A simple and general method for writing Dot Structures - Lewis Structures is given in a previous
article entitled “Lewis
Structures and the Octet Rule”. Relevant worked examples were given in the following
articles: Examples #1,
#2,
#3
, #4,
#5,
#6,
#7,
#8, #9, #10, #11, #12,
#13, #14, #15, #16, #17, #18, #19, #20, #21, #22, #23, #24, #25, #26, #27, #28, #29, #30, #31, #32, #33, #34 , #35, #36 , #37, #38, #39 and #40.
Let us consider
the case of the BF molecule. Boron monofluoride is an unstable gas but forms stable ligands when combines with transition metals1, like the CO molecule. The experimental BF bond length has been found to be 1.263 Angstrom. The bond order for the BF bond has been calculated to be 1.4.2
Step 1: Connect the atoms with
single bonds.
Fig. 1 : Connect the atoms
of the BF molecule with single bonds.
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Step 2: Calculate the # of
electrons in π bonds (multiple bonds) using Lewis structure formula (1):
Where n in this
case is 2 since BF consists
of two atoms.
Where V = (3 +
7) = 10 , V is the number of valence electrons of the ion.
Therefore, P = 6n
+ 2 – V = 6 * 2 + 2 – 10 = 4 So, there are 2 double or 1
triple bond.
Since there are
only 2 atoms in the BF molecule there is no possibility that 2 double bonds
will be present.
Step 3 & 4: The Lewis electron dot resonance structures
of BF are
as follows:
Fig. 2 : Plausible Lewis
Resonance Structures of boron fluoride
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Resonance structure #3 is the most plausible since there is no
charge separation. Lewis resonance structure #2 is more possible than #1 since
there is less charge separation.
Quantum mechanical and theoretical studies have shown that the bond
order in BF is ~1.4 – the bond between the B and the F atom is between a single
and a double bond.
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