# Boron monofluoride monoxide

Boron monofluoride monoxide or oxoboryl fluoride or fluoroxoborane is an unstable inorganic molecular substance with formula FBO. It is also called boron fluoride oxide, fluoro(oxo)borane or fluoro-oxoborane. The molecule is stable at high temperatures, but below 1000 °C condenses to a trimer (BOF)$_3$ called trifluoroboroxin. FBO can be isolated as a triatomic non-metallic molecule in an inert gas matrix, and has been condensed in solid neon and argon. When an attempt is made to condense the gas to a solid in bulk, a polymeric glass is formed, which is deficient in fluoride, and when heated forms a glassy froth like popcorn. Boron fluoride oxide has been studied because of its production in high energy rocket fuels that contain boron and fluorine, and in the form of an oxyfluoride glass. BOF glass is unusual in that it can condense directly from gas.

## Properties
### Monomer

The FBO molecule is linear with structure F-B=O. The F-B bond length is 1.283 Å, and B-O bond is 1.207 Å.
The infrared spectrum of BFO has vibrational bands at 1900, 1050, and 500 cm$^{−1}$. Spectroscopic constants of the $^{10}$BFO molecule are B=9349.2711 MHz D=3.5335 kHz and for $^{11}$BFO molecule they are B=9347.3843 MHz D=3.5273 kHz The monomer is stable either at low pressures, or temperatures over 1000 °C. Below this temperature, the monomers associate to form a trimer called trifluoroboroxole.
Heat of formation Δ$_f$H$^⦵$ $_{298K}$ is predicted to be -146.1 kcal/mol. Proton affinity 149.6 kcal/mol.

### Trimer

If a hot BFO gas is cooled slowly it dismutates back into B$_2$O$_3$ and BF$_3$. At room temperature this dismutation completes in an hour.
Boron fluoride oxide forms a trimer with a ring composed of alternating oxygen and boron atoms, with fluorine bonded to the boron. (BFO)$_3$. The ring structure puts it in the class of boroxols. This is also called trifluoroboroxin. The trimer is the predominant form in gas at 1000K. When heated to 1200K it mostly converts to the monomer BFO. Boron oxyfluoride can be condensed from vapour to a fluorine deficient glass at temperatures below 190° by very rapid cooling. When heated this deposit has a temperature at which it loses more BF$_3$ to form a frothy or porous glass that resembles popcorn. The glass deposited at lower temperatures has a higher proportion of fluorine. Deposits at -40 °C are predicted to have a 1:1 ratio of fluorine to oxygen. Below -135° (BFO)$_3$ is stable.
The heat of formation of the trimer from the monomer (BFO)$_3$ → 3BFO is 131 kcal/mol.

### Glass

Boron oxyfluoride glass is transparent and colourless. It is stable in dry air, but it is hygroscopic and in normal air becomes white and opaque. When heated the glass will encounter a glass transition temperature (T$_g$) at which it ceases to be a glass, and produces BF$_3$ gas and a boron oxyfluoride with less fluorine is left behind. This glass transition temperature is determined from where the pressure of BF$_3$ produced exceeds the strength of the glass. The hypothetical structure of BOF glass, is of long chains of B-O-B-O with fluorine attached to each boron. These can be considered as BO$_2$F triangles linked in a chain by O atoms. These chains are tangled up like spaghetti in the glass. When the substance becomes fluorine deficient, crosslinks with oxygen form between the chains, and it becomes more two dimensional in structure. BF$_3$ is produced when the terminals of two linear −(BF)O− chains join with each other. These ends contain -O-BF$_2$, and when two meet, BF$_3$ can be eliminated and the chain extended with oxygen.

## Occurrence

BFO is expected to form in supernovae II output in gas between 1,000 and 2,000 °C and pressures around 10$^{−7}$ bar.

## Preparation

Otto Ruff noticed that a mixture of BF$_3$ and SiF$_4$ passing over molten B$_2$O$_3$ produced some SiO$_2$ and redistributed B$_2$O$_3$ into cold parts of the reaction tube. He speculated that there must be some heat stable intermediate that converted back into the original components on cooling. Several years later, Paul Baumgarten and Werner Bruns made the boron oxyfluoride trimer by passing BF$_3$ over solid B$_2$O$_3$ at 450 °C.
BFO is an intermediate in the hydrolysis of BF$_3$ along with BF(OH)$_2$, BF$_2$OH and boric acid.
* BF$_3$ + H$_2$O → BFO + 2HF;
* BF$_2$OH → BFO + HF;
* BF(OH)$_2$ → BFO + H$_2$O
Another way in which BFO can be made is to vapourise B$_2$O$_3$ with BF$_3$.
When BF$_3$ is heated with air, BFO gas predominates from 2800° to 4000 °C, being a maximum at 3200°. Above 4000 °C BO dominates.
Hot BF$_3$ passed over some oxides such as SiO$_2$ forms BFO. Other oxides that can yield boron oxyfluoride are magnesium oxide, titanium dioxide, carbonates or alumina.
In the plasma phase HF reacts with BO$_2$H$^+$ $_2$, B$_2$OH$^+$, B$_3$O$^+$ $_4$, B$_2$O$^+$ $_4$, B$_2$O$^+$ $_2$, B$_2$OH$^+$ to make FBO, and other products including FBOH and FBO$^+$.

## Related

The B-O-F molecule theoretically exists but it releases energy when it rearranges to F-B-O. A related molecule is BOF$_2$. Molecules related to the trimer include B$_3$O$_3$ClF$_2$, B$_3$O$_3$Cl$_2$F, and (BOCl)$_3$.
FBO is predicted to be able to insert noble gas atoms between the fluorine and boron atom yielding FArBO, FKrBO and FXeBO. The molecules are predicted to be linear.

## Uses

Boron oxyfluoride could be used in boriding steel. By using a gas, sticking solids onto the steel is avoided. Also this method allows control of the boron concentration, and mostly forms Fe$_2$B instead of the more brittle FeB. Burning boron releases much energy, so its use in explosives or fuel is being researched. To maximise energy output, both fluorine and oxygen are used to react, and thus FBO and related molecules are formed and may be in the exhaust.