vertical detachment energy (VDE) and adiabatic detachment energy (ADE), defined respectively as ∆E , (r, ω) ] , , ∆E , , , (, , , (5a) 5b Where, A is the electron affinity of the ion A q- in gas phase. In order to have an explicit expression for VDE and ADE of the system containing finite number of solvent particles, what is needed is a relation between the pair distribution function g i (r, ω) of the infinite system and its finite system counterpart g i (r, ω, n). Such a relation may be derived by following the approach of Salacuse et.al. by means of Taylor-series expansion in powers of 1/n. 84 Here, the derivation is extended from the nonpolar system to the case of ionpolar system. Semi-grand canonical ensemble is considered where only the number of solvent molecules is allowed to fluctuate but the single negative ion is kept fixed in each member of the ensemble. 85 In this semi grand canonical ensemble, the two-particle distribution function may be expressed as , , P P , ,, 6 Where, P is the probability that in equilibrium the system contains n solvent molecules and a single ion and P , ,, is the pair distribution function for a system containing a single anion and n solvent molecules. Here, , and represent the position vector of the ion, and the position vector and orientation of the solvent molecule, respectively. Now expanding , ,, in the number of particles around the average number of particles, one get 126
P 7 P , , P , ,, 1 ∂ 2 ∂ P , ,, 1 6 ∂ ∂ P , ,, ………………… 8 where, the averages of fluctuation of the number of solvent particles are defined as P 0 P for m 1 9 9 In the homogeneous limit, one can write P , , g i(r,ω); P , ,, g i(r,ω) 10 where, ρ and ρ represent the ion and solvent density, respectively, and r r d r s . Approximating the average density (=/V) to be equal to the solvent density, Eq.(6 ) can be reduced to g , g , , 1 ρ ∂ 2 n ∂ρ ρg , , 1 6 ρ ∂ ∂ρ ρg , , . 11 The effect of a single ion on g , enters through the fluctuation of the number of solvent particles and pair distribution g , , for the finite system. For simplicity, the effect of a single ion on the fluctuation of the number of solvent particles is neglected. This approximation is a reasonably good one if the system contains an appreciable 127
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MICROSOLVATION OF CHARGED AND NEUTR
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STATEMENT BY AUTHOR This dissertati
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Dedicated to my Daughter, Wife and
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CONTENTS Page No. SYNOPSIS LIST OF
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CHAPTER 4 Solubility of Halogen Gas
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7.3.4. IR and Raman Spectra 117-121
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S Macroscopic Microscopic Dual leve
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molecular level interaction during
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Chapter 3: This chapter describes I
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In this system the conformers of a
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LIST OF FIGURES Page No. Fig. 1.1 2
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Fig. 2.6 54 (I) Plot of calculated
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(IIIA) Cl 2 .3H 2 O; (IIIB) Br 2 .3
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Fig. 6.3 104-105 Calculated scaled
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LIST OF TABLES Page No. Table. 2.1
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CHAPTER 1 Introduction 1.1. Microso
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1.2. Motivation 1.2.1. Macrosolvati
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ulk water and pure neutral water cl
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insight about the electronic struct
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Newton -Raphson (NR) method expand
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potential energy surface for these
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terms, the energy can be written in
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Boyd proposed the use of Gaussian t
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eported experimental findings. Theo
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hydrated halide series, X¯.nH 2 O,
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anions (Cl •− 2 , Br •− 2 &
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geometrical parameters close to MP2
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symmetrical DHB, SHB or WHB arrange
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of I-I axis and having the least I-
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Br •− 2 .nH 2 O hydrated cluste
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VI-F VI-G VII-A VII-B VII-C VII-D V
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To see the effect of hydration on t
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Five minimum energy structures disp
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arrangements. In total, it has one
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NO 3 − .nH2 O (n ≥ 6), a few eq
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V-E V-F V-G V-H V-I VI-A VI-B VI-C
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VII-D VII-E VII-F VII-G VII-H VII-I
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VIII-K VIII-L Fig.2.2. Fully optimi
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clusters. Hydrated cluster having c
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However, these calculations do not
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Table 2.1. Weighted average energy
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Where, E[I •− 2 .nH 2 O] is the
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The variation of the weighted avera
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CHAPTER 3 IR Spectra of Water Embed
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ecome more meaningful. At present,
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I-A II-A II-B III-A III-B III-C III
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Cluster experiments are carried out
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3350-3500 cm -1 (scaling factor ~0.
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these systems, X. nH 2 O (X= Br 2
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CHAPTER 4 Solubility of Halogen Gas
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including polarized and diffuse fun
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and I 2 systems. The most stable st
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- Page 155: possible breakdown of these laws ma
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- Page 161 and 162: known. However, for most of the com
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- Page 167 and 168: References 1. Ohtaki, H.; Radani, T
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- Page 171 and 172: 61. (a) Ehrler, O. T.; Neumark, D.
- Page 173 and 174: LIST OF PUBLICATIONS *1. “σ/σ
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