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有机化学中的光谱学第6版(英语红外部分)

有机化学中的光谱学第6版(英语红外部分)
有机化学中的光谱学第6版(英语红外部分)

Infrared spectra

Introduction

The infrared spectra of organic compounds are associated with transitions between vibrational energy level. Molecular vibrations may be detected and measured either in an infrared spectrum or indirectly in a Raman spectrum. The most useful vibrations, from the point of view of the organic chemist , occur in the narrower range of 2.5-16μm. The position of an absorption band in the spectrum may be expressed in microns, but standard practice uses a frequency scale in the form of wavenumbers, which are the reciprocals of the wavelength,cm-1.The useful range of the infrared for an organic chemist is between 4000 cm-1 at the high-frequency end and 625 cm-1 at the low frequency end.

Many function groups have vibration frequencies,characteristic of that functional group,within well-defined regions of the range;these are summarised in Charts 1-4 at the end of this chapter, with more detail in the tables of data that follow.because many functional groups can be identified by their characteristic vibration frequencies,the infrared spectrum is the simplest, most rapid, and often most most reliable means for identifying the functional groups.

Equation 2.1,which is derived from the model of a mass m

vibrating at frequency v on the end of a fixed spring, is useful in understanding the range of values of the vibrational frequencies of various kinds of bonds.

Where k is a measure of the strength of spring.However,in chemical bonds, one end of the “spring”(bond) is not fixed, but rather there are two mass(m1 and m2)involved and each is able to move.the m of Eq.2.1 is mow determined by the relationship in Eq.2.2

If one of the masses (say,m1) is infinitely large 1/m1 is then zero,and the relevant mass m for Eq.2.1 is simply that of m2 --making it analogous to the case where one end of the “spring”is fixed.

Simple substitutions of masses in these equations allow us to understand that with other things being equal:(1)C-H bonds will have higher stretching frequencies than C-C bonds , which in turn are likely to be higher than C-halogen bonds;(2)O-H bonds will have higher stretching frequencies than O-D bonds ;and (3),since k increases with increasing bond order ,the relative stretching frequencies of carbon-carbon bonds lie in the order:

These generalisations are useful, and Eqs. 2.1and 2.2 allow an increased understanding of the empirical data that are subsequently presented in this chapter. You may often be able to

extend the use of the model in a way that will make it easier to understand the trends that are observed.However, because of the other variables that influence vibrational frequencies,the equations should be taken as no more than a frequently useful guide.

2.2Preparetion of samples and examination in an infrared spectrometer

Older spectrometers used a source of infrared light which had been split into two beams of equal intensity.Only one of these was passed through the sample, and the difference in intensities of the two beams was then plotted as a function of https://www.doczj.com/doc/8c15921781.html,ing this old technology,a scan typically took about 10 minutes . Most spectrometers in use today use a Fourier transform method,and the spectra are called Fourier transform infrared (FTIR) spectra. A source of infrared light , emitting radiation throughout the whole frequency range of the instrument,typically 4600-400cm-1,is again divided into two beams of equal intensity. Either one beam is passed through the sample , or both are passed,but one beam is made to traverse a longer path than the other . Recombination of the two beams produces an interference pattern that is the sun of all the interference patterns created by each wavelength in the beam.By systematically changing the difference into the paths,

the interference patterns change to produce a detected signal varying with optical path difference,as modified by the selective absorption by the sample of some frequencies. This pattern is known as the interferogram , and looks nothing like a spectrum . However Fourier transformation of the interferogram, using a computer built into the instrument, converts it into a plot of absorption against wavenumber just like that from the older method . There are several advantages to FTIR over the old method , and few whole spectrum is measured in at most a few seconds .Because it is not necessary to scan each wavenumber successively , the whole spectrum is measured in at most a few seconds.Because it is not dependent upon a slit and a prism or grating , high resolution in FTIR iseasier to obtain without sacrificing sensitivity.FTIR is especially useful for examining small samples (several scans can be added together ) and for taking the spectrum of compounds produced only for a short period in the outflow of a chromatograph. Finally,the digital form in which the data are handled in the computer allows for adjustment and refinement. For example,by subtracting the background absorption of the medium in which the spectrum was taken, or by subtracting the spectrum of a known impurity from that of a known impurity from that of a mixture to reveal the spectrum of the pure

component . However, the way in which infrared spectra are taken does not affect their appearance.The older spectra and FTIR spectra look very similar , and older spectra in the literature are still valuable for comparison . Compounds may be examined in the vapour phase , as pure liquids , in solution,and in the solid state.

In the vapour phase.The vapour is introduced into a cell ,usually about 10 cm long,which can then be placed directly in the path of one of the infrared beams.The end walls of the cell are usually made of sodium chloride , which is transparent to infrared in the usual range . Most organic compounds have too low a vapour pressure for this phase to be useful .

As a liquid.A drop of the liquid is squeezed between flat plates of sodium chloride (transparent through the 4000-625cm-1 region). This is the simplest of all produces. Alternatively,if the sample of the liquid is not suitable for dispensing as a drop , a solution in a volatile and dry solvent may be deposited directly onto the surface of a sodium chloride plate , and the solvent allowed to evaporate in a dry atmosphere to leave a thin film.

In solution. The compound is dissolved to give ,typically, a 1-5% solution in carbon tetrachloride or ,for its better solvent properties , alcohol-free chloroform . This solution is introduced

into a cell , 0.1-1 mm thick ,made of sodium chloride . A second cell of equal thickness , but containing pure solvent , is placed in the path of the other beam of the spectormeter in order that solvent absorptions should be balanced.Spectra taken in such dilute solutions in non-polar solvents are generally the most desirable ,because they are normally better resolved than spectra taken on solids, and also because intermolecular forces ,which are especially strong in the crystalline state, are minimised. On the other hand , many compounds are not soluble in non-polar solvents,and all solvents absorb in the infrared; when the solvent absorption exceeds about 65% of the incident light, useful spectra cannot be obtained because insufficient light is transmitted to work the detection mechanism efficiently . Carbon tetrachloride and chloroform , fortunately, absorb over 65% of the incident light only in those region(Fig.2.1)which are of little interest in diagnosis. Other solvents, of course , may be used but the areas of usefulness in each case should be checked beforehand, taking account of the size of the cell being used. In rare cases aqueous solvents are useful ; special calcium fluoride cells are then used.

In the solid state.About 1mg of a solid is finely ground in a small agate mortar with a drop of a liquid hydrocarbon (Nujol Kaydol)or ,if C-H vibration are to be examined ,with

hexachlorobutadiene. The mull is then pressed between highly polished flat plates of sodium chloride. Alternatively,the solid ,often much less than 1 mg ,is ground with 10-100 times its bulk of pure potassium bromide and the mixture pressed into a disc using a mould and a hydraulic press. The use of KBr eliminates the problem (usually not troublesome)of bands from the mulling agent and tends,on the whole ,to give rather almost always appears(see Fig.2.7).Solids may alsobe deposited,either from a melt or ,as with liquids described above,by evaporation from a solution directly onto the surface of a sodium chloride plate ,with a sacrifice ,usually small ,from scattering off a crystalline surface.Because of intermolecular interactions,band positions in solid state spectra are offen different from those of the corresponding solution spectra. This is particularly true of those functional groups which take part in hydrogen bonding.On the other hand ,the number of resolve lines is often greater in solid state spectra,so that comparison of the spectra of,for example,synthetic and natural samples in order to determine identify is best done in the solid state. This is only true,of course,when the same crystalline modification is in use; racemic,synthetic material,for example,should be compared with enantiomerically pure,

nature material in solution.

2.3Examination in a Raman spectrometer

Raman spectra are generally taken on instruments using laser sources,and the quantity of material needed is now of the order of a few mg.A liquid or a concentrated solution is irradiated with monochromatic light,and the scattered light is examined by a spectometer using photoelectric detection.Most of the scattered light consists of the parent line produced by absorption and re-emission.Much weaker lines,which constitute the Raman spectrum,occur at lower and higher energy and are caused by absorption and re-emission of light coupled with vibrational excitation or decay,respectively.The difference in frequency between the parent line and the Raman line is the frequency of the corresponding vibration.Raman spectroscopy is not used by organic chemists routinely for structure determination,but for the detection of certain functional groups(see Fig.2.12)and for the analysis of mixtures-of deuterated compounds for example-it has found some use,especilly by analytical chemists.

2.4 Selection rules

If the frequency of a vibration of the sample molecule falls within the range of the instrument,the molecule may absorb energy of this frequency from the light,but only when the

oscillating dipole moment (from a molecular vibration)interacts with the oscillating electric vector of the infrared beam.

A simple rule for deciding if this interaction (and hence absorption of light)occurs is that the dipole moment at one extreme of a vibration must be different from the dipole moment at the other extreme of the vibration.In the Raman effect a corresponding interaction occurs between the light and the molecule's polarisability,resulting in different selection rules. The most important consequence of these selection rules is that in a molecule with a center of symmetry those vibrations symmetrical about the center of symmetry are active in the Raman and inactive in the infrared (see Fig.2.12);those vibrations which are not centrosymmetric are inactive in the Raman and usually active in the infrared. This is doubly useful,for it means that that the two types of spectrum are complementary.Furthermore ,the more easily obtained,the infrared ,is the more useful ,because most functional groups are not centrosymmetric.The symmetry properties of a molecule in a solid can be different from those of an isolated molecule. This can lead to the appearance of infrared absorption bands in a solid state spectrum which would be forbidden in solution or in the vapour phase.

2.5The infrared spectrum

A complex molecule has many vibrational modes which involve the whole molecule.To a good approximation,however,many of these molecular vibrations are largely associated with the vibrations of individual bonds and are called localised vibrations.These localised vibrations are useful for the identification of functional groups,especially the sterching vibrations of O-H and N-H single bonds and all kinds of triple and double bonds,almost all of which occur with frequencies greater than 1500cm-1.The stretching vibrations of other single bonds,most bending vibrations and the soggier vibrations of the molecule as a whole give rise to a series of absorption bands at lower energy,blow 1500cm-1,the positions of which are characteristic of that molecule.The net result is a region above 1500cm-1 showing absorption bands assignable to a number of functional groups,and a region containing many bands,characteristic of the compound in question and no other compound,below 1500cm-1 .For obvious reasons,this is called the fingerprint region.

Fig.2.2shows a representative infrared spectrum,that of cortisone acetate1.It shows the strong absorption from the stretching vibrations above 1500cm-1 demonstrating the

presence of each of the functional groups:the O-H group,three different C=O groups and the weaker absorption of the C=C double bond ,as well as displaying a characteristic fingerprint below 1500cm-1.

By convention absorbance is plotted downwards,opposite to the convention for ultraviolet spectra,but the maxima are still called peaks or bands.Rotational fine structure is smoothed out,and the intensity is frequently not recorded.When intensity is recorded,it is usually experssed subjectively as strong(s),medium(m),or weak(w).To obtain a high-quality spectrum,the quantity of substance is adjusted so that the strongest peaks absorb something close to 90% of the light.The scale on the abscissa is linear in frequency,but most instruments change the scale,either at 2200cm-1 or at 2000cm-1 to double the scale at the low-frequency end .The ordinate is linear in percent transmittance,with 100% at the top and 0% at the bottom.

The regions in which the different functional groups absorb are summarised below F.2.2.The stretching vibrations of single bonds to hydrogen give rise to the absorption at the high-frequency end of the spectrum as a result of the low mass of the hydrogen atom,making it easy to detect the presence of O-H and N-H groups.Since most organic compounds have C-H

bonds,the absorption close to 3000cm-1 is rarely usefully although C-H bonds attached to double and triple bonds van be usefully identified. Thereafter,the order of stretching frequencies follows the order:triple bonds at higher frequency than double bond between two similar atoms the higher the frequency of the vibration.Bending vibrations are of lower frequency and usually appear in the fingerprint region below 1500cm-1,but one exception N-H bending vibration,which appears in the 1600-1500cm-1 region.Polysyrene is sometimes used to provide accurately placed calibration lines at 2924,1603,1028,and 906cm-1.

Although many absorption bands are associated with the vibrations of individual bonds,other vibrations are coupled vibrations of two or more components of the whole molecule .Whether localised or not ,stretching vibrations are given the symbol v,and the various bending vibrations are given the symbol o.Coupled vibrations may be subdivided into asymmetric and symmetric stretching,and the various bending modes into scissoring ,rocking ,wagging and twisting,as defined for a methylene group in Fig.2.3. A coupled asymmetric and symmetric stretching pair is also found with many other groups,like carboxylic anhydrides,carboxylate ions and nitro

groups,each of which has two equal bonds close together.

2.6 The use of the tables of characteristic group frequencies Reference charts and tables of data are collected together at the end of this chapter for ready reference.Each of the three frequency ranges above 1500cm-1 shown in Fig.2.2 is expanded to give more detail in Charts 1-4 in Sec.2.1

3.Thesa charts summarise the narrower ranges within which each of the functional groups absorbs.The absorption bands which are found in the fingerprint region and which are assignable to functional groups are occasionally useful,either because they are sometimes strong bands in otherwise featureless regions or because their absence may rule out incorrect structures,but such identifications should be regarded as helpful rather than as definitive,since there are usually many bands in this area. Tables of detailed information can be found in Sec.2.14 at the end of this chapter,arranged by functional groups roughly in descending order of their stretching frequencies.

One could deal with the spectrum of an unknown as follows. Examine each of the three main regions of the spectrum above the fingerprint regions of the spectrum above the fingerprint region,as identified on Fig.2.2; at this stage certain combinations of structures can be ruled out --the absence of O-H

or C=O ,for example --and some tentative conclusions reached.Where there is still ambiguity --which kind of carbonyl group,for example -the tables corresponding to those groups that might be present should be consulted.It is important to be sure that the bands under consideration are of the appropriate intensity for the structure suspected.A weak signal in the carbonyl region,for example,for example ,it is more likely to be an overtone or to have been produced by an impurity.

The text following this section amplifies some of the detail for each the main functional groups,and shows the appearance,sometimes characteristic,of several of the functional groups,and shows the appearance,sometimes characteristic,of several of the bands.Cross-reference to the tables at the end is inevitable and will need to be frequent.

2.7 Absorption frequencies of single bonds to hydrogen 3600-2000

cm-1

C-H Bonds. The precise position of the various CH,CH2,and CH3 symmetrical and unsymmetrical vibration frequencies are well known.C-H bonds do not take part in hydrogen bonding and so their position is little affected by the state of measurement or their chemical environment.C-C vibrations,

which absorb in the fingerprint region,are generally weak and not practically useful . Since many organic molecules possess saturated C-H bonds,their absorption bands,stretching in the 3000-2800cm-1 region and bending in the fingerprint region,are of little diagnostic value,but a few special structral features in saturated C-H groupings do give rise to characteristic absorption bands(Table 2.1).Thus,methyl and methylene groups usually show two sharp bands from the symmetric and asymmetric stretching(Fig.2.3),which can sometimes be picked out but the general appearance of the accumulation of all the saturated C-H stretching vibrations often leads to broader and not fully resolved bands like those illustrated in many of the spectra below . The absence of saturated C-H absorption in a spectrum is ,of course,diagnostic evidence for the absence of such a part structure in the corresponding compound. Unsaturated and aromatic C-H stretching frequencies (Table 2.1)can be distinguished from the saturated C-H absorption,since they occur a little above 3000cm-1 and are relatively weak,as in the spectrum of ethyl benzoate 2(Fig.2.4)and benzonitrile 14(Fig.2.7).Terminal acetylenes give rise to a characteristic strong,sharp line close to 3300cm-1 from ¥C-H stretching,as in the spectrum of hexyne3(Fig.2.4),and ethers and amines

also show bands in the low-frequency region 2850-2750cm-1.When the antiperiplanar arrangement is rigidly fixed ,as in axially-oriented C-H bonds in six-membered cyclic amines,C-H stretching has an unusually low frequency,giving rise to absorption known as Bohlmann bands.

The C-H bending vibrations are in the fingerprint region,with methine C-H bending and CH3 and CH2 symmetrical bending giving rise in many organic compounds to two bands close to 1450and 1380cm-1,as seen in the common mulling agent Nujol.The out-of -plane vibration of trans-C=CH- diuble bonds is one of the more usefully diagnostic bending vibrations .It occurs in a narrow range 970-960cm-1,or at slightly higher frequency if conjugated ,and it is always strong.In contrast,the corresponding vibration of the cis isomer is of lower intensity and at lower frequency,typically in the range 730-675cm-1.The band at 975cm-1in the fingerprint of ethyl trans-crotonate5(Fig.2.4)clearly shows that such a feature may be present ;if it were not there,it would be diagnostic of the absence of this feature,as in the spectrum of the cis-alkene 20 in Fig.2.12

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