The structure of T3R3f hexameric human insulin has been determined at 100 K
from two different crystals at 1.2 and 1.3 Angstrom resolution and refined
to residuals of 0.169 and 0.176, respectively. Owing to a phase change, th
e c axis is double its room-temperature value and the asymmetric unit conta
ins two independent TRf insulin dimers. Compared with the orientation in th
e room-temperature structure, one dimer undergoes a rotation about the c ax
is of -5 degrees, while the second is rotated +4 degrees. A superposition o
f the backbone atoms of the two independent dimers shows that the C-alpha a
toms of five residues within the R-f-state monomers are displaced by more t
han 1.0 Angstrom; smaller displacements are observed for the T-state monome
rs. Four zinc ions lie on the crystallographic threefold axis and each form
s bonds to three symmetry-related HisB10 N-epsilon2 atoms from the T- and R
-f-state trimers. While three of the zinc ions are tetrahedrally coordinate
d with a chloride ion completing the coordination sphere, mixed tetrahedral
/octahedral coordination is observed for one of the T-state zinc ions. The
three symmetry-related 'phenolic binding sites' in one hexamer contain wate
r molecules and a glycerol molecule, but the same sites in the second hexam
er are occupied by a zinc ion coordinated to an alternate conformation of H
isB10, a symmetry-related HisB5 and two chloride ions. Two additional and p
artially occupied zinc ion sites are observed at the interface between the
two independent dimers. One zinc ion is coordinated by a T-state HisB5 of o
ne dimer, an R-state HisB5 of the second dimer and two water molecules; the
second zinc ion is coordinated by an alternate side-chain conformation of
the T-state HisB5 and three water molecules. The carboxyl group of one GluB
13 side chain, which exists in two discrete conformations, appears to be pr
otonated, because short contacts exist to a second carboxyl group or to a c
arbonyl O atom.