2 research outputs found
The Nonbilayer Lipid MGDG and the Major Light-Harvesting Complex (LHCII) Promote Membrane Stacking in Supported Lipid Bilayers
The
thylakoid membrane of algae and land plants is characterized
by its intricate architecture, comprising tightly appressed membrane
stacks termed grana. The contributions of individual components to
grana stack formation are not yet fully elucidated. As an <i>in vitro</i> model, we use supported lipid bilayers made of
thylakoid lipid mixtures to study the effect of major light-harvesting
complex (LHCII), different lipids, and ions on membrane stacking,
seen as elevated structures forming on top of the planar membrane
surface in the presence of LHCII protein. These structures were examined
by confocal laser scanning microscopy, atomic force microscopy, and
fluorescence recovery after photobleaching, revealing multilamellar
LHCII–membrane stacks composed of connected lipid bilayers.
Both native-like and non-native interactions between the LHCII complexes
may contribute to membrane appression in the supported bilayers. However,
applying <i>in vivo</i>-like salt conditions to uncharged
glycolipid membranes drastically increased the level of stack formation
due to enforced LHCII–LHCII interactions, which is in line
with recent crystallographic and cryo-electron microscopic data [Wan,
T., et al. (2014) <i>Mol. Plant 7</i>, 916–919; Albanese,
P., et al. (2017) <i>Sci. Rep. 7</i>, 10067–10083].
Furthermore, we observed the nonbilayer lipid MGDG to strongly promote
membrane stacking, pointing to the long-term proposed function of
MGDG in stabilizing the inner membrane leaflet of highly curved margins
in the periphery of each grana disc because of its negative intrinsic
curvature [Murphy, D. J. (1982) <i>FEBS Lett. 150</i>, 19–26]
A Versatile Dinucleating Ligand Containing Sulfonamide Groups
Copper,
iron, and gallium coordination chemistries of the new pentadentate
bis-sulfonamide ligand 2,6-bisÂ(<i>N</i>-2-pyridylmethylsulfonamido)-4-methylphenol
(psmpH<sub>3</sub>) were investigated. PsmpH<sub>3</sub> is capable
of varying degrees of deprotonation, and notably, complexes containing
the fully trideprotonated ligand can be prepared in aqueous solutions
using only divalent metal ions. Two of the copperÂ(II) complexes, [Cu<sub>2</sub>(psmp)Â(OH)] and [Cu<sub>2</sub>(psmp)Â(OAc)<sub>2</sub>]<sup>−</sup>, demonstrate the anticipated 1:2 ligand/metal
stoichiometry and show that the dimetallic binding site created for
exogenous ligands possesses high inherent flexibility since additional
one- and three-atom bridging ligands bridge the two copperÂ(II) ions
in each complex, respectively. This gives rise to a difference of
0.4 Å in the Cu···Cu distances. Complexes with
2:3 and 2:1 ligand/metal stoichiometries for the divalent and trivalent
metal ions, respectively, were observed in [Cu<sub>3</sub>(psmp)<sub>2</sub>Â(H<sub>2</sub>O)] and [MÂ(psmpH)Â(psmpH<sub>2</sub>)], where M = Ga<sup>III</sup>, Fe<sup>III</sup>. The deprotonated
tridentate <i>N</i>-2-pyridylsulfonylmethylphenolato moieties
chelate the metal ions in a meridional fashion, whereas in [Cu<sub>3</sub>(psmp)<sub>2</sub>Â(H<sub>2</sub>O)] the rare μ<sub>2</sub>-<i>N</i>-sulfonamido bridging coordination mode
is observed. In the bis-ligand mononuclear complexes, one picolyl
arm of each ligand is protonated and uncoordinated. Magnetic susceptibility
measurements on the doubly and triply bridged dicopperÂ(II) complexes
indicate strong and medium strength antiferromagnetic coupling interactions,
with <i>J</i> = 234 cm<sup>–1</sup> and 115 cm<sup>–1</sup> for [Cu<sub>2</sub>(psmp)Â(OH)] and [Cu<sub>2</sub>(psmp)Â(OAc)<sub>2</sub>]<sup>−</sup>, respectively (in H<sub>HDvV</sub> =...+<i>JS</i><sub>1</sub><i>S</i><sub>2</sub> convention).
The trinuclear [Cu<sub>3</sub>(psmp)<sub>2</sub>Â(H<sub>2</sub>O)], in which the central copper ion is linked to two flanking copper
atoms by two μ<sub>2</sub>-<i>N</i>-sulfonamido bridges
and two phenoxide bridges shows an overall magnetic behavior of antiferromagnetic
coupling. This is corroborated computationally by broken-symmetry
density functional theory, which for isotropic modeling of the coupling
predicts an antiferromagnetic coupling strength of <i>J</i> = 70.5 cm<sup>–1</sup>