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Rocket Propulsion Chemistry

 

 

 

 

An understanding of the energetics and dynamics of elementary reactions of boron monoxide (BO) radicals with key unsaturated hydrocarbons [acetylene, ethylene, methylacetylene  allene), diacetylene, and benzene] and the inherent formation of small boron-bearing molecules is of considerable interest to understand boron combustion processes, to the physical organic commu-nity due to the isoelectronic nature of boron monoxide and the cyano radical, and to the reaction dynamics community (reaction dynamics of transient radicals) both from the experimental and theoretical viewpoints. Computations are conducted in collaboration with Profs. Bartlett (University of Florida), Mebel (FIU), and Chang (NDHU, Taiwan). Boron monoxide presents a crucial transient radical in boron-based combustion processes, but the reaction dynamics of this radical have not been investigated so far. Here, due to its high energy density, boron has long been regarded as a good candidate for rocket fuel additives. This interest has also been expanded recently to ramjet and scramjet propulsion systems. The oxidation of boron is initially unable to reach full energy release due to the formation of boron oxide (B2O3) as an inert layer, which coats the non-reacted boron preventing further reaction. Essentially, the carbon-based fuel ignites and reaches a high enough temperature to remove the boron oxide layer, which, in turn, allows clean boron to be accessible for the combustion phase. The very first boron-bearing species formed in these processes is the boron oxide radical (BO), which can either react to boron oxide (B2O3) or with the hydrocarbon fuel to form carbon-, hydrogen-, oxygen-, and boron-bearing molecules (CHOB molecules). Compared to ‘classical’ hydrocarbon flames, the incorporation of boron results in a more complex, high temperature (1,800 – 4,000 K) organo boron chemistry. These considerations have led to the development of boron-based combustion models involving detailed experimental input parameters such as reaction products, intermediates, and rate constants. Although the reaction dynamics of boron atoms with hydrocarbon molecules have emerged during the recent years utilizing the crossed molecular beam approach thus accessing the B/C/H system, dynamics studies in the B/O/C/H system, in particular those involving reactions of the boron monoxide radical (BO) with hydrocarbon molecules, have been elusive to date. Therefore, a critical shortcoming of all boron-based combustion models is the fact that elementary reactions in the B/O system have never been coupled with those occurring in the B/C/H system. Crossed beam studies of the reaction of boron monoxide (BO) with acetylene (C2H2) showed that the HCCBO molecule plus atomic hydrogen can be formed.

 

 

 

 

 

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Boron monoxide radicals are produced via laser ablation of boron at 266 nm and reaction of the ablated boron atoms with carbon dioxide, which also acts as a seeding gas. The beam is characterized by laser induced fluorescence (LIF). Here, an LIF excitation spectrum of A 2Π – X 2Σ+ system in (0,0) vibrational band of boron monoxide is shown. Experimental spectrum (upper curve) and best-fit simulation (lower curve) corresponding to the rotational temperature Trot = 250 K. The double headed appearance of the spectrum is caused by spin-orbit splitting of the upper state.

 

 

 

 

 

 

 

 

 

 

 

 

AFOSR 2009

AFOSR 2010

AFOSR 2011

 

Highlight 2011

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AFOSR Publications

The Crossed Beams Machine

 

 

 

 

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