atoms with ethene also lead to the formation of CH2CHBr. 207
Balabanovich et al. reported the detection of the M12 molecule in their pyrolysis 208
experiments. Analogously, bimolecular reactions of Br/HBr with the M1/M10 species 209
could brominate their vinyl-side chains yielding a wide spectrum of products identified 210
experimentally. 211
212
213
3.4. Pre-intermediates for the formation of PBDDs 214
215
Pyrolysis of the PTBPE has resulted in appreciable yields of PBDDs. Literature provides 216
detailed description of reaction networks leading to the formation of PBDDs from various 217
precursors, more specifically, brominated phenoxy,19 brominated diphenyl ethers 218
(PBDEs)12 and hydroxylated brominated diphenyl ethers.20 Initial decomposition of the 219
PTBPE molecule produces predominantly three building blocks for the formation of 220
PBDDs, namely, 2,4,6-tribromophenoxy (M2), 2,4,6-tribromophenol (M9) and 1,3,5-221
tribromo-2-(vinyloxy)benzene (M10). Figure 6 depicts initial coupling pathways leading 222
11
to the formation of direct pre-PBDDs intermediates from the bimolecular condensations of 223
two 2,4,6-tribromophenol molecules (a), a 2,4,6-tribromophenol molecule and its derived 224
radical (b), 2,4,6-tribromophenol and 1,3,5-tribromo-2-(vinyloxy)benzene molecules (c) 225
and a 2,4,6-tribromophenoxy radical and a 1,3,5-tribromo-2-(vinyloxy)benzene molecules 226
(d). Closed-shell pathways illustrated in Figures 6a and 6c characterise the bimolecular 227
displacement of HBr, H2O and CH(OH)CH2 moieties. These channels require activation 228
enthalpies in a narrow range of 54.4 kcal/mol and 62.0 kcal/mol. Barrierless attachments 229
of phenoxy O in the M2 radical at ortho or para radical sites in the M9 (Figure 6b) and 230
M10 (Figure 6d) molecules result in subsequent ejection of Br, OH and OCHCH2 radicals 231
with trivial exothermicity. 232
233
Open-shell elimination of HBr requires a markedly lower activation enthalpy than the 234
corresponding closed-shell process; i.e., 46.8 kcal/mol (TS9) versus 56.9 kcal/mol (TS7). 235
Pathways shown in Figure 6 explain potent corridors for the formation of PBDE 236
congeners. Balabanovich et al.9 reported multiple identifications of these products in 237
experiments involving the pyrolysis of the PTBPE molecule.12 Our recent study12 on 238
PBDEs has shown unequivocally that, their oxidation proceeds in complex and very 239
exothermic reactions leading to the generation of PBDDs, even when the four ortho 240
carbon atoms bear bromine. Central to these mechanisms is loss of ortho Br atoms from 241
M13-M17 molecules and subsequent addition of oxygen molecules to the apparent ortho 242
radical sites. As Balabanovich et al.9 performed their experiments under reducing 243
conditions, there should be no contribution of M13-M17 to the formation of PBDDs. It 244
follows that, the major pathways for the production of PBDDs involve self-condensation 245
of M2 radicals and unimolecular rearrangement of the hydroxy-PBDE (M13). 246
247
12
3.5. Pathways leading to PBDFs 248
249
Cross-coupling of two bromophenoxy radicals at their ortho carbons, producing a keto-250
keto mesomer, initiates formation of PBDFs. Subsequent enolisation step leading to the 251
formation of a keto-enol adduct necessitates one of the two ortho carbon atoms to bear a 252
hydrogen atom. This in turn indicates that, the presence of two ortho C(Br) sites in the 253
M2 radical hinders formation of PBDFs from self-condensation of two M2 radicals: 254
255
Scheme 2: 256
257
258
259
The picture in Scheme 2 concurs with the absence of any PBDFs congeners from the 260
experimentally detected product species. However, we reveal in Figure 7 that, a radical 261
(M2)/molecule (M9) coupling mode provides an energy-accessible pathway for the 262
formation of PBDFs. Addition of ortho C(Br) site in the M2 radical to ortho C(Br) and 263
C(OH) sites of the M9 molecule affords the M19 and M20 adducts where modest reaction 264
enthalpies accompany their formation. Loss of Br and OH moieties from the C-C bridge 265
produces two oxygen-centred radicals, M21 and M22. Ring-closure reactions, starting 266
O
BrBr
Br
• O
BrBr
Br
•
+
OBr
Br
Br
O
BrBr
Br
OBr
Br
Br
O
BrBr
BrSteric
hindrance of
voluminous
Br atoms prevents this
step
PBDFs
keto-ketoenol-keto
13
from M21 and M22 radicals, produce M23 and M24 intermediates passing through modest 267
activation enthalpies of 29.2 kcal/mol (TS13) and 31.2 kcal/mol (TS14), respectively. 268
Finally, the loss of out-of-plane Br and OH moieties affords the formation of the 4,6,7,9-269
TBDF molecule. 270
271
Experimental considerations might have prevented Balabanovich et al.9 from detecting all 272
PBDD/Fs. Their analysis involved no specialised clean-up of the samples to remove 273
interfering species and no sample concentration. The single quadrupole mass 274
spectrometer allowed no attenuation of the baseline noise that would have been possible 275
with a MS/MS (triple quadrupole) machine, using the multiple reaction monitoring 276
(MRM) technique commonly applied in such situations. Furthermore, the gas-277
chromatography column might have been too long to permit the elution of all PBDD/Fs in 278
the time allowed for the gas chromatographic analysis. Bearing this in mind, more 279
congeners of PBDD/Fs might have been formed but had not been detected. Nonetheless, 280
the co-generation of PBDDs and PBDFs from pyrolysis21 and oxidation22 of bromophenols 281
congeners and the formation of five congeners of PBDD in the study of Balabanovich et 282
al.9 support the formation of these species in the present system. 283
284
285
3.6. On the effect of polymeric materials 286
287
As miscible systems of BFRs and polymers are deployed in practical applications, 288
polymeric entities may significantly influence the generation of PBBD/Fs in the thermal 289
treatment of BFRs. The effect of the carbon matrix on formation of PBDD/Fs can be 290
summarised in two focal points. Firstly, hydrocarbon chains provide sources of secondary 291
14
and primary alkyl radicals which serve as building blocks for PBDD/Fs. Secondly, the de 292
novo synthesis that proceeds via burning off the carbon matrix represents a primary 293
contributing pathway for the formation of PBDD/Fs.17 Several contributions17 suggest 294
that, the latter is more relevant to the formation of PBDD/Fs if compared with the 295
formation of PCDD/Fs, which appear mainly due to coupling of structurally-related 296
precursors either homogeneously or heterogeneously.23-26 297
298
Herein, we briefly show that, adsorption of 2,4,6-tribromophenoxy radical on a radical site 299
in a hydrocarbon chain may form a nucleus for the build-up of PBDD/Fs or other 300
brominated aromatics such as naphthalene. Cyclohexane and its radicals often represent 301
model compounds of hydrocarbon chains.27 For this reason, we simulate the carbon 302
matrix by a cyclohexane molecule. 303
304
Figure 8 depicts a radical centre in a cyclohexane ring preferentially abstracting a 305
hydroxyl H atom from a 2,4,6-tribromophenol molecule. We calculate barrier of this 306
reaction to be 6.6 kcal/mol (TS15). The alternative pathway constituting bromine 307
abstraction is associated with a slightly higher enthalpic barrier of 14.6 kcal/mol (TS16). 308
The 2-4,6-tribromophenoxy radical, which arises in this process, will eventually 309
participate in the formation of PBDD/Fs. Along the same line of enquiry, we find that 310
adsorption of a 2,4,5-tribromophenoxy moiety on a radical site of the cyclohexane ring is 311
excessively exothermic, by 67.2 kcal/mol: 312
313
Scheme 3: 314
315
15
316
317
The high stability of the M25 adduct in Scheme 3 suggests that it is a long-lived 318
intermediate enabling it to undergo further reactions. Formation of PBDD/Fs, initiated by 319
the M25 intermediate, may follow two plausible scenarios. The first scenario 320
encompasses analogous Langmuir–Hinshelwood (LH) and Eley–Rideal (ER) mechanisms 321
involving gaseous or adsorbed bromophenols. The second scenario is characterised by 322
successive addition of small gaseous brominated alkenes to react with 2,4,6-323
tribromophenoxy radical via a Diels-Alder mechanism. These reaction pathways warrant 324
further investigation. In order to test the convergence of energetics in Figure 8 with regard 325
to deploying a bigger model compound of the hydrocarbon chain, corresponding values 326
obtained with using a cyclododecane are included in Figure 8 for comparison. Values 327
calculated based on cyclododecane are lower than analogous results based on cyclohexane 328
by 1.0 – 2.0 kcal/mol. Nevertheless, the two set of values are in a reasonable agreement 329
330
Beside a plausible role of acting as a catalyst for the formation of PBDD/Fs via facilitating 331
the occurrence of prominent steps (i.e. formation of bromophenoxy and bromophenyl 332
radicals from bromophenols), hydrocarbon chains also promote the initial decomposition 333
of BFRs. In their experimental study on the co-pyrolysis of polypropylene (PP) with 334
PBDEs, Balabanovich et al.28 demonstrated that, radicals produced from degradation of PP 335
greatly accelerate thermal decomposition of PBDEs. Scission of polymeric hydrocarbon 336
16
chains produces two types of radicals, namely, primary and secondary in addition to 337
diradical moieties.29 Evident from formation of several alkyl bromides,28 reactions of 338
these species with PBDEs proceed via abstraction of aromatic Br atoms. In case of the 339
BTBPE molecule, reactions of radicals and diradicals could potentially occur through 340
abstraction of either H or Br atoms. To study relevant reactions with the BTBPE 341
molecule, we adopt n-propyl radical (CH2CH2CH3), i-propyl radical (CH3CHCH3) and a 342
methylene (:CH2) triplet to represent primary radicals, secondary radicals and diradical 343
species, respectively. Table 1 enlists calculated reaction enthalpies and activation 344
enthalpies for reactions of the BTBPE molecule with n-propyl radical, i-propyl and 345
methylene. Abstractions of an H atom by the three considered species from the -CH2- 346
entity hold lower activation enthalpies if compared with abstraction of Br atoms from one 347
of the two aromatic rings. This finding implies that reactions of alkyl radicals and 348
diradicals (typically produced from initial pyrolysis of any polymeric material) with the 349
BTBPE molecule lead to the formation of the M7 moiety, which readily decomposes into 350
the two building blocks of PBDD/Fs, M2 and M10. 351
352
In conclusion, we have mapped out pathways for the formation of major experimental 353
products from thermal decomposition of the BTBPE molecule. Although formation of 354
PBDDs could be linked with several structurally-related precursors present in the system, 355
the unexpected absence of PBDFs in the experimental measurements prompted us to 356
explore all possible pathways that underpin their formation. It seems plausible that 357
PBDFs might have formed but remained undetected in the study of Balabanovich et al.9 358
While the presence of two ortho C(Br) sites in 2,4,6-tribromophenoxy radicals acts to 359
prohibit the well-established initial enolisation step in radical/radical condensation mode, 360
radical/molecule coupling schemes provide an accessible corridor for the formation of 361
17
PBDFs. Adsorption of a 2,4,6-tribromophenoxy on a radical site of a hydrocarbon chain is 362
very exothermic and may initiate Langmuir-Hinshelwood, Eley-Rideal and Diels-Alder 363
like mechanisms leading to formation of PBDD/Fs. Finally, Figure 9 collates major 364
reactions investigated in this study. 365
366
367
Supporting Information Available 368
369
Cartesian coordinates, vibrational frequencies, and total energies for all structures. This 370
material is available free of charge via the Internet at http://pubs.acs.org. 371
372
373
Conflict of Interest: The authors declare that they have no conflict of interest. 374
375
376
Acknowledgement 377
378
This study has been supported by a grant of computing time from the National 379
Computational Infrastructure (NCI), Australia and the iVEC supercomputer facilities in 380
Perth as well as funds from the Australian Research Council (ARC). 381
382
383
384
385
386
18
References 387
388
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476
477
478
20
Table 1. Calculated reaction (∆H, in kcal) and activation (∆H≠) enthalpies for bimolecular 479
reactions of the BTBPE molecule with n-propyl radical, i-propyl radical and a methylene. 480
Values are in kcal/mol. 481
482
Reaction ∆H ∆H≠
PTBPE + CH2CH2CH3 → M6 + CH2BrCH2CH3 14.4 18.4
PTBPE + CH2CH2CH3 → M7 + CH3CH2CH3 -3.2 10.0
PTBPE + CH3CHCH3 → M6 + CH3CHBrCH3 11.6 14.9
PTBPE + CH3CHCH3 → M7 + CH3CH2CH3 -3.2 11.9
PTBPE + CH2 → M6 + CH2Br 4.3 9.1
PTBPE + CH2 → M7 + CH3 -10.4 3.8
483
484
485
486
487
488
489
490
491
492
21
493
494
Figure 1: Optimised structure of the BTBPE molecule. Distances are in Å. 495
496
497
Figure 2: Energy profiles for internal rotations in the BTBPE molecule. 498
499
22
500
501
502
Figure 3. Pathways operating in the self-decomposition of the PTBPE molecule. 503
Values in bold and italics signify reaction (in kcal) and activation (in kcal/mol) 504
enthalpies at 298.15 K, respectively. 505
506
Figure 4. Branching ratios for 1,3-hydrogen shift and O-CH2 fission reactions. 507
508
O O
Br
Br
Br
Br
Br
Br
O O
BrBr
Br
Br Br
Br
+
••
O
O
BrBr
Br
Br Br
Br
+
•
•
OO
BrBr
Br
Br Br
Br
+
•
•
O O
Br
Br
Br
Br
Br •
+ Br
O O
Br
Br
Br
Br
Br
+ H
Br
•
OOH
BrBr
Br
Br Br
Br
+
O O
Br
Br
Br
Br
Br
Br
+ H•
BTBPE66.0
109.888.0
80.2
101.0
95.6
63.7
10.4
M1M2
M3 M3
M4M5
M6
M7
M8
M10M9
TS1
- C2H4
1.6
400 600 800 1000 1200 1400
0.0
0.2
0.4
0.6
0.8
1.0
M9 + M10 M1 + M2
Bran
chin
g ra
tios
T(K)
23
509
510
Figure 5. Decomposition of the BTBPE molecule initiated by H abstractions from a 511
CH2 site. Values in bold and italics signify reaction (in kcal) and activation (in 512
kcal/mol) enthalpies at 298.15 K, respectively. 513
514
515
O O
Br
Br
Br
Br
Br
Br
BTBPE
+ H- H2+ Br-HBr
O O
Br
Br
Br
Br
Br
Br M7
•+ H
O O
Br
Br
Br
Br
Br
Br M11
Br
OOH
BrBr
Br
Br Br
Br
+
15.0
M12M9
Br
O
O
BrBr
Br
Br Br
Br
+•
•
M13
M2
Br
O
BrBr
Br
•
M2+
O
Br Br
Br
•
M14
Br
O
BrBr
Br
•
M3O
BrBr
Br
•
M2
+
+CH2CHBr
CH2CHBr
-5.6
2.4
65.9
10.4
62.9
5.4
TS2TS3
-6.9
TS5
TS6
23.6
8.08.9 65.6
OO
BrBr
Br
Br Br
Br
+
•
3.2
14.5
M10M2
TS4
+HBr
24
516
517
Figure 6. Pathways for the formation of poly brominated diphenyl ethers. Values in 518
bold and italics signify reaction (in kcal) and activation (in kcal/mol) enthalpies at 519
298.15 K, respectively. 520
521
522
OH
BrBr
Br
+OH
BrBr
Br
OH
O
Br
Br Br
Br
Br
Br
O
Br
Br Br BrBr
+ HBr
+ H2O
TS7
TS8
7.3M13
M14
56.9
62.09.1
(a)
(c)OH
BrBr
Br
+
OH
O
O
Br
Br
Br
O
O
BrBr
+ HBr
TS10
TS11
2.6
M16
M17
54.4
52.3
2.9
Br
O
Br
Br Br BrBr
+ CH(OH)CH2
TS12
M14
58.4 8.7
+ HBr
O
Br Br
Br
M10
M9
M9
M9
OH
BrBr
Br
TS9
M9
(b)
O
BrBr
Br
•
M2
OH
O
Br
Br Br
Br
Br
+ Br
M13
Br
O
Br
Br Br BrBr
+ OH
M14
Br
O
O
Br Br BrBr
M15
+ HBr•
(d)
+
O
Br Br
Br
M10
O
BrBr
Br
•
M2
Br
Br
Br
O
O
BrBr
Br
Br
+ Br
Br
Br
OH
O
O
Br
Br
+ Br
-12.1
M16Br
Br
M17
Br
OO
BrBr
+ Br
M18Br
Br
Br
Br
O
Br
Br Br BrBr
+ OCHCH2
M14
•
-6.5
-3.8
9.8
-5.4
-7.7
20.5
•
46.8
25
523
524
525
Figure 7. Pathways for the formation of 4,6,7,9-TetraPBDF. Values in bold and 526
italics signify reaction (in kcal) and activation (in kcal/mol) enthalpies at 298.15 K, 527
respectively. 528
529
OH
BrBr
Br
M9
O
BrBr
Br
•
M2
+
OBr
Br
Br
OH
BrBr
Br
•
OBr
Br
Br
BrHO
•
Br Br
O
Br
Br
OH
Br
Br
+ 2Br
O
Br
Br
Br
Br
Br
+ OH
+ Br
OOH
•
Br
BrBr
Br
OOH
•
Br
BrBr
Br O
Br
BrBr
Br
TS1329.2
•
•
TS14
31.2
11.8 M19
M20
M21
M22
M23
M24
4,6,7,9-TetraPBDF
14.5
41.2
34.5
16.7
-4.7
- OH
- Br
-20.3
-26.8
26
530
531
532
Figure 8. Reaction of 2,4,6-tribromophenol with a cyclohexane as a model 533
compound for hydrocarbon chains. Values in bold and italics signify reaction (in 534
kcal) and activation (in kcal/mol) enthalpies at 298.15 K, respectively. Values in 535
brackets refer to using cyclododecane as a model compound for the carbon matrix. 536
537
27
538
539
540
Figure 9. Schematic summary for considered reactions. 541
542
543
O O
Br
Br
Br
Br
Br
Br
O
O
BrBr
Br
Br Br
Br
•
•
O
OH
BrBr
Br
Br Br
Br
BTBPE
+
Unimolecular decomposition
+ Precursors for the generation of PBDD/Fs
+Plausible catalysing effect for the carbon matrix on formation of PBDD/Fs
+
Polymeric hydrocarbons chains
Scission reactions
Primary radicals, secondary radicals and diradicals
+
H abstractions
O O
Br
Br
Br
Br
Br
Br
•
O
BrBr
Br
•O
Br Br
Br
+