Michel Groesbeek

Helix packing in polytopic membrane proteins: role of glycine in transmembrane helix association.

The nature and distribution of amino acids in the helix interfaces of four polytopic membrane proteins (cytochrome c oxidase, bacteriorhodopsin, the photosynthetic reaction center of Rhodobacter sphaeroides, and the potassium channel of Streptomyces lividans) are studied to address the role of glycine in transmembrane helix packing. In contrast to soluble proteins where glycine is a noted helix breaker, the backbone dihedral angles of glycine in transmembrane helices largely fall in the standard alpha-helical region of a Ramachandran plot. An analysis of helix packing reveals that glycine residues in the transmembrane region of these proteins are predominantly oriented toward helix-helix interfaces and have a high occurrence at helix crossing points. Moreover, packing voids are generally not formed at the position of glycine in folded protein structures. This suggests that transmembrane glycine residues mediate helix-helix interactions in polytopic membrane proteins in a fashion similar to that seen in oligomers of membrane proteins with single membrane-spanning helices. The picture that emerges is one where glycine residues serve as molecular notches for orienting multiple helices in a folded protein complex.

Magic angle spinning NMR spectroscopy of membrane proteins.

The passage of molecules and information across cell membranes is mediated largely by membrane-spanning proteins acting as channels, pumps, receptors and enzymes. These proteins perform many tasks: they control electrochemical gradients across the membrane, receive signals from the environment or from other cells, convert light energy into chemical signals, transport small molecules into and out of cells, and harness proton gradients to generate the energy consumed in metabolism. Indeed, of the estimated 50000–100000 genes in the human genome, fully 20–40 % are thought to encode integral membrane proteins. If one also includes membrane-associated proteins, which are attached to the membrane surface through fatty acyl chains or electrostatic interactions, this percentage is likely to be much higher.

Implications of threonine hydrogen bonding in the glycophorin A transmembrane helix dimer.

The transmembrane helix of glycophorin A contains a seven-residue motif, LIxxGVxxGVxxT, that mediates protein dimerization. Threonine is the only polar amino acid in this motif with the potential to stabilize the dimer through hydrogen-bonding interactions. Polarized Fourier transform infrared spectroscopy is used to establish a robust protocol for incorporating glycophorin A transmembrane peptides into membrane bilayers. Analysis of the dichroic ratio of the 1655-cm(-1) amide I vibration indicates that peptides reconstituted by detergent dialysis have a transmembrane orientation with a helix crossing angle of <35 degrees. Solid-state nuclear magnetic resonance spectroscopy is used to establish high resolution structural restraints on the conformation and packing of Thr-87 in the dimer interface. Rotational resonance measurement of a 2.9-A distance between the gamma-methyl and backbone carbonyl carbons of Thr-87 is consistent with a gauche- conformation for the chi1 torsion angle. Rotational-echo double-resonance measurements demonstrate close packing (4.0 +/- 0.2 A) of the Thr-87 gamma-methyl group with the backbone nitrogen of Ile-88 across the dimer interface. The short interhelical distance places the beta-hydroxyl of Thr-87 within hydrogen-bonding range of the backbone carbonyl of Val-84 on the opposing helix. These results refine the structure of the glycophorin A dimer in membrane bilayers and highlight the complementary role of small and polar residues in the tight association of transmembrane helices in membrane proteins.

Spectral tuning in salamander visual pigments studied with dihydroretinal chromophores.

In visual pigments, opsin proteins regulate the spectral absorption of a retinal chromophore by mechanisms that change the energy level of the excited electronic state relative to the ground state. We have studied these mechanisms by using photocurrent recording to measure the spectral sensitivities of individual red rods and red (long-wavelength-sensitive) and blue (short-wavelength-sensitive) cones of salamander before and after replacing the native 3-dehydro 11-cis retinal chromophore with retinal analogs: 11-cis retinal, 3-dehydro 9-cis retinal, 9-cis retinal, and 5,6-dihydro 9-cis retinal. The protonated Schiffs bases of analogs with unsaturated bonds in the ring had broader spectra than the same chromophores bound to opsins. Saturation of the bonds in the ring reduced the spectral bandwidths of the protonated Schiffs bases and the opsin-bound chromophores and made them similar to each other. This indicates that torsion of the ring produces spectral broadening and that torsion is limited by opsin. Saturating the 5,6 double bond in retinal reduced the perturbation of the chromophore by opsin in red and in blue cones but not in red rods. Thus an interaction between opsin and the chromophoric ring shifts the spectral maxima of the red and blue cone pigments, but not that of the red rod pigment.

SYNTHESIS OF DOUBLY AND MULTIPLY ISOTOPICALLY LABELED RETINALS

Abstract— In this paper a consecutive synthetic scheme is described that allows the synthesis of multiply 13C labeled retinals with labels in the conjugated chain. This scheme can be extended to incorporation of 2H labels in the conjugated chain. Also carotenoids can be multiply 13C labeled with this strategy. The same approach has been used to label amino acids.

Changes in structure of the chromophore in the photochemical process of bovine rhodopsin as revealed by FTIR spectroscopy for hydrogen out-of-plane vibrations

The hydrogen out-of-plane bending (HOOP) vibrations were studied in the difference Fourier transform infrared spectra of lumirhodopsin and metarhodopsin I by use of a series of specifically deuterated retinal derivatives of bovine rod outer segments. The 947 cm-1 band of lumirhodopsin and the 950 cm-1 band of metarhodopsin I were assigned to the mode composed of both 11-HOOP and 12-HOOP vibrations. This result suggests that the perturbation near C12-H of the retinal in the earlier intermediate, bathorhodopsin (Palings, van den Berg, Lugtenburg and Mathies, Biochemistry, 28 (1989) 1498-1507), is extinguished in lumirhodopsin and metarhodopsin I. Unphotolyzed rhodopsin and metarhodopsin I exhibited the 14-HOOP bands in the 12-D derivatives at 901 and 886 cm-1, respectively. Lumirhodopsin, however, did not show the 14-HOOP in the 12-D derivatives. The result suggests a change in geometrical alignment of the C14-H bond in lumirhodopsin with respect to the N-H bond of the Schiff base.

A Resonance Raman Study Of the C=C Stretch Modes in Bovine and Octopus Visual Pigments with Isotopically Labeled Retinal Chromophores

Abstract— Previous resonance Raman spectroscopic studies of bovine and octopus rhodopsin and bathorhodopsin in the C–C stretch fingerprint region have shown drastically different spectral patterns, which suggest different chromophore‐protein interactions. We have extended our resonance Raman studies of bovine and octopus pigments to the C=C stretch region in order to reveal a more detailed picture about the difference in retinal‐protein interactions between these two pigments. The C=C stretch motions of the protonated retinal Schiff base are strongly coupled to form highly delocalized ethylenic modes located in the 1500 to 1650 cm−1 spectral region. In order to decouple these vibrations, a series of 11,12‐D2‐labeled retinals, with additional 13C labeling at C8, C10, C11 and C14, respectively, are used to determine the difference of specific C=C stretch modes between bovine and octopus pigments. Our results show that the C9=C10 and C13=C14 stretch mode are about 20 cm−1 lower in the Raman spectrum of octopus bathorhodopsin than in bovine bathorhodopsin, while the other C=C stretch modes in these two bathorhodopsins are similar. In contrast, only the C9=C10 stretch mode in octopus rhodopsin is about 10 cm−1 lower than in bovine rhodopsin, while other C=C stretches are similar.

Structure of hypsorhodopsin : analysis by Fourier transform infrared spectroscopy at 10 K

Abstract— Vibrational bands of hypsorhodopsin in the difference Fourier transform infrared spectra were identified as the bands which arose after formation of isorhodopsin by successive irradiations of bovine rhodopsin at 10 K with >500 nm light, and also as the bands disappeared upon conversion to bathorhodopsin by warming. The chromophore bands were assigned by the bands which shifted upon deuterium substitution of the polyene chain of the retinylidene chromophore. The presence of chromophore bands which shift by D2O exchange clearly shows that the Schiff base chromophore of hypsorhodopsin is protonated. The amide I bands and several other protein bands of hypsorhodopsin appeared at the same frequencies as those of bathorhodopsin, but they are different from those of rhodopsin and isorhodopsin. Furthermore, like bathorhodopsin, hypsorhodopsin displays the Cl—H out‐of‐plane bending mode which is weakly coupled with C12‐‐–H out‐of‐plane mode. These facts show that hypsorhodopsin has a chromophore conformation and chromophore‐opsin interaction more similar to bathorhodopsin than to rhodopsin and isorhodopsin.