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curricula and courses, and technology-mediated teaching process.
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Desired Qualification:
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Name
Mr. Sankarampadi ARAVAMUDHAN
Address
LOWER NEW COLONY HOUSE No.220, LAITUMKHRAH WARD 2 SHILLONG, 793003 EK HILLS District MEGHALAYA
Shillong, Meghalaya - 793003
India
The necessity for trying to calculate the intra
molecular proton shielding tensor has been enumerated in the
introduction by this author(1). A feasibility study has been reported
(2) at the ISMAR-CA’98. Those results indicated that it seemed possible
to obtain results which can be compared with experimental values for the
case of the peripheral proton in the benzene ring, However, at that
time, no comparison with QM calculations were made though the comparison
with experimental results on aromatic protons was reported. Moreover,
the contribution of the C-H bond susceptibility to the proton bonded to
that carbon could not be used for reasons of reasonable validity of the
point dipole approximation. The effort to apply the magnetic dipole
model for the calculation of demagnetization factors (3) proved that
depending on the parameters used for fragmenting a susceptibility
tensor, the point dipole approximation could become valid better even at
much closer proximity to the proton location (4). Thus, the possibility
of using this model for details could be envisaged typically for the
case of benzene molecule (5). In the present contribution, the results
obtained earlier (2) could be improved, and a comparison of the results
of the use magnetic dipole model could be compared also with the QM
calculations of Shielding Tensors. In addition as envisaged in (4) and
(5) the C-H bond contribution to the shielding of the attached proton
could also be added for inclusion instead of trying to use a value
derived from QM calculations on ethylene proton. These results would be
discussed in view of the necessary further improvements. Such efforts
might eventually provide an explanation to the remark made earlier (6)
about the atom and bond susceptibility tensors obtained from the very
same set of Molecular Susceptibility values.
(1) https://saravamudhan.tripod.com/index.html
(2) https://saravamudhan.tripod.com/id2.html
(3) https://saravamudhan.tripod.com/id4.html
https://saravamudhan.tripod.com/id5.html
http://www.ugc-inno-nehu.com/isc2009nehu.html
(4) https://saravamudhan.tripod.com/id6.html
http://nehuacin.tripod.com/pre_euromar_compilation/id5.html
http://nehuacin.tripod.com/id6.html
(5) https://saravamudhan.tripod.com/id3.html
(6) On page-682,at the end of first column by
W.H.Flygare,Chemical Reviews, Vol.74, page-653(1974).
Research programme
INDUCED FIELD DISTRIBUTIONN CALCULATIONS IN MAGNETIZED
SPECIMEN A more convnient, less laborious and less time consuming
method could be evoleved and this has also proved that this came about
because of the concomitant improvement in the applicability of point
dipole approximation. Demagnetization ffactors available now for more
than 30 years as calculated by integartion procedures could be
reproduced by a pockaet calculator verion of the calculation, and this
made possible calculating shielding tensors. Intra molecular
intermolecular contributions have to be calculated and the details have
to be eventuallyn leading to information for improving quantum chemical
formailsms for the calculation of these second order magnetic
properties like the shielding tensor and susceptibility tensor. The
induced field calculation method holds promise in several ways for
biophysical contexts and macro molecular PMR. Some of these have been
borne out by the several contributions to the various symposia and
conferences and the work is in progress.
Plan of teaching
Also the improvement in the validitty of point dipole
approximation requires specialle emphasis now in the graduate and school
level teaching of magnetic properties, electrostatic and magnetism
aspects related to interaction of radiation with matter for the conrtext
of spectroscopic studies. These can be found imentionee in the
descriptions at this authors url saravamudhan dot tripod dot com slash
biodata dot html
I hereby declare that the information given by me in the proforma
is correct and no relevant information has been concealed.