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Anais da Academia Brasileira de Ciências

Print version ISSN 0001-3765On-line version ISSN 1678-2690

An. Acad. Bras. Ciênc. vol.75 no.1 Rio de Janeiro Mar. 2003

https://doi.org/10.1590/S0001-37652003000100005 

Selectivity and efficiency of pyrene attachment to alkanes induced by broadband X-rays

 

GERALD O. BROWNI; NOEL A. GUARDALAII; JACK L. PRICEII; RICHARD G. WEISSI

IDepartment of Chemistry, Georgetown University, Washington, DC 20057-1227 USA
IINaval Surface Warfare Center, Carderock Division, 9500 MacArthur Boulevard
West Bethesda, MD 20817 USA

Correspondence

 

 


ABSTRACT

Bombardment of pyrene-doped n-heneicosane (C21H44) in its orthorhombic solid phase with <1.3> MeV broadband X-rays results in the formation of both mono- and di-heneicosylpyrenes, whereas the same dose in liquid cyclohexane yields only monosubstituted pyrene. In both cases, the reaction efficiency decreases as pyrene concentration is increased from 10-5 to 10-2 M. Qualitatively, the overall attachment efficiency is higher in orthorhombic n-heneicosane than in liquid cyclohexane, but the selectivity of attachment is greater in cyclohexane. Differences between these results and those from irradiations of the same samples with eV range photons are discussed.

Key words: broadband x-rays, pyrene, cyclohexane, heneicosane.


RESUMO

A exposição de n-heneicosano (C21H44) dopado com pireno, em sua fase ortorrômbica sólida, a Raios X de faixa larga a <1.3> MeV resulta na formação de mono- e di-heneicosilpirenos, enquanto que a mesma dose em ciclo-hexano líquido produz apenas pireno monossubstituído. Em ambos os casos, a eficiência da reação diminui quando a concentração de pireno aumenta de 10-5 a 10-2 M. Qualitativamente, a eficiência global de ligação é maior em n-heneicosano ortorrômbico do que em ciclohexano líquido, mas a seletividade de ligação é maior em ciclo-hexano. As diferenças entre estes resultados e os de irradiação das mesmas amostras com fotons na faixa de eV são discutidas.

Palavras-chave: raios X de faixa larga, pireno, ciclo-hexano, heneicosano.


 

 

INTRODUCTION

The misconception that pyrene ( PyH), a polycyclic aromatic hydrocarbon, is inert when irradiated with UV (eV range) photons in saturated hydrocarbon media has persisted widely despite several reports to the contrary (Lamotte et al. 1985, 1987, 1991). Irradiations in solid and liquid alkane phases produce 1-alkylpyrenes in addition to other photoproducts whose number and type depend on photon wavelength. Thus, 248 nm radiation yields 1-and 4-alkylpyrenes (via two-photon processes) whereas 185 nm radiation leads to alkylpyrenes and dihydropyrene photoproducts (via one-photon processes).

More recently, we have found that pyrene, when doped in films and irradiated with > 300 nm radiation (Naciri and Weiss 1989, Luo et al. 2002, Brown et al. 2002c, Yamaki et al. 2002), can be covalently attached to chains of polyethylene and other polymers. In an effort to determine the sites within the polymer matrices most likely to lead to attachment, the consequences of irradiations of pyrene in a series of n-alkanes and an alkene were examined while monitoring the influences of radiation wavelength, solvent phase, pyrene concentration, and alkane chain length on the efficiency and selectivity of attachment (Zimerman and Weiss 1999). It was determined that pyrene molecules reside and react preferentially at interfaces between lamellae in solid phases of long-chained n-alkanes and that the photochemistry in the solid phases can be very selective when the radiation wavelength is > 300 nm and the alkane chain contains at least 21 carbon atoms; only one photoproduct, 1-n-alkylpyrene, was detected in these cases.

Recently, we have demonstrated that bombardment of pyrene-doped polyethylene films with MeV range charged particles (electrons, protons, and alpha particles) results in the formation of both mono- and di-substituted pyrenes (i.e., pyrene molecules attached to one or two polyethylene chains) (Brown et al. submitted). By contrast, only monosubstituted products are detected when the same samples were exposed to > 300 nm radiation (Brown et al. 2002 a,b,c).

Few studies have compared the modes of energy deposition by eV photons and MeV particles (g-rays, electrons, protons, etc.) in organic media (Caldwell et al. 1966, Hammond et al. 1968, Penner et al. 1970, Penner and Hammond 1971). Here, we examine the effects of exposing pyrene in liquid phase cyclohexane and solid (orthorhombic) phase n-heneicosane ( C21; C21H44) to <1.3> MeV broadband X-rays and compare the results with those obtained previously from eV range UV irradiations. The differing energy deposition modes lead to clearly observable changes in the distributions of attachment products and their mechanisms of formation.

 

MATERIALS AND METHODS

MATERIALS

Pyrene (Aldrich, 99%) was recrystallized from benzene, passed through an alumina column using benzene as eluant, and recrystallized twice from ethanol to yield pale yellow crystals, mp 148.6 - 149.1ºC (lit. (Perrin and Amarego 1988) mp 149 - 150ºC). Cyclohexane (EM Science, Reagent Grade) was washed with conc. H2SO4, passed through a short column of basic alumina, and then refluxed under a nitrogen atmosphere in the presence of CaH2 for 1 day. It was then distilled into a receiving flask containing freshly activated 5 Å molecular sieves. C21 (Humphrey Chemical Company), mp 40 - 41ºC (lit. (Sirota and Singer 1994) mp 40.14 C), was recrystallized three times from 95:5 acetone:hexane.

PREPARATION AND ANALYSIS OF PYRENE IN SOLID C21 AND LIQUID CYCLOHEXANE SOLUTIONS

Prior to bombardment, concentrations of pyrene in the liquid phases of C21 and cyclohexane were determined by UV-vis absorption spectra (1 mm pathlength quartz cells) and Beer's law. Then, an aliquot of pyrene and solvent was transferred to a flattened glass capillary (8 mm (i.d.) ´  0.8 mm (i.d.) ´  30 mm; 300 nm transmittance cutoff; Vitrocom) and flame-sealed after being degassed by four freeze-pump-thaw cycles at < 10-5 Torr on a mercury-free vacuum line.

Following bombardment, the cyclohexane and (heated, liquefied) C21 samples were dissolved in equivalent volumes of THF and analyzed by gel permeation chromatography (GPC) on a Hewlett-Packard Series 1100 ChemStation equipped with a diode array detector (4 nm bandwidth) using a Polymer Laboratories PLgel (3mm MIXED-E; 300 mm length ´  7.5 mm ID) size exclusion column and tetrahydrofuran (THF; Fisher Scientific, HPLC grade) as the eluant.

BROADBAND X-RAY GENERATION

Broadband X-rays were generated by a 2.5 MeV electron beam from a Febetron 705 on a thick tantalum converter operated at the Naval Surface Warfare Center (NSWC; Carderock Division, West Bethesda, MD). The mean energy of the continuous X-ray photon spectrum was <1.3> MeV. The width of the electron beam pulses was approximately 20 ns and the total dose given to each sample was 400 Gy.

 

RESULTS AND DISCUSSION

X-RAY BOMBARDMENT OF PYRENE IN SOLID C21 AND LIQUID CYCLOHEXANE SOLUTIONS

In previous work, we have shown that the attachment of pyrene to several saturated alkanes, including solid C21 and liquid cyclohexane is very dependent on solvent phase, pyrene concentration, radiation wavelength, and alkane chain length when induced by UV-vis radiation (Zimerman and Weiss 1999). For instance, at 5 ´ 10-6 M pyrene, attachment in liquid C21 (> 45ºC) was much less efficient and selective than in its orthorhombic phase, below 32.5ºC (Dorset et al. 1991). At higher pyrene concentrations, the efficiency of attachment to C21 in its orthorhombic phase decreased due to the formation of ground state aggregates.

As in the case with UV-vis irradiation, reaction efficiency of X-ray bombardment decreased with increasing pyrene concentration. However, X-ray bombardment of 10-5 or 10-2 M pyrene in orthorhombic C21 led to the formation of both mono- and di-alkylated pyrene products; the only photoproduct detected upon UV-vis irradiations was 1-heneicosylpyrene ( C21Py; eqn 1). The absorption spectra and retention volumes of the peaks labeled "M'' and "D'' in the GPC chromatograms in Figures 1 and 2 are consistent with their structural assignments as mono- and di-heneicosylpyrenes. In addition to generating large concentrations of heneicosyl radicals at various positions along the alkane chain (via C-H bond cleavage), MeV range X-rays can cleave C-C bonds, creating shortened chains terminated with radical centers (Wu et al. 2000). Each radical type can add (preferentially) to the 1-position of pyrene (Mitchell et al. 1979), yielding an alkylpyrene after loss of a hydrogen atom (Lapouyade et al. 1986). The peak at 5.8 min is assigned to a dialkylated pyrene ( C21PyC21; eqn 1). Its retention volume is smaller than those of mono-alkylated pyrenes and pyrene and its absorption spectrum is red-shifted by ca. 7 nm relative to those of mono-alkylated pyrenes (Figure 2). The absorption and emission spectra of pyrene analogues are known to shift incrementally to longer wavelengths as the number of alkyl substituents on the rings increases (De Clercq and Martin 1955).

 

 

 

 

 

 

Bombardment of 10-5 M pyrene in liquid cyclohexane with <1.3> MeV X-rays yielded no products that could be ascribed to an alkylated pyrene, and only a very small amount of this product was detected when the pyrene concentration was increased to 10-2 M. A much lower efficiency in liquid ( or plastic phase) cyclohexane than in solid heneicosane has also been observed when the attachment is initiated by eV range photons (Zimerman and Weiss 1999). Regardless of the radiation type, the much greater ability of radicals to diffuse within liquid (or plastic) cyclohexane than in orthorhombic C21 is the probable reason for the lower efficiency.

The proposed mechanism of pyrene attachment using eV photons requires that an upper electronic excited state of pyrene transfer its energy to a nearby alkane molecule, inducing C-H bond cleavage (Zimerman and Weiss 1999). For attachment to occur, a pyrene molecule and an alkane must be vicinal for a sufficient period after energy transfer to allow C-H bond cleavage to occur and the resulting alkyl radical to attach itself to (the now ground-state) pyrene. In liquid cyclohexane, separation of the pair via diffusion is competitive with their attachment.

MeV broadband X-rays and eV photons deposit their energy into hydrocarbon solutions of pyrene very differently. eV photons deposit energy initially into pyrene chromophores, creating electronically excited states of pyrene. Initially, MeV broadband X-rays deposit their energy indiscriminately into alkane solutions; due to their much greater concentrations, the alkane solvent molecules receive a much greater portion of the energy than the pyrene solutes. Furthermore, the initial deposition of energy by ionizing radiation like X-rays creates local concentrations of high energy (i.e., single ionization spurs) within an alkane medium (Spinks and Woods 1964). Within spurs, processes such as electron ejection leads to hole formation and the generation of stable pyrene radical cations and anions which, upon recombination with electrons, form pyrene excited states (Biscoglio and Thomas 2000, Szadkowska-Nicze et al. 1992). The predominant processes within the spurs are C-H and C-C bond scissions that lead to the formation of lower molecular weight alkanes (Zagórski 2002) in addition to the attachment processes mentioned here. The radicals generated upon bond scission are located preferentially at the ends of n-alkane chains (Toriyama et al. 1982). In the solid phase of C21, the radical centers are near the interlayer interfaces where the pyrene molecules reside, and formation of henicosylpyrene is facilitated spatially.

 

CONCLUSIONS

We have shown that selective and relatively efficient attachment of pyrene to liquid cyclohexane and solid (orthorhombic phase) heneicosane can be attained via irradiation with <1.3> MeV broadband x-rays. Irradiation of the pyrene/n-heneicosane samples yield both mono- and di-heneicosylpyrenes, whereas the only attachment product detected in liquid cyclohexane after the same dose is monosubstituted. In both cases, the reaction efficiency decreases when pyrene concentration is increased from 10-5 to 10-2 M. Qualitatively, the overall attachment efficiency is higher in orthorhombic C21 than in liquid cyclohexane, but the selectivity of attachment is greater in cyclohexane.

In liquid cyclohexane, selectivities of pyrene attachment initiated by irradiations with UV/vis (eV range) radiation or <1.3> MeV X-rays are similar. However, UV/vis and X-ray irradiations of pyrene in solid heneicosane follow rather different courses. The eV range photons initiate only mono-attachment while X-rays produce both mono- and di-substituted pyrenes. These results suggest that the density of alkane-based radicals generated by the broadband X-rays around a pyrene molecule in C21 is much greater than by the UV/vis photons. Surprisingly, both forms of radiation lead to relatively selective photoreactions, even though the modes of initial energy deposition into the samples are very different.

 

ACKNOWLEDGMENTS

We are grateful to Mr. Jeff King from NSWC for performing the broadband x-ray exposures and the U. S. National Science Foundation for financial support. This paper is dedicated to Professor Paschoal Senise, an institution in Brazilian science who built an Institute.

 

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Correspondence to
Richard G. Weiss
E-mail: weissr@georgetown.edu

Manuscript received on December 20, 2002;
accepted for publication on December 27, 2002;
contributed by RICHARD G. WEISS*

*Foreign Member of Academia Brasileira de Ciências

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