scholarly journals Aspartic acid 85 in bacteriorhodopsin functions both as proton acceptor and negative counterion to the Schiff base.

1992 ◽  
Vol 267 (36) ◽  
pp. 25730-25733 ◽  
Author(s):  
S Subramaniam ◽  
D.A. Greenhalgh ◽  
H.G. Khorana
1989 ◽  
Vol 86 (23) ◽  
pp. 9228-9232 ◽  
Author(s):  
H. Otto ◽  
T. Marti ◽  
M. Holz ◽  
T. Mogi ◽  
M. Lindau ◽  
...  

2016 ◽  
Vol 113 (14) ◽  
pp. E1993-E2000 ◽  
Author(s):  
Oleg A. Sineshchekov ◽  
Hai Li ◽  
Elena G. Govorunova ◽  
John L. Spudich

A recently discovered family of natural anion channelrhodopsins (ACRs) have the highest conductance among channelrhodopsins and exhibit exclusive anion selectivity, which make them efficient inhibitory tools for optogenetics. We report analysis of flash-induced absorption changes in purified wild-type and mutant ACRs, and of photocurrents they generate in HEK293 cells. Contrary to cation channelrhodopsins (CCRs), the ion conducting state of ACRs develops in an L-like intermediate that precedes the deprotonation of the retinylidene Schiff base (i.e., formation of an M intermediate). Channel closing involves two mechanisms leading to depletion of the conducting L-like state: (i) Fast closing is caused by a reversible L⇔M conversion. Glu-68 in Guillardia theta ACR1 plays an important role in this transition, likely serving as a counterion and proton acceptor at least at high and neutral pH. Incomplete suppression of M formation in the GtACR1_E68Q mutant indicates the existence of an alternative proton acceptor. (ii) Slow closing of the channel parallels irreversible depletion of the M-like and, hence, L-like state. Mutation of Cys-102 that strongly affected slow channel closing slowed the photocycle to the same extent. The L and M intermediates were in equilibrium in C102A as in the WT. In the position of Glu-123 in channelrhodopsin-2, ACRs contain a noncarboxylate residue, the mutation of which to Glu produced early Schiff base proton transfer and strongly inhibited channel activity. The data reveal fundamental differences between natural ACR and CCR conductance mechanisms and their underlying photochemistry, further confirming that these proteins form distinct families of rhodopsin channels.


2021 ◽  
Author(s):  
Elamathi Chennakrishnan ◽  
R. J. Butcher ◽  
Mohankumar Amirthalingam ◽  
Palanisamy Sundararaj ◽  
Kuppanagounder Elango ◽  
...  

Quinoline based Schiff base 6-methyl-2-oxo-1,2-dihydro-quinoline-3carboxaldehyde-4(N)-phenylsemicarbazone (6MPS) sensor has been developed for selective sensing of methionine and aspartic acid in aqueous medium through selective detection of copper ion as “on-off-on” type....


Biochemistry ◽  
2014 ◽  
Vol 53 (37) ◽  
pp. 5923-5929 ◽  
Author(s):  
Jun Sasaki ◽  
Hazuki Takahashi ◽  
Yuji Furutani ◽  
Oleg A. Sineshchekov ◽  
John L. Spudich ◽  
...  

2018 ◽  
Vol 115 (14) ◽  
pp. 3557-3562 ◽  
Author(s):  
Albert Ardevol ◽  
Gerhard Hummer

Channelrhodopsin-2 (ChR2) is a light-sensitive ion channel widely used in optogenetics. Photoactivation triggers a trans-to-cis isomerization of a covalently bound retinal. Ensuing conformational changes open a cation-selective channel. We explore the structural dynamics in the early photocycle leading to channel opening by classical (MM) and quantum mechanical (QM) molecular simulations. With QM/MM simulations, we generated a protein-adapted force field for the retinal chromophore, which we validated against absorption spectra. In a 4-µs MM simulation of a dark-adapted ChR2 dimer, water entered the vestibules of the closed channel. Retinal all-trans to 13-cis isomerization, simulated with metadynamics, triggered a major restructuring of the charge cluster forming the channel gate. On a microsecond time scale, water penetrated the gate to form a membrane-spanning preopen pore between helices H1, H2, H3, and H7. This influx of water into an ion-impermeable preopen pore is consistent with time-resolved infrared spectroscopy and electrophysiology experiments. In the retinal 13-cis state, D253 emerged as the proton acceptor of the Schiff base. Upon proton transfer from the Schiff base to D253, modeled by QM/MM simulations, we obtained an early-M/P2390–like intermediate. Rapid rotation of the unprotonated Schiff base toward the cytosolic side effectively prevents its reprotonation from the extracellular side. From MM and QM simulations, we gained detailed insight into the mechanism of ChR2 photoactivation and early events in pore formation. By rearranging the network of charges and hydrogen bonds forming the gate, water emerges as a key player in light-driven ChR2 channel opening.


2021 ◽  
Author(s):  
◽  
Orawan Jakdetchai

KR2 is a light-driven sodium ion pump found in marine flavobacterium Krokinobacter Eikastus. The protein belongs to the microbial rhodopsin family, which is characterized by seven transmembrane helices and a retinal cofactor covalently bound to a conserved lysine residue through a Schiff base linkage. Specific features of KR2 and other sodium pumping rhodopsins are the NDQ motif, the N-terminal helix capping the protein at the extracellular side, and the sodium ion bound at the protomer interface in the pentameric structure. The ability to pump sodium ions was a surprising discovery since the positive charge at the Schiff base was long thought to hinder the transport of non-proton cations and the Grotthuss mechanism could not be applied to explain the Na+ transport. The photocycle of KR2 revealed by flashed photolysis and ultrafast femtosecond absorption spectroscopy consists of consecutive intermediates, named K, L, M, and O. Here, DNP-enhanced ssNMR was used to analyze various aspects of these intermediate states. The K/L-state can be generated and trapped by in-situ illumination inside the magnet at 110 K. The trapping of L-state together with the K-state at this temperature is unexpected as this usually leads to the trapping of only K-state in bacteriorhodopsin (BR), proteorhodopsin (PR), and channelrhodopsin 2 (ChR2). This observation suggests a lower energy barrier between K- and L-state in KR2. For the O-state, the intermediate was generated by illuminating outside the magnet, followed by rapid freezing in liquid nitrogen and transfer to the magnet. Based on these procedures, the retinal conformation, and the electrostatic environment at the Schiff base in KR2 dark, K-, L- and O-intermediates were probed using 13C-labeled retinals bound to 15N-labeled KR2 by both 1D and 2D magic angle spinning (MAS) NMR experiments. The obtained data show an all-trans retinal conformation with the distortion of 150° at H-C14-C15-H in the dark state whereas the retinal has a 13-cis, 15-anti conformation in the K- and L-state after light activation. Differences between K- and L-intermediates were observed. The retinal chemical shifts of the K-state show a large deviation from the model compound behavior between the middle and end part of the polyene chain. In the L-state, these differences are much less pronounced. These observations indicate that the light energy stored in the K-state dissipates into the protein in the subsequent photointermediate states. Furthermore, an additional shielding observed for C14 in L-state indicates the slight rotation toward a more compact 13-cis, 15-syn conformation. The distortion of the H-C14-C15-H angle in the L-state (136°) is larger than in the dark state. This twist of the retinal in the L-state would play an important role in lowering the pKa of the Schiff base, which is a prerequisite for the proton transfer from the Schiff base to the proton acceptor (D116). The electrostatic environments at the Schiff base in K- and L-states cause a de-shielding of the 15N nitrogen compared to the dark state. This indicates a stepwise stronger interaction with the counterion as the Schiff base proton moves away from the Schiff base and comes closer to the D116 in the transition from K- to L-state and approaches the proton transfer step during the M-state formation. In the O-state, the retinal was found to be in the all-trans conformation but differed to the dark state in the C13, C20, and Schiff base nitrogen chemical shifts. The largest effect (9 ppm) was observed for the Schiff base nitrogen, which could be explained by the effect of the positive charge of bound Na+ near the Schiff base in the O-state, coordinated by N112 and D116 as observed in the O-state crystal structure in the pentameric form. The structural change at the opsin followed the retinal isomerization and the energy transfer from the chromophore to the surrounding were also investigated in this thesis using various amino acids labeling schemes. Moreover, 1H-13C hNOE in combination with CE-DNP was applied to probe the dynamics of retinylidene methyl groups and 23Na MAS NMR was employed to detect the bound sodium ion at the protomer interface in KR2 dark state.


Biochemistry ◽  
1994 ◽  
Vol 33 (36) ◽  
pp. 10878-10882 ◽  
Author(s):  
Frank Jaeger ◽  
Karim Fahmy ◽  
Thomas P. Sakmar ◽  
Friedrich Siebert

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