Cargando…
The effect on ion channel of different protonation states of E90 in channelrhodopsin-2: a molecular dynamics simulation
Channelrhodopsin-2 (ChR2) is a cationic channel protein that has been extensively studied in optogenetics. The ion channel is opened via a series of proton transfers and H-bond changes during the photocycle but the detailed mechanism is still unknown. Molecular dynamics (MD) simulations with enhance...
Autores principales: | , , , , , , , |
---|---|
Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
The Royal Society of Chemistry
2021
|
Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8697799/ https://www.ncbi.nlm.nih.gov/pubmed/35424009 http://dx.doi.org/10.1039/d1ra01879e |
_version_ | 1784620124671574016 |
---|---|
author | Cheng, Jie Zhang, Wenying Zhou, Shuangyan Ran, Xu Shang, Yiwen Lo, Glenn V. Dou, Yusheng Yuan, Shuai |
author_facet | Cheng, Jie Zhang, Wenying Zhou, Shuangyan Ran, Xu Shang, Yiwen Lo, Glenn V. Dou, Yusheng Yuan, Shuai |
author_sort | Cheng, Jie |
collection | PubMed |
description | Channelrhodopsin-2 (ChR2) is a cationic channel protein that has been extensively studied in optogenetics. The ion channel is opened via a series of proton transfers and H-bond changes during the photocycle but the detailed mechanism is still unknown. Molecular dynamics (MD) simulations with enhanced sampling were performed on the dark-adapted state (i.e., D470) and two photocycle intermediates (P(1)(500) and P(2)(390)) to study the proton transfer path of the Schiff base and the subsequent conformational changes. The results suggest there are two possible proton transfer pathways from the Schiff base to proton acceptors (i.e., E123 or D253), depending on the protonation of E90. If E90 is protonated in the P(1)(500) state, the proton on the Schiff base will transfer to E123. The polyene chain of 13-cis retinal tilts and opens the channel that detours the blocking central gate (CG) and forms a narrow channel through the transmembrane helices (TM) 2, 3, 6 and 7. In contrast, if E90 deprotonates after retinal isomerization, the primary proton acceptor is D253, and an almost-open channel through TM1, 2, 3 and 7 is generated. The channel diameter is very close to the experimental value. The potential mean force (PMF) suggests that the free energy is extremely low for ions passing through this channel. |
format | Online Article Text |
id | pubmed-8697799 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2021 |
publisher | The Royal Society of Chemistry |
record_format | MEDLINE/PubMed |
spelling | pubmed-86977992022-04-13 The effect on ion channel of different protonation states of E90 in channelrhodopsin-2: a molecular dynamics simulation Cheng, Jie Zhang, Wenying Zhou, Shuangyan Ran, Xu Shang, Yiwen Lo, Glenn V. Dou, Yusheng Yuan, Shuai RSC Adv Chemistry Channelrhodopsin-2 (ChR2) is a cationic channel protein that has been extensively studied in optogenetics. The ion channel is opened via a series of proton transfers and H-bond changes during the photocycle but the detailed mechanism is still unknown. Molecular dynamics (MD) simulations with enhanced sampling were performed on the dark-adapted state (i.e., D470) and two photocycle intermediates (P(1)(500) and P(2)(390)) to study the proton transfer path of the Schiff base and the subsequent conformational changes. The results suggest there are two possible proton transfer pathways from the Schiff base to proton acceptors (i.e., E123 or D253), depending on the protonation of E90. If E90 is protonated in the P(1)(500) state, the proton on the Schiff base will transfer to E123. The polyene chain of 13-cis retinal tilts and opens the channel that detours the blocking central gate (CG) and forms a narrow channel through the transmembrane helices (TM) 2, 3, 6 and 7. In contrast, if E90 deprotonates after retinal isomerization, the primary proton acceptor is D253, and an almost-open channel through TM1, 2, 3 and 7 is generated. The channel diameter is very close to the experimental value. The potential mean force (PMF) suggests that the free energy is extremely low for ions passing through this channel. The Royal Society of Chemistry 2021-04-19 /pmc/articles/PMC8697799/ /pubmed/35424009 http://dx.doi.org/10.1039/d1ra01879e Text en This journal is © The Royal Society of Chemistry https://creativecommons.org/licenses/by-nc/3.0/ |
spellingShingle | Chemistry Cheng, Jie Zhang, Wenying Zhou, Shuangyan Ran, Xu Shang, Yiwen Lo, Glenn V. Dou, Yusheng Yuan, Shuai The effect on ion channel of different protonation states of E90 in channelrhodopsin-2: a molecular dynamics simulation |
title | The effect on ion channel of different protonation states of E90 in channelrhodopsin-2: a molecular dynamics simulation |
title_full | The effect on ion channel of different protonation states of E90 in channelrhodopsin-2: a molecular dynamics simulation |
title_fullStr | The effect on ion channel of different protonation states of E90 in channelrhodopsin-2: a molecular dynamics simulation |
title_full_unstemmed | The effect on ion channel of different protonation states of E90 in channelrhodopsin-2: a molecular dynamics simulation |
title_short | The effect on ion channel of different protonation states of E90 in channelrhodopsin-2: a molecular dynamics simulation |
title_sort | effect on ion channel of different protonation states of e90 in channelrhodopsin-2: a molecular dynamics simulation |
topic | Chemistry |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8697799/ https://www.ncbi.nlm.nih.gov/pubmed/35424009 http://dx.doi.org/10.1039/d1ra01879e |
work_keys_str_mv | AT chengjie theeffectonionchannelofdifferentprotonationstatesofe90inchannelrhodopsin2amoleculardynamicssimulation AT zhangwenying theeffectonionchannelofdifferentprotonationstatesofe90inchannelrhodopsin2amoleculardynamicssimulation AT zhoushuangyan theeffectonionchannelofdifferentprotonationstatesofe90inchannelrhodopsin2amoleculardynamicssimulation AT ranxu theeffectonionchannelofdifferentprotonationstatesofe90inchannelrhodopsin2amoleculardynamicssimulation AT shangyiwen theeffectonionchannelofdifferentprotonationstatesofe90inchannelrhodopsin2amoleculardynamicssimulation AT loglennv theeffectonionchannelofdifferentprotonationstatesofe90inchannelrhodopsin2amoleculardynamicssimulation AT douyusheng theeffectonionchannelofdifferentprotonationstatesofe90inchannelrhodopsin2amoleculardynamicssimulation AT yuanshuai theeffectonionchannelofdifferentprotonationstatesofe90inchannelrhodopsin2amoleculardynamicssimulation AT chengjie effectonionchannelofdifferentprotonationstatesofe90inchannelrhodopsin2amoleculardynamicssimulation AT zhangwenying effectonionchannelofdifferentprotonationstatesofe90inchannelrhodopsin2amoleculardynamicssimulation AT zhoushuangyan effectonionchannelofdifferentprotonationstatesofe90inchannelrhodopsin2amoleculardynamicssimulation AT ranxu effectonionchannelofdifferentprotonationstatesofe90inchannelrhodopsin2amoleculardynamicssimulation AT shangyiwen effectonionchannelofdifferentprotonationstatesofe90inchannelrhodopsin2amoleculardynamicssimulation AT loglennv effectonionchannelofdifferentprotonationstatesofe90inchannelrhodopsin2amoleculardynamicssimulation AT douyusheng effectonionchannelofdifferentprotonationstatesofe90inchannelrhodopsin2amoleculardynamicssimulation AT yuanshuai effectonionchannelofdifferentprotonationstatesofe90inchannelrhodopsin2amoleculardynamicssimulation |