Spectroscopic Properties of Inorganic and Organometallic Compounds
Adams, D M
Sold by PBShop.store US, Wood Dale, IL, U.S.A.
AbeBooks Seller since 7 April 2005
New - Hardcover
Condition: New
Ships within U.S.A.
Quantity: 15 available
Add to basketSold by PBShop.store US, Wood Dale, IL, U.S.A.
AbeBooks Seller since 7 April 2005
Condition: New
Quantity: 15 available
Add to basketNew Book. Shipped from UK. Established seller since 2000.
Seller Inventory # CX-9780851861135
Reflecting the growing volume of published work in this field, researchers will find this book an invaluable source of information on current methods and applications.
Chapter 1 Nuclear Magnetic Resonance Spectroscopy By B. E. Mann,
Chapter 2 Nuclear Quadrupole Resonance Spectroscopy By K. B. Dillon,
Chapter 3 Microwave Spectroscopy By A.P. Cox,
Chapter 4 Vibrational Spectra of Small Symmetric Species; Single-crystal and Other Solid-state Spectroscopy By D. M. Adams,
Chapter 5 Characteristic Vibrations of Main-group Element Compounds By S. Cradock,
Chapter 6 Vibrational Spectra of Transition-element Compounds By J. S. Ogden,
Chapter 7 Vibrational Spectra of Some Co-ordinated Ligands By G. Davidson,
Chapter 8 Mössbauer Spectroscopy By J. D. Donaldson and M. J. Tricker,
Nuclear Magnetic Resonance Spectroscopy
BY B. E. MANN
1 Introduction
Following the criteria established in earlier volumes, only books and reviews directly relevant to this chapter are included, and the reader who requires a complete list is referred to the Specialist Periodical Report 'Nuclear Magnetic Resonance',' where a complete list of books and reviews is given. Reviews that are of direct relevance to a section of this report are included in the beginning of that section rather than here. Papers where only 1H n.m.r. spectroscopy is used are only included when the 1H n.m.r. spectra make a non-routine contribution, but complete coverage of relevant papers is still attempted where nuclei other than the proton are involved.
Several relevant books have been published during 1979. The book 'Phosphorus-31 and Carbon-13 N.M.R of Transition Metal Phosphine Complexes' provides a welcome selective source of data. In addition, 'Nitrogen-15 Nuclear Magnetic Resonance Spectroscopy' and 'N.M.R. in Inorganic Fluorides: Structure and Chemical Bonding' have also appeared. 'N.M.R. Spectra; Its Application to the Organometallic Compounds' has also been reviewed.
A number of papers have been published that are too broadly based to fit into a later section and are included here. N.m.r. spectroscopy has been applied to condensed systems with asymmetric centres. The relaxation, including effects of chemical exchange, of spin-5/2 and -7/2 nuclei has been examined. An analytical perturbation extension of the Pople-Santry theory of the Fermi contact term in reduced spin-coupling constants, 1K(M-L), has been developed for the substituted compounds MLnL'm, where the ligands L have a valence ns orbital. It was found that changes in 1K(M–L) under substitution should typically follow changes in s-contribution to the E–L bond overlap population. Subsequently this treatment was applied to phosphorus(III) compounds and good agreement with experiment was found.
1H relaxation times have been measured for H2 in liquid neon, argon, and krypton. The results of coupled Hartree–Fock computations for the n.m.r. shielding constant have been reported for LiH, HF, and PH3. 13C n.m.r. spectra have been reported for diamagnetic cyano complexes in D2O. Except for (Fe(CN)6]4- the 13C resonance in all the cyano complexes examined is at lower frequency than uncomplexed |CN|- and the range of chemical shift spans 92.5 p.p.m. Chemical shift differences were discussed in terms of changes in σ and π-bonding of |CN|- to the metal ion. 1JMC was observed for [59Co(CN)6]3- (126 Hz), [103Rh(CN)6]3- (33.6 Hz), [195Pt(CN)6]2- (808 Hz), and [195Pt(CN)4]2- (1034 Hz). T1, values were also reported for selected compounds and interpreted as being consistent with scalar coupling to 14N.
The equivalent dipole model of the benzene ring current has been applied to both inter- and intra molecular geometries to give detailed conformational information in n.m.r. studies of metalloporphyrins. 13C chemical shifts have been measured for [SCN]-, [NCO]-, and [SeCN]- in a variety of transition-metal complexes. The effects of cation and solvent changes upon the chemical shifts of the ionic pseudo-halides were determined. Changes in hybridization are more important than electron excitation energy changes and substitution changes in determining chemical shifts for both ionic and complexed species. The ordering of the ions in terms of increasing shielding is [SCN]-< [OCN]-< [SeCN|-. The ordering of [SCN]- and [SeCN]- in terms of increasing shielding as a function of bonding mode is M-NCS < [NCS]-< M-SCN. Unsupervised 13C n.m.r. pattern recognition has permitted the qualitative classification of NN-dialkyldithio-carbamate complexes into five classes: free ligands, complexes of main-group elements, and complexes of transition metals, with the latter two groups being divided by a free oxidation number of 0.5 or greater than 0.5. Within the transition-metal complexes metals with electron configuration d6 or d8 and d0 or d]10 can be further distinguished. The class of main-group elements is subdivided into organic dithiocarbamates and a subclass of main-group element complexes. Changes of 31P chemical shifts during co-ordination of phosphoryl compounds have been discussed.
The 17O n.m.r. shifts of some metal carbonyls are 400 to 300 p.p.m. to high frequency from 17OH2. The δ(17O) trends are generally opposite to those for the carbon monoxide 13C chemical shifts and this is explained by metal π-back-bonding in carbon monoxide π*-orbitals. A metal-triad effect is observed for 17O chemical shifts. There is a low-frequency shift of δ(17O) on descending a given group in the Periodic Table. Over 100 17O n.m.r. chemical shifts have been reported for 27 diamagnetic polyoxoanions of the early transition metals. Efficient procedures for obtaining 17O-enriched compounds were described and the factors controlling sensitivity and spectral resolution are examined and discussed in detail. Comparison of chemical-shift values with structural data shows that chemical shifts are determined largely by metal-oxygen bond strengths. As complexes of 3-mesitylacetylacetone show very small chemical-shift differences between their o- and p-methyl signals, 0.11 to 0.23 p.p.m., it was concluded that they do not possess magnetic anisotropies in the chelate rings comparable with those of benzene. The nature of the ligand L and the position of the resonance lines of non-equivalent fluorine atoms in the 19F n.m.r. spectra of pseudo-octahedral fluoro complexes have been reviewed.
2 Stereochemistry
This section is subdivided into ten parts containing n.m.r. information about lithium, magnesium, and transition-metal complexes, presented by Groups, according to the Periodic Table. Within each Group classification is by ligand type.
Complexes of Groups IA and IIA. — 1H n.m.r. spectroscopy has been used to determine the concentration of n-butyl-lithium. In the anionic polymerization of 1-phenyl-1,3-butadiene the propagating species was shown by 1H and 13C n.m.r. spectra to be the 4,1-anion. The 13C n.m.r. spectra of (1) and related compounds have been reported, while for LiCBr31J(13C, 7Li) is 43 Hz. Low-temperature 13C n.m.r. spectra of some lithiated chiral oxazolines show the presence of two isomers. 1H n.m.r. spectra have been used to show chair conformations for complexes of sparteine and α-isosparteine with Li+.
From 1H n.m.r. spectroscopy it has been concluded that tetracyanoquinodi-methane interacts with chlorophyll by a donor–acceptor mechanism with the nitrogen atom of the second ring of the pigment molecule acting as p-donor.
1H and 13C n.m.r. spectra of the alkaline-earth and diamagnetic rare-earth metal complexes of diethylenetriaminepenta-acetate have been discussed in terms of the labilities of the metal–oxygen and metal–nitrogen bonds. The various resonance-splitting patterns observed in the alkaline-earth spectra were correlated with the patterns predicted for possible hexadentate structures involving all three nitrogen donors and averaging for the other three co-ordination sites by four of the ligand carboxylate groups. A heptadentate structure was proposed for the complexes with the lanthanides.
Complexes of Y, La, Lu, U, Ti, Zr, Zr, Hf, and Th. — An examination of the 89Y n.m.r. chemical shifts for several inorganic salts in aqueous solution in the pH range 0 — 6 showed little or no change, indicating that Y T2 values are not pH-dependent. The resonances are always very sharp (half-widths ca. 0.3 Hz) and probably limited only by magnet homogeneity. Certainly there is no reduction in signal-to-noise ratio in this pH range. The observation of 2J(89Y, 31P) in [Y{S2P(OEt)2|4]- has been interpreted as evidence for covalent bonding. The magnitude of 2KYP is of the same order as 2KRhP and 2KPtP in [Rh(S2P(OEt2)2}3] and [Pt{S2P(OEt)2}2], indicating similarity in the covalent contribution to their bonds.
The g-factor of the first excited state in 138La has been measured by the time-differential perturbed angular distribution method. A 180 MHz 1H n.m.r. study of the lanthanide (2.2.1)cryptates in CD3CN and D2O solution has been performed. The compound [La(2.2.1)]3+ is the first example of an f-orbital co-ordination complex to exhibit a strong ligand conformation preference. Moreover, a 1H n.m.r. examination of the various paramagnetic [Ln(2.2.1)]3+ ions has demonstrated that these species are quite similar in structure across the entire series. N.m.r. data have also been reported for [{YCp2Me}2] (13C), [M(NNN'N-tetramethyl-α-carboxamidoanisamide)3] (M = Y. La; 13C), [Lu(CH2SiMe3)4]- (13C), [{(Me3Si)2N}2M(µ-CH2)(µ-NsiMe3)SiMe2 (M = Th, U; 13C), [UO2(OC{CF3)3}2 (THF)2] (19F), and [U(OMe)F5] (13C, 19F).
For [Th{(CH2)nC5H4}2X2] the varying degrees of splitting between the high-field portions of an A2B2 resonance pattern due to the cyclopentadienyl hydrogen atoms have been interpreted in terms of bonding geometries. The 13C n.m.r. spectra were also reported. According to 19F n.m.r. spectra TiF4 reacts with phosphoryl-containing ligands to give cis-[TiF4L2. With decreasing donor capacity of L the 19F n.m.r. signals are shifted to high frequency. Significant shifts were observed for the 19F atom trans to Bu3PO and Bu3PO4. 13C shielding parameters have been determined for the N-phosphorylated aniline and O-phosphorylated phenol derivatives PhYP(O)Z2 (Y = NH, O) and for their complexes with TiCl4. Inductive and resonance substituent parameters were calculated. N.m.r. data have also been reported for [MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII].
On the basis of 31P n.m.r. spectroscopy [MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII] dissociates in solution to [MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII]. 13C n.m.r. spectroscopy has been used as a probe of electron density on nitrogen in Group IVA and Group VA t-butylimido derivatives. 13C n.m.r. spectroscopy has been used to show that commercial [HfCp2Cl2] contains ca. 10% zirconium. N.m.r. data have also been reported for [MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII].
Complexes of V, Nb, and Ta. — The 51V n.m.r. spectrum of [(Me3SO)3V=NBut] shows a 14N coupling of 95 Hz. The compositions and structures of vanadium oxyfluorochloro complexes formed by the reaction of VOCl3 with HF or KF in MeCN solutions have been studied by 51V n.m.r. spectra. Some phosphoro-vanadium complexes have been studied in solution by n.m.r. Peroxovanadium(v) species of notional formulae [VO(O2)]+, [HVO2(O2)2]2-, [H2VO2(O2)2]-, [VO(O2)3]3-, [HVO(O2)3]2-. [V(O2)4]3-. [H{VO(O2)2}2O]3-, and [VO(NH3)-(O2)]- have been identified in aqueous solution by 51V n.m.r. spectroscopy and the pKa determined. 51V n.m.r. spectra of vanadyl esters dissolved in nematic liquid crystals show a seven-line system, which is due to a first-order quadrupole interaction. Quadrupole splittings vary from 3.6 to 1.93 kHz. N.m.r. data have also been reported for [MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII].
A high-resolution n.m.r. study of [{Nb(tetraphenylporphyrin}O2O3} and |Nb(tetraphenylporphyrin)(O)(O2CMe)xnMeCO2H] has been claimed to show that the anisochrony of the methylenic protons is induced by the out-of-plane position of the metal atom. However, it would appear that the true cause is the presence of different ligands on the two sides of the plane. The 93Nb n.m.r. spectra of NbX5, (X = Cl, Br) in MeCN solutions in the presence of HF indicate the formation of [NbFnX6-n] (n = 0-6). NbX5, in MeCN in the presence of KNCS gave [Nb(NCS)nX6-n] and [Nb(NCS)7]2-; similar mixed-ligand anions were observed in the NbX5-KNCO-MeCN systems. 93Nb n.m.r. spectra have shown that the reaction of [NbOCl3] and [NbOBr3] with [NCS]-, [NCO]-, and F- in MeCN yields complexes of the type [NbOXnY4-n(NCMe)]-. 19F n.m.r. chemical-shift data for [NbF3{(RC6H4)3PO)] and [TaF5 {(RC6H4)3PO}] indicate that with increasing basicity of the ligand the 19F n.m.r. signal is shifted to low frequency. T1, and T2, of the 93Nb nucleus were measured as a function of temperature in [NbClnBr6-n]-. The rate of relaxation in all the complexes except fac]NbCl3Br3]- was determined by the quadrupole interaction. In fac-[NbCl3Br3]- the mechanism of relaxation is caused by exchange processes, related to intramolecular cis-trans isomerization. According to the 19F n.m.r. spectra, acetoxime (HL) reacts with TaF5 in MeCN to give [TaLF5]- and cis-[TaF4L2]-. With ethylmethyl ketoxime (HQ) |TaF5(syn-Q)]-, [TaF5(anti-Q), [TaF4(syn-Q)2]-, and [TaF4(anti-Q2)]- are formed. TaL5 reacts with Et3NHF to give trans- and cis-[TaF3L3]-. [TaF5ONCHPh2]- and [TaF4- (ONCHPh)2]- were also formed. The 19F n.m.r. spectra of TaF5 and R3PS show the formation of [TaF5(SPR3)], and the donor capacity of SPR3 was established. The 19F n.m.r. spectrum of equimolar solutions of TaF5 and Ph3AsS in CH2Cl2 indicates the formation of [TaF5(Ph3AsS)], in which the Ph3AsS is co-ordinated through the sulphur atom. Equimolar solutions of TaF5 and R3AsO (R = Ph, Bu) form [TaF5(R3AsO)] and cis- and trans-[TaF4(R3AsO)]+. According to the n.m.r. data, the donor properties of R3AsO are greater than those of Ph3AsS. On the basis of the chemical shift of analogous complexes with [TaF5(OPR3)] and [TaF5(SPR3)], the donor capability for these ligands decreases in the series R3AsO > R3PO > R3AsS ~ R3PS. N.m.r. data have also been reported for [MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII].
Excerpted from Spectroscopic Properties of Inorganic and Organometallic Compounds Volume 13 by D. M. Adams, E. A. V. Ebsworth. Copyright © 1980 The Royal Society of Chemistry. Excerpted by permission of The Royal Society of Chemistry.
All rights reserved. No part of this excerpt may be reproduced or reprinted without permission in writing from the publisher.
Excerpts are provided by Dial-A-Book Inc. solely for the personal use of visitors to this web site.
"About this title" may belong to another edition of this title.
Returns Policy
We ask all customers to contact us for authorisation should they wish to return their order. Orders returned without authorisation may not be credited.
If you wish to return, please contact us within 14 days of receiving your order to obtain authorisation.
Returns requested beyond this time will not be authorised.
Our team will provide full instructions on how to return your order and once received our returns department will process your refund.
Please note the cost to return any...
If you are a consumer you can cancel the contract in accordance with the following. Consumer means any natural person who is acting for purposes which are outside his trade, business, craft or profession.
INFORMATION REGARDING THE RIGHT OF CANCELLATION
Statutory Right to cancel
You have the right to cancel this contract within 14 days without giving any reason.
The cancellation period will expire after 14 days from the day on which you acquire, or a third party other than the carrier and indicated by you acquires, physical possession of the the last good or the last lot or piece.
To exercise the right to cancel, you must inform us, Paperbackshop-US, 901 Penhorn Avenue, Unit 6, 07094, Secaucus, New Jersey, U.S.A., 44 1285 712917, of your decision to cancel this contract by a clear statement (e.g. a letter sent by post, fax or e-mail). You may use the attached model cancellation form, but it is not obligatory. You can also electronically fill in and submit a clear statement on our website, under "My Purchases" in "My Account". If you use this option, we will communicate to you an acknowledgement of receipt of such a cancellation on a durable medium (e.g. by e-mail) without delay.
To meet the cancellation deadline, it is sufficient for you to send your communication concerning your exercise of the right to cancel before the cancellation period has expired.
Effects of cancellation
If you cancel this contract, we will reimburse to you all payments received from you, including the costs of delivery (except for the supplementary costs arising if you chose a type of delivery other than the least expensive type of standard delivery offered by us).
We may make a deduction from the reimbursement for loss in value of any goods supplied, if the loss is the result of unnecessary handling by you.
We will make the reimbursement without undue delay, and not later than 14 days after the day on which we are informed about your decision to cancel with contract.
We will make the reimbursement using the same means of payment as you used for the initial transaction, unless you have expressly agreed otherwise; in any event, you will not incur any fees as a result of such reimbursement.
We may withhold reimbursement until we have received the goods back or you have supplied evidence of having sent back the goods, whichever is the earliest.
You shall send back the goods or hand them over to us or Paperbackshop-US, PaperbackShopUS, 801 Penhorn Avenue Unit 5, 07094, Secaucus, New Jersey, U.S.A., 44 1285 712917, without undue delay and in any event not later than 14 days from the day on which you communicate your cancellation from this contract to us. The deadline is met if you send back the goods before the period of 14 days has expired. You will have to bear the direct cost of returning the goods. You are only liable for any diminished value of the goods resulting from the handling other than what is necessary to establish the nature, characteristics and functioning of the goods.
Exceptions to the right of cancellation
The right of cancellation does not apply to:
Model withdrawal form
(complete and return this form only if you wish to withdraw from the contract)
To: (Paperbackshop-US, 901 Penhorn Avenue, Unit 6, 07094, Secaucus, New Jersey, U.S.A., 44 1285 712917)
I/We (*) hereby give notice that I/We (*) withdraw from my/our (*) contract of sale of the following goods (*)/for the provision of the following goods (*)/for the provision of the following service (*),
Ordered on (*)/received on (*)
Name of consumer(s)
Address of consumer(s)
Signature of consumer(s) (only if this form is notified on paper)
Date
* Delete as appropriate.
Books are shipped from our US or UK warehouses. Delivery estimates allow for delivery from either location.
| Order quantity | 7 to 14 business days | 7 to 14 business days |
|---|---|---|
| First item | £ 0.00 | £ 0.00 |
Delivery times are set by sellers and vary by carrier and location. Orders passing through Customs may face delays and buyers are responsible for any associated duties or fees. Sellers may contact you regarding additional charges to cover any increased costs to ship your items.