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withdrawing power of the groups neighbouring the halogen on the carbon
skeleton [51]. Chlorine in CH 3 Cl does not present any positive electrostatic
potential, but it appears in CH 2 FCl, and becomes even greater in CF 3 Cl; the
most positive chlorine potential in HOCH 2 CH 2 Cl is - 1.1 but it becomes 7.8
in O 2 NCH 2 CH 2 Cl. Similarly, the atomic charge increases with the fluorina-
tion degree in iodomethane derivatives, being 0.009 in CH 3 I and 0.165 in
CF 3 I [52].
The possibility to carefully tune the XB strength of a given halocarbon
by modifying the substituents on the carbon skeleton is also confirmed ex-
perimentally. As expected, the stronger an XB, the shorter the interaction
length (see onwards). The N
I-C interaction length in the infinite chain
given by 1,4-BPY with 1,4-diiodobenzene (1,4-DIB) is 3.032 A and the N
···
···
I
Table 2 Interaction of 1,4-DIB and 1,4-DITFB with XB acceptors
Co-crystals
I
···
Ndistance
I
···
Ninteraction
X-ray
DFT calculations
energy (DFT)
[A]
[A]
[kcal mol -1 ]
1,4-BPY · 1,4-DIB
3.032
3.151
3.29
1,4-BPY
·
1,4-DITFB
2.851
2.936
5.81
BPE
·
1,4-DIB
2.996
3.119
3.44
BPE
·
1,4-DITFB
2.810
2.891
6.02
·
HMTA
1,4-DIB
3.011
3.124
3.52
HMTA · 1,4-DITFB
2.844
2.919
6.07
On interaction with a variety of XB acceptors, 1,4-DITFB forms shorter and stronger con-
tacts than 1,4-DIB. Clearly, the electron withdrawing ability of fluorine boosts the donor
ability of the iodine atoms
Fig. 3 Due to the anisotropic distribution of the electron density, halogen atoms show
a negative electrostatic potential and a larger radius ( r max ) in the equatorial region and
a positive electrostatic potential and a smaller radius ( r min ) in the polar region. As a con-
sequence of this, halogens behave as nucleophiles at the equator and as electrophiles at
the pole
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