Author:
Lincoln SF,Hambley TW,Pisaniello DL,Coates JH
Abstract
The molecular structure of
R,S,R,S-[Ni {(-N(Me)(CH2)2N(Me)(CH2)3-)2}
(OCHNMe2)](SO3CF3)2 has been
determined in the solid state by X-ray diffraction methods. The geometry about
nickel(11) is midway between square based pyramidal and trigonal bipyramidal with OCHNMe2 occupying the axial or
an equatorial site in these geometries respectively. The nickel(II) is
displaced 0.29 � from the least-squares tetraaza
plane on the same side as the four methyl groups and OCHNMe2. In OCHNMe2
solution the formation of this five-coordinate high-spin species by
coordination of OCHNMe2 by its four-coordinate low-spin precursor is
characterized by K(298.2 K) = 10 � 2, ∆H = -12.8 � 2.7 kJ mol-1
and ∆S = -24.1 � 9.O JK-l mol-1 as determined by spectrophotometry. 1H (300 MHz) n.m.r. studies
show that kwx(298.2 K) = (1.6 � 0.2) × 107
s-1, ∆H‡ = 27.8 � 0.4 kJ mol-1 and ∆S‡ =
-13.O � 2.0 JK-1 mol-1 characterize the exchange of
OCHNMe2 on R,S,R,S-[Ni {(-N(Me)(CH2)2N(Me)(CH2)3-)2
}(OCHNMe2)]2+.
Cited by
29 articles.
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