From chemistry-request@ccl.net Fri May 21 09:24:34 2004
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Date: Thu, 20 May 2004 18:37:07 +0300 (EEST)
From: Arvydas Tamulis <tamulis/at/mserv.itpa.lt>
To: CHEMISTRY/at/ccl.net
Subject: Re: CCL:The pi-pi stacking of hetero-aromatic ring 
Message-ID: <20040520183613.D65761-100000/at/mserv.itpa.lt>
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Dear Netters,

Would you please to advise us the quantum chemical methods and programs
that might properly calculate stacking interactions including
dispersion effects in oligomeric nucleic acids (two types of interactions:
in parallel planes and when planes are perpendicular).

Thanking your in advance.
With best regards, Arvydas Tamulis
****************************************

On Fri, 14 May 2004, Tanja van Mourik wrote:

> Dear Arvydas,
>
> > While I still am not sure for my obtained result because it was done by HF
> > 6-31G. I have plans to repeat optimization using DFT PBE 6-31++G* where
> > exist possibility to include fine effects of quantum mechanical dispersion
> > van-der-Waals interactions.
>
> Please be cautious with using DFT for calculating stacking interactions.
> DFT doesn't correctly describe dispersion effects, see, for example:
>
> Kohn, Meir and Makarov, Phys. Rev. Lett. 80, 4153 (1998)
> Tuma, Boese and Handy, Phys. Chem. Chem. Phys. 1, 3939 (1999)
> Hobza, Sponer and Reschel, J. Comput. Chem. 16, 1315 (1995)
> Van Mourik and Gdanitz, J. Chem. Phys. 116, 9620 (2002)
>
> Best wishes,
>
> Tanja
> --
>   =================================================================
>    Tanja van Mourik
>    Royal Society University Research Fellow
>    Chemistry Department
>    University College London  phone:  +44 (0)20-7679-4663
>    20 Gordon Street          e-mail: work: T.vanMourik/at/ucl.ac.uk
>    London WC1H 0AJ, UK               home: tanja/at/van-mourik.me.uk
>
>    http://www.chem.ucl.ac.uk/people/vanmourik/index.html
>   =================================================================
>



From chemistry-request@ccl.net Fri May 21 09:20:14 2004
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Subject: We have some problems with frecuential calculaions
Date: Thu, 20 May 2004 18:05:24 -0400
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This is a multi-part message in MIME format.

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Content-Type: text/plain; charset=iso-8859-1; format=flowed

Hi,We are a group of theoretical Chemistry in Venezuelan,we have been trying 
to do a frecuenciat job at the level mp2/6-31g,(169 basis functions),but I 
wonder why we cant do it?

Problems with this type job
a) Actual scratch disk usage is more large Estimated scratch disk usage
b) writwa
c)LINK 811(Construction molecular orbitals)
We read in the web around of How does it?
We intent to do create multiple files for example(8 files each one of 
2GB).later of it,only complety 5 files and finally present an error with 
said above.
We have an PC Super Power1.7GHz with 1000 MB memory and 40 GB hard disk).
The operating system is WINDOWS 2000.

_________________________________________________________________
MSN Amor: busca tu = naranja http://latam.msn.com/amor/

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 filename="=?iso-8859-1?B?VFNDTE9ST2NvbmNvcnJlY2Np8242LTMxRyhkKS5vdXQ=?="

Entering Link 1 = C:\G98W\l1.exe PID=  -1905313.

Copyright (c) 1988,1990,1992,1993,1995,1998 Gaussian, Inc.
                  All Rights Reserved.

This is part of the Gaussian(R) 98 program.  It is based on
the Gaussian 94(TM) system (copyright 1995 Gaussian, Inc.),
the Gaussian 92(TM) system (copyright 1992 Gaussian, Inc.),
the Gaussian 90(TM) system (copyright 1990 Gaussian, Inc.),
the Gaussian 88(TM) system (copyright 1988 Gaussian, Inc.),
the Gaussian 86(TM) system (copyright 1986 Carnegie Mellon
University), and the Gaussian 82(TM) system (copyright 1983
Carnegie Mellon University). Gaussian is a federally registered
trademark of Gaussian, Inc.

This software contains proprietary and confidential information,
including trade secrets, belonging to Gaussian, Inc.

This software is provided under written license and may be
used, copied, transmitted, or stored only in accord with that
written license.

The following legend is applicable only to US Government
contracts under DFARS:

                    RESTRICTED RIGHTS LEGEND

Use, duplication or disclosure by the US Government is subject
to restrictions as set forth in subparagraph (c)(1)(ii) of the
Rights in Technical Data and Computer Software clause at DFARS
252.227-7013.

Gaussian, Inc.
Carnegie Office Park, Building 6, Pittsburgh, PA 15106 USA

The following legend is applicable only to US Government
contracts under FAR:

                    RESTRICTED RIGHTS LEGEND

Use, reproduction and disclosure by the US Government is subject
to restrictions as set forth in subparagraph (c) of the
Commercial Computer Software - Restricted Rights clause at FAR
52.227-19.

Gaussian, Inc.
Carnegie Office Park, Building 6, Pittsburgh, PA 15106 USA


---------------------------------------------------------------
Warning -- This program may not be used in any manner that
competes with the business of Gaussian, Inc. or will provide
assistance to any competitor of Gaussian, Inc.  The licensee
of this program is prohibited from giving any competitor of
Gaussian, Inc. access to this program.  By using this program,
the user acknowledges that Gaussian, Inc. is engaged in the
business of creating and licensing software in the field of
computational chemistry and represents and warrants to the
licensee that it is not a competitor of Gaussian, Inc. and that
it will not use this program in any manner prohibited above.
---------------------------------------------------------------


Cite this work as:
Gaussian 98, Revision A.11,
M. J. Frisch, G. W. Trucks, H. B. Schlegel, G. E. Scuseria,
M. A. Robb, J. R. Cheeseman, V. G. Zakrzewski, J. A. Montgomery, Jr.,
R. E. Stratmann, J. C. Burant, S. Dapprich, J. M. Millam,
A. D. Daniels, K. N. Kudin, M. C. Strain, O. Farkas, J. Tomasi,
V. Barone, M. Cossi, R. Cammi, B. Mennucci, C. Pomelli, C. Adamo,
S. Clifford, J. Ochterski, G. A. Petersson, P. Y. Ayala, Q. Cui,
K. Morokuma, P. Salvador, J. J. Dannenberg, D. K. Malick,
A. D. Rabuck, K. Raghavachari, J. B. Foresman, J. Cioslowski,
J. V. Ortiz, A. G. Baboul, B. B. Stefanov, G. Liu, A. Liashenko,
P. Piskorz, I. Komaromi, R. Gomperts, R. L. Martin, D. J. Fox,
T. Keith, M. A. Al-Laham, C. Y. Peng, A. Nanayakkara, M. Challacombe,
P. M. W. Gill, B. Johnson, W. Chen, M. W. Wong, J. L. Andres,
C. Gonzalez, M. Head-Gordon, E. S. Replogle, and J. A. Pople,
Gaussian, Inc., Pittsburgh PA, 2001.

**********************************************
Gaussian 98:  x86-Win32-G98RevA.11 25-Sep-2001
                  20-May-2004
**********************************************
%chk=transcloropruebamirna
%mem=18MW
%nproc=1
Will use up to    1 processors via shared memory.
Default route:  MaxDisk=4000MB
-------------------------------------------------------------------
#P rmp2/6-31g(d) Freq=(ReadIso) nosymm guess=read geom=connectivity
-------------------------------------------------------------------
1/10=4,30=1,38=1,57=2/1,3;
2/15=1,17=6,18=5,40=1/2;
3/5=1,6=6,7=1,11=1,25=1,30=1/1,2,3;
4/5=1,7=1/1;
5/5=2/2;
8/6=3,8=1,10=1,19=11,23=2,27=524288000,30=-1/1;
9/15=3,16=-3,27=524288000/6;
11/6=1,8=1,15=11,17=12,24=-1,27=1,28=-2,29=300,31=1,32=6,42=1/1,2,10;
10/6=2,21=1,31=1/2;
8/6=4,8=1,10=1,19=11,23=2,27=524288000,30=-1/11,4;
10/5=1,20=4,31=1/2;
11/12=2,14=11,16=11,17=2,28=-2,31=1,42=1/2,10,12;
6/7=2,8=2,9=2,10=2/1;
7/8=2,10=1,12=2,25=1,30=1,44=2/1,2,3,16;
1/10=4,30=1/3;
99//99;
Leave Link    1 at Thu May 20 09:36:54 2004, MaxMem=   18874368 cpu:       
1.0
(Enter C:\G98W\l101.exe)
------------------------------
buscando el frecuencial del ts
------------------------------
Symbolic Z-matrix:
Charge =  0 Multiplicity = 1
N
C                    1    B1
H                    2    B2       1    A1
H                    2    B3       1    A2       3    D1       0
H                    2    B4       1    A3       3    D2       0
C                    1    B5       2    A4       3    D3       0
H                    6    B6       1    A5       2    D4       0
H                    6    B7       1    A6       2    D5       0
H                    6    B8       1    A7       2    D6       0
C                    1    B9       2    A8       6    D7       0
O                    10   B10      1    A9       2    D8       0
O                    10   B11      1    A10      2    D9       0
C                    12   B12      10   A11      1    D10      0
H                    13   B13      12   A12      10   D11      0
C                    13   B14      12   A13      10   D12      0
H                    11   B15      10   A14      1    D13      0
H                    15   B16      13   A15      12   D14      0
H                    13   B17      12   A16      10   D15      0
C                    15   B18      13   A17      12   D16      0
H                    19   B19      15   A18      13   D17      0
H                    19   B20      15   A19      13   D18      0
Cl                   19   B21      15   A20      13   D19      0
       Variables:
  B1                    1.45276
  B2                    1.0875
  B3                    1.09455
  B4                    1.09617
  B5                    1.45149
  B6                    1.09621
  B7                    1.08753
  B8                    1.09473
  B9                    1.35869
  B10                   1.29445
  B11                   1.28875
  B12                   1.85593
  B13                   1.08709
  B14                   1.40709
  B15                   1.21414
  B16                   1.0896
  B17                   1.0853
  B18                   1.49986
  B19                   1.0923
  B20                   1.09262
  B21                   1.80558
  A1                  109.04907
  A2                  109.44099
  A3                  110.49852
  A4                  117.15548
  A5                  110.46315
  A6                  109.04963
  A7                  109.63822
  A8                  121.05615
  A9                  118.12021
  A10                 118.4409
  A11                 116.09458
  A12                  89.48242
  A13                 113.92518
  A14                 102.53238
  A15                 116.01133
  A16                  91.8087
  A17                 118.24346
  A18                 112.95266
  A19                 110.69481
  A20                 112.85216
  D1                 -119.8551
  D2                  120.48085
  D3                  177.62381
  D4                   60.64796
  D5                 -178.99987
  D6                  -59.01563
  D7                  172.11014
  D8                    3.91955
  D9                 -176.48023
  D10                -162.14606
  D11                 123.19119
  D12                  -0.04059
  D13                 161.63193
  D14                -112.30614
  D15                -123.03125
  D16                 103.27139
  D17                  95.22375
  D18                 -26.68748
  D19                -145.77338
Leave Link  101 at Thu May 20 09:36:55 2004, MaxMem=   18874368 cpu:       
0.0
(Enter C:\G98W\l103.exe)

GradGradGradGradGradGradGradGradGradGradGradGradGradGradGradGradGradGrad
Berny optimization.
Initialization pass.
                       ----------------------------
                       !    Initial Parameters    !
                       ! (Angstroms and Degrees)  !
----------------------                            ----------------------
!      Name          Value   Derivative information (Atomic Units)     !
------------------------------------------------------------------------
!       B1          1.4528   calculate D2E/DX2 analytically            !
!       B2          1.0875   calculate D2E/DX2 analytically            !
!       B3          1.0946   calculate D2E/DX2 analytically            !
!       B4          1.0962   calculate D2E/DX2 analytically            !
!       B5          1.4515   calculate D2E/DX2 analytically            !
!       B6          1.0962   calculate D2E/DX2 analytically            !
!       B7          1.0875   calculate D2E/DX2 analytically            !
!       B8          1.0947   calculate D2E/DX2 analytically            !
!       B9          1.3587   calculate D2E/DX2 analytically            !
!       B10         1.2944   calculate D2E/DX2 analytically            !
!       B11         1.2887   calculate D2E/DX2 analytically            !
!       B12         1.8559   calculate D2E/DX2 analytically            !
!       B13         1.0871   calculate D2E/DX2 analytically            !
!       B14         1.4071   calculate D2E/DX2 analytically            !
!       B15         1.2141   calculate D2E/DX2 analytically            !
!       B16         1.0896   calculate D2E/DX2 analytically            !
!       B17         1.0853   calculate D2E/DX2 analytically            !
!       B18         1.4999   calculate D2E/DX2 analytically            !
!       B19         1.0923   calculate D2E/DX2 analytically            !
!       B20         1.0926   calculate D2E/DX2 analytically            !
!       B21         1.8056   calculate D2E/DX2 analytically            !
!       A1        109.0491   calculate D2E/DX2 analytically            !
!       A2        109.441    calculate D2E/DX2 analytically            !
!       A3        110.4985   calculate D2E/DX2 analytically            !
!       A4        117.1555   calculate D2E/DX2 analytically            !
!       A5        110.4631   calculate D2E/DX2 analytically            !
!       A6        109.0496   calculate D2E/DX2 analytically            !
!       A7        109.6382   calculate D2E/DX2 analytically            !
!       A8        121.0561   calculate D2E/DX2 analytically            !
!       A9        118.1202   calculate D2E/DX2 analytically            !
!       A10       118.4409   calculate D2E/DX2 analytically            !
!       A11       116.0946   calculate D2E/DX2 analytically            !
!       A12        89.4824   calculate D2E/DX2 analytically            !
!       A13       113.9252   calculate D2E/DX2 analytically            !
!       A14       102.5324   calculate D2E/DX2 analytically            !
!       A15       116.0113   calculate D2E/DX2 analytically            !
!       A16        91.8087   calculate D2E/DX2 analytically            !
!       A17       118.2435   calculate D2E/DX2 analytically            !
!       A18       112.9527   calculate D2E/DX2 analytically            !
!       A19       110.6948   calculate D2E/DX2 analytically            !
!       A20       112.8522   calculate D2E/DX2 analytically            !
!       D1       -119.8551   calculate D2E/DX2 analytically            !
!       D2        120.4809   calculate D2E/DX2 analytically            !
!       D3        177.6238   calculate D2E/DX2 analytically            !
!       D4         60.648    calculate D2E/DX2 analytically            !
!       D5       -178.9999   calculate D2E/DX2 analytically            !
!       D6        -59.0156   calculate D2E/DX2 analytically            !
!       D7        172.1101   calculate D2E/DX2 analytically            !
!       D8          3.9195   calculate D2E/DX2 analytically            !
!       D9       -176.4802   calculate D2E/DX2 analytically            !
!       D10      -162.1461   calculate D2E/DX2 analytically            !
!       D11       123.1912   calculate D2E/DX2 analytically            !
!       D12        -0.0406   calculate D2E/DX2 analytically            !
!       D13       161.6319   calculate D2E/DX2 analytically            !
!       D14      -112.3061   calculate D2E/DX2 analytically            !
!       D15      -123.0312   calculate D2E/DX2 analytically            !
!       D16       103.2714   calculate D2E/DX2 analytically            !
!       D17        95.2237   calculate D2E/DX2 analytically            !
!       D18       -26.6875   calculate D2E/DX2 analytically            !
!       D19      -145.7734   calculate D2E/DX2 analytically            !
------------------------------------------------------------------------
Trust Radius=3.00D-01 FncErr=1.00D-07 GrdErr=1.00D-07
Number of steps in this run=  70 maximum allowed number of steps= 120.
GradGradGradGradGradGradGradGradGradGradGradGradGradGradGradGradGradGrad

Leave Link  103 at Thu May 20 09:36:56 2004, MaxMem=   18874368 cpu:       
0.0
(Enter C:\G98W\l202.exe)
------------------------------------------------------------------------
                         Z-MATRIX (ANGSTROMS AND DEGREES)
CD Cent Atom  N1     Length/X     N2    Alpha/Y     N3     Beta/Z      J
------------------------------------------------------------------------
   1   1  N
   2   2  C     1   1.452757(  1)
   3   3  H     2   1.087500(  2)   1  109.049( 22)
   4   4  H     2   1.094555(  3)   1  109.441( 23)   3 -119.855( 42)   0
   5   5  H     2   1.096167(  4)   1  110.499( 24)   3  120.481( 43)   0
   6   6  C     1   1.451486(  5)   2  117.155( 25)   3  177.624( 44)   0
   7   7  H     6   1.096208(  6)   1  110.463( 26)   2   60.648( 45)   0
   8   8  H     6   1.087535(  7)   1  109.050( 27)   2 -179.000( 46)   0
   9   9  H     6   1.094733(  8)   1  109.638( 28)   2  -59.016( 47)   0
  10  10  C     1   1.358690(  9)   2  121.056( 29)   6  172.110( 48)   0
  11  11  O    10   1.294446( 10)   1  118.120( 30)   2    3.920( 49)   0
  12  12  O    10   1.288747( 11)   1  118.441( 31)   2 -176.480( 50)   0
  13  13  C    12   1.855927( 12)  10  116.095( 32)   1 -162.146( 51)   0
  14  14  H    13   1.087088( 13)  12   89.482( 33)  10  123.191( 52)   0
  15  15  C    13   1.407089( 14)  12  113.925( 34)  10   -0.041( 53)   0
  16  16  H    11   1.214144( 15)  10  102.532( 35)   1  161.632( 54)   0
  17  17  H    15   1.089597( 16)  13  116.011( 36)  12 -112.306( 55)   0
  18  18  H    13   1.085296( 17)  12   91.809( 37)  10 -123.031( 56)   0
  19  19  C    15   1.499864( 18)  13  118.243( 38)  12  103.271( 57)   0
  20  20  H    19   1.092298( 19)  15  112.953( 39)  13   95.224( 58)   0
  21  21  H    19   1.092620( 20)  15  110.695( 40)  13  -26.687( 59)   0
  22  22  Cl   19   1.805580( 21)  15  112.852( 41)  13 -145.773( 60)   0
------------------------------------------------------------------------
                         Z-Matrix orientation:
---------------------------------------------------------------------
Center     Atomic     Atomic              Coordinates (Angstroms)
Number     Number      Type              X           Y           Z
---------------------------------------------------------------------
    1          7             0        0.000000    0.000000    0.000000
    2          6             0        0.000000    0.000000    1.452757
    3          1             0        1.027948    0.000000    1.807693
    4          1             0       -0.513812   -0.895169    1.817064
    5          1             0       -0.520824    0.884860    1.836616
    6          6             0       -1.290380   -0.053546   -0.662468
    7          1             0       -1.897767    0.817209   -0.389447
    8          1             0       -1.136494   -0.065119   -1.738998
    9          1             0       -1.822862   -0.960335   -0.358105
   10          6             0        1.145305    0.207436   -0.700918
   11          8             0        2.251665    0.328511   -0.039935
   12          8             0        1.076128    0.265610   -1.986492
   13          6             0        2.674286    0.034365   -2.901304
   14          1             0        2.230845   -0.795092   -3.446394
   15          6             0        3.785142   -0.178975   -2.064414
   16          1             0        3.091593    0.122651   -0.892160
   17          1             0        4.529855    0.616206   -2.046802
   18          1             0        2.567456    0.992550   -3.399637
   19          6             0        4.315580   -1.575568   -1.931167
   20          1             0        5.145272   -1.782741   -2.610730
   21          1             0        3.525647   -2.307777   -2.114726
   22         17             0        4.961045   -1.926101   -0.281737
---------------------------------------------------------------------
                    Distance matrix (angstroms):
                    1          2          3          4          5
     1  N    0.000000
     2  C    1.452757   0.000000
     3  H    2.079526   1.087500   0.000000
     4  H    2.089750   1.094555   1.782818   0.000000
     5  H    2.104137   1.096167   1.783958   1.780150   0.000000
     6  C    1.451486   2.478331   3.388098   2.731203   2.778173
     7  H    2.102622   2.768224   3.749008   3.117092   2.618379
     8  H    2.078455   3.388681   4.155487   3.704362   3.750537
     9  H    2.091245   2.743044   3.706756   2.539531   3.149102
    10  C    1.358690   2.448074   2.519907   3.210707   3.110300
    11  O    2.275853   2.721405   2.240342   3.548760   3.393768
    12  O    2.274808   3.613451   3.803775   4.282797   4.189258
    13  C    3.945954   5.109877   4.988614   5.769836   5.777539
    14  H    4.181683   5.441555   5.448354   5.936931   6.189032
    15  C    4.315221   5.170089   4.756823   5.836078   5.906870
    16  H    3.220084   3.882219   3.400424   4.623289   4.590941
    17  H    5.008862   5.757275   5.244063   6.530873   6.376713
    18  H    4.374302   5.578774   5.520102   6.345996   6.080084
    19  C    4.983578   5.705926   5.222070   6.151033   6.606111
    20  H    6.038866   6.794403   6.297061   7.240053   7.681121
    21  H    4.714667   5.521137   5.191310   5.811339   6.494610
    22  Cl   5.329278   5.597347   4.852302   5.953305   6.514584
                    6          7          8          9         10
     6  C    0.000000
     7  H    1.096208   0.000000
     8  H    1.087535   1.783066   0.000000
     9  H    1.094733   1.779397   1.783082   0.000000
    10  C    2.449929   3.119154   2.521607   3.207993   0.000000
    11  O    3.616572   4.192704   3.810693   4.285338   1.294446
    12  O    2.730432   3.420360   2.250852   3.543830   1.288747
    13  C    4.553976   5.275030   3.985336   5.261334   2.685040
    14  H    4.549633   5.384225   3.845392   5.098762   3.117868
    15  C    5.267077   6.007773   4.933696   5.913689   2.996193
    16  H    4.391525   5.062494   4.316146   5.060627   1.957499
    17  H    6.019974   6.640900   5.715459   6.759748   3.665199
    18  H    4.844513   5.387968   4.194715   5.686789   3.149921
    19  C    5.945833   6.834322   5.660698   6.366593   3.839695
    20  H    6.942871   7.829318   6.570444   7.369230   4.858799
    21  H    5.512234   6.492729   5.187123   5.788597   3.740478
    22  Cl   6.536951   7.387871   6.539637   6.852731   4.391761
                   11         12         13         14         15
    11  O    0.000000
    12  O    2.274846   0.000000
    13  C    2.907330   1.855927   0.000000
    14  H    3.587043   2.142376   1.087088   0.000000
    15  C    2.589905   2.746358   1.407089   2.169172   0.000000
    16  H    1.214144   2.297847   2.053924   2.847324   1.395051
    17  H    3.049662   3.472000   2.124112   3.039090   1.089597
    18  H    3.439225   2.179330   1.085296   1.819659   2.153613
    19  C    3.385561   3.726532   2.495375   2.692800   1.499864
    20  H    4.409006   4.598189   3.080922   3.188678   2.172667
    21  H    3.588565   3.555123   2.613264   2.395426   2.145150
    22  Cl   3.533056   4.775182   3.991845   4.329922   2.759191
                   16         17         18         19         20
    16  H    0.000000
    17  H    1.909291   0.000000
    18  H    2.705344   2.413050   0.000000
    19  C    2.337012   2.205257   3.436215   0.000000
    20  H    3.286579   2.540020   3.869076   1.092298   0.000000
    21  H    2.755005   3.092366   3.668963   1.092620   1.773378
    22  Cl   2.839868   3.124853   4.895824   1.805580   2.340663
                   21         22
    21  H    0.000000
    22  Cl   2.359214   0.000000
                           Interatomic angles:
       N1-C2-H3=109.0491       N1-C2-H4=109.441        H3-C2-H4=109.578
       N1-C2-H5=110.4985       H3-C2-H5=109.5617       H4-C2-H5=108.6987
       C2-N1-C6=117.1555       N1-C6-H7=110.4631       N1-C6-H8=109.0496
       H7-C6-H8=109.4749       N1-C6-H9=109.6382       H7-C6-H9=108.6152
       H8-C6-H9=109.5861      C2-N1-C10=121.0561      C6-N1-C10=121.3033
     N1-C10-O11=118.1202     N1-C10-O12=118.4409    O11-C10-O12=123.4376
    C10-O12-C13=116.0946    O12-C13-H14= 89.4824    O12-C13-C15=113.9252
    H14-C13-C15=120.3036    C10-O11-H16=102.5324    C13-C15-H17=116.0113
    O12-C13-H18= 91.8087    H14-C13-H18=113.7818    C15-C13-H18=118.9908
    C13-C15-C19=118.2435    H17-C15-C19=115.8739    C15-C19-H20=112.9527
    C15-C19-H21=110.6948    H20-C19-H21=108.5139   C15-C19-Cl22=112.8522
   H20-C19-Cl22=105.0687   H21-C19-Cl22=106.3688
Symmetry turned off by external request.
Stoichiometry    C6H12ClNO2
Framework group  C1[X(C6H12ClNO2)]
Deg. of freedom   60
Full point group                 C1      NOp   1
Rotational constants (GHZ):      1.8079226      0.5736436      0.4719325
Isotopes: 
N-14,C-12,H-1,H-1,H-1,C-12,H-1,H-1,H-1,C-12,O-16,O-16,C-12,H-1,C-12,H-
1,H-1,H-1,C-12,H-1,H-1,Cl-35
Leave Link  202 at Thu May 20 09:36:57 2004, MaxMem=   18874368 cpu:       
1.0
(Enter C:\G98W\l301.exe)
Standard basis: 6-31G(d) (6D, 7F)
Integral buffers will be    262144 words long.
Raffenetti 1 integral format.
Two-electron integral symmetry is turned off.
   178 basis functions      352 primitive gaussians
    44 alpha electrons       44 beta electrons
       nuclear repulsion energy       640.5874148911 Hartrees.
Leave Link  301 at Thu May 20 09:36:58 2004, MaxMem=   18874368 cpu:       
1.0
(Enter C:\G98W\l302.exe)
One-electron integrals computed using PRISM.
NBasis=   178 RedAO= T  NBF=   178
NBsUse=   178 1.00D-04 NBFU=   178
Leave Link  302 at Thu May 20 09:37:48 2004, MaxMem=   18874368 cpu:      
50.0
(Enter C:\G98W\l303.exe)
DipDrv:  MaxL=1.
Leave Link  303 at Thu May 20 09:37:59 2004, MaxMem=   18874368 cpu:       
5.0
(Enter C:\G98W\l401.exe)
Initial guess read from the checkpoint file:
transcloropruebamirna.chk
Guess basis functions will be translated to current atomic coordinates.
Leave Link  401 at Thu May 20 09:38:12 2004, MaxMem=   18874368 cpu:      
10.0
(Enter C:\G98W\l502.exe)
IExCor=   0 DFT=F Ex=HF Corr=None ScaHFX= 1.0000
ScaDFX=  0.0000  0.0000  0.0000  0.0000
IRadAn=      0 IRanWt=     -1 IRanGd=            0 ICorTp=0
Using DIIS extrapolation.
Closed shell SCF:
Requested convergence on RMS density matrix=1.00D-08 within  64 cycles.
Requested convergence on MAX density matrix=1.00D-06.
Two-electron integral symmetry not used.
IEnd=    108745 IEndB=    108745 NGot=  18874368 MDV=  18801710
LenX=  18801710
Fock matrices will be formed incrementally for  20 cycles.

Cycle   1  Pass 1  IDiag 1:
Symmetry not used in FoFDir.
MinBra= 0 MaxBra= 2 Meth= 1.
IRaf=       0 NMat=   1 IRICut=       1 DoRegI=T DoRafI=F ISym2E= 0 
JSym2E=0.
E=-0.103992411426457D+04
DIIS: error= 7.58D+00 at cycle   1.
T= 3000. Gap= 0.029 NK=0 IS=    1 IE=  178
          NO(<0.9)=   1  NV(>0.1)=   1  43.82e < EF 0.18e >EF  Err=9.1D-11
RMSDP=1.05D+00 MaxDP=5.86D+01

Cycle   2  Pass 1  IDiag 1:
RMSU=  2.97D-01    CP:  2.27D-02
E=-0.133227733400360D+04 Delta-E=     -292.353219739031
DIIS: error= 4.65D-01 at cycle   2.
Coeff:-0.706D-02-0.993D+00
T= 2700. Gap= 0.028 NK=0 IS=    1 IE=  178
          NO(<0.9)=   1  NV(>0.1)=   1  43.84e < EF 0.16e >EF  Err=8.5D-11
RMSDP=3.07D-01 MaxDP=3.30D+01

Cycle   3  Pass 1  IDiag 1:
RMSU=  7.76D-02    CP:  2.34D-02  5.13D-04
E=-0.115023405980192D+04 Delta-E=      182.043274201684
DIIS: error= 8.34D-01 at cycle   3.
Coeff:-0.440D-02-0.720D+00-0.275D+00
T= 2400. Gap= 0.010 NK=0 IS=    1 IE=  178
          NO(<0.9)=   1  NV(>0.1)=   1  43.63e < EF 0.37e >EF  Err=4.0D-11
RMSDP=8.75D-02 MaxDP=2.45D+00

Cycle   4  Pass 1  IDiag 1:
RMSU=  6.72D-02    CP:  1.36D-02  8.13D-03  2.91D-01
E=-0.146708118239270D+04 Delta-E=     -316.847122590779
DIIS: error= 3.46D-01 at cycle   4.
Coeff:-0.214D-02-0.359D+00-0.729D-01-0.566D+00
T= 2100. Gap= 0.033 NK=0 IS=    1 IE=  178
          NO(<0.9)=   0  NV(>0.1)=   0  43.90e < EF 0.10e >EF  Err=8.9D-11
RMSDP=1.16D-01 MaxDP=6.12D+00

Cycle   5  Pass 1  IDiag 1:
RMSU=  8.97D-02    CP:  4.82D-02  2.87D-02 -8.86D-02  1.48D-01
E=-0.148650601577206D+04 Delta-E=      -19.424833379362
DIIS: error= 2.71D-01 at cycle   5.
Coeff:-0.146D-02-0.223D+00-0.521D-01-0.428D+00-0.296D+00
T= 2100. Gap= 0.029 NK=2 IS=   40 IE=   51
          NO(<0.9)=   0  NV(>0.1)=   1  43.66e < EF 0.34e >EF  Err=1.4D-14
RMSDP=1.00D-01 MaxDP=6.80D+00

Cycle   6  Pass 1  IDiag 1:
RMSU=  2.96D-02    CP:  4.55D-03  2.48D-02  1.09D-01  2.16D-01  7.36D-02
E=-0.153504395441660D+04 Delta-E=      -48.537938644540
DIIS: error= 1.28D-01 at cycle   6.
Coeff:-0.291D-03-0.325D-01-0.902D-02-0.127D+00-0.109D+00-0.722D+00
T= 1500. Gap= 0.044 NK=0 IS=    1 IE=  178
          NO(<0.9)=   0  NV(>0.1)=   0  43.99e < EF 0.01e >EF  Err=5.2D-11
RMSDP=2.23D-02 MaxDP=9.23D-01

Cycle   7  Pass 1  IDiag 1:
RMSU=  1.80D-02    CP:  2.09D-03  1.73D-02  8.67D-02  1.35D-01  9.56D-02
                    CP:  6.18D-01
E=-0.153614250797987D+04 Delta-E=       -1.098553563266
DIIS: error= 1.23D-01 at cycle   7.
Coeff:-0.415D-04-0.942D-02-0.693D-02-0.180D-01 0.168D-02-0.400D+00
Coeff:-0.568D+00
T= 1500. Gap= 0.288 NK=4 IS=   36 IE=   58
          NO(<0.9)=   0  NV(>0.1)=   0  44.00e < EF 0.00e >EF  Err=2.8D-14
RMSDP=9.88D-03 MaxDP=2.82D-01

Cycle   8  Pass 1  IDiag 1:
RMSU=  8.16D-03    CP:  1.50D-03  1.55D-02  9.41D-02  1.32D-01  8.15D-02
                    CP:  6.67D-01  7.14D-01
E=-0.153821497395267D+04 Delta-E=       -2.072465972810
DIIS: error= 4.04D-02 at cycle   8.
Coeff:-0.120D-04 0.579D-02 0.589D-03-0.132D-02 0.322D-02-0.624D-02
Coeff:-0.216D+00-0.786D+00
T=  900. Gap= 0.429 NK=0 IS=    1 IE=  178
          NO(<0.9)=   0  NV(>0.1)=   0  44.00e < EF 0.00e >EF  Err=0.0D+00
RMSDP=1.99D-03 MaxDP=6.24D-02

Cycle   9  Pass 1  IDiag 1:
RMSU=  1.87D-03    CP:  1.35D-03  1.62D-02  9.10D-02  1.30D-01  8.09D-02
                    CP:  6.59D-01  7.38D-01  9.66D-01
E=-0.153832470182727D+04 Delta-E=       -0.109727874597
DIIS: error= 1.87D-02 at cycle   9.
Coeff: 0.127D-06 0.932D-03 0.104D-03-0.145D-02 0.656D-03 0.516D-01
Coeff:-0.575D-01-0.776D-01-0.917D+00
T=  600. Gap= 0.476 NK=0 IS=    1 IE=  178
          NO(<0.9)=   0  NV(>0.1)=   0  44.00e < EF 0.00e >EF  Err=0.0D+00
RMSDP=8.98D-04 MaxDP=3.08D-02

Cycle  10  Pass 1  IDiag 1:
RMSU=  7.47D-04    CP:  1.36D-03  1.57D-02  9.04D-02  1.30D-01  8.17D-02
                    CP:  6.48D-01  7.55D-01  9.73D-01  1.04D+00
E=-0.153834577571776D+04 Delta-E=       -0.021073890486
DIIS: error= 6.65D-03 at cycle  10.
Coeff:-0.324D-06 0.738D-03-0.191D-03-0.585D-03-0.363D-03 0.750D-03
Coeff:-0.106D-01 0.769D-01 0.207D+00-0.127D+01
T=  300. Gap= 0.485 NK=0 IS=    1 IE=  178
          NO(<0.9)=   0  NV(>0.1)=   0  44.00e < EF 0.00e >EF  Err=0.0D+00
RMSDP=4.45D-04 MaxDP=1.07D-02

Cycle  11  Pass 1  IDiag 1:
RMSU=  2.08D-04    CP:  1.37D-03  1.58D-02  8.98D-02  1.30D-01  8.21D-02
                    CP:  6.44D-01  7.63D-01  9.67D-01  1.14D+00  1.39D+00
E=-0.153834949126455D+04 Delta-E=       -0.003715546797
DIIS: error= 1.74D-03 at cycle  11.
Coeff:-0.160D-06 0.319D-03-0.190D-04-0.250D-03 0.113D-04-0.333D-02
Coeff: 0.145D-02 0.121D-02 0.140D+00-0.698D-01-0.107D+01
RMSDP=1.45D-04 MaxDP=3.70D-03

Cycle  12  Pass 1  IDiag 1:
RMSU=  6.36D-05    CP:  1.38D-03  1.57D-02  8.97D-02  1.30D-01  8.22D-02
                    CP:  6.43D-01  7.65D-01  9.67D-01  1.15D+00  1.52D+00
                    CP:  1.28D+00
E=-0.153834979814613D+04 Delta-E=       -0.000306881573
DIIS: error= 4.43D-04 at cycle  12.
Coeff: 0.296D-07 0.853D-05-0.109D-04-0.107D-03 0.784D-04 0.546D-03
Coeff: 0.815D-03-0.138D-01-0.129D-01 0.708D-01 0.674D-01-0.111D+01
RMSDP=4.15D-05 MaxDP=1.21D-03

Cycle  13  Pass 1  IDiag 1:
RMSU=  2.55D-05    CP:  1.38D-03  1.57D-02  8.98D-02  1.30D-01  8.22D-02
                    CP:  6.43D-01  7.64D-01  9.67D-01  1.13D+00  1.53D+00
                    CP:  1.33D+00  1.32D+00
E=-0.153834982555433D+04 Delta-E=       -0.000027408205
DIIS: error= 1.47D-04 at cycle  13.
Coeff: 0.453D-08-0.748D-05-0.958D-06-0.150D-04 0.207D-04 0.475D-04
Coeff: 0.404D-03-0.176D-03-0.517D-02-0.164D-01 0.117D+00-0.543D-01
Coeff:-0.104D+01
RMSDP=1.51D-05 MaxDP=3.60D-04

Cycle  14  Pass 1  IDiag 1:
RMSU=  7.21D-06    CP:  1.38D-03  1.57D-02  8.98D-02  1.30D-01  8.22D-02
                    CP:  6.43D-01  7.64D-01  9.68D-01  1.13D+00  1.52D+00
                    CP:  1.34D+00  1.47D+00  1.28D+00
E=-0.153834982919234D+04 Delta-E=       -0.000003638010
DIIS: error= 6.27D-05 at cycle  14.
Coeff:-0.156D-07 0.187D-06 0.150D-05 0.120D-05-0.170D-05-0.256D-04
Coeff: 0.136D-03 0.114D-02 0.382D-03-0.569D-02-0.112D-01 0.114D+00
Coeff: 0.572D-01-0.116D+01
RMSDP=6.82D-06 MaxDP=1.91D-04

Cycle  15  Pass 1  IDiag 1:
RMSU=  2.89D-06    CP:  1.38D-03  1.57D-02  8.98D-02  1.30D-01  8.22D-02
                    CP:  6.43D-01  7.64D-01  9.68D-01  1.13D+00  1.52D+00
                    CP:  1.33D+00  1.51D+00  1.44D+00  1.29D+00
E=-0.153834982976227D+04 Delta-E=       -0.000000569930
DIIS: error= 2.40D-05 at cycle  15.
Coeff:-0.136D-07 0.604D-06-0.869D-06 0.497D-05-0.502D-06-0.234D-04
Coeff: 0.290D-04 0.611D-05 0.684D-03 0.159D-02-0.139D-01 0.761D-02
Coeff: 0.116D+00 0.105D-01-0.112D+01
RMSDP=2.27D-06 MaxDP=5.15D-05

Cycle  16  Pass 1  IDiag 1:
RMSU=  7.93D-07    CP:  1.38D-03  1.57D-02  8.98D-02  1.30D-01  8.22D-02
                    CP:  6.43D-01  7.64D-01  9.68D-01  1.13D+00  1.52D+00
                    CP:  1.33D+00  1.52D+00  1.48D+00  1.46D+00  1.39D+00
E=-0.153834982982640D+04 Delta-E=       -0.000000064131
DIIS: error= 5.75D-06 at cycle  16.
Coeff:-0.258D-08-0.559D-06 0.120D-06-0.569D-06 0.504D-06 0.159D-05
Coeff:-0.333D-05-0.171D-03-0.200D-04 0.884D-03-0.498D-03-0.122D-01
Coeff: 0.672D-02 0.139D+00-0.183D+00-0.950D+00
RMSDP=6.99D-07 MaxDP=1.99D-05

Cycle  17  Pass 1  IDiag 1:
RMSU=  3.09D-07    CP:  1.38D-03  1.57D-02  8.98D-02  1.30D-01  8.22D-02
                    CP:  6.43D-01  7.64D-01  9.68D-01  1.13D+00  1.52D+00
                    CP:  1.33D+00  1.52D+00  1.49D+00  1.48D+00  1.56D+00
                    CP:  1.24D+00
E=-0.153834982983370D+04 Delta-E=       -0.000000007301
DIIS: error= 2.60D-06 at cycle  17.
Coeff: 0.192D-08-0.149D-06-0.428D-07-0.366D-06 0.208D-06-0.161D-06
Coeff:-0.206D-05 0.430D-05-0.294D-04-0.147D-03 0.129D-02-0.204D-02
Coeff:-0.897D-02 0.697D-02 0.125D+00-0.898D-01-0.103D+01
RMSDP=3.12D-07 MaxDP=6.73D-06

Cycle  18  Pass 1  IDiag 1:
RMSU=  1.43D-07    CP:  1.38D-03  1.57D-02  8.98D-02  1.30D-01  8.22D-02
                    CP:  6.43D-01  7.64D-01  9.68D-01  1.13D+00  1.52D+00
                    CP:  1.33D+00  1.52D+00  1.49D+00  1.49D+00  1.63D+00
                    CP:  1.44D+00  1.33D+00
E=-0.153834982983514D+04 Delta-E=       -0.000000001432
DIIS: error= 1.01D-06 at cycle  18.
Coeff: 0.343D-09 0.334D-07-0.717D-07 0.226D-07 0.100D-06 0.171D-05
Coeff:-0.204D-05 0.221D-04-0.511D-04-0.794D-04 0.431D-03 0.163D-02
Coeff:-0.106D-02-0.209D-01 0.306D-01 0.130D+00 0.101D-01-0.115D+01
RMSDP=1.58D-07 MaxDP=4.01D-06

Cycle  19  Pass 1  IDiag 1:
RMSU=  5.09D-08    CP:  1.38D-03  1.57D-02  8.98D-02  1.30D-01  8.22D-02
                    CP:  6.43D-01  7.64D-01  9.68D-01  1.13D+00  1.52D+00
                    CP:  1.33D+00  1.52D+00  1.49D+00  1.50D+00  1.64D+00
                    CP:  1.52D+00  1.62D+00  1.54D+00
E=-0.153834982983549D+04 Delta-E=       -0.000000000349
DIIS: error= 3.86D-07 at cycle  19.
Coeff:-0.486D-09 0.975D-07-0.271D-08-0.981D-07-0.181D-07 0.732D-06
Coeff: 0.910D-07 0.247D-05 0.119D-04 0.270D-05-0.131D-03 0.361D-03
Coeff: 0.126D-02-0.354D-02-0.196D-01 0.367D-01 0.133D+00-0.107D-01
Coeff:-0.114D+01
RMSDP=7.28D-08 MaxDP=1.21D-06

Cycle  20  Pass 1  IDiag 1:
Restarting incremental Fock formation.
E=-0.153834982983562D+04 Delta-E=       -0.000000000136
DIIS: error= 2.54D-07 at cycle   1.
RMSDP=2.39D-08 MaxDP=6.10D-07

Cycle  21  Pass 1  IDiag 1:
RMSU=  2.39D-08    CP:  1.00D+00
E=-0.153834982983558D+04 Delta-E=        0.000000000042
DIIS: error= 1.51D-07 at cycle   2.
Coeff:-0.337D+00-0.663D+00
RMSDP=8.78D-09 MaxDP=3.23D-07

SCF Done:  E(RHF) =  -897.762414945     A.U. after   21 cycles
             Convg  =    0.8779D-08             -V/T =  2.0013
             S**2   =   0.0000
KE= 8.965523143849D+02 PE=-3.402772737345D+03 EE= 9.678705931246D+02
Leave Link  502 at Thu May 20 10:15:36 2004, MaxMem=   18874368 cpu:    
2242.0
(Enter C:\G98W\l801.exe)
Range of M.O.s used for correlation:    15   178
NBasis=   178 NAE=    44 NBE=    44 NFC=    14 NFV=     0
NROrb=    164 NOA=    30 NOB=    30 NVA=   134 NVB=   134
Leave Link  801 at Thu May 20 10:15:37 2004, MaxMem=   18874368 cpu:       
0.0
(Enter C:\G98W\l906.exe)
Frozen-core derivative calculation, NFC=  14 NFV=   0.
FulOut=F Deriv=T AODrv=T
   MMem=           0  MDisk=          30 MDiskD=          30
  W3Min=     1394096 MinDsk=     3812475 NBas6D=         178
NBas2D=       16207    NTT=       15931    LW2=     2000000
    MDV=    16691780 MDiskM=        1146 NBas2p=       15291
Disk-based method using ON**2 memory for 30 occupieds at a time.
Permanent disk used for amplitudes=    43192622 words.
Estimated scratch disk usage=   299688290 words.
IMap=  1  2  3  4  5  6  7  8  9 10 11 12 13 14 15 16 17 18 19 20
IMap= 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40
IMap= 41 42 43 44
Actual    scratch disk usage=   289309026 words.
JobTyp=1 Pass  1:  I=  15 to  44.
writwa


------=_NextPart_000_7768_40a2_3fca--


From chemistry-request@ccl.net Fri May 21 12:09:38 2004
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References: <20040520183613.D65761-100000)at(mserv.itpa.lt>
Date: Fri, 21 May 2004 19:09:08 +0200
To: Arvydas Tamulis <tamulis)at(mserv.itpa.lt>
From: Per-Ola Norrby <pon)at(kemi.dtu.dk>
Subject: Re: CCL:The pi-pi stacking of hetero-aromatic ring
Cc: CHEMISTRY)at(ccl.net
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>Would you please to advise us the quantum chemical methods and programs
>that might properly calculate stacking interactions including
>dispersion effects in oligomeric nucleic acids (two types of interactions:
>in parallel planes and when planes are perpendicular).

	I don't think there is any QM method able to treat oligomeric 
nucleic acids which can also include accurate dispersion.  DFT or HF 
do NOT include dispersion.  The lowest level I know which does 
include some of the dispersion is MP2, and with any feasible basis 
set for this large system, the basis set deficiency error would be 
expected to totally swamp the dispersion.  The same would be true for 
any correlated method.  (I'll probably be flamed for this statement, 
but I believe it; I don't have proof though, so don't ask for it). 
Counterpoise correction might bring the error down, but certainly not 
to zero.

	You can get the dispersion term accurately from empirical 
force fields.  This is a very well known term, and it has been 
accurately parameterized for many years.  With many force fields, you 
will treat other non-bonded terms erroneously (like in any method 
that uses Lennard-Jones, where the repulsion is strongly 
overestimated), and the electrostatics are always a problem.  I saw a 
JCC article a few years ago which augmented DFT with an empirical 
dispersion term (I don't have the reference), that seems a feasible 
approach.  Otherwise, I'd take a force field that has proven to treat 
DNA well, like AMBER, it's probably superior in quality to any 
achievable QM.  And of course it's several orders of magnitude 
faster...  Not that I use it myself, I'm an MM3 fan, but I wouldn't 
advocate MM3 for oligonucleotides unless you take the electrostatics 
> from a QM source.

	Note that in DFT and HF, you always see an attractive force 
at something similar to the vdW distance.  It's not dispersion, it's 
a simple basis set superposition error together with any 
electrostatic attraction your complex might have.  Sometimes it has a 
similar value to the dispersion, but I wouldn't trust the predictive 
value of this error cancellation.

	If you absolutely have to have your dispersion from QM, you 
could probably set up some kind of extrapolation scheme, like IMOMO 
or ONIOM, where you use CCSD(T) with a large basis for a very small 
core.  It will only give you accurate dispersion for a small 
subsystem though.  You can always validate your final result by 
comparing to a good empirical force field...

	/Per-Ola
-- 
Per-Ola Norrby, Assoc. Professor, http://organisk.kemi.dtu.dk/PON/
Technical University of Denmark, Department of Chemistry
Building 201, Kemitorvet, DK-2800 Kgs. Lyngby, Denmark
Email: pon)at(kemi.dtu.dk  tel +45-45252123,  fax +45-45933968

From chemistry-request@ccl.net Fri May 21 10:25:28 2004
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From: "Robert W. Zoellner" <rwz7001[at]humboldt.edu>
Subject: CCL:  Gasuuian MAXCYCLE question
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Greetings All,

My student and I are attempting to run a job with Gaussian that requires
more optimization cycles than are allowed by the OPT(MAXCYCLE=2000)
numerical limit.  How can we change MAXCYCLE= to allow more than the 2000
cycle limit?  (We've attempted to do this by using the input
MAXCYCLE=1.0e5, for example, without success.)

Thanks for the assistance.

All the best,

Bob Z.

Robert W. Zoellner, Ph.D.
Professor
Department of Chemistry
Humboldt State University
One Harpst Street
Arcata, California  95521-8299

telephone:  (707)826-3244
fax:  (707)826-3279


From chemistry-request@ccl.net Fri May 21 12:13:22 2004
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Date: Thu, 20 May 2004 13:27:02 -0500
From: "Ivanciuc, Ovidiu I." <oiivanci[at]utmb.edu>
Subject: CCL: The hydrophocities for 20 amino acids
To: chemistry[at]ccl.net
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Hi,

>I need the experimental results of the hydrophobicities for 20 amino
>acids, could you please show me how I can get them? Any tips will be
>welcome!

The AAindex (Amino acid indices and similarity matrices) database,
http://www.genome.ad.jp/dbget/aaindex.html contains numerical
values for the major hydrophobicity scales.

Another source of hydrophobicity scales for amino acids is
the ProtScale from ExPASY: http://us.expasy.org/cgi-bin/protscale.pl


Regards,
Ovidiu Ivanciuc




From chemistry-request@ccl.net Fri May 21 10:09:34 2004
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Date: Fri, 21 May 2004 16:12:20 +0100 (BST)
From: =?iso-8859-1?q?Jeff=20C?= <orbital_jc[at]yahoo.co.uk>
Subject: running GAMESS using Beowulf cluster 
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Dear Comp Chem Experts,

I am new to this field so I will apologize in advance
if the following question is too trivial to the
skilled researchers. 

Currently I am trying to learn how to use gamess. The
procedure is simple when comes to running gamess with
single CPU. However, I am clueless when trying to run
gamess on our newly built 16 nodes Beowulf cluster
using MPI. I hope someone out there can give me the
step-by-step guide.

Much appreciated.

Jeff Chen   



	
	
		
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From chemistry-request@ccl.net Fri May 21 09:49:00 2004
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From: "Noel O'Boyle" <noel.oboyle2~at~mail.dcu.ie>
Subject: Summary: Gaussian MSK charges
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Thanks to everyone that answered my email about choosing the correct radius
for Ru in a Gaussian MSK (Merz-Singh-Kollman) atomic charge calculation.

My original email is included below as well as very helpful replies from:
G|nter Klatt, David Shobe, Vincent Xianlong Wang, Errol Lewars and Marcel
Swart.

Noel

>Hello CCLers,
>
>I am trying to calculate Merz-Singh-Kollman charges for a ruthenium complex
>using Gaussian03 and the POP=MK keyword.
>
>Gaussian stops with an error message because it has no Merz-Kollman radius
>for Ruthenium.
>
>I know how to include a radius for Ruthenium (the POP=(MK,ReadRadii) keyword)
>but I don't know what value I should use. Can anybody help me?
>
>H is 1.20
>C is 1.50
>N is 1.50
>Ru is ??
>
>Are these numbers related to the van der Waal radii, or are they simply
>scaling factors?
>
>Noel

Hello Noel

The radius should be the van der Waals radius of Ru in the proper oxidation
state, probably somewhere around 1.7 A. Have a look at our recent paper

Lienke et al., Inorg. Chem. 2001, 40, 2352-2357

and references therein (especially Bondi's and Hambley's!)

Regards

Guenter

Noel,

I had the same problem with the Breneman radii for CHELPG. I never really
got an answer, either from CCL or from the journal article that introduced
the method. In CHELPG at least, the atomic radii are there to create exclusion
zones around each atom, and as long as you took reasonable radii that were
a bit *larger* than tabulated van der Waals radii, the results were not
very radius dependent.

The Merz-Kollman radii appear to be similar to the CHELPG radii so probably
you can do what I ended up doing, which was add 0.2 Angstroms to the van
der Waals radii. But you may want to try a few values to verify that the
choice of radius is not important--and then consistently use the same radius
for "production" calculations. 

--David Shobe, Ph.D., M.L.S.

Try web of elements.
http://www.webelements.com/

Vincent

hello,
I have not done this kind of calc. with G03, but:
If nothing better comes up, I suggest you plot a graph of the 
Merz-Kollman radii which you have (H 1.20, C 1.50, ...) against van der

Waals radii; assuming you know the van der Walls radius of Ru, you 
should be able to get from this the Ru Merz-Kollman radius.

EL

See a related message from sometime ago. Although that one dealt with 
CHELPG instead of
MSK, the same problem is present.

Begin forwarded message:

> From: Valentin Gogonea <v.gogonea~at~csuohio.edu>
> Date: November 28, 2002 2:42:36 PM CET
> To: chemistry~at~ccl.net
> Subject: CCL:Summary: CHelpG calculation for Fe
>
> Dear CCLers,
>
> A couple of weeks ago I asked for advice for selecting the radius for

> Fe(2+) for CHelpG calculations. Thank you very much to all who 
> answered.
>
> Valentin Gogonea
> Cleveland State University
>
> Here are the replies that I received:
> -----------------------------------------------------------------------

> -----------------------------------------------------------------------

> --------------------
> We never tried to go that far down in the periodic table when we 
> developed some
> of the radii for other atoms, but I suggest that you use a 
> (consistent) value
> that represents the van der Waals radius of the atom. The danger of 
> using too
> large a radius is the loss of information from the other atoms in the

> molecule,
> and an underdetermined charge fitting model. Good luck with your
> experimentation. I suggest you try several reasonable values and then

> see if
> the charges computed for all of the atoms are reasonably consistent.
>
> Curt Breneman
> RPI Chemistry
>
> -----------------------------------------------------------------------

> -----------------------------------------------------------------------

> --------------------
>
> From gromacs list:
>
> I did gaussian 98 calculations on Fe(III). Here are my notes
> concerning the radii that I used. Hope it helps,
>
> Cheers,
> Marc
>
> For iron there are several ionic radii. Let's use radii from
> http://www.webelements.com/webelements/elements/text/Fe/radii.html.
>
> o Fe(III) 6-coordinate, octahedral 69 pm
>
> o Fe(III) 6-coordinate, octahedral, high spin 78.5 pm
>
> Note: The "efective ionic radii" quoted here assume that the ionic
> radius of F- is 133 pm and that of O2- is 140 pm. The values for iron
> thus correspond quite well to che tabulated Gaussian Merz-Kollman
> radii, and will be scaled for Francl and Breneman, with a mean factor
> for F- and O2-. Values depend upon the coordination number and for
> d-block metals on the fact whether or not the metal is in a high or
> low spin state.
>
> Atomnb AtTyp Merz-Kollman Francl Breneman
> (CHELP) (CHELPG)
>> ............. ............. ............. ............. .............
> 26 Fe 0.69 0.75 0.85
> 6-coordinate,
> octahedral
> 26 Fe 0.785 0.85 0.97
> 6-coordinate,
> octahedral,
> high spin
>
> -----------------------------------------------------------------------

> -----------------------------------------------------------------------

> --------------------
>
> you could try a number of different radii and see where the charges
> are approximately constant. I would guess a radius of 2.0 A.
> Please, see our article, where we determine a radius for Cu2+:
> E. Sigfridsson & U. Ryde (1998) "A comparison of methods for deriving

> atomic charges from the electrostatic potential and moments". J. 
> Comp. Chem. 19, 377-395.
>
> Best regards,
> Ulf
> -----------------------------------------------------------------------

> -----------------------------------------------------------------------

> --------------------
>
> We typically use Fe radius of 1.5A, sometimes even 1.3A, but the Fe(3+)
> or Fe(2+) is nearly always surrounded by ligands and the whole complex
> is treated by quantum calc's (DFT), so the Fe radius is not important.
> Use of the bare ion alone will lead to poor properties, as we showed
> in an Inorg. Chem. paper on metal cations in water in 1996.
> Best Regards,
> Lou Noodleman
> -----------------------------------------------------------------------

> -----------------------------------------------------------------------

> --------------------
>
> To read in a radius for Fe, use the option 
> "pop=(chelpg,ReadAtRadii)". These values are usually not the textbook

> van der Waals radii, but radii that have been chosen by the authors of

> a given charge scheme. The choice of a radius for an element that was

> not in the original parameter set is a judgment call and depends 
> somewhat on the task at hand (whether the atom is ionic, for example).

> Below is an example input file in which I arbitrarily chose to use the

> metallic radius of Fe.
>
> #p rhf/sto-3g scf=tight symm=loose pop=(chelpg,readradii) test
>
> ferrocene example
>
> 0 1
> Fe -0.000000 -0.000000 0.000000
> X -0.000000 0.000000 -2.160000
> C -0.000000 1.250000 -2.160000
> C 1.188821 0.386271 -2.160000
> C -1.188821 0.386271 -2.160000
> H 0.113936 2.334029 -2.160000
> C 0.734732 -1.011271 -2.160000
> H 2.255002 0.612895 -2.160000
> C -0.734732 -1.011271 -2.160000
> H -2.184585 0.829614 -2.160000
> H 1.279732 -1.955239 -2.160000
> H -1.464084 -1.821299 -2.160000
> X 0.000000 0.000000 2.160000
> C 0.000000 1.250000 2.160000
> C -1.188821 0.386271 2.160000
> C 1.188821 0.386271 2.160000
> H -0.113936 2.334029 2.160000
> C -0.734732 -1.011271 2.160000
> H -2.255002 0.612895 2.160000
> C 0.734732 -1.011271 2.160000
> H 2.184585 0.829614 2.160000
> H -1.279732 -1.955239 2.160000
> H 1.464084 -1.821299 2.160000
>
> Fe 1.24
>
>
>
> Regards,
> Jim Hess
>
>
> -= This is automatically added to each message by mailing script =-
> CHEMISTRY~at~ccl.net -- To Everybody | CHEMISTRY-REQUEST~at~ccl.net -- To 
> Admins
> Ftp: ftp.ccl.net | WWW: http://www.ccl.net/chemistry/ | Jan: 
> jkl~at~ccl.net
>
>
>
>
>
>
>
????????????????????????????????????????????
dr. Marcel Swart





From chemistry-request@ccl.net Fri May 21 10:17:41 2004
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From: Mehdi Bounouar <mehdi.bounouar~at~ch.tum.de>
To: CHEMISTRY~at~ccl.net
Subject: ECP gamess input 
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Hello,

If someone knows why the following input in GAMESS does not work, or
manages to make it run, I would really appreciate any advice.

Thanks

Regards





          ECP POTENTIALS
          --------------
 **** ERROR READING VARIABLE NGPOT  ^@ CHECK COLUMN  1
 C2-ECP NONE

....V....1....V....2....V....3....V....4....V....5....V....6....V....7....V....8

 *** ERROR ***
 AN UNEXPECTED $END WAS ENCOUNTERED IN $ECP GROUP.
 EVERY ATOM IN THE MOLECULE MUST BE DEFINED IN $ECP.





 $CONTRL SCFTYP=ROHF RUNTYP=ENERGY ECP=READ MULT=2 COORD=UNIQUE $END
 $SCF DIRSCF=.true. $END
 $SYSTEM MWORDS=120 TIMLIM=40000 $END
 $DATA
ETHANE with QCP1: JCP 116 (2002), 9578
C1
 C1  6   0.000000     0.000000     0.000000
    L   1
     1    0.12D0    1.00D0    1.00D0
    L   1
     1    0.36D0    1.00D0    1.00D0
    L   1
     1    1.08D0    1.00D0    1.00D0
    L   1
     1    3.24D0    1.00D0    1.00D0
    L   1
     1    9.72D0    1.00D0    1.00D0
    D   1
     1    0.626D0   1.00D0

 C2  6   0.000000     0.000000     1.526681
  N31 6
    D   1
     1       0.800000000          1.00000000

 H  1   1.012207     0.000000    -0.392775
  N31 6
   P   1
     1    1.10000000          1.00000000

 H  1   -0.506104    -0.876597    -0.392775
  N31 6
   P   1
     1    1.10000000          1.00000000

 H  1   -0.506104     0.876597    -0.392775
  N31 6
   P   1
     1    1.10000000          1.00000000

 $END
 $ECP
C1-ECP  GEN  5  2
  2      -----   POTENTIAL     -----
   -0.86     1       8.14
   -2.60     1       1.29
  3      -----   POTENTIAL     -----
    5.90     0      10.16
   -7.30     1       2.56
    26.11    2       3.62
C2-ECP NONE
H-ECP NONE
H-ECP NONE
H-ECP NONE
 $END




From chemistry-request@ccl.net Fri May 21 10:00:00 2004
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Date: Fri, 21 May 2004 09:05:14 +0200 (CEST)
Subject: CCL: dft/mrci
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Dear CCLers,

Does anybody know any software which implements DFT/MRCI method?

Yours,

Marcin Makowski
Ph.D. student
in Theoretical Chemistry
Jagiellonian University





From chemistry-request@ccl.net Fri May 21 16:35:42 2004
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From: Eugen Leitl <eugen/at/leitl.org>
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Subject: [Beowulf] CCL:Question regarding Mac G5 performance (fwd from konstantin_kudin/at/yahoo.com)
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----- Forwarded message from Konstantin Kudin <konstantin_kudin/at/yahoo.com> =
-----

From: Konstantin Kudin <konstantin_kudin/at/yahoo.com>
Date: Fri, 21 May 2004 14:23:48 -0700 (PDT)
To: beowulf/at/beowulf.org
Subject: [Beowulf] CCL:Question regarding Mac G5 performance

> Again...SPEC was included, among a number of others. Would you happen

> to have a cross section of code relevant to computational chemistry =20

> that might offer a fair example of platform performance? I'd enjoy a=20
> chance to get it into the labs and see how Itanuim 2 might stack up.

 While I can't speak for every code out there, for Gaussian03 I2 seems
to work extremely well:
http://www.princeton.edu/~kkudin/g03_b5_tests_1.txt

 Note that these are ~1 hour long jobs, which surely do not fit in
cache.

 The interesting part is that for some real life codes I2 performance
matches what SPEC numbers would predict. The cost, of course, is a
different issue altogether.

 Konstantin
=20


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	=09
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From chemistry-request@ccl.net Fri May 21 15:52:10 2004
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Date: Thu, 20 May 2004 20:58:35 +0200
From: Alessandro Contini <alessandro.contini-.at.-unimi.it>
Subject: amber parameters in G03 MM
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Hi, I'm triyng to set up a oniom calculation using the amber ff for the MM 
part. I'm using GaussView3.09 to set up the run, but I noticed that some 
aminoacids, in particular histidine, have missing parameters and the charge 
is not automatically added to the AT definition in the input file. I found 
this surprising as such parameters are included in the standard amber ff. 
Could anybody suggest me how to include those missing parameters? 

Thanks a lot for your help

Alessandro 

   
-- 
Alessandro Contini, Ph.D.
Istituto di Chimica Organica "Alessandro Marchesini"
Universit` degli Studi di Milano, Facolt` di Farmacia
Via Venezian, 21 20133 Milano 
Tel. +390250314480 Fax. +390250314476
e-mail alessandro.contini-.at.-unimi.it





