{"title":"离子通过生物膜通道的势能分布的物理模型","authors":"C. Zou, K. Cheng","doi":"10.1109/SBEC.1995.514421","DOIUrl":null,"url":null,"abstract":"To attempt to explain what determines a single particle (an ion or an ion group) penetration of a cell membrane channel, a physical model of potential energy profiles V/sub 2/(x) of a channel is proposed, based on the authors' previous study of one dimensional (1-D) steady state Schrodinger equation in a single particle system and in a time independent field. In this model, a V/sub 2/(x) is simplified as an effective constant height of potential energy barrier V/sub 2/ in a channel to obtain analytical solutions in mathematics. This model elucidates that: (1) Ion selectivity of a channel is determined by V/sub 2/. V/sub 2/ is divided into a V/sub 2c/ for a cation and V/sub 2a/ for an anion. V/sub 2c/ and V/sub 2a/ may be or may be not the same value depending on electrical characteristics of the particles and the channel. It is called a cation channel if a V/sub 2c/ is much lower than a V/sub 2a/ and vice versa. It is called a cation-anion cotransporter if a V/sub 2e/ and a V/sub 2a/ are equal or almost equal. (2) Whether a particle can penetrate through a channel is mostly determined by the repulsion energies (barriers) rather than the attraction energies (wells). (3) A channel's conformation can be changed when the channel is stimulated strongly enough. The variation of the conformation could influence V/sub 2/(x) and V/sub 2/, and eventually result in open or close of the channel.","PeriodicalId":332563,"journal":{"name":"Proceedings of the 1995 Fourteenth Southern Biomedical Engineering Conference","volume":"1 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1995-04-07","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"A physical model of potential energy profiles of ions going through a biological membrane channel\",\"authors\":\"C. Zou, K. Cheng\",\"doi\":\"10.1109/SBEC.1995.514421\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"To attempt to explain what determines a single particle (an ion or an ion group) penetration of a cell membrane channel, a physical model of potential energy profiles V/sub 2/(x) of a channel is proposed, based on the authors' previous study of one dimensional (1-D) steady state Schrodinger equation in a single particle system and in a time independent field. In this model, a V/sub 2/(x) is simplified as an effective constant height of potential energy barrier V/sub 2/ in a channel to obtain analytical solutions in mathematics. This model elucidates that: (1) Ion selectivity of a channel is determined by V/sub 2/. V/sub 2/ is divided into a V/sub 2c/ for a cation and V/sub 2a/ for an anion. V/sub 2c/ and V/sub 2a/ may be or may be not the same value depending on electrical characteristics of the particles and the channel. It is called a cation channel if a V/sub 2c/ is much lower than a V/sub 2a/ and vice versa. It is called a cation-anion cotransporter if a V/sub 2e/ and a V/sub 2a/ are equal or almost equal. (2) Whether a particle can penetrate through a channel is mostly determined by the repulsion energies (barriers) rather than the attraction energies (wells). (3) A channel's conformation can be changed when the channel is stimulated strongly enough. The variation of the conformation could influence V/sub 2/(x) and V/sub 2/, and eventually result in open or close of the channel.\",\"PeriodicalId\":332563,\"journal\":{\"name\":\"Proceedings of the 1995 Fourteenth Southern Biomedical Engineering Conference\",\"volume\":\"1 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1995-04-07\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Proceedings of the 1995 Fourteenth Southern Biomedical Engineering Conference\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/SBEC.1995.514421\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Proceedings of the 1995 Fourteenth Southern Biomedical Engineering Conference","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/SBEC.1995.514421","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
A physical model of potential energy profiles of ions going through a biological membrane channel
To attempt to explain what determines a single particle (an ion or an ion group) penetration of a cell membrane channel, a physical model of potential energy profiles V/sub 2/(x) of a channel is proposed, based on the authors' previous study of one dimensional (1-D) steady state Schrodinger equation in a single particle system and in a time independent field. In this model, a V/sub 2/(x) is simplified as an effective constant height of potential energy barrier V/sub 2/ in a channel to obtain analytical solutions in mathematics. This model elucidates that: (1) Ion selectivity of a channel is determined by V/sub 2/. V/sub 2/ is divided into a V/sub 2c/ for a cation and V/sub 2a/ for an anion. V/sub 2c/ and V/sub 2a/ may be or may be not the same value depending on electrical characteristics of the particles and the channel. It is called a cation channel if a V/sub 2c/ is much lower than a V/sub 2a/ and vice versa. It is called a cation-anion cotransporter if a V/sub 2e/ and a V/sub 2a/ are equal or almost equal. (2) Whether a particle can penetrate through a channel is mostly determined by the repulsion energies (barriers) rather than the attraction energies (wells). (3) A channel's conformation can be changed when the channel is stimulated strongly enough. The variation of the conformation could influence V/sub 2/(x) and V/sub 2/, and eventually result in open or close of the channel.