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From: Matthias Gottschalk <gottschalk=at=gfz-potsdam.de>
Subject: CCL:Heat capacities with g03
Date: Tue, 20 Apr 2004 07:47:22 +0200
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Dear CCL,

as a naive geoscientist I try to calculate the heat capacities of 
specific single
molecules using g03 with something like that for Si2O7H6:

%chk=si2ooh6.chk
%mem=2048MB
%nproc=1
# opt=(restart, verytight) Int=UltraFine freq pbepbe/6-311++g(3d,2p)
geom=connectivity temperature=298.15 pressure=0.9869233
.
.
.
.


Everything runs fine. At the end I do get the following warnings within 
my results:

  -------------------
  - Thermochemistry -
  -------------------
  Temperature   298.150 Kelvin.  Pressure    .98700 Atm.
  Molecular mass:   173.96521 amu.
  Principal axes and moments of inertia in atomic units:
                            1         2         3
      EIGENVALUES --   890.447432428.485422488.20921
            X            -.63183    .74944    .19780
            Y            -.05907   -.30101    .95179
            Z             .77285    .58968    .23446
  This molecule is an asymmetric top.
  Rotational symmetry number  1.
  Warning -- assumption of classical behavior for rotation
            may cause significant error
  Rotational temperatures (Kelvin)       .09727      .03567      .03481
  Rotational constants (GHZ):           2.02678      .74316      .72532
  Zero-point vibrational energy     237943.2 (Joules/Mol)
                                    56.86979 (Kcal/Mol)
  Warning -- explicit consideration of  20 degrees of freedom as
            vibrations may cause significant error
  Vibrational temperatures:     22.32    47.39   164.92   198.54   252.18
           (Kelvin)            274.49   292.94   351.57   352.45   378.41
                               424.27   433.89   483.89   496.09   507.09
                               529.63   559.68   590.08   792.66   885.13
                              1071.96  1143.85  1168.05  1211.52  1224.45
                              1259.83  1274.99  1281.78  1340.88  1371.30
                              1389.84  1430.93  1501.79  5248.42  5427.26
                              5454.86  5462.94  5466.36  5467.29

  Zero-point correction=                            .090628 
(Hartree/Particle)
  Thermal correction to Energy=                     .103807
  Thermal correction to Enthalpy=                   .104751
  Thermal correction to Gibbs Free Energy=          .050334
                      E (Thermal)             CV                S
                       KCal/Mol        Cal/Mol-Kelvin    Cal/Mol-Kelvin
  Total                   65.140             46.134            114.529
  Electronic                .000               .000               .000
  Translational             .889              2.981             41.394
  Rotational                .889              2.981             30.066
  Vibrational             63.362             40.173             43.069
  Vibration  1              .593              1.986              7.139
  Vibration  2              .594              1.983              5.644
  Vibration  3              .608              1.937              3.189
  Vibration  4              .614              1.915              2.832
  Vibration  5              .627              1.873              2.378
  Vibration  6              .634              1.853              2.220
  Vibration  7              .639              1.835              2.100
  Vibration  8              .660              1.772              1.771
  Vibration  9              .660              1.771              1.767
  Vibration 10              .670              1.741              1.642
  Vibration 11              .689              1.683              1.446
  Vibration 12              .694              1.671              1.408
  Vibration 13              .717              1.603              1.230
  Vibration 14              .723              1.586              1.190
  Vibration 15              .729              1.570              1.155
  Vibration 16              .741              1.538              1.088
  Vibration 17              .757              1.494              1.004
  Vibration 18              .774              1.448               .926
  Vibration 19              .906              1.138               .542
  Vibration 20              .975              1.000               .424

In this regard I do have the following questions:

1. Some rotations might be frozen at low temperatures, but the 
rotational temperatures are here
so low that I can ignore the first warning at ambient temperatures and 
above. Right?

2. Most if not all of the vibrational temperatures are significant. The 
calculated total heat capacity
is too high because not all vibrations are active at the chosen 
temperature. Right? What can I do
to get reliable heat capacities.

Are there other options in g03?
How to choose the right vibrational contributions to cv?
Can I reduce the explicit consideration of  20 degrees of freedom?
Where can I learn more how to deal with the problem practically?

Any help is welcome.

Matthias

-- 

PD Dr. Matthias Gottschalk
GeoForschungsZentrum
Projektbereich 4.1
Telegrafenberg
14473 Potsdam
Germany

tel/fax  +49 (0) 331 288-1418/1402

--Apple-Mail-2-1053627796
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Dear CCL,


as a naive geoscientist I try to calculate the heat capacities of
specific single 

molecules using g03 with something like that for Si2O7H6:


<fontfamily><param>Courier</param>%chk=si2ooh6.chk

%mem=2048MB

%nproc=1

# opt=(restart, verytight) Int=UltraFine freq pbepbe/6-311++g(3d,2p) 

geom=connectivity temperature=298.15 pressure=0.9869233

.

.

.

.

</fontfamily>


Everything runs fine. At the end I do get the following warnings
within my results:


 <fontfamily><param>Courier</param>-------------------

 - Thermochemistry -

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

 Temperature   298.150 Kelvin.  Pressure    .98700 Atm.

 Molecular mass:   173.96521 amu.

 Principal axes and moments of inertia in atomic units:

                           1         2         3

     EIGENVALUES --   890.447432428.485422488.20921

           X            -.63183    .74944    .19780

           Y            -.05907   -.30101    .95179

           Z             .77285    .58968    .23446

 This molecule is an asymmetric top.

 Rotational symmetry number  1.

 Warning -- assumption of classical behavior for rotation

           may cause significant error

 Rotational temperatures (Kelvin)       .09727      .03567      .03481

 Rotational constants (GHZ):           2.02678      .74316      .72532

 Zero-point vibrational energy     237943.2 (Joules/Mol)

                                   56.86979 (Kcal/Mol)

 Warning -- explicit consideration of  20 degrees of freedom as

           vibrations may cause significant error

 Vibrational temperatures:     22.32    47.39   164.92   198.54  
252.18

          (Kelvin)            274.49   292.94   351.57   352.45  
378.41

                              424.27   433.89   483.89   496.09  
507.09

                              529.63   559.68   590.08   792.66  
885.13

                             1071.96  1143.85  1168.05  1211.52 
1224.45

                             1259.83  1274.99  1281.78  1340.88 
1371.30

                             1389.84  1430.93  1501.79  5248.42 
5427.26

                             5454.86  5462.94  5466.36  5467.29

 

 Zero-point correction=                            .090628
(Hartree/Particle)

 Thermal correction to Energy=                     .103807

 Thermal correction to Enthalpy=                   .104751

 Thermal correction to Gibbs Free Energy=          .050334

                     E (Thermal)             CV                S

                      KCal/Mol        Cal/Mol-Kelvin    Cal/Mol-Kelvin

 Total                   65.140             46.134            114.529

 Electronic                .000               .000               .000

 Translational             .889              2.981             41.394

 Rotational                .889              2.981             30.066

 Vibrational             63.362             40.173             43.069

 Vibration  1              .593              1.986              7.139

 Vibration  2              .594              1.983              5.644

 Vibration  3              .608              1.937              3.189

 Vibration  4              .614              1.915              2.832

 Vibration  5              .627              1.873              2.378

 Vibration  6              .634              1.853              2.220

 Vibration  7              .639              1.835              2.100

 Vibration  8              .660              1.772              1.771

 Vibration  9              .660              1.771              1.767

 Vibration 10              .670              1.741              1.642

 Vibration 11              .689              1.683              1.446

 Vibration 12              .694              1.671              1.408

 Vibration 13              .717              1.603              1.230

 Vibration 14              .723              1.586              1.190

 Vibration 15              .729              1.570              1.155

 Vibration 16              .741              1.538              1.088

 Vibration 17              .757              1.494              1.004

 Vibration 18              .774              1.448               .926

 Vibration 19              .906              1.138               .542

 Vibration 20              .975              1.000               .424</fontfamily>


In this regard I do have the following questions:


1. Some rotations might be frozen at low temperatures, but the
rotational temperatures are here 

so low that I can ignore the first warning at ambient temperatures and
above. Right?


2. Most if not all of the vibrational temperatures are significant.
The calculated total heat capacity 

is too high because not all vibrations are active at the chosen
temperature. Right? What can I do 

to get reliable heat capacities.


Are there other options in g03?

How to choose the right vibrational contributions to cv?

Can I reduce the explicit consideration of  20 degrees of freedom?

Where can I learn more how to deal with the problem practically?


Any help is welcome.


Matthias


-- 


PD Dr. Matthias Gottschalk

GeoForschungsZentrum

Projektbereich 4.1

Telegrafenberg

14473 Potsdam

Germany


tel/fax  +49 (0) 331 288-1418/1402


--Apple-Mail-2-1053627796--




From chemistry-request@ccl.net Mon Apr 19 19:30:53 2004
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Date: Tue, 20 Apr 2004 10:31:32 +1000
From: Renate Griffith <Renate.Griffith(at)newcastle.edu.au>
Subject: CCL: MM2004 - Register Now!!!
To: CHEMISTRY(at)ccl.net
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Closing Dates:		
Abstract Submission: 		23 Apr 04
Early Bird Registration: 	30 Apr 04

The 9th Australian Molecular Modelling Workshop, MM2004, will be held in Sydney, Australia
DATES:		Wed 30th June till Sat 3rd July 2004 
VENUE:		InterContinental Hotel, Central Sydney

Full details available at     	http://www.pco.com.au/mm2004

The workshop is a joint conference of the Molecular Graphics and Modelling Society (MGMS), the Royal Australian Chemical Institute (RACI), and the Modellers of Australia.

The workshop will cover a broad range of topics spanning biological, chemical, and physical applications including:

Bioinformatics
StructureBased Drug Design
LigandBased Drug Design
Protein Modelling
1st Principles Techniques
Teaching Molecular Modelling
Material Science


Confirmed Speakers include:

Prof. Peter Boyd, University of Auckland
Prof. Tim Clark, University of ErlangenN|rnberg
Dr David Edwards, Accelrys San Diego
Prof. Marcus Elstner, University of Paderborn
Dr Michael Frisch, Gaussian Inc.
Dr Valerie Gillet, University of Sheffield
Dr Jill Gready, Australian National University
Prof. David Jones, University College London
Dr Ricardo Mancera, De Novo Pharmaceuticals
Prof. Leo Radom, University of Sydney
Prof. Gustavo Scuseria, Rice University
Dr Mark Smythe, Institute for Molecular Bioscience
Prof. Catherine Stampfl, University of Sydney
Prof. David Winkler, CSIRO Molecular Science
Dr Irene Yarovsky, RMIT University
Dr Brian Yates, University of Tasmania

 
MM2004 will start with a joint session on Wednesday afternoon, with the 6th Australia / Japan
Symposium on Drug Design and Development (6DDD). 6DDD starts 27th June, also in Sydney.
http://www.usyd.edu.au/pharmacology/aalab/6DDD/

MM2004 will also be preceded in Sydney by a workshop sponsored by Gaussian Inc. on ab initio, density functional, solid-state, and biological molecular computational methods, running  from Monday 28th June till Thursday 1st July.  
http://www.gaussian.com/g_workshops/ws_sydney.htm

MM2004 will finish in time for attendees to travel on to Cairns, Queensland, Australia, for the meeting of the Organic Chemistry Division of the RACI, which starts  4th July, 2004. 
http://www.cairnsconferences.com.au/ISMCORG2004

For more information contact: 
Dr Renate Griffith, School of Environmental and Life Sciences, University of Newcastle
Email:  Renate.Griffith(at)newcastle.edu.au


Dr. Renate Griffith
Lecturer in Medicinal Chemistry and Molecular Design
School of Environmental and Life Sciences
Life Sciences Building
(Mail to: Biology Building)
The University of Newcastle
Callaghan, NSW  2308, Australia
Email: Renate.Griffith(at)newcastle.edu.au
Phone: +61 2 4921 6990
Fax: +61 2 4921 6923



From chemistry-request@ccl.net Tue Apr 20 08:01:02 2004
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Date: Tue, 20 Apr 2004 07:01:07 -0600
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Subject: Re: CCL:converting an sdf database into a chemfinder database
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Hi all

I should note that the file that I am trying to open and convert, 
CANS03.sdf, is a file that I obtained from the NCI database (I don't 
have the url with me, it's at work), and it originally couldn't be 
opened with CACTVS,  until someone at the NCI "fixed" it.  CACTVS now 
reads it, but won't write it out, at least not the whole file.  The part 
that CACTVS does write out, can be read by Chemfinder, however.  CACTVS 
will currently write out the first 37 structures I believe and then not 
write anymore, but only if I write the first 15 and then append the next 
15 and so on.  SO it writes two sets of 15 structures and then 7 of the 
next 15 and then stops.  I'm doing this using the CACTVS browser, btw.

I hope this helps all of those that responded with questions/suggestions.

TIA,
Richard

Richard L. Wood wrote:

>Hi all
>
>I'm wondering if there is anyway to convert an sdf database into something
>that Chemfinder can read easily.
>
>Chemfinder is supposed to be able to import sdf databases, but the file I
>have must not be formatted correctly, because chemfinder can't read it.
>
>Thanks in advance,
>Richard
>
>
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-- 
Richard L. Wood, Ph. D.
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From chemistry-request@ccl.net Tue Apr 20 06:12:00 2004
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Date: Tue, 20 Apr 2004 14:12:48 +0300 (EEST)
From: Satyan Sharma <satyan..at..sun3.oulu.fi>
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Dear CCLers:

I am trying do study enzyme reaction. The system has active site residues
with substrate bound. I want to treat the species involved in
reaction at higher level and rest at PM3 level. For this I am
using ONIOM Calculation in G03. But I get following Error.
--------------------------------------------------
 dumping /fiocom/, unit = 2 NFiles =     1 SizExt =         0 WInBlk =
1024
                   defal = F LstWrd =       66560 FType=2 FMxFil=10000

 Number           0
 Base         40960
 End          66560
 End1         66560
 Wr Pntr      40960
 Rd Pntr      40960
 Length       25600


 dumping /fiocom/, unit = 3 NFiles =     1 SizExt =    524288 WInBlk =
512
                   defal = T LstWrd =       66048 FType=2 FMxFil=10000

 Number           0
 Base         40448
 End          66048
 End1         66048
 Wr Pntr      40448
 Rd Pntr      40448
 Length       25600
 Error termination in NtrErr:
 NtrErr Called from FileIO.

--------------------------------------------------------
Any clues anybody,

With best regards,
Satyan


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As far as the warning goes:
Warning -- assumption of classical behavior for rotation=20
may cause significant error=20
there is an option freq=3Dhindrot that recognizes internal rotations and =
treats them accordingly.  Not that I've had the need to use it in my own =
calculations.  The algorithm was I'm sure designed with organic =
molecules in mind, and perhaps it won't handle the ~180=B0 Si-O-H and =
Si-O-Si angles found in siloxanes well, but it's one option. =20
=20
If you have some independent way to calculate the internal rotational =
enthalpy and entropy, you can:
    take Gaussian's total enthalpy and entropy, and=20
    subtract the contribution of the suspect "vibrations"=20
        (That's what the lines beginning "Vibration 1", etc. are for), =
and=20
    add in the independently calculated internal rotational enthalpy and =
entropy.
=20
As for the vibrational temperatures: I wouldn't worry about these. AFAIK =
Gaussian correctly determines the thermodynamic contributions of each =
vibration, regardless of the vibration temperature, subject only to the =
assumption that the vibrational modes are harmonic oscillators and =
independent of other molecular motions.  I *hope* this is correct, =
anyway!
=20
--David Shobe, Ph.D., M.L.S.=20
S=FCd-Chemie, Inc.=20
phone (502) 634-7409=20
fax (502) 634-7724=20

Don't bother flaming me: I'm behind a firewall.=20

-----Original Message-----
From: Computational Chemistry List [mailto:chemistry-request=at=ccl.net]On =
Behalf Of Matthias Gottschalk
Sent: Tuesday, April 20, 2004 1:47 AM
To: Computational Chemistry List
Subject: CCL:Heat capacities with g03


Dear CCL,=20

as a naive geoscientist I try to calculate the heat capacities of =
specific single=20
molecules using g03 with something like that for Si2O7H6:=20

%chk=3Dsi2ooh6.chk=20
%mem=3D2048MB=20
%nproc=3D1=20
# opt=3D(restart, verytight) Int=3DUltraFine freq pbepbe/6-311++g(3d,2p) =

geom=3Dconnectivity temperature=3D298.15 pressure=3D0.9869233=20
>.=20
>.=20
>.=20
>.=20


Everything runs fine. At the end I do get the following warnings within =
my results:=20

-------------------=20
- Thermochemistry -=20
-------------------=20
Temperature 298.150 Kelvin. Pressure .98700 Atm.=20
Molecular mass: 173.96521 amu.=20
Principal axes and moments of inertia in atomic units:=20
1 2 3=20
EIGENVALUES -- 890.447432428.485422488.20921=20
X -.63183 .74944 .19780=20
Y -.05907 -.30101 .95179=20
Z .77285 .58968 .23446=20
This molecule is an asymmetric top.=20
Rotational symmetry number 1.=20
Warning -- assumption of classical behavior for rotation=20
may cause significant error=20
Rotational temperatures (Kelvin) .09727 .03567 .03481=20
Rotational constants (GHZ): 2.02678 .74316 .72532=20
Zero-point vibrational energy 237943.2 (Joules/Mol)=20
56.86979 (Kcal/Mol)=20
Warning -- explicit consideration of 20 degrees of freedom as=20
vibrations may cause significant error=20
Vibrational temperatures: 22.32 47.39 164.92 198.54 252.18=20
(Kelvin) 274.49 292.94 351.57 352.45 378.41=20
424.27 433.89 483.89 496.09 507.09=20
529.63 559.68 590.08 792.66 885.13=20
1071.96 1143.85 1168.05 1211.52 1224.45=20
1259.83 1274.99 1281.78 1340.88 1371.30=20
1389.84 1430.93 1501.79 5248.42 5427.26=20
5454.86 5462.94 5466.36 5467.29=20
Zero-point correction=3D .090628 (Hartree/Particle)=20
Thermal correction to Energy=3D .103807=20
Thermal correction to Enthalpy=3D .104751=20
Thermal correction to Gibbs Free Energy=3D .050334=20
E (Thermal) CV S=20
KCal/Mol Cal/Mol-Kelvin Cal/Mol-Kelvin=20
Total 65.140 46.134 114.529=20
Electronic .000 .000 .000=20
Translational .889 2.981 41.394=20
Rotational .889 2.981 30.066=20
Vibrational 63.362 40.173 43.069=20
Vibration 1 .593 1.986 7.139=20
Vibration 2 .594 1.983 5.644=20
Vibration 3 .608 1.937 3.189=20
Vibration 4 .614 1.915 2.832=20
Vibration 5 .627 1.873 2.378=20
Vibration 6 .634 1.853 2.220=20
Vibration 7 .639 1.835 2.100=20
Vibration 8 .660 1.772 1.771=20
Vibration 9 .660 1.771 1.767=20
Vibration 10 .670 1.741 1.642=20
Vibration 11 .689 1.683 1.446=20
Vibration 12 .694 1.671 1.408=20
Vibration 13 .717 1.603 1.230=20
Vibration 14 .723 1.586 1.190=20
Vibration 15 .729 1.570 1.155=20
Vibration 16 .741 1.538 1.088=20
Vibration 17 .757 1.494 1.004=20
Vibration 18 .774 1.448 .926=20
Vibration 19 .906 1.138 .542=20
Vibration 20 .975 1.000 .424=20

In this regard I do have the following questions:=20

1. Some rotations might be frozen at low temperatures, but the =
rotational temperatures are here=20
so low that I can ignore the first warning at ambient temperatures and =
above. Right?=20

2. Most if not all of the vibrational temperatures are significant. The =
calculated total heat capacity=20
is too high because not all vibrations are active at the chosen =
temperature. Right? What can I do=20
to get reliable heat capacities.=20

Are there other options in g03?=20
How to choose the right vibrational contributions to cv?=20
Can I reduce the explicit consideration of 20 degrees of freedom?=20
Where can I learn more how to deal with the problem practically?=20

Any help is welcome.=20

Matthias=20

--=20

PD Dr. Matthias Gottschalk=20
GeoForschungsZentrum=20
Projektbereich 4.1=20
Telegrafenberg=20
14473 Potsdam=20
Germany=20

tel/fax +49 (0) 331 288-1418/1402=20


------_=_NextPart_001_01C426F2.2997CF80
Content-Type: text/html;
	charset="iso-8859-1"
Content-Transfer-Encoding: quoted-printable

<!DOCTYPE HTML PUBLIC "-//W3C//DTD HTML 4.0 Transitional//EN">
<HTML><HEAD>
<META HTTP-EQUIV=3D"Content-Type" CONTENT=3D"text/html; =
charset=3Diso-8859-1">
<TITLE></TITLE>

<META content=3D"MSHTML 6.00.2800.1226" name=3DGENERATOR></HEAD>
<BODY>
<DIV><FONT face=3DArial color=3D#0000ff size=3D2><SPAN =
class=3D695354315-20042004>As far=20
as the warning goes:</SPAN></FONT></DIV>
<DIV><FONT><SPAN class=3D695354315-20042004>
<DIV><STRONG><FONT face=3DArial color=3D#0000ff size=3D2>Warning -- =
assumption of=20
classical behavior for rotation </FONT></STRONG></DIV>
<DIV><STRONG><FONT face=3DArial color=3D#0000ff size=3D2>may cause =
significant error=20
</FONT></STRONG></DIV>
<DIV><SPAN class=3D695354315-20042004><FONT face=3DArial color=3D#0000ff =
size=3D2>there=20
is an option freq=3Dhindrot that recognizes internal rotations and =
treats them=20
accordingly.&nbsp; Not that I've had the need to use it in my own=20
calculations.&nbsp; The algorithm was I'm sure designed with organic =
molecules=20
in mind, and perhaps it won't handle the ~180=B0 Si-O-H and Si-O-Si =
angles found=20
in siloxanes well, but it's one option.&nbsp; </FONT></SPAN></DIV>
<DIV><SPAN class=3D695354315-20042004><FONT face=3DArial color=3D#0000ff =

size=3D2></FONT></SPAN>&nbsp;</DIV>
<DIV><SPAN class=3D695354315-20042004><FONT face=3DArial color=3D#0000ff =
size=3D2>If you=20
have some independent way to calculate the internal rotational enthalpy =
and=20
entropy, you can:</FONT></SPAN></DIV>
<DIV><SPAN class=3D695354315-20042004><FONT face=3DArial color=3D#0000ff =

size=3D2>&nbsp;&nbsp;&nbsp; take Gaussian's total enthalpy and entropy, =
and=20
</FONT></SPAN></DIV>
<DIV><SPAN class=3D695354315-20042004><FONT face=3DArial color=3D#0000ff =

size=3D2>&nbsp;&nbsp;&nbsp; subtract the contribution of the suspect =
"vibrations"=20
</FONT></SPAN></DIV>
<DIV><SPAN class=3D695354315-20042004><FONT face=3DArial color=3D#0000ff =

size=3D2>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; (That's what the =
lines=20
beginning "Vibration 1", etc. are for), and </FONT></SPAN></DIV>
<DIV><SPAN class=3D695354315-20042004><FONT face=3DArial color=3D#0000ff =

size=3D2>&nbsp;&nbsp;&nbsp; add in the independently calculated internal =

rotational enthalpy and entropy.</FONT></SPAN></DIV>
<DIV><SPAN class=3D695354315-20042004><FONT face=3DArial color=3D#0000ff =

size=3D2></FONT></SPAN>&nbsp;</DIV>
<DIV><SPAN class=3D695354315-20042004><FONT face=3DArial color=3D#0000ff =
size=3D2>As for=20
the vibrational temperatures: </FONT></SPAN><SPAN =
class=3D695354315-20042004><FONT=20
face=3DArial color=3D#0000ff size=3D2>I wouldn't worry about these. =
AFAIK Gaussian=20
correctly determines the thermodynamic contributions of each vibration,=20
regardless of the vibration temperature, subject only to the assumption =
that the=20
vibrational modes are harmonic oscillators and independent of other =
molecular=20
motions.&nbsp; I *hope* this is correct, anyway!</FONT></SPAN></DIV>
<DIV><SPAN class=3D695354315-20042004><FONT face=3DArial color=3D#0000ff =

size=3D2></FONT></SPAN>&nbsp;</DIV>
<DIV><SPAN class=3D695354315-20042004>
<P><FONT face=3DArial size=3D2>--David Shobe, Ph.D., M.L.S.</FONT> =
<BR><FONT=20
face=3DArial size=3D2>S=FCd-Chemie, Inc.</FONT> <BR><FONT face=3DArial =
size=3D2>phone=20
(502) 634-7409</FONT> <BR><FONT face=3DArial size=3D2>fax (502) =
634-7724</FONT> </P>
<P><FONT face=3DArial size=3D2>Don't bother flaming me: I'm behind a=20
firewall.</FONT> </P></SPAN></DIV></SPAN></FONT></DIV>
<BLOCKQUOTE dir=3Dltr style=3D"MARGIN-RIGHT: 0px">
  <DIV class=3DOutlookMessageHeader dir=3Dltr align=3Dleft><FONT =
face=3DTahoma=20
  size=3D2>-----Original Message-----<BR><B>From:</B> Computational =
Chemistry List=20
  [mailto:chemistry-request=at=ccl.net]<B>On Behalf Of </B>Matthias=20
  Gottschalk<BR><B>Sent:</B> Tuesday, April 20, 2004 1:47 =
AM<BR><B>To:</B>=20
  Computational Chemistry List<BR><B>Subject:</B> CCL:Heat capacities =
with=20
  g03<BR><BR></FONT></DIV><!-- Converted from text/enriched format -->
  <DIV>Dear CCL, </DIV><BR>
  <DIV>as a naive geoscientist I try to calculate the heat capacities of =

  specific single </DIV>
  <DIV>molecules using g03 with something like that for Si2O7H6: =
</DIV><BR>
  <DIV><FONT face=3DCourier>%chk=3Dsi2ooh6.chk </DIV>
  <DIV>%mem=3D2048MB </DIV>
  <DIV>%nproc=3D1 </DIV>
  <DIV># opt=3D(restart, verytight) Int=3DUltraFine freq =
pbepbe/6-311++g(3d,2p)=20
  </DIV>
  <DIV>geom=3Dconnectivity temperature=3D298.15 pressure=3D0.9869233 =
</DIV>
  <DIV>&gt;. </DIV>
  <DIV>&gt;. </DIV>
  <DIV>&gt;. </DIV>
  <DIV>&gt;. </DIV>
  <DIV></FONT></DIV><BR><BR>
  <DIV>Everything runs fine. At the end I do get the following warnings =
within=20
  my results: </DIV><BR>
  <DIV><FONT face=3DCourier>------------------- </DIV>
  <DIV>- Thermochemistry - </DIV>
  <DIV>------------------- </DIV>
  <DIV>Temperature 298.150 Kelvin. Pressure .98700 Atm. </DIV>
  <DIV>Molecular mass: 173.96521 amu. </DIV>
  <DIV>Principal axes and moments of inertia in atomic units: </DIV>
  <DIV>1 2 3 </DIV>
  <DIV>EIGENVALUES -- 890.447432428.485422488.20921 </DIV>
  <DIV>X -.63183 .74944 .19780 </DIV>
  <DIV>Y -.05907 -.30101 .95179 </DIV>
  <DIV>Z .77285 .58968 .23446 </DIV>
  <DIV>This molecule is an asymmetric top. </DIV>
  <DIV>Rotational symmetry number 1. </DIV>
  <DIV>Warning -- assumption of classical behavior for rotation </DIV>
  <DIV>may cause significant error </DIV>
  <DIV>Rotational temperatures (Kelvin) .09727 .03567 .03481 </DIV>
  <DIV>Rotational constants (GHZ): 2.02678 .74316 .72532 </DIV>
  <DIV>Zero-point vibrational energy 237943.2 (Joules/Mol) </DIV>
  <DIV>56.86979 (Kcal/Mol) </DIV>
  <DIV>Warning -- explicit consideration of 20 degrees of freedom as =
</DIV>
  <DIV>vibrations may cause significant error </DIV>
  <DIV>Vibrational temperatures: 22.32 47.39 164.92 198.54 252.18 </DIV>
  <DIV>(Kelvin) 274.49 292.94 351.57 352.45 378.41 </DIV>
  <DIV>424.27 433.89 483.89 496.09 507.09 </DIV>
  <DIV>529.63 559.68 590.08 792.66 885.13 </DIV>
  <DIV>1071.96 1143.85 1168.05 1211.52 1224.45 </DIV>
  <DIV>1259.83 1274.99 1281.78 1340.88 1371.30 </DIV>
  <DIV>1389.84 1430.93 1501.79 5248.42 5427.26 </DIV>
  <DIV>5454.86 5462.94 5466.36 5467.29 </DIV>
  <DIV></DIV>
  <DIV>Zero-point correction=3D .090628 (Hartree/Particle) </DIV>
  <DIV>Thermal correction to Energy=3D .103807 </DIV>
  <DIV>Thermal correction to Enthalpy=3D .104751 </DIV>
  <DIV>Thermal correction to Gibbs Free Energy=3D .050334 </DIV>
  <DIV>E (Thermal) CV S </DIV>
  <DIV>KCal/Mol Cal/Mol-Kelvin Cal/Mol-Kelvin </DIV>
  <DIV>Total 65.140 46.134 114.529 </DIV>
  <DIV>Electronic .000 .000 .000 </DIV>
  <DIV>Translational .889 2.981 41.394 </DIV>
  <DIV>Rotational .889 2.981 30.066 </DIV>
  <DIV>Vibrational 63.362 40.173 43.069 </DIV>
  <DIV>Vibration 1 .593 1.986 7.139 </DIV>
  <DIV>Vibration 2 .594 1.983 5.644 </DIV>
  <DIV>Vibration 3 .608 1.937 3.189 </DIV>
  <DIV>Vibration 4 .614 1.915 2.832 </DIV>
  <DIV>Vibration 5 .627 1.873 2.378 </DIV>
  <DIV>Vibration 6 .634 1.853 2.220 </DIV>
  <DIV>Vibration 7 .639 1.835 2.100 </DIV>
  <DIV>Vibration 8 .660 1.772 1.771 </DIV>
  <DIV>Vibration 9 .660 1.771 1.767 </DIV>
  <DIV>Vibration 10 .670 1.741 1.642 </DIV>
  <DIV>Vibration 11 .689 1.683 1.446 </DIV>
  <DIV>Vibration 12 .694 1.671 1.408 </DIV>
  <DIV>Vibration 13 .717 1.603 1.230 </DIV>
  <DIV>Vibration 14 .723 1.586 1.190 </DIV>
  <DIV>Vibration 15 .729 1.570 1.155 </DIV>
  <DIV>Vibration 16 .741 1.538 1.088 </DIV>
  <DIV>Vibration 17 .757 1.494 1.004 </DIV>
  <DIV>Vibration 18 .774 1.448 .926 </DIV>
  <DIV>Vibration 19 .906 1.138 .542 </DIV>
  <DIV>Vibration 20 .975 1.000 .424</FONT> </DIV><BR>
  <DIV>In this regard I do have the following questions: </DIV><BR>
  <DIV>1. Some rotations might be frozen at low temperatures, but the =
rotational=20
  temperatures are here </DIV>
  <DIV>so low that I can ignore the first warning at ambient =
temperatures and=20
  above. Right? </DIV><BR>
  <DIV>2. Most if not all of the vibrational temperatures are =
significant. The=20
  calculated total heat capacity </DIV>
  <DIV>is too high because not all vibrations are active at the chosen=20
  temperature. Right? What can I do </DIV>
  <DIV>to get reliable heat capacities. </DIV><BR>
  <DIV>Are there other options in g03? </DIV>
  <DIV>How to choose the right vibrational contributions to cv? </DIV>
  <DIV>Can I reduce the explicit consideration of 20 degrees of freedom? =
</DIV>
  <DIV>Where can I learn more how to deal with the problem practically?=20
  </DIV><BR>
  <DIV>Any help is welcome. </DIV><BR>
  <DIV>Matthias </DIV><BR>
  <DIV>-- </DIV><BR>
  <DIV>PD Dr. Matthias Gottschalk </DIV>
  <DIV>GeoForschungsZentrum </DIV>
  <DIV>Projektbereich 4.1 </DIV>
  <DIV>Telegrafenberg </DIV>
  <DIV>14473 Potsdam </DIV>
  <DIV>Germany </DIV><BR>
  <DIV>tel/fax +49 (0) 331 288-1418/1402 =
</DIV></BLOCKQUOTE></BODY></HTML>

------_=_NextPart_001_01C426F2.2997CF80--


From chemistry-request@ccl.net Tue Apr 20 07:36:48 2004
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Date: Tue, 20 Apr 2004 13:37:39 +0100
From: Patricia Lozano-Casal <P.Lozano-Casal|at|ed.ac.uk>
To: chemistry|at|ccl.net
Subject: QUESTION ABOUT COULOMBIC POTENTIAL
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SUBJECT: QUESTION ABOUT COULOMBIC POTENTIAL

Dear all,

I am trying to write a program to calculate the electrostatic contribution of
the lattice energy for molecular crystals. I have run plane-wave DFT
calculations (using the CASTEP package) to calculate the total lattice energy
and using Mulliken charges I hoped to estimate the electrostatic contribution
by coding a simple Coulombic potential. But, I get really weird results!! I am
overestimating my lattice energy by many orders of magnitude.

I know that Mulliken charges are not the ideal point charge to use for this but
I had not expected my numbers to be that wrong. Could anybody help or if not,
could anybody recommend and existing program to use instead (preferably free)?

Many thanks,

Patricia Lozano-Casal (p.lozano-casal|at|ed.ac.uk)


--
Room 85, School of Chemistry,
Joseph Black Building,
Kings Buildings,
West Mains Road,
Edinburgh, EH9 3JJ
United Kingdom
Tel: +441316504804


From chemistry-request@ccl.net Tue Apr 20 15:21:16 2004
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Date: Tue, 20 Apr 2004 16:14:15 -0400
From: "Igor Filippov [Contr]" <igorf..at..helix.nih.gov>
To: Richard Wood <rlw28..at..cornell.edu>
cc: "chemistry..at..ccl.net" <chemistry..at..ccl.net>
Subject: Re: CCL:converting an sdf database into a chemfinder database
In-Reply-To: <40851F13.7010108..at..cornell.edu>
Message-ID: <Pine.SGI.4.58.0404201607310.14835297..at..helix.nih.gov>
References: <4316.129.123.250.158.1082407282.squirrel..at..webmail.cornell.edu>
 <40851F13.7010108..at..cornell.edu>
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	servernd.ccl.net

Richard,

Is it possible that you're talking about NCI database processed by our
group (CADD @ LMC @ NCI-Frederick) ? The website is
http://cactus.nci.nih.gov where you can download public portion of NCI
database (processed). As the whole processing was done in CACTVS
it is hard to imagine that one is not able to read/write the structures
anymore. If you downloaded NCI database somewhere else then it is, of
course, impossible to tell what did you get and what the problem with it
might be.

Regards,

Igor Filippov
Contractor - SAIC-Frederick
Computer Aided Drug Design group
Laboratory of Medicinal Chemistry
National Cancer Institute


On Tue, 20 Apr 2004, Richard Wood wrote:

> Hi all
>
> I should note that the file that I am trying to open and convert,
> CANS03.sdf, is a file that I obtained from the NCI database (I don't
> have the url with me, it's at work), and it originally couldn't be
> opened with CACTVS,  until someone at the NCI "fixed" it.  CACTVS now
> reads it, but won't write it out, at least not the whole file.  The part
> that CACTVS does write out, can be read by Chemfinder, however.  CACTVS
> will currently write out the first 37 structures I believe and then not
> write anymore, but only if I write the first 15 and then append the next
> 15 and so on.  SO it writes two sets of 15 structures and then 7 of the
> next 15 and then stops.  I'm doing this using the CACTVS browser, btw.
>
> I hope this helps all of those that responded with questions/suggestions.
>
> TIA,
> Richard
>
> Richard L. Wood wrote:
>
> >Hi all
> >
> >I'm wondering if there is anyway to convert an sdf database into something
> >that Chemfinder can read easily.
> >
> >Chemfinder is supposed to be able to import sdf databases, but the file I
> >have must not be formatted correctly, because chemfinder can't read it.
> >
> >Thanks in advance,
> >Richard
> >
> >
> >
> >
> >
> >
> >
>
> --
> Richard L. Wood, Ph. D.
> Computational Chemist
> SynVax, Inc.
> N. Logan, UT 84341
>
>
>
>
>
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Dear all,

I have some difficult to view two molecular structure in ONE window
with licorice model. I set the  "Cyl.rad" to 0.1, one molecule will
change to the correct view, however, the other also display in licorice
model but with "Cyl.rad" at 0.3. In one word, the change of  "Cyl.rad"
and/or  "Sph.rad" just change one molecule.

Can anyone here give me some help? Any suggestions will be really
appreciated.

Best wishes,

Jinsong  

=====
(Mr.) Jinsong Zhao
Ph.D. Candidate
School of the Environment
Nanjing University
No.22 Hankou Road, Najing 210093
P.R. China
E-mail: zh_jinsong<<at>>yahoo.com.cn

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Subject: CCL: Basis sets for transitional metals
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Hi!

I am using G98 now, and I am trying to get the electronic structure of CO molecule. By using all the methods implemented in G98, I found that all the result give a similar result - O gets charges from C and has a negative charge. This is quite different from the description I found in books, C should get charge from O and has a negative charge. This makes me confused. 

What should I do to make a correct calculation of CO? 

I hope that you would not mind giving me some detailed instruction on the calculation.

Sincerely yours

Xin, Liu



