From owner-chemistry@ccl.net Wed Oct 11 01:22:01 2006 From: "Dr. Ponnadurai Ramasami ramchemi__intnet.mu" To: CCL Subject: CCL: Second Workshop on Computational Chemistry and Its Applications (Part of ICCS 2007)/ Call for Paper Message-Id: <-32754-061011011858-11448-5DtVt5UGAVOLf8tI3VDqFA(_)server.ccl.net> X-Original-From: "Dr. Ponnadurai Ramasami" Content-Type: multipart/alternative; boundary="----=_NextPart_000_0022_01C6ED17.5433F600" Date: Wed, 11 Oct 2006 09:26:27 +0400 MIME-Version: 1.0 Sent to CCL by: "Dr. Ponnadurai Ramasami" [ramchemi~!~intnet.mu] This is a multi-part message in MIME format. ------=_NextPart_000_0022_01C6ED17.5433F600 Content-Type: text/plain; charset="iso-8859-1" Content-Transfer-Encoding: quoted-printable Dear All This is a first call for The Second Workshop on Computational Chemistry = and Its Applications (Part of ICCS 2007). Please visit http://pages.intnet.mu/ramasami/iccs_2007.htm=20 Kind regards Ramasami ------=_NextPart_000_0022_01C6ED17.5433F600 Content-Type: text/html; charset="iso-8859-1" Content-Transfer-Encoding: quoted-printable
Dear All
This is a first call for The = Second=20 Workshop on Computational Chemistry and Its Applications (Part of ICCS=20 2007).
Please visit http://pages.intnet.mu/ramasami/iccs_2007.htm<= FONT=20 face=3D"Book Antiqua" size=3D4> 
Kind regards
Ramasami
------=_NextPart_000_0022_01C6ED17.5433F600-- From owner-chemistry@ccl.net Wed Oct 11 02:39:01 2006 From: "Rafal A. Bachorz rafal.bachorz-#-chemie.uni-karlsruhe.de" To: CCL Subject: CCL: Ionization potential and Electron affinity of Donor-Acceptor system Message-Id: <-32755-061011023729-9175-WYXd0PHle5xilLBvxRHofA/./server.ccl.net> X-Original-From: "Rafal A. Bachorz" Content-Disposition: inline Content-Transfer-Encoding: 7bit Content-Type: text/plain; charset=ISO-8859-1; format="flowed" Date: Wed, 11 Oct 2006 08:34:31 +0200 MIME-Version: 1.0 Sent to CCL by: "Rafal A. Bachorz" [rafal.bachorz~~chemie.uni-karlsruhe.de] Dear Agalya, > Can anyone tell me how to calculate ionization potential of donor and > electron affinity of acceptor in donor-acceptor system? > > In one journal in have seen, that they mentioned HOMO energy as the > ionization potential of donor and LUMO energy as the electron > affinity of acceptor. That would be correct from the point of view of Koopmans theorem. Koopmans theorem sometimes works fine for ionization potentials, but it is almost always wrong about the electron affinity which is much more difficult to evaluate. > Is that the correct way of calculating ionization potential of donor > and electron affinity of acceptor in donor-acceptor system? I would say that it is a very crude approximation, but perhaps it is the only one way you can afford the calculation for you systems. Probaly the most correct way is to use the definition of the quantities of you interest: EA=E_N-E_A IP=E_N-E_C where E_N is the energy of the neutral, E_A is the energy of the anion and E_C is the energy of the cation. Have a good day, Rafal -- www.bachorz.eu From owner-chemistry@ccl.net Wed Oct 11 03:13:01 2006 From: "Alfred Gil agil-#-cesca.es" To: CCL Subject: CCL: =?ISO-8859-1?Q?Schr=F6dinger_Seminar_on_Drugs_Design_=26?= =?ISO-8859-1?Q?_Jaguar?= Message-Id: <-32756-061011022235-2695-VIGG9D0YaIO6PlWNpvW6TA=server.ccl.net> X-Original-From: Alfred Gil Content-Type: multipart/alternative; boundary="------------080404060400060906020903" Date: Wed, 11 Oct 2006 08:22:04 +0200 MIME-Version: 1.0 Sent to CCL by: Alfred Gil [agil]~[cesca.es] This is a multi-part message in MIME format. --------------080404060400060906020903 Content-Type: text/plain; charset=ISO-8859-1; format=flowed Content-Transfer-Encoding: 8bit Dear CCL users, Schrödinger and CESCA have the pleasure of announcing a seminar on drugs design and Jaguar package which will be held at CESCA on October, 18th. This seminar will focus on structure-based lead discovery, structure-based lead optimization and ligand-based design. Furthermore, the Schrödinger's vision for future software solutions in drug discovery will be presented. In addition, an overview of Jaguar will be shown. Jaguar is a high-performance /ab initio/ package for both gas and solution phase simulations, with particular strength in treating metal containing systems, making it the most practical quantum mechanical tool for solving real-world problems. The main topics to be covered are the following: § Accurate docking and scoring for lead optimization § Introduction of Quantum Mechanics in protein/ligand docking § PHASE: A New Engine for Pharmacophore Perception, 3D QSAR Model Development, and 3D Database Screening § Overview of Jaguar: an /ab inito/ electronic structure package Schedule: 9.30 am-13.00 pm Address: CESCA Gran Capitŕ, s/n (Edifici Annexus) 08034 Barcelona Attending is free, but it's necessary to register in advance by sending an email to secretaria++cesca.es . Cordially, ------------------------------------------------------------------------ Departament de Secretaria i Promoció Gran Capitŕ, 2-4 (Edifici Nexus) . 08034 Barcelona T. 93 205 6464 . F. 93 205 6979 . promocio ++cesca.es --------------080404060400060906020903 Content-Type: multipart/related; boundary="------------050908020702050301030102" --------------050908020702050301030102 Content-Type: text/html; charset=ISO-8859-1 Content-Transfer-Encoding: 7bit
Dear CCL users,
 
Schrödinger and CESCA have the pleasure of announcing a seminar on drugs design and Jaguar package which will be held at CESCA on October, 18th.
 
This seminar will focus on structure-based lead discovery, structure-based lead optimization and ligand-based design. Furthermore, the Schrödinger’s vision for future software solutions in drug discovery will be presented. In addition, an overview of Jaguar will be shown. Jaguar is a high-performance ab initio package for both gas and solution phase simulations, with particular strength in treating metal containing systems, making it the most practical quantum mechanical tool for solving real-world problems.

The main topics to be covered are the following:

§         Accurate docking and scoring for lead optimization

§         Introduction of Quantum Mechanics in protein/ligand docking

§         PHASE: A New Engine for Pharmacophore Perception, 3D QSAR Model Development, and 3D Database Screening

§        Overview of Jaguar: an ab inito electronic structure package
Schedule: 9.30 am-13.00 pm
 
Address:
 
CESCA
Gran Capità, s/n (Edifici Annexus)
08034 Barcelona
 
Attending is free, but it's necessary to register in advance by sending an email to secretaria++cesca.es.
 
Cordially,
 

Departament de Secretaria i Promoció

Gran Capità, 2-4 (Edifici Nexus) 08034 Barcelona
T. 93 205 6464 F. 93 205 6979 • promocio++cesca.es

--------------050908020702050301030102 Content-Type: image/jpeg Content-Transfer-Encoding: base64 Content-ID: /9j/4AAQSkZJRgABAQEBLAEsAAD/4Qu+RXhpZgAATU0AKgAAAAgABwESAAMAAAABAAEAAAEa AAUAAAABAAAAYgEbAAUAAAABAAAAagEoAAMAAAABAAIAAAExAAIAAAAdAAAAcgEyAAIAAAAU AAAAj4dpAAQAAAABAAAAowAAAM0AAAEsAAAAAQAAASwAAAABQWRvYmUgUGhvdG9zaG9wIENT IE1hY2ludG9zaAAyMDA0OjExOjEyIDEwOjQ0OjE3AAADoAEAAwAAAAEAAQAAoAIABAAAAAEA AAIqoAMABAAAAAEAAAFeAAAAAAAGAQMAAwAAAAEABgAAARoABQAAAAEAAAEbARsABQAAAAEA AAEjASgAAwAAAAEAAgAAAgEABAAAAAEAAAErAgIABAAAAAEAAAqLAAAAAAAAAEgAAAABAAAA SAAAAAH/2P/gABBKRklGAAEBAAABAAEAAP/bAEMACAYGBwYFCAcHBwkJCAoMFA0MCwsMGRIT DxQdGh8eHRocHCAkLicgIiwjHBwoNyksMDE0NDQfJzk9ODI8LjM0Mv/bAEMBCQkJDAsMGA0N GDIhHCEyMjIyMjIyMjIyMjIyMjIyMjIyMjIyMjIyMjIyMjIyMjIyMjIyMjIyMjIyMjIyMjIy Mv/AABEIADwAXwMBIgACEQEDEQH/xAAfAAABBQEBAQEBAQAAAAAAAAAAAQIDBAUGBwgJCgv/ xAC1EAACAQMDAgQDBQUEBAAAAX0BAgMABBEFEiExQQYTUWEHInEUMoGRoQgjQrHBFVLR8CQz YnKCCQoWFxgZGiUmJygpKjQ1Njc4OTpDREVGR0hJSlNUVVZXWFlaY2RlZmdoaWpzdHV2d3h5 eoOEhYaHiImKkpOUlZaXmJmaoqOkpaanqKmqsrO0tba3uLm6wsPExcbHyMnK0tPU1dbX2Nna 4eLj5OXm5+jp6vHy8/T19vf4+fr/xAAfAQADAQEBAQEBAQEBAAAAAAAAAQIDBAUGBwgJCgv/ xAC1EQACAQIEBAMEBwUEBAABAncAAQIDEQQFITEGEkFRB2FxEyIygQgUQpGhscEJIzNS8BVi ctEKFiQ04SXxFxgZGiYnKCkqNTY3ODk6Q0RFRkdISUpTVFVWV1hZWmNkZWZnaGlqc3R1dnd4 eXqCg4SFhoeIiYqSk5SVlpeYmZqio6Slpqeoqaqys7S1tre4ubrCw8TFxsfIycrS09TV1tfY 2dri4+Tl5ufo6ery8/T19vf4+fr/2gAMAwEAAhEDEQA/APYdTtNRlkuvJFwWZkMLxT7VVAV3 Lt3L8xw3Pv1FVpdN1ySB4xdP5biQhTKVeM4+QbgeR078HuQafqg1w3dwLIzrHvTBwpUR4XO0 ZB3Z3fhn2q9M16k9uxW5khWEECHALSd9+T0xjH457V2qUoxVmv6RJnR6drMepBnmme1+1Fwq TE4j+bGcuD6Z7YxwTml1Cx1mW8umt2uFhaUHif76fJwo3DbjD55XOe9MC+Jmj+cMtzsdAUdf LBYqVbp/CC499oqU3OvFJC1tKshQqFTaVDmMAEH0DhvzFXefNe8RE+o22qNexSWfmlBEAwM2 BkHJAGfvHpzke470ZNM12RpbhrmcBpMi3SXkIW3YzvAyBxwR35PFSmPxKV2+aoIDssgVTnMg AVl74TcQfpnpzpaQ+qF7ldRjwhbfAdwJC9Npx34B/wCBH0qeaVON04u33j3M23sNYjnc3bTz wGZ2VIrgqQD90klhwOcgHHI4PNIbTX18s25ZZFGZzNPuWZxzlRztU4weBw3TiunorH6zK97I djmLbT9eglFzcXUlwYmCmFHx5yg8tydoPtx1PNC6fr8HlGGbc48t5TJcMwcqgBQA5xuJb06C unoo+syvsvuCxzcllqzQoFFwJQ2bhvtPEwzzs5+XIyBwMZ/GtXSYJbayMciNGgc+VE77mjTs pPOe/c+mav0VE6zlHlaCwUUjMFUsxAUDJJPArnLj4g+EbW4ME3iHTxIDggTBsH6jilTo1Kml OLforg2ludJRWdP4g0a1sLe+uNVsobS4AMM8k6qkmRkbSTg8VT/4TXwt/wBDJpP/AIGR/wCN NUKstVF/cF0btFRWt1b3ttHc2s8c8EgykkTBlYeoI61x/j7xZqmiWJtPD2k3moapIPvw27SJ bj1bA6+g/wAl0cPOtUVKO/npb1BtJXNfxJ4y0LwnCH1a+SJ2GUhUbpH+ij+fSsTwv8VvDviv Vxplp9pgumBMS3CACTAycEE8455r5r1+x8Qx3TX/AIgs9QinuWJ868iZC59iwrW+GELzfEfR drbRHMZXYnAVVUk5P0FfXPh3DU8JKpKfNJJu620MPbNysfW9Fc1N8QvCFvOYZPEWnhwcHEwY D8RxXQwTw3VvHcW8iSwyqHSRDkMp5BB9K+PnRqU0nOLV+6N00ySishfFXh9tS/s5da083vme V9nFwu/fnG3bnOc9q16UoSh8SsO54X8cvF16uoW/hawleONoxJc7DgyFj8qfTv759q0/DfwI 0ddLhl16e5nvZFDPHC+xIyf4fU49a5z466Fd2Pie08RwoxtpkRC4HCSJ0B+ox+Rrv/Dfxi8L 6npULajfLp96FAlimVsbu5VgMEV9VN4mnltF4C9nfmcd7/n3/Aw0c3zHMfG/TbfR/Anh/TbQ MLe2uPKjDtk7Qhxk1h+HPDnwtuvDlhPq+tGHUXhBuI/tO3a/cYxxXQfHe9ttR8GaHeWcyzW0 10XjkXowKHkVheG7L4SP4b099aulXUzCDcrvm4fv0GPyrfCSmstg25p8zvyK73e4pW53seka x4n0X4ffDyyk0yUTwtGI9PDNu8zPO7PcAHP6d60/FV94jfw1Be+DEtbudysh83B3xFScryAT nFfOHj7X7bWtcjtNKZv7G06MWtiuTjYOrc88n9AK6zwrbfFjwssa6fpl3LZ9RbXBV48H0G7K /hisp5NGnShWlJc7bbU9L36PzXXzYKpd26HMeOvF/ifxA8Nh4kt0t5LRyyx+QYmBIxznrXKW 5uPN8q3Zw837vCHBbJ6fyr6k8eeDn8b+HNNimto7fUxLEWcYPkqf9YM9wBn6kCvJPiv4Rfwf r+najpkBTT/KiSJwMhZYxjn3OAffmvUyvNcNVjHDwioyd9Ftdf5/oyJwa1O50D4DaJDp0Ta3 cXNzesoMiwybEQ+g7nHrXe6vd2ngrwPPNHkQada7IQ7ZJIG1Bn64Fc9oHxi8Karp0Ut7fpp9 3tHmwTK2A3fDAYIrkvjn4qhutE0nSdPnEsd9i6dk6NGPufmST+FfOqjj8bjIUcXe1+u2m9um xteMY3ieWLpmqw6FH42EjZ/tIxh8c7wN+/6ZyK+sNA1eHXtAsdVgx5d1CsmAeh7j8DkV8+ye DviZ/wAIf/Yz2Sf2Qi+b5IeLI53Z65zXZfAPxB9q0O90KZ/3lm/mwg/8826j8G/9Cr0c7gsV hnWjKMnCX2Xe0XtfzIpvllbuetXtla6jZyWl5BHPbyja8ci5Vh9K4Kf4J+C5rgyraXMQJz5c dw239cmvRKK+VoYuvQv7KbjfszdxT3OcvvAvh3UtDsdGvLAzWNjj7PGZXG3Ax1BBPHrXL+Iv hb4K0zwzqt/Don722s5Zk/0iU/MqEj+L1Fel1Fc28V3azW06B4ZkMbqe6kYI/KtaOPxFOStU la97Jv5/eJxT6Hw+DggjqK9M8N+OviX4k1KLTNJ1JpJMAE/Zotsa9MsdvAqS1+HujT/EGfRW luxaJKQAJF3Y9M7a+gNB8N6T4ZsBZ6TZx28XViOWc+rMeSa+yznM8PSpx5qSlJrS6TSOenBt 7kmiWN5YabHFqGoSX96RmadwFDN7KAABVi/0+01Syks763juLaQYeORcg1Zor4Nzk5c+z8tD qsedTfBLwXLOZFtbqJSc+Wlw239cmtmX4a+FLi5tLifTDLNaRxxws88nyqn3RjOP0rrKK6ZZ ji5WvVlp5snkj2Cuc0XwH4b8Pao+paVp/wBmunVlZ1mcggnJGCcdhXR0Vzwq1IRcYyaT38/U dkz/2f/bAEMABQMEBAQDBQQEBAUFBQYHDAgHBwcHDwsLCQwRDxISEQ8RERMWHBcTFBoVEREY IRgaHR0fHx8TFyIkIh4kHB4fHv/bAEMBBQUFBwYHDggIDh4UERQeHh4eHh4eHh4eHh4eHh4e Hh4eHh4eHh4eHh4eHh4eHh4eHh4eHh4eHh4eHh4eHh4eHv/AABEIAF8AlgMBIgACEQEDEQH/ xAAdAAEAAgIDAQEAAAAAAAAAAAAABwgFBgIECQMB/8QARBAAAQMDAgQEAwMGDAcBAAAAAQID BAUGEQASBxMhQQgiMWEUFVEycZEJFkJScoEkMzZic3WClaGxs9IjJzQ1VpPC0f/EABwBAAEF AQEBAAAAAAAAAAAAAAACAwQFBwEGCP/EADURAAECBAUCBAQEBwEAAAAAAAECEQADBCEFEjFB YQZRE3GBkRQiMqEVgrHRI1KiwdLh8PH/2gAMAwEAAhEDEQA/ALQXBJnzbyjW6zWX6NHVAXLD sdLZekrCwkoSXEqSEoBBVgZO9HUAHOqVWs3RGfveVHqtReiUSI4IruYvJ3ppzToUpPL5ilFx ZVkEJ6gYwMakGvxLdqYYptfjUqZzFbmY81Dbm5Q6ZSlfqevbXVNJsw1pTZplANUUzyVJLDPP LfL27D03beX0x6benpq2pqmVLSM0t7fyg7gu+t9OPK0NkE7xqTtyXBKr8S150p6kVNNLmSJD sRpBRICCxyn2S4lQ2ncsFByUkkHPlUcNFuW6GKnZ8U1yoyTUqfT5DzjzMUR1OPOKLgeIQlSQ UJUlvZjz7QSc9ZXnv0iPJjJnvQWn3MtRw8pKVK3YylGepzgZA9tfOXEoLEZQlxqa0wy02hXN QgJQ2lWWwc9AkKHlHoCOmly66SlIHgi/A1vcWffR9mgKT3jWuFc2vVJmbOq8me80uQ+hgvLj 8rah9xA2JbQFjASB5ydavKue4afSFVFFxOTZE16sNfBOss/wVEcSi283tQFYSWW0nfuB3j0O MyRQ4FsxnHKhQ4dIZXMUeZIhtNpL6sknKkjzHOT376/YlHtqK7KXEpdIYcnLU3KU1HbSZCjk qSvA85PUkHPfSfi5ImrUZdi1mFrG27d7attBlLC8Yuz36s3Zr02sTJLcjll0P1FyOoNjlg7i WUpSEA5OD19evprW7UuGstVWjUaq1SW/NVUFM1AvmOttwKhLdRyltISChRQVDIC/UEYxrfaL TqFTGHINGg02E0pSlOMRGkNpKuiSSlIHXoAddFNDs1NGk0pNHoIpiVF6RFEZrkBQJG9SMbc5 SepH6J+mkJqJLzMyPq0sLbf8Ny1xHWNrxoVIuC86xc8RimzJT7AdcdXsRGEcxxUn2ypwqHMI +HbARy+pIBPQk6x6Lmu2Pw5pldmz7hW5OfjqWqMmE66tstOrXyEcsAZ2p6LycDA65zMUOJT4 6gIcWKyWWkxxym0pKEJ6pR09EjOQPTrrq063Lepy1Lp9CpcNSnA4osRG2yVjOFHA9RuVg+5+ un/xKnc/wQzhrDmz+o22jmQ94063Z9cuGQmLULoNMch0uHJUaeGCJanUFS39ziFAtZG0bcDI VknIx15tcrIturXcm43GpMCc+w3Rg2zyVlt5TaI6sp5hdcATghQ8y0kAp6HeJltW5NZjMzKB SpLcQkxkOw21pZyc+QEeXr9Nc3aBQnayitO0WmrqaAAmYqKgvpwMdF43envpr42nzPkt2Yeo /N31GgeDKe8RnU+JNbjLqTCIzZW3VFyI7m3yilRni3JWf5wUytPtz2jrki4LzRLn1JUyUmjt V74JbkhEblpT80aZCWdg3hIZ5oWXO+0pPqdSiqmU1UZUZVPiFhTa21NllO0oWcrSRjGFHqR3 765Lp8BcJ6EuFGVFf385ktJKHN5JXuTjB3EknPrk50r8QpkgBMka3e9v3/u8GRXeI+r1Trku s1BqHcc2AzHuWLTkCK2wRynI0dawSttXUKWsg9txBzgAdFniXUPmNyONR3ZUQQpL1CSqG6hL zkVJ3DmbQlzmkFaNhPkQdSVCo1HhQGoEKlQY0RlfMaYajoQ2hWc7gkDAOeuRr7IgQUMxWUQo yWomPhkBpISzhJSNgx5cJJHTsSNJFbTBOVUp2DbDtc2dyR30JD3gynvGlTpNTpFLplQj3ZKr ap82GghSI/LWha/MWghAISoHAyVYGOuck4qjzpyIVvXsa/8AG1GuvRIsiAWWQ3scX52msIDq SzvWo7lH+LXuH6u/Qbct6C869CoNLjOvOJdcWzEbQpa0nKVEgdSCSQexOuUagUKLVnavGotN ZqL2eZLbioS8vPrlYGTn79ArZISRld+Ehx248xe3sZTGS0001Uw5Ef3/AE34m60PSLSfuGK9 SHYqG0ttlIdLqSApSyAjoM7u2OnXXR4e0Kr0i8pZrKqm/IUIwMlMVpcaQpEBhtbheKeaCVoW MbgOg6dTmTtNWKcSWmSZLBiG+7+np+0IyB3jR1xfgL0rEmq25JqwqTrBgy2mEPBppLaE8hWT lsJcC3MnCTzPXII1hKZR7tVd0q4qlSI64NcLsaVGMguOMsJT/BStop2p2bDnCj5pCj26Snpo RiKkgjKLgDfQBrX4B8w8GSIZTbt6IgW5JpdGjsfmvTIpYjuSSyt+SW0GSEpSkpXubBZBUU4U tZ99ZcM1Vl8yPkVUWIFzOVNSUsjLsdxtxvLfXzKHMCin1wDjJwNSfpp1eLLX9SB999d+T6kx wS2iJabalfm3FHrjCZVGlJFTlRHHeoQp6U0ptt9APmSttJJT6jsUqSCEGz6nIh27Kq1Nfivq qk41qJHdDiHYxfkSmkKOPOnnBnHpkOKBGFKGpa00KxicQzDjj6v8nHYhxu54YiNuHtMvGmXU 9Vq3AYSzcCFPTUsylOqjPpJUyFJKQEhLR5JKSrJbR9+pJ001Cqqk1K85AG1uNPYW8hC0pYND TTTUaOw0000QQ0000QQ0000QQ0000QQ0000QQ0000QQ0000QQ0000QQ1jLnr9GtiiyK1X6jH p8COMuPPKwB9AO5J7AZJ7axnEu+KBw+tWRcNwSeWw35Wmk4Lkhwjo2gdyfwAyT0GvPTjNxUu TifcBn1d4sQGlH4KntqPKjp/+lnuo9T7DAHremOlKjG5mc/LKGqu/A5+w+0MTp4ljmJo4seL WrS5DtP4dwUU+KCUiozGwt5fuhs+VA/a3H2Goej8cOLLNTTUE31V1upVu2LcCmj7FsjZj2xq O9NbXRdNYXRSvClyEnuSASfMn/yK5U5ai5MemXAO/TxH4ZU65H2W2ZpKo81tv7KXkHBI9iMK A7bsa3zUC+BSE7F4HF9wEJmVWQ83nukBDf8AmhWp618+49TSqXEp8mT9KVEDi+nppFpKJKAT DTTTVTDkNNNNEENNNNEEdC4qxTbfocyt1iUiJAhNKefdX6JSP8z2AHUnA1RXjH4lb0u2ovxL YmSLcoYUUtJjK2SXk/rLcHVJP6qSAPTr66lr8oFcsmFaVv2tHcUhupyHJEnBxuSyE7Un23Lz 96BqH/Bzw4pl+cQ5Muux0SqVRWUyHI6xlLzqlYbSod09FKI77QD0J1qfSmE0NDha8ark5mfK DdgC2mjk2D6RCnrUpfhpjSaFbvFe6WxUqRTLtqjazkSm0vLSo+y/Q/jq4vg8pt80mx6tCvqP WWJSahuipqS1qVyi2noncThOQeg76m5pttppLTSEttoASlKRgJA9AB21y1QY71lMxanNN4CU pcEHUhubfpDsqnEsu8ebN68TuI0e8q3Hj33crTLVQkIbbRU3glKQ4oAAbugA1sCYvicUkKSe JRBGQQ7K6/46jK/f5dV/+s5P+qrVyI3i64atx2m1Ui6cpQEnEVnsP6bWl4v8RRyZBoKNM1xf 5Rawb3v7RDlsonMpoxPhJY4wtcQairiF+d3yz5WsM/NlvFrnc1vGN5xu27vfGdWZqM2LT4ip Ux5LTQUlGT3UpQSlI+pKiAB3JA1HnB3jTavFKoz4NvQqvHdgspedM1ltAIUcDG1auuoF8SfH EHjFQ6LSnS7QrWqzEqeGz/1UhtwFSfcIAKR/Oyew1m0/C6/HsXVLXIEpQS6gAwAAt6qsBEsL TKlu7xZ27LOs2syVVq7aXAqSYjSilVSAWxGbAyohKvIn0yVYz06nAAEfGX4Ygcf8tP8A1Rf/ AM1I1WiUHiLw+kQ25vxVGrkIoTIiudShY+0k9iPoR6jBHbVOeJ/hVvW3ubNtR9u5oCcnlIAa lIH7BOF/2Tk/q6R07IpaomRW1a5KgWAdh7mwL7Wjs0qTdKXjUfFQ5ZTnFEKsL5N8o+Xs/wDa koDPMyvd9jpu9M/u1FGvtNiyoMt2HNjvRpLKyh1l1BQtCh6gg9QfbXyKFhAcKVBBJAVjoSMZ H+I/HW7UFMKWmlyQoqygBzqeYrFHMSYk6dxsvGPZVJsy1pztvUanRg0fhFbX5DhypxxTg6jc tSjtTjAODn11iaFbvFe6WxUqRTLtqjazkSm0vLSo+y/Q/jrdvB1w5pl+cQ5EuusIlUqispkO R1jKX3VKw2lQ7p6KUR32gHoTq/rTbbTSGmkJbbQAlKUjASB6ADsNZ/1B1PS9P1BpaSQkrN1E 9ze+5J11/wBSpUlU0ZlG0Qj4O6bfNJsirQr6j1liSmoboqaktalcotpGE7icJyD0Hc6kfi3d bVkcN65c7hSFwoqiwFeinleVtP71lOtp1VD8oDePKg0OxYrvmeUajNSD+inKGgfYnmH+yNZ9 h8pXUWOJzJAC1OoDQAa+7e5iWs+FLitCuI3EFSio3zc2ScnFVf8A92r9eGS9F3xwdo9SlSFP 1GIkwZylKypTreBuUe5UkoUT9VHVV7N4V/MvCXct4qjZqJnImxFbevw8bchzB+nneJ/YGs74 B7x+W3tU7Nku4Yq7HxEYE+j7QJIH7SCon9ga0LqympMUw2eqlSAqnXdgNgM3pf8ApiJIKkLG beLr6aaaxWLGKs/lB7fkybetm5WW1KYgvvRZBAzt5oSpBPtltQ+8jUWeDLiHS7I4hyqfXJCI tNrjKGDIWcIaeQolsqPZJ3KTnsSCemdXjvC3qVddtT7drcYSIE5otuo9CO4UD2UCAQexA1Qf jD4fb4sSoPvQafJr1D3EszYbRWpCfo6hOSgjufs+/bWr9J4nQ4jhKsFrFZTdtnBLhuQdt7cx BnoUhfiJj0NSpKkhSSFJIyCDkEa/deYlucS+JFrx002j3bW4LDflRG56lIR7BCsgfcBq4/g4 uS9rns6sz70mVCW8JyUxXJbWzLfLBO3oARnXncd6JqMIp1VKpqVJBA3BL8afeHpVSJhZopBf v8uq/wD1nJ/1VauhG8JvC9yM04qVcWVIBOJjfcf0eqp3vYF9v3pXH2LKuR1pyoyFoWilvFKk lxRBBCeoOtgFa8SISEh3iSABgAMShgfhrS8YlVVbJkChq0ysov8ANq4Dadr+8QpZSknMl4n2 97ZtHw2cPK7cVpSqma1WWk06GJb6XNrhyd6QEj7I3K7jIA76pItanFqWtRUtRypROST9dbLf txX1VpaKbe9VrkmTBUSmNU3HN7BUAT5V9Ukjb+7GsbaKIbl2Uhuocr4NU5hMjmnCOWXE7txP oMZzqywHDJmHU65tRM8Wau5V3AHygeQ/WEzVhZYBhGf4b8Ub44fSAq2a4+xGKtzkN3/iR3Pr ls9AT9Rg++rleG7j2jilOkUCp0UU6tRopkqWwsqYeQFJSojPVBypPQk/fr7fmt4ZPpw//vJn /frN2tUOBNkCTKtur2VTHH0hLqok5lTrgB6JGFFR6/ojv21nPUOLYfi8lRTRLE46KZr8tr6v EuVLXLP1WiK/G3w3+e1W1axb1PDleqk75W4hsYMjKCpClfshCsqPon16DWm+KXhIxYXCCy/l aOcmmvPM1OQlP8a++lCuYfoMtlIz6DaNXIajw6g9Cq64y+a02ox+cgpU2FgZO09UqIAHXqAS OmSNfC77epV121Pt6txhIgTmi06j0P1CgeygQCD2IGqbDer6mi+FkqcokkuNy7hvyg259IcX ICsx7xRrwZcQ6XZHESVArkhEWm1thLBkrOENPJVlsqPZJ3KTnsSCemdX5SpK0hSVBSSMgg5B GvPPjD4fb4sSoPvQKfJr1D3EszYbRWtCfo6hOSkjufs+/bWoW7xL4j2tGTTqRdtbgx2uiI3P UUI9ghWQn7gNe0xvpin6mmDEMPnpcgO+ltNLgtYgiI8ucZIyLEenalBKSpRAAGST215k8dbv N88Vq7cKHCuK5ILUP6BhvyN4+mQN33qOp9sC/wDiVV/Dhes6eK7Xq3KlJp9O5cRS3EodbAWp IQn0SkrOfrjUd+GnhPcVT4w0dVzWpVYlJglUx8z4DjbSygeRHnSAcrKencA6idLYfK6fVV1V UtJVLGUMdWAUWe97AW1Bjs9Zm5Up3jDUTj/f9Hspmz4RpAo7UQwwyuCCVNkEKyc9ScnJ99aD Y1wSrUvCk3JCzz6dLbkBION4SfMk+xGQfY69OPzNtD/xWhf3e1/t1T7xg8KatH4nNVaz7Vmy afUoaFuN0yApbbLyPIoYbThOUhB9yTqf091ThdfULpU04leICSXDKO72GoJhM2QtICndounR qhEq9Ih1WC6HYkxhEhhY/SQtIUk/gRpqI/B7PuBXCVqg3LR6nTZlGfVHaE2KtkuMHzII3gZx lSenoEjTWRYnR/BVcyndwkkA9xsfURPQrMkGJn0001BhUcFMsqXvU0gqHcpGdc9NNDwQ0000 QR5i8dZj0/jPeUh8kqFalNjPZKHVISPwSNaXqyPix4J3BAvipXrQo7UujVV4yHhzkIXHfV1W CFEbgo5UCM+pB9MnReG/h/4hXu4h2LEhwKfuwuZJlIKU/clBKif3Ae+vpHDcdw4YZKnmalKQ kC5FiBo2r8RULlLzkNEWRmH5UluNGZcffdUENttpKlLUTgAAdST9NXS8Lnh5FsrjXnfMZDla GHINPVhSYf0WvsXPoPRP3/ZkDgnwItDhmlE5tBq9e24VUZKAC39Q0jqGx75KvfHTUsazjqrr pVak0tA4lnVWhVwOw+543lyKbL8ytYaaaazWJkNcFMsqXvU02VfUpGdc9NDtBDTTTRBDTTTR BDTTTRBH/9k= --------------050908020702050301030102-- --------------080404060400060906020903-- From owner-chemistry@ccl.net Wed Oct 11 03:49:00 2006 From: "Karol Langner karol.langner===kn.pl" To: CCL Subject: CCL: Second Workshop on Computational Chemistry and Its Applications (Part of ICCS 2007)/ Call for Paper Message-Id: <-32757-061011025226-19905-ZDaXArFlIDjoaK3DbWvrNw[-]server.ccl.net> X-Original-From: Karol Langner Content-Disposition: inline Content-Transfer-Encoding: 7bit Content-Type: text/plain; charset="utf-8" Date: Wed, 11 Oct 2006 08:51:42 +0200 MIME-Version: 1.0 Sent to CCL by: Karol Langner [karol.langner .. kn.pl] On Wednesday 11 of October 2006 07:29, Dr. Ponnadurai Ramasami ramchemi__intnet.mu wrote: > Please visit http://pages.intnet.mu/ramasami/iccs_2007.htm=20 This link does not work from where I am. -- written by Karol Langner Wed Oct 11 08:49:30 CEST 2006 From owner-chemistry@ccl.net Wed Oct 11 04:24:01 2006 From: "Nehru Viji Shankaran chat2viji#,#gmail.com" To: CCL Subject: CCL: SMILE to 2D structure Message-Id: <-32758-061011030852-28829-ZYTHldgG3BcBP2czlrZ18Q]^[server.ccl.net> X-Original-From: "Nehru Viji Shankaran" Date: Wed, 11 Oct 2006 03:08:52 -0400 Sent to CCL by: "Nehru Viji Shankaran" [chat2viji^-^gmail.com] Dear all, I want a program which would convert the SMILE strings (simple)into 2D structure probably a connection table,z-matrix. If possible kindly provide me with the source code for it. Thanks in advance, Nehru viji Shankaran. nehruviji:+:yahoo.co.in chat2viji:+:gmail.com. From owner-chemistry@ccl.net Wed Oct 11 04:59:00 2006 From: "Alain Borel alain.borel*o*epfl.ch" To: CCL Subject: CCL: Second Workshop on Computational Chemistry and Its Applications (Part of ICCS 2007)/ Call for Paper Message-Id: <-32759-061011044057-25719-rzywyrICdJ8nA2TPGV8t1Q*_*server.ccl.net> X-Original-From: Alain Borel Content-Transfer-Encoding: 8bit Content-Type: text/plain; charset=ISO-8859-1 Date: Wed, 11 Oct 2006 10:40:45 +0200 MIME-Version: 1.0 Sent to CCL by: Alain Borel [alain.borel]*[epfl.ch] Karol Langner karol.langner===kn.pl wrote: > Sent to CCL by: Karol Langner [karol.langner .. kn.pl] > On Wednesday 11 of October 2006 07:29, Dr. Ponnadurai Ramasami > ramchemi__intnet.mu wrote: > >>Please visit http://pages.intnet.mu/ramasami/iccs_2007.htm=20 > > > This link does not work from where I am. It does if you remove the final =20. It's a silly line ending added by some e-mail programs. Best regards, Alain Borel Bibliothčque Scientifique Commune UNIL-EPFL BCH EPFL - SB - SCGC-BCH 1015 Lausanne, Switzerland. Tel.: +41 21 693 9800 Fax.: +41 21 693 9805 e-mail: alain.borel at epfl.ch http://biscom.epfl.ch From owner-chemistry@ccl.net Wed Oct 11 05:34:00 2006 From: "enb===rice.edu" To: CCL Subject: CCL:G: ***SPAM*** CCL:G: PM3 parameters Message-Id: <-32760-061011050132-16441-QTSK6M3f/1F8NgNs+FMNPg],[server.ccl.net> X-Original-From: enb_-_rice.edu Content-Transfer-Encoding: 8bit Content-Type: text/plain; charset=ISO-8859-1 Date: Wed, 11 Oct 2006 03:06:13 -0500 MIME-Version: 1.0 Sent to CCL by: enb..rice.edu There are two arguments as to how correlation enters semi-empirical calculations. 1) AM1 and PM3 (and subsequent methods) contain modified core-core repulsion functions based on Gaussians. By correctly optimizing these parameters, you could create a core-core interaction that replicates van der Waals distances, etc, effectively mimicking the role of correlation. I believe this is what the quote you attached refers to. 2) HF does poorly for heats of formation, while correlated methods do much better. Since the parameters are fit versus experimental values, the idea is that you get parameters that would approach the values from correlated calculations. For example, in MNDO (and maybe AM1, in PM3 they are optimized if I remember correctly) the one-center two-electron integrals come from experiment, and are lower than analytical values. This lowering is attributed to implicit inclusion of correlation effects in the experimental values. Ed Brothers. Quoting "T-Tsuru coral t-tsuru]-[coral.dti.ne.jp" : > Sent to CCL by: "T-Tsuru coral" [t-tsuru . coral.dti.ne.jp] > Hello, CCLers. > > I like to know the parameters which play important roll of electron > correlation in > PM3 method. > > I've read Stewart's PM3 paper (J.Comp.Chem. 10, p209, 1989) and know there > are > 18 parameters each atom (Hydrogen is 11.) But I can't find suitable > parameters from > them. The description of the parameters for electron correlation of this > paper is: > In other words, the correlation effects, which in ab initio methods > require > extensive calculations of the Meiller-Plesset type, can, at the MNDO > level > of approximation, be represented by simple gaussian functions. > > I can't imagine the relationship between the parameters and gaussian > functions. > > PM3 is derived from MNDO method. In the point of view of the parameter's > meaning, > there are common parameters between PM3 and MNDO. So I've read several > articles > of MNDO, but I can't find the suitable description too. > > If you know such PM3 parameters or article description, please teach me. > When I receive the replies, I will summarize them and send to CCL. > > > > Thanks. > > Sincerely yours, > ---------------------------------------------------- > Telkuni Tsuru t-tsuru]-[coral.dti.ne.jp > Bunshi Gijyutu> > > > > !DSPAM:452c332815629162251375! > From owner-chemistry@ccl.net Wed Oct 11 06:09:01 2006 From: "Dr. Ponnadurai Ramasami ramchemi=intnet.mu" To: CCL Subject: CCL: Fw: Second Workshop on Computational Chemistry and Its Applications (Part of ICCS 2007)/ Call for Paper Message-Id: <-32761-061011050350-21257-kbCmKt1w9WF3queLgY9yqg,,server.ccl.net> X-Original-From: "Dr. Ponnadurai Ramasami" Content-Type: multipart/alternative; boundary="----=_NextPart_000_0047_01C6ED36.C26DF200" Date: Wed, 11 Oct 2006 13:11:27 +0400 MIME-Version: 1.0 Sent to CCL by: "Dr. Ponnadurai Ramasami" [ramchemi::intnet.mu] This is a multi-part message in MIME format. ------=_NextPart_000_0047_01C6ED36.C26DF200 Content-Type: text/plain; charset="iso-8859-1" Content-Transfer-Encoding: quoted-printable Dear All This is a first call for The Second Workshop on Computational Chemistry = and Its Applications (Part of ICCS 2007). Please visit http://pages.intnet.mu/ramasami/iccs_2007.htm=20 If the link does not work, contact me ramchemi%intnet.mu Kind regards Ramasami ------=_NextPart_000_0047_01C6ED36.C26DF200 Content-Type: text/html; charset="iso-8859-1" Content-Transfer-Encoding: quoted-printable

Dear All
This is a first call for The = Second=20 Workshop on Computational Chemistry and Its Applications (Part of ICCS=20 2007).
Please visit http://pages.intnet.mu/ramasami/iccs_2007.htm<= FONT=20 face=3D"Book Antiqua" size=3D4> 
If the link does not work, = contact me ramchemi%intnet.mu
Kind regards
Ramasami
------=_NextPart_000_0047_01C6ED36.C26DF200-- From owner-chemistry@ccl.net Wed Oct 11 07:30:00 2006 From: "Marcin Krol mykrol*cyf-kr.edu.pl" To: CCL Subject: CCL: PCM vs. explicit water with PCM - effect on reaction profile Message-Id: <-32762-061011070701-19414-/g4lbIUpJUNpwVImvZRD1Q##server.ccl.net> X-Original-From: Marcin Krol Content-Type: TEXT/PLAIN; charset=US-ASCII Date: Wed, 11 Oct 2006 11:38:00 +0200 (METDST) MIME-Version: 1.0 Sent to CCL by: Marcin Krol [mykrol=-=cyf-kr.edu.pl] Dear Gonzalo, The problem of adding explicit solvent molecules to continuum solvation models was recently discussed in: Kelly etal, JCTC 1:1133-1152, 2005 The authors were able to get better solvation energy estimate if they added one explicit solvent molecule to the solute and performed implict solvent calculations on such system using their SM6 model. However, for other implicit solvation models adding an explict solvent molecule made the results worse (which goes in line with what you wrote). See also papers by JR Pliego JPCA 105:7241, 2001; JPCA 106:7434, 2002 where he developed and tested mixed implict-explict solvent models. Hope this helps marcin On Tue, 10 Oct 2006, Gonzalo Jimenez Oses gonzalo.jimenez*_*dq.unirioja.es wrote: > Sent to CCL by: "Gonzalo Jimenez Oses" [gonzalo.jimenez+*+dq.unirioja.es] > Dear CCL'ers > > I am also very interesting in the differences emerging from introducing > one or more explicit solvent molecules in PCM calculations (or any other > continuum models). I also asked something related to this question, and > probably the most valuable answer I obtained was offered by Dr. Frank > Jensen (thank you!): > > "One thing to consider is that PCM type models are parameterized models, > and the values of the parameters have been derived to fit experiments, > _without_ an explicit first solvation shell. A large fraction of > solvation is the first shell, and that has been absorbed by the > parameters. Introducing an explicit solvation shell and then put a PCM > on top of that may therefore give you a kind of double counting. Of > course the cavity changes, and there are the usual problems of electron > density outside the cavity, etc.... In short, there is a risk that the > results will _deteriorate_ when putting in an explicit first solvation > shell. I am not aware of any study where the performance of PCM type > models where the first solvation shell is considered explicitly, but if > you find any, I would appreciate the reference(s). In principle such an > approach should be able to provide more accurate results than a pure > continuum model, but the PCM parameters may have to be returned. This, > of course, is not trivial, and the optimal set of parameters may depend > on which method you use for the solvent molecules (HF, DFT, MP2, etc). > Sorting this out should keep you busy for a while ;-)" > > I hope this could help a little. In my experience, this kind of > discrepancies are much more accusated in the case of charged molecules, > in which the inclusion of solvent effects are usually needed. When > possible, a good alternative should include one or more counterions to > neutralize the charges. > > In any case, I recommend you to read the interesting posts coming from > Prof. Andreas Klamt (COSMO model), which is an expert on this field. > > Best regards, > > Gonzalo From owner-chemistry@ccl.net Wed Oct 11 09:14:01 2006 From: "Christopher Cramer cramer~!~chem.umn.edu" To: CCL Subject: CCL: PCM vs. explicit water with PCM - effect on reaction profile Message-Id: <-32763-061010190121-946-8uvwtQyoolytcVgiM9JNvQ:_:server.ccl.net> X-Original-From: Christopher Cramer Content-Type: multipart/alternative; boundary=Apple-Mail-34--324735766 Date: Tue, 10 Oct 2006 17:16:14 -0500 Mime-Version: 1.0 (Apple Message framework v752.2) Sent to CCL by: Christopher Cramer [cramer**chem.umn.edu] --Apple-Mail-34--324735766 Content-Transfer-Encoding: quoted-printable Content-Type: text/plain; charset=WINDOWS-1252; delsp=yes; format=flowed > > "One thing to consider is that PCM type models are parameterized =20 > models, and the values of the parameters have been derived to fit =20 > experiments, _without_ an explicit first solvation shell. A large =20 > fraction of solvation is the first shell, and that has been =20 > absorbed by the parameters. Introducing an explicit solvation shell =20= > and then put a PCM on top of that may therefore give you a kind of =20 > double counting. Of course the cavity changes, and there are the =20 > usual problems of electron density outside the cavity, etc.... In =20 > short, there is a risk that the results will _deteriorate_ when =20 > putting in an explicit first solvation shell. > I am not aware of any study where the performance of PCM type =20 > models where the first solvation shell is considered explicitly, =20 > but if you find any, I would appreciate the reference(s). In =20 > principle such an approach should be able to provide more accurate =20 > results than a pure continuum model, but the PCM parameters may =20 > have to be returned. This, of course, is not trivial, and the =20 > optimal set of parameters may depend on which method you use for =20 > the solvent molecules (HF, DFT, MP2, etc). Sorting this out should =20 > keep you busy for a while ;-)" > Rare for me to disagree with Frank, but I would say that, if you =20 "materialize" a solvent molecule out of the continuum, your results =20 should not change if you are using a decent continuum model. The =20 exception to this rule is simple -- when the solvent molecule being =20 materialized is in fact not behaving at all like a solvent molecule, =20 but instead is part of a supersolute because it enjoys some uniquely =20 strong interaction with the solute. There are many examples of this, =20 e.g., the first coordination shell of highly charged monatomic ions =20 (where, indeed, we do not refer to the ion as an isolated species, =20 but as an aquo complex, if the solvent is water, for example). Or, =20 again using water because it is simple, an organic molecule with a =20 hydrogen bond donor and an acceptor separated by exactly one water =20 molecule's width (i.e., that water snuggles right in there and =20 becomes an intimate part of the molecule, not a typical solvent). It is true that good continuum models are parameterized to account =20 for the deviation of the first shell from bulk electrostatic =20 behavior. But, of course, if they ARE good then the materialization =20 of the solvent molecule (or the "explicitization", if you will) =20 covers the surface area being excluded with exactly the effects that =20 the model is losing, and exposes new first-shell area (the area about =20= the new piece of the supersolute) that itself will now have first =20 solvation shell effects. Way, way back in 1992 we considered this to =20 be an important test for a solvation model, and we showed, for =20 instance, that the aqueous solvation free energy for piperidine using =20= the SM2 and SM3 solvation models remained unaffected by materializing =20= first one and then a second water molecule, hydrogen bonding to the =20 two secondary amine groups. (Of course, one must use the proper =20 thermodynamic cycle to evaluate this, where the sum of the gas-phase =20 free energy of complexation plus the free energy of continuum =20 solvation for the cluster must equal the sum of the solvation free =20 energies of the isolated solute and isolated water molecules.) See =20 Cramer, C. J.; Truhlar, D. G. "Comparative Analysis of the AM1-SM2 =20 and PM3-SM3 Parametrized SCF Solvation Models for Free Energies in =20 Aqueous Solution" J. Comput.-Aid. Mol. Des. 1992, 6, 629. More recently, we have evaluated this in the context of our latest =20 solvation model, SM6, where we showed that it is indeed important to =20 materialize at leat one water in order to compute accurate solvation =20 free energies for ions having concentrated charge, and that adding =20 more waters did not have much effect when the charge was only +/- 1. =20 See Kelly, C. P.; Cramer, C. J.; Truhlar, D. G. "Aqueous Solvation =20 Free Energies of Ions and Ion-Water Clusters Based on An Accurate =20 Value for the Absolute Aqueous Solvation Free Energy of the Proton" =20 J. Phys. Chem. B 2006, 110, 16066. and its precursor Kelly, C. P.; =20 Cramer, C. J.; Truhlar, D. G. "SM6: A Density Functional Theory =20 Continuum Solvation Model for Calculating Aqueous Solvation Free =20 Energies of Neutrals, Ions, and Solute-Water Clusters" J. Chem. =20 Theory Comput. 2005, 1, 1133. And, finally, if I may plagiarize myself (assuming Wiley will be =20 reluctant to sue me), Section 12.5.4 of Essentials of Computational =20 Chemistry, entitled Mixed Explicit/Implicit Models opines: Having identified the strongest points of the explicit and implicit =20 solvent models, it seems an obvious step to try to combine them in a =20 way that takes advantage of the strengths of each. For instance, to =20 the extent first-solvation-shell effects are qualitatively different =20 > from those deriving from the bulk, one might choose to include the =20 first solvation shell explicitly and model the remainder of the =20 system with a continuum (see, for instance, Chalmet, Rinaldi, and =20 Ruiz-Lopez, 2001). There are certain instances where this approach may be regarded as an =20= attractive option. For example, Cossi and Crescenzi (2003) found that =20= accurate computation of 17O NMR chemical shifts for alcohols, ethers, =20= and carbonyls in aqueous solution required at least one explicit =20 solvent shell, but that beyond that shell a continuum could be used =20 to replace what would otherwise be a need for a much larger cluster. =20 However, just as the strengths of the two models are combined, so are =20= the weaknesses. A typical first shell of solvent for a small molecule =20= may be expected to be composed of a dozen or so solvent molecules. =20 The resulting supermolecular cluster will inevitably be characterized =20= by a large number of accessible structures that are local minima on =20 the cluster PES, so that statistical sampling will have to be =20 undertaken to obtain a proper equilibrium distribution. Thus, QM =20 methods require a substantial investment of computational resources. =20 In addition, certain technical points require attention, e.g., how =20 does one keep the first solvent shell from =91exchanging=92 with the =20 continuum since both, in principle, foster identical solvation =20 interactions? So, while there is growing interest in hybrid models of all sorts (as =20= discussed in more detail in the next chapter), the choice of a mixed =20 solvent model is not necessarily intrinsically better than a pure =20 explicit or pure implicit model. In general, unless there is a strong =20= suspicion that first-solvation-shell effects are drastically =20 different from those more typically encountered, there is no =20 particularly compelling reason to pursue a mixed modeling strategy. =20 An example of such a situation might be the aqueous coordination =20 sphere surrounding a highly charged metal cation. In that case, the =20 electrostriction of the first shell makes the water molecules more =20 ligand-like than solvent-like, and their explicit inclusion in the =20 solute complex is entirely warranted. where the references are: Chalmet, S., Rinaldi, D., and Ruiz-L=ABopez, =20= M. F. 2001. Int. J. Quantum Chem., 84, 559 and Cossi, M. and =20 Crescenzi, O. 2003. J. Chem. Phys., 118, 8863. Returning to the original post, I would say that the energy changes =20 that were reported upon inclusion of a specific solvent molecule are =20 not unusual for a case where one (or more) solvent molecules are =20 indeed playing a role as part of a supersolute. Sadly, the only way =20 to determine this is to do the experiment, but one's intuition can =20 often be good after a bit of experience. Chris -- Christopher J. Cramer University of Minnesota Department of Chemistry 207 Pleasant St. SE Minneapolis, MN 55455-0431 -------------------------- Phone: (612) 624-0859 || FAX: (612) 626-2006 Mobile: (952) 297-2575 cramer*pollux.chem.umn.edu http://pollux.chem.umn.edu/~cramer (website includes information about the textbook "Essentials of Computational Chemistry: Theories and Models, 2nd Edition") --Apple-Mail-34--324735766 Content-Transfer-Encoding: quoted-printable Content-Type: text/html; charset=WINDOWS-1252

"One thing to consider is that PCM type models are = parameterized models, and the values of the parameters have been derived = to fit experiments, _without_ an explicit first solvation shell. A large = fraction of solvation is the first shell, and that has been absorbed by = the parameters. Introducing an explicit solvation shell and then put a = PCM on top of that may therefore give you a kind of double counting. Of = course the cavity changes, and there are the usual problems of electron = density outside the cavity, etc.... In short, there is a risk that the = results will _deteriorate_ when putting in an explicit first solvation = shell.
I am not aware of any study = where the performance of PCM type models where the first solvation shell = is considered explicitly, but if you find any, I would appreciate the = reference(s). In principle such an approach should be able to provide = more accurate results than a pure continuum model, but the PCM = parameters may have to be returned. This, of course, is not trivial, and = the optimal set of parameters may depend on which method you use for the = solvent molecules (HF, DFT, MP2, etc). Sorting this out should keep you = busy for a while ;-)"

Rare for me to disagree with Frank, but I = would say that, if you "materialize" a solvent molecule out of the = continuum, your results should not change if you are using a decent = continuum model. The exception to this rule is simple -- when the = solvent molecule being materialized is in fact not behaving at all like = a solvent molecule, but instead is part of a supersolute because it = enjoys some uniquely strong interaction with the solute. There are many = examples of this, e.g., the first coordination shell of highly charged = monatomic ions (where, indeed, we do not refer to the ion as an isolated = species, but as an aquo complex, if the solvent is water, for example). = Or, again using water because it is simple, an organic molecule with a = hydrogen bond donor and an acceptor separated by exactly one water = molecule's width (i.e., that water snuggles right in there and becomes = an intimate part of the molecule, not a typical solvent).


It is true that good continuum models are parameterized to = account for the deviation of the first shell from bulk electrostatic = behavior. But, of course, if they ARE good then the materialization of = the solvent molecule (or the "explicitization", if you will) covers the = surface area being excluded with exactly the effects that the model is = losing, and exposes new first-shell area (the area about the new piece = of the supersolute) that itself will now have first solvation shell = effects. Way, way back in 1992 we considered this to be an important = test for a solvation model, and we showed, for instance, that the = aqueous solvation free energy for piperidine using the SM2 and SM3 = solvation models remained unaffected by materializing first one and then = a second water molecule, hydrogen bonding to the two secondary amine = groups. (Of course, one must use the proper thermodynamic cycle to = evaluate this, where the sum of the gas-phase free energy of = complexation plus the free energy of continuum solvation for the cluster = must equal the sum of the solvation free energies of the isolated solute = and isolated water molecules.) See=A0Cramer, C. J.; Truhlar, D. G. "Comparative = Analysis of the AM1-SM2 and PM3-SM3 Parametrized SCF Solvation Models = for Free Energies in Aqueous Solution" J. Comput.-Aid. = Mol. Des. = 1992, 6, 629.


More recently, we have = evaluated this in the context of our latest solvation model, SM6, where = we showed that it is indeed important to materialize at leat one water = in order to compute accurate solvation free energies for ions having = concentrated charge, and that adding more waters did not have much = effect when the charge was only +/- 1. See=A0Kelly, C. P.; = Cramer, C. J.; Truhlar, D. G. "Aqueous Solvation Free Energies of Ions = and Ion-Water Clusters Based on An Accurate Value for the Absolute = Aqueous Solvation Free Energy of the Proton" J. Phys. Chem. = B = 2006, 110, 16066. and its precursor=A0Kelly, C. P.; = Cramer, C. J.; Truhlar, D. G. "SM6: A Density Functional Theory = Continuum Solvation Model for Calculating Aqueous Solvation Free = Energies of Neutrals, Ions, and Solute-Water Clusters" J. Chem. = Theory Comput. 2005, 1, 1133.


And, finally, if I may = plagiarize myself (assuming Wiley will be reluctant to sue me), Section = 12.5.4 of Essentials of Computational Chemistry, entitled Mixed = Explicit/Implicit Models opines:


Having identified the strongest points of the = explicit and implicit solvent models, it seems an obvious step to try to = combine them in a way that takes advantage of the strengths of each. For = instance, to the extent first-solvation-shell effects are qualitatively = different from those deriving from the bulk, one might choose to include = the first solvation shell explicitly and model the remainder of the = system with a continuum (see, for instance, Chalmet, Rinaldi, and = Ruiz-Lopez, 2001).
There are certain = instances where this approach may be regarded as an attractive option. = For example, Cossi and Crescenzi (2003) found that accurate computation = of 17O NMR chemical shifts for alcohols, ethers, and carbonyls in = aqueous solution required at least one explicit solvent shell, but that = beyond that shell a continuum could be used to replace what would = otherwise be a need for a much larger cluster. However, just as the = strengths of the two models are combined, so are the weaknesses. A = typical first shell of solvent for a small molecule may be expected to = be composed of a dozen or so solvent molecules. The resulting = supermolecular cluster will inevitably be characterized by a large = number of accessible structures that are local minima on the cluster = PES, so that statistical sampling will have to be undertaken to obtain a = proper equilibrium distribution. Thus, QM methods require a substantial = investment of computational resources. In addition, certain technical = points require attention, e.g., how does one keep the first solvent = shell from =91exchanging=92 with the continuum since both, in principle, = foster identical solvation interactions?
So,= while there is growing interest in hybrid models of all sorts (as = discussed in more detail in the next chapter), the choice of a mixed = solvent model is not necessarily intrinsically better than a pure = explicit or pure implicit model. In general, unless there is a strong = suspicion that first-solvation-shell effects are drastically different = > from those more typically encountered, there is no particularly = compelling reason to pursue a mixed modeling strategy. An example of = such a situation might be the aqueous coordination sphere surrounding a = highly charged metal cation. In that case, the electrostriction of the = first shell makes the water molecules more ligand-like than = solvent-like, and their explicit inclusion in the solute complex is = entirely warranted.

where = the references are:=A0=A0Chalmet, S., Rinaldi, D., and Ruiz-L=ABopez, M. = F. 2001. Int. J. Quantum Chem., 84, 559 and=A0Cossi, M. and Crescenzi, = O. 2003. J. Chem. Phys., 118, 8863.

Returning= to the original post, I would say that the energy changes that were = reported upon inclusion of a specific solvent molecule are not unusual = for a case where one (or more) solvent molecules are indeed playing a = role as part of a supersolute. Sadly, the only way to determine this is = to do the experiment, but one's intuition can often be good after a bit = of experience.

Chris


--


Christopher J. Cramer

University of Minnesota

Department of Chemistry

207 Pleasant St. = SE

Minneapolis, MN 55455-0431

--------------------------

=

Phone:=A0 (612) 624-0859 || FAX:=A0 (612) 626-2006

Mobile: (952) = 297-2575

cramer*pollux.chem.umn.edu<= /FONT>

http://pollux.chem.umn.edu/~cr= amer

(website = includes information about the textbook "Essentials

=A0 =A0 of Computational = Chemistry:=A0 Theories and = Models, 2nd Edition")


= --Apple-Mail-34--324735766-- From owner-chemistry@ccl.net Wed Oct 11 09:49:01 2006 From: "mire.zloh mire.zloh++pharmacy.ac.uk" To: CCL Subject: CCL: Second Workshop on Computational Chemistry and Its Applications (Part of ICCS 2007)/ Call for Paper Message-Id: <-32764-061011052441-4820-YmmI2mdmh04vSPfK74ridw(-)server.ccl.net> X-Original-From: "mire.zloh" Content-Transfer-Encoding: 7bit Content-Type: text/plain; charset="us-ascii" Date: Wed, 11 Oct 2006 09:47:04 +0100 MIME-Version: 1.0 Sent to CCL by: "mire.zloh" [mire.zloh|a|pharmacy.ac.uk] Hi, Delete =20 from the end of the link, Correct link is: http://pages.intnet.mu/ramasami/iccs_2007.htm Best regards, Mire -----Original Message----- > From: owner-chemistry__ccl.net [mailto:owner-chemistry__ccl.net] Sent: 11 October 2006 08:56 To: Zloh, Mire Subject: CCL: Second Workshop on Computational Chemistry and Its Applications (Part of ICCS 2007)/ Call for Paper Sent to CCL by: Karol Langner [karol.langner .. kn.pl] On Wednesday 11 of October 2006 07:29, Dr. Ponnadurai Ramasami ramchemi__intnet.mu wrote: > Please visit http://pages.intnet.mu/ramasami/iccs_2007.htm=20 This link does not work from where I am. -- written by Karol Langner Wed Oct 11 08:49:30 CEST 2006http://www.ccl.net/cgi-bin/ccl/send_ccl_messagehttp://www.ccl.net/chemistry/sub_unsub.shtmlhttp://www.ccl.net/spammers.txt From owner-chemistry@ccl.net Wed Oct 11 10:58:00 2006 From: "Rajarshi Guha rajarshi.guha---gmail.com" To: CCL Subject: CCL: SMILE to 2D structure Message-Id: <-32765-061011100526-19009-lSE/tHwMl4VLZ292wxVQgw#,#server.ccl.net> X-Original-From: "Rajarshi Guha" Content-Type: multipart/alternative; boundary="----=_Part_25042_1725099.1160572160744" Date: Wed, 11 Oct 2006 09:09:20 -0400 MIME-Version: 1.0 Sent to CCL by: "Rajarshi Guha" [rajarshi.guha]*[gmail.com] ------=_Part_25042_1725099.1160572160744 Content-Type: text/plain; charset=ISO-8859-1; format=flowed Content-Transfer-Encoding: 7bit Content-Disposition: inline On 10/11/06, Nehru Viji Shankaran chat2viji#,#gmail.com < owner-chemistry],[ccl.net> wrote: > > Sent to CCL by: "Nehru Viji Shankaran" [chat2viji^-^gmail.com] > Dear all, > > I want a program which would convert the SMILE strings (simple)into > 2D structure probably a connection table,z-matrix. > If possible kindly provide me with the source code for it. > The CDK will do this. Example code is at http://cheminfo.informatics.indiana.edu/~rguha/code/java/#smi2sdf -- Rajarshi Guha ------=_Part_25042_1725099.1160572160744 Content-Type: text/html; charset=ISO-8859-1 Content-Transfer-Encoding: 7bit Content-Disposition: inline

On 10/11/06, Nehru Viji Shankaran chat2viji#,#gmail.com <owner-chemistry],[ccl.net> wrote:
Sent to CCL by: "Nehru Viji Shankaran" [chat2viji^-^gmail.com]
Dear all,

       I want a program which would convert the SMILE strings (simple)into
       2D structure probably a connection table,z-matrix.
       If possible kindly provide me with the source code for it.

The CDK will do this. Example code is at
http://cheminfo.informatics.indiana.edu/~rguha/code/java/#smi2sdf

--
Rajarshi Guha ------=_Part_25042_1725099.1160572160744-- From owner-chemistry@ccl.net Wed Oct 11 11:32:00 2006 From: "gonzalo jimenez oses gonzalo.jimenez++dq.unirioja.es" To: CCL Subject: CCL: PCM vs. explicit water with PCM - effect on reaction profile Message-Id: <-32766-061011110634-5358-s3FozE7ZELazZrJurhZ2dw_-_server.ccl.net> X-Original-From: "gonzalo jimenez oses" Date: Wed, 11 Oct 2006 11:06:33 -0400 Sent to CCL by: "gonzalo jimenez oses" [gonzalo.jimenez[A]dq.unirioja.es] Dear CCL'ers This short message is only to thank all the valuable opinions reported with respect to explicit/implicit solvation, specially those coming from Chris Cramer. His comments are always very accurate and, in fact, I strongly recommend the reading of his "Essentials..." to have a deep view of these kind of concepts. I also would like to thank the reported references, which is always the most straightforward way to obtain the different viewpoints. Best regards, Gonzalo From owner-chemistry@ccl.net Wed Oct 11 13:59:00 2006 From: "Barry Hardy barry.hardy[*]tiscalinet.ch" To: CCL Subject: CCL: Invitation to Open Event on Screening, ELNs, KM in R&D & Comp Chem Message-Id: <-32767-061011135438-22753-p6aXGvYBHq/1KgFeroNVtA,,server.ccl.net> X-Original-From: Barry Hardy Content-Type: multipart/alternative; boundary="=====================_22020412==_.ALT" Date: Wed, 11 Oct 2006 19:57:26 +0200 Mime-Version: 1.0 Sent to CCL by: Barry Hardy [barry.hardy{}tiscalinet.ch] --=====================_22020412==_.ALT Content-Type: text/plain; charset="us-ascii"; format=flowed For those in the neighborhood of Philadelphia next week and interested in the topics of Virtual Screening, Electronic Lab Notebooks (ELNs), Knowledge Management in R&D & Chemistry Research - please consider coming along for the Open Event & Knowledge Cafe at Thomas Great Hall, Bryn Mawr College, the evening of Tuesday Oct 17th starting from 16.00 and running to 21.00. The event is free to attend and includes food, refreshments, good networking and an interactive format. To take a place on the guest list simply RSVP with your name and organization by forwarding a copy of this email to innovationwell [at] douglasconnect.com and indicate with xs which of the activities below you would like to join. Activities: * Screening Forum on "Could we take a Community Approach to Comparing Virtual Screening Methods?" [ ] or * Presentation and Discussion of ELNs [ ] and * Panel Discussion on Knowledge Management in R&D [ ] and * Knowledge Cafe (i.e., more informal group discussions at tables with food and refreshments) [ ] One table's theme at the Knowledge Cafe will be Computational Chemistry Research and ELNs whose discussion I would like to join [ ] More Information at: Knowledge Management in R&D and ELNs: http://barryhardy.blogs.com/theferryman/2006/09/electronic_lab_.html or http://www.echeminfo.com/COMTY_conferenceopenevent/ and Post on Comparing Virtual Screening Methods recently posted by John Irwin (UCSF) and I at http://barryhardy.blogs.com/cheminfostream/2006/10/could_we_take_a.html best regards Barry Hardy eCheminfo Community of Practice Douglas Connect, Switzerland +41 61 851 0170 (office) www.douglasconnect.com --=====================_22020412==_.ALT Content-Type: text/html; charset="us-ascii" For those in the neighborhood of Philadelphia next week and interested in the topics of Virtual Screening, Electronic Lab Notebooks (ELNs), Knowledge Management in R&D & Chemistry Research - please consider coming along for the Open Event & Knowledge Cafe at Thomas Great Hall, Bryn Mawr College, the evening of Tuesday Oct 17th starting from 16.00 and running to 21.00.

The event is free to attend and includes food, refreshments, good networking and an interactive format.

To take a place on the guest list simply RSVP with your name and organization by forwarding a copy of this email to innovationwell [at] douglasconnect.com and indicate with xs which of the activities below you would like to join.

Activities:
* Screening Forum on "Could we take a Community Approach to Comparing Virtual Screening Methods?" [  ]
or
* Presentation and Discussion of ELNs  [   ]
and
* Panel Discussion on Knowledge Management in R&D  [   ]
and
* Knowledge Cafe (i.e., more informal group discussions at tables with food and refreshments) [   ]

One table's theme at the Knowledge Cafe will be Computational Chemistry Research and ELNs whose discussion I would like to join  [  ]

More Information at:
Knowledge Management in R&D and ELNs:
http://barryhardy.blogs.com/theferryman/2006/09/electronic_lab_.html
or
http://www.echeminfo.com/COMTY_conferenceopenevent/
and
Post on Comparing Virtual Screening Methods recently posted by John Irwin (UCSF) and I at http://barryhardy.blogs.com/cheminfostream/2006/10/could_we_take_a.html


best regards
Barry Hardy
eCheminfo Community of Practice
Douglas Connect, Switzerland
+41 61 851 0170 (office)
www.douglasconnect.com --=====================_22020412==_.ALT-- From owner-chemistry@ccl.net Wed Oct 11 16:23:00 2006 From: "Gilles Marcou gilles.marcou/./pharma.u-strasbg.fr" To: CCL Subject: CCL: SMILE to 2D structure Message-Id: <-32768-061011141606-4905-l7EkcGOGDesiXY3R07zEjw]~[server.ccl.net> X-Original-From: Gilles Marcou Content-Disposition: inline Content-Transfer-Encoding: 8bit Content-Type: text/plain; charset="iso-8859-15" Date: Wed, 11 Oct 2006 20:27:55 +0200 MIME-Version: 1.0 Sent to CCL by: Gilles Marcou [gilles.marcou/./pharma.u-strasbg.fr] Hi all, In fact I like very much Cactvs. http://www2.chemie.uni-erlangen.de/software/cactvs/ It is able to do that. It is not as pretty as other tools but it is 100% Tcl/Tk and it is very robust. Ciao, > > I want a program which would convert the SMILE strings > > (simple)into 2D structure probably a connection table,z-matrix. > > If possible kindly provide me with the source code for it. > > The CDK will do this. Example code is at > http://cheminfo.informatics.indiana.edu/~rguha/code/java/#smi2sdf -- Gilles Marcou Université Louis Pasteur de Strasbourg Institut de Chimie de Strasbourg Laboratoire d' infochimie, UMR7077 4, rue Blaise Pascal, 67000 Strasbourg eMail: g.marcou^chimie.u-strasbg.fr From owner-chemistry@ccl.net Wed Oct 11 21:46:00 2006 From: "Wolf-D. Ihlenfeldt wdi|a|xemistry.com" To: CCL Subject: CCL: SMILE to 2D structure Message-Id: <-32769-061011213202-29176-SNVYbEydnRdCr0LeodD5Wg*o*server.ccl.net> X-Original-From: "Wolf-D. Ihlenfeldt" Content-Transfer-Encoding: 8bit Content-Type: text/plain; charset="iso-8859-1" Date: Wed, 11 Oct 2006 20:31:40 -0400 MIME-Version: 1.0 Sent to CCL by: "Wolf-D. Ihlenfeldt" [wdi_-_xemistry.com] Gilles, thanks for the praise! However, that dowmload location has only ancient versions of the toolkit. The official download site for the toolkit for academic users is www.xemistry.com/academic. For commercial customers, dedicted batch conversion and depiction programs are available. Btw, it is *not* 100% Tcl/Tk. There is a very powerful Tcl scripting layer for rapid application prototyping, and lots of sample programs which were scripted in Tcl or Tk, but the core library is written in ANSI C, including the 2D layout algorithms. The Tcl/Tk components are available as source, but not the core. W. D. Ihlenfeldt Xemistry GmbH wdi]^[xemistry.com > -----Original Message----- > From: owner-chemistry]^[ccl.net [mailto:owner-chemistry]^[ccl.net] > Sent: Wednesday, October 11, 2006 4:29 PM > To: Ihlenfeldt, W.d. > Subject: CCL: SMILE to 2D structure > > Sent to CCL by: Gilles Marcou [gilles.marcou/./pharma.u-strasbg.fr] > Hi all, > > In fact I like very much Cactvs. > http://www2.chemie.uni-erlangen.de/software/cactvs/ > > It is able to do that. It is not as pretty as other tools but > it is 100% Tcl/Tk and it is very robust. > > Ciao, > > > > I want a program which would convert the SMILE strings > > > (simple)into 2D structure probably a connection table,z-matrix. > > > If possible kindly provide me with the source code for it. > > > > The CDK will do this. Example code is at > > http://cheminfo.informatics.indiana.edu/~rguha/code/java/#smi2sdf > > > -- > Gilles Marcou > Université Louis Pasteur de Strasbourg > Institut de Chimie de Strasbourg > Laboratoire d' infochimie, UMR7077 > 4, rue Blaise Pascal, > 67000 Strasbourg > eMail: g.marcou_-_chimie.u-strasbg.fr > > > > -= This is automatically added to each message by the mailing > script =- > To recover the email address of the author of the message, > please change> Conferences: > http://server.ccl.net/chemistry/announcements/conferences/ > > Search Messages: http://www.ccl.net/htdig (login: ccl, > Password: search)> > -+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+-+ > -+-+-+-+-+ > > > > From owner-chemistry@ccl.net Wed Oct 11 22:50:00 2006 From: "Zhijian Wu zhijw..hotmail.com" To: CCL Subject: CCL: solid molecular N2 Message-Id: <-32770-061011042439-14179-Pb0G1G1it9Xbsq47c8Upew|server.ccl.net> X-Original-From: "Zhijian Wu" Content-Type: text/html; format=flowed Date: Wed, 11 Oct 2006 03:10:41 -0400 Mime-Version: 1.0 Sent to CCL by: "Zhijian Wu" [zhijw],[hotmail.com]
Hi,
 
Does anybody know the cell constants and fractional coordinates of solid molecular N2 (nitrogen gas) in ALPHA-phase?
 
Thank you very much for any of your input.
 
Regards,
 
Zhijian WU