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Signal Characteristics Wavenumber

For every bond, the wavenumber of absorption associated with bond stretching is dependent on two factors (1) bond strength and (2) masses of the atoms sharing the bond. The impact of these two factors can be rationalized when we treat a bond as if it were a vibrating spring cotmecring two weights. [Pg.677]

Using this analogy, we can construct the following equation, derived from Hooke s law, which enables us to approximate the frequency of vibration for a bond between two atoms of mass mi and m2  [Pg.677]

While appears in the denominator of the equation, the force constant (/) appears in the numerator. This means that stronger bonds will vibrate at higher frequencies, thereby corresponding to a higher wavenumber of absorption. For example, compare the following bonds. The C N bond is the strongest of the three bonds and therefore appears at the highest wavenumber. [Pg.677]

An IR absorbance spectrum divided into regions based on bond strength and atomic mass. [Pg.677]

In the previous section, we saw that bonds to hydrogen (such as C—H bonds) appear on the left side of an IR spectrum (high wavenumber). We will now compare various kinds of C—H bonds. [Pg.678]


Every signal in an IR spectmm has three characteristics wavenumber, intensity, and shape. We wiH now explore each of these three characteristics, starting with wavenumber. [Pg.676]

Remember that each signal appearing in the diagnostic region wiU have three characteristics (wavenumber, intensity, and shape). Make sure to analyTe all three characteristics. [Pg.690]

Every signal has three characteristics—wavenumber, intensity, and shape. Analyze all three. [Pg.712]

Although the idea of generating 2D correlation spectra was introduced several decades ago in the field of NMR [1008], extension to other areas of spectroscopy has been slow. This is essentially on account of the time-scale. Characteristic times associated with typical molecular vibrations probed by IR are of the order of picoseconds, which is many orders of magnitude shorter than the relaxation times in NMR. Consequently, the standard approach used successfully in 2D NMR, i.e. multiple-pulse excitations of a system, followed by detection and subsequent double Fourier transformation of a series of free-induction decay signals [1009], is not readily applicable to conventional IR experiments. A very different experimental approach is therefore required. The approach for generation of 2D IR spectra defined by two independent wavenumbers is based on the detection of various relaxation processes, which are much slower than vibrational relaxations but are closely associated with molecular-scale phenomena. These slower relaxation processes can be studied with a conventional... [Pg.561]

Bands, which do shift upon lithium substitution, were found in both compounds below 600 cm . The two absorption bands observed near 500 cm in methyllithium appeared at much higher wavenumbers in the corresponding Li compound. Most of the shifts observed upon Li substitution (Table 1) are smaller than the characteristic shifts for harmonic C—Li bonds (about 26 cm for bands near 500 cm ) , as expected since they represent complex vibrational modes. Furthermore, aU of these signals are significantly shifted upon deuterium substitution, which indicates that they involve the motion of hydrogen as well as lithium (Table 1) . ... [Pg.231]

Romanian amber (Colti, Buzau County) 389 3200 OH frequencies, alcoholic (phenolic free OH and bound intramolecular OH) from hydro -acids observed wavenumbers shifte characteristic of amorphous structures. Less intense signals in this region for archaeological samples and slight shifts... [Pg.358]

In summary, the amplitude of the interferogram as observed after detection and amplification is proportional not only to the intensity of the source but also to the beamsplitter efficiency, detector response, and amplifier characteristics. Of these factors, only 7(vo) varies from one measurement to the next for a given system configuration, while all the other factors remain constant. Therefore, Eq. 2.4 may be modified by a single wavenumber-dependent correction factor, 7/(vo), so that the ac signal, 5(8) (in volts), from the amplifier is... [Pg.23]


See other pages where Signal Characteristics Wavenumber is mentioned: [Pg.671]    [Pg.677]    [Pg.677]    [Pg.679]    [Pg.671]    [Pg.677]    [Pg.677]    [Pg.679]    [Pg.177]    [Pg.1006]    [Pg.294]    [Pg.398]    [Pg.210]    [Pg.118]    [Pg.251]    [Pg.447]    [Pg.112]    [Pg.5]    [Pg.5]    [Pg.7]    [Pg.91]    [Pg.113]    [Pg.407]    [Pg.112]    [Pg.374]    [Pg.202]    [Pg.96]    [Pg.62]    [Pg.314]    [Pg.355]    [Pg.628]    [Pg.768]    [Pg.258]    [Pg.210]    [Pg.328]    [Pg.247]    [Pg.84]    [Pg.668]    [Pg.36]    [Pg.229]    [Pg.241]    [Pg.23]    [Pg.148]    [Pg.457]    [Pg.460]    [Pg.3216]   


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