Advanced Pharmaceutical Analysis 2nd Semester, Year 5 (2023) Lecture 1 Advanced Pharmaceutical Analysis “Introduction” Prof. Dr. Asim A. Balakit Pharmaceutical Chemistry Dept., College of Pharmacy, Babylon University 1 Introduction to Spectrochemical Methods How can we determine the structure of certain molecule? How can we determine the concentrations? What are the ingredients of these formulations? What is the concentration of the active compound in each of them? 2 Spectroscopy: is the study of the interaction between matter and radiant energy. Spectroscopic analytical methods are based on measuring the amount of radiation absorbed (absorption spectroscopy) or produced (emission spectroscopy) by molecular or atomic species of interest. Spectrochemical methods provide the most widely used tools for the elucidation of molecular structure as well as the quantitative and qualitative determination of both inorganic and organic compounds. 3 Electromagnetic radiation is radiant energy having the properties of both particles and waves. A particle of electromagnetic radiation is called a photon. Because electromagnetic radiation has both particle-like and wave-like properties, it can be characterized by either: Wavelength (Greek lambda; 𝜆): the distance from one wave maximum to the next, it is generally measured in micrometers (μm; 10-6 m) or nanometers (nm; 10-9 m). or Frequency (Greek nu; 𝝂): the number of waves that pass by a fixed point per unit time, usually given in reciprocal seconds (s-1), or hertz (Hz), 1 Hz = 1 s-1 Amplitude: is the height of the wave measured from midpoint to the peak. The intensity of the radiant energy is proportional to the square of the wave’s 4 amplitude. 5 The frequency of electromagnetic radiation is equal to the speed of light (c) divided by the radiation’s wavelength: 𝜈= 𝑐 𝜆 c = 3 x 1010 cm/s The relationship between the energy (E) of a photon and the frequency (or the wavelength) of the electromagnetic radiation is described by the equation: ℎ𝑐 𝐸 = ℎ𝜈 = 𝜆 where ℎ is the proportionality constant called Planck’s constant, named after the German physicist who discovered the relationship. 6 7 Classification of spectroscopic methods according to region of the electromagnetic spectrum involved: γ–ray, Xray, ultraviolet (UV), visible, infrared (IR), microwave, and radio frequency (RF). 8 Infrared Spectrophotometry 9 10 Ultraviolet and Visible Spectroscopy 11 12 Nuclear Magnetic Resonance Spectroscopy 13 Mass spectrometry 14 15 The reference on which the lectures are based is: 16 Other references: 17 Infrared Spectroscopy Lecture 1 Based on: Pharmaceutical Analysis, David G. Watson, 3rd Edition Organic Chemistry, L. G. Wade, Jr., 6th Edition 18 Principles Electromagnetic radiation ranging between 400 cm-1 and 4000 cm-1 (2500 and 20000 nm) is passed through a sample and is absorbed by the bonds of the molecules in the sample causing them to stretch or bend. The wavelength of the radiation absorbed is characteristic of the bond absorbing it. Applications A qualitative fingerprint check for the identity of raw material used in manufacture and for identifying drugs. Used in synthetic chemistry as a preliminary check for compound identity, particularly for the presence or absence of a carbonyl group, which is difficult to check by any other method. Can be used to characterize samples in the solid and semi-solid states such as creams and tablets. Used as a fingerprint test for films, coatings and packaging plastics. Can be used to detect polymorphs of drugs (polymorphs are different crystal forms of a molecule that have different physical properties such as solubility and melting point, which may be important in the manufacturing process and bioavailability). Strengths Provides a complex fingerprint which is unique to the compound being examined. Computer control of instruments means that matching of the spectrum of a compound to its standard fingerprint can now be readily carried out. Limitations Rarely used as a quantitative technique because of relative difficulty in sample preparation and the complexity of spectra. Usually can only detect gross impurities in samples. Sample preparation requires a degree of skill, particularly when potassium bromide (KBr) discs are being prepared. The technique is lacking in robustness since sample handling can have an effect on the spectrum obtained and thus care has to be taken in sample processing. Vibration Modes: Covalent bonds are not static and they are constantly vibrating . 21 The vibrations are quantized, that means they occur only at specific frequencies, which correspond to the frequency of IR light. During the bombardment of a molecule with IR light, when the frequency of IR light matches the frequency of a particular vibrational mode, the molecule will absorb the IR light , causing the amplitude of the particular bond stretch or bond bend to increase. By determining the wave numbers of the energy absorbed by a compound, we can know the kinds of bonds it has. 22 Molecular Vibrations: Stretching Vibrations HCl has an absorbance maximum at ca 2900 cm-1, which results from the transition between the bottom vibrational state V0 and the first excited state V1 23 Factors determining intensity and energy level of absorption in IR spectra: A- Intensity of absorption The intensity with which a bond absorbs radiation depends on its dipole moment. Thus the order of intensity of absorption for the following C–X bonds is: The intensity depends on the relative electronegativity of the atoms involved in the bond. The intensity of the stretching of carbon–carbon double bonds is increased when they are conjugated to a polar double bond. The order of intensity is as follows: B- Energy level of absorption The frequency of the stretching vibration depends on two factors: 1- Masses of the Atoms : Heavier atoms vibrate more slowly than lighter ones which means frequency decreases with increasing atomic weight. e.g. The characteristic frequency of a C-D bond is lower than that of a C-H bond. 2- Stiffness of the Bond: Stronger bonds are generally stiffer, they are requiring more force to stretch or compress them. Thus, stronger bonds usually vibrate faster than weaker bonds (assuming the atoms have similar masses). In a group of bonds having atoms of similar masses, frequency increases with bond energy. e.g. 1- O-H bonds are stronger than C-H bonds, and 0-H bonds vibrate at higher frequencies. 2- Triple bonds are stronger than double bonds, so triple bonds vibrate at higher frequencies than double bonds. 25 In a group of bonds with similar bond energies, the frequency decreases with increasing atomic weight. In a group of bonds between similar atoms, the frequency increases with bond energy. 26 Are all the vibrations IR-active?! The rapidly reversing electric field (E) is one of the components of an electromagnetic wave. This field alternately stretches and compresses a polar bond. If this alternate stretching and compressing of the bond occurs at the frequency of the molecule's natural rate of vibration, energy may be absorbed. Vibrations of bonds with dipole moments generally result in IR absorptions and are said to be IR active. 27 So, what is the IR-inactive vibration?! If a bond is symmetrical and has zero dipole moment, the electric field does not interact with the bond. e.g. The triple bond of the acetylene molecule: H-C≡C-H which has zero dipole moment (whether the bond is stretched or compressed), so the vibration does not produce any change in the dipole moment and consequently there is no energy absorption. This kind of vibrations said to be IR-inactive because it produces no absorption in the IR spectrum. 28 What is the infrared spectrum? It is a graph of the energy absorbed by a molecule as a function of the frequency or wavelength of light. e.g. The IR spectrum of methanol: 29 IR Spectrometer: Dispersive IR Spectrophotometer A monochromator is used to select each wavenumber in turn in order to monitor its intensity after the radiation has passed through the sample 30 Fourier Transform IR Spectrophotometer It generates a radiation source in which individual wavenumbers can be monitored within a ca 1 s pulse of radiation without dispersion being required. Michelson interferometer used in FT–IR instruments. The advantage of this technique is that a full spectral scan can be acquired in about 1 s, compared with the 2–3 min required for a dispersive instrument to acquire a spectrum. Also, because the instrument is attached to a computer, several spectral scans can be taken 31 and averaged in order to improve the signal : noise ratio for the spectrum. 32 Sample preparation: The sample is run as a film sandwiched between two NaCl or potassium chloride (KCl) discs. For this method the sample must be a liquid, in which case it can be run without preparation, or must be ground to a paste in a liquid matrix, usually liquid paraffin. In this case the liquid paraffin (Nujol) contributes some peaks to the spectrum at ca 3000 cm1 and ca 1400–1500 cm-1. However, sample preparation is relatively simple and this procedure is used where a chemist just wants a quick identification of certain structural features in a molecule. This procedure is also used to identify different crystal forms (polymorphs) of a drug because the pressures used to prepare KBr discs can cause polymorph interconversion. The sample is ground to a powder with KBr or KCl. KBr is usually used unless a hydrochloride salt is being analysed, in which KCl is used to avoid halogen exchange. On a weight-for-weight basis, the weight of the sample used is about 1% of the weight of KBr used. This is the procedure used in pharmacopoeial methods to prepare a drug for analysis by IR. IR spectra of liquids or solutions in an organic solvent, commonly chloroform, may be obtained by putting the liquid into a short pathlength cell with a width of ca 1 mm. Cells are constructed from sodium or potassium chlorides and obviously aqueous samples cannot be used. Diffuse Reflectance Technique: The diffuse reflectance technique is widely used in near-infrared spectrophotometry and it can also be used to examine films and coatings if they are put onto a reflective background. It is also a useful technique for examining polymorphs since the sample can be prepared for analysis with minimal grinding and compression, which can cause interconversion of polymorphs. Attenuated total reflectance (ATR) Sample may be run in a gel or cream, and this method may be used to characterise both formulation matrices and their interactions with the drugs present in them. If the active ingredient is relatively concentrated and if a blank of the matrix is run using the same technique it may be subtracted from the sample to yield a spectrum of the active ingredient. ATR also provides another technique which can be used for the characterisation of polymorphs. Infrared Spectroscopy Lecture 2 38 IR Spectroscopy of Hydrocarbons Hydrocarbons contain only carbon-carbon bonds and carbon-hydrogen bonds. Carbon-Carbon Bond Stretching C - C single bond absorptions (and most other absorptions in the fingerprint region) are not very reliable. An infrared spectrum does not provide enough information to identify a structure conclusively (unless an authentic spectrum is available to compare "fingerprints"). But, the absorptions of the carbon-carbon and carbon-hydrogen bonds can indicate the presence of double and triple bonds. Carbon-carbon bond stretching frequencies: 39 Effect of Conjugation: Most unsymmetrically substituted double bonds produce observable stretching absorptions in the region of 1600 to 1680 cm - 1 . Isolated double bonds absorb around 1640 to 1 680 cm- 1, and conjugated double bonds absorb around 1620 to 1 640 cm- 1 . 40 The aromatic C=C bonds are more like 1.5 bonds than true C=C. Their reduced π bonding results in less stiff bonds with lower stretching frequencies, around 1600 cm-1. Characteristic C=C stretching frequencies: 41 Because C≡C bonds are stronger and stiffer than C=C, they absorb IR light at higher frequencies. Most alkyne C≡C bonds have stretching frequencies between 2100 and 2200 cm-1. Terminal alkynes usually give sharp C≡C stretching signals of moderate intensity. The C≡C stretching absorption of an internal alkyne may be weak or absent, however, due to the symmetry of the disubstituted triple bond with a very small or zero dipole moment. 42 Carbon-Hydrogen Bond Stretching The S orbital is closer to the nucleus than the p orbitals, and stronger, stiffer bonds result from orbitals with more s character. C-H bond with higher S character absorbs IR light at higher frequency. 43 Hydrocarbons stretching frequencies: 44 45 46 47 48 Problem: For each hydrocarbon spectrum, determine whether the compound is an alkane, an alkene, an alkyne, or an aromatic hydrocarbon. More than one unsaturated group may be present. 49 Characteristic Absorptions of Alcohols and Amines: The 0-H bonds of alcohols and the N-H bonds of amines are strong and stiff. The vibration frequencies of 0-H and N-H bonds therefore occur at higher frequencies than those of most C-H bonds (except for alkynyl ≡C-H bonds). 50 The free O-H stretch is a sharp peak at 3650–3600 cm−1. This band appears in combination with the hydrogen-bonded O-H peak when the alcohol is dissolved in a solvent. The hydrogen-bonded O-H band is a broad peak at 3400–3300 cm−1. This band is usually the only one present in an alcohol that has not been dissolved in a solvent (neat liquid). When the alcohol is dissolved in a solvent, the free O-H and hydrogen-bonded O-H bands are present together, with the relatively weak free O-H on the left. (a) Hydrogen-bonded O-H only (neat liquid). (b) Free and hydrogen-bonded O-H (dilute solution). (c) Free and hydrogen-bonded O-H (very dilute solution). 51 C-O-H Bending appears as a broad and weak peak at 1440–1220 cm−1, often obscured by the CH3 bendings. C-O Stretching vibration usually occurs in the range 1260–1000 cm−1. This band can be used to assign a primary, secondary, or tertiary structure of an alcohols, or to determine whether a phenolic compound is present. 52 Methyl salicylate Intramolecular hydrogen bonding, present in ortho-carbonyl-substituted phenols, usually shifts the broad O-H band to a lower frequency. For example, the O-H band is centered at about 3200 cm−1 in the neat spectrum of methyl salicylate, while O-H bands from normal phenols are centered at about 3500 cm−1. The intramolecular hydrogen-bonded band does not change its position significantly even at high dilution because the internal bonding is not altered by a change in concentration. 53 These numbers should be considered base values. These C-O absorptions are shifted to lower frequencies when unsaturation is present on adjacent carbon atoms or when the O-H is 54 attached to a ring. Shifts of 30 to 40 cm−1 from the base values are common. Primary (1°) and secondary (2°) amines give absorptions of moderate strength in the 3300– 3500 cm-1 region. Primary amines exhibit two peaks in this region due to symmetric and asymmetric stretching of the two N-H bonds. Secondary amines exhibit a single peak (weak one for aliphatic compounds and a stronger one for aromatic secondary amines). Hydrogen bonding causes N-H stretching peaks of 1° and 2° amines to broaden. Tertiary amines show no N-H absorption because they have no such bond. 55 N-H Bend (scissoring) in primary amines results in a broad band in the range 1640– 1560 cm−1. In aromatic secondary amines, the band shifts to a lower frequency and appears near 1500 cm−1. However, in aliphatic secondary amines the N-H bending vibration is very weak and usually is not observed. N-H Out-of-plane bending absorption can sometimes be observed near 800 cm-1. C-N Stretch occurs in the range 1350–1000 cm-1. Aliphatic amines absorb from 1250 to 1000 cm−1, whereas aromatic amines absorb from 1350 to 1250 cm−1. (Why?!) 56 57 58 59 Characteristic Absorptions of Carbonyl Compounds: Because it has a large dipole moment, the C=O double bond produces intense infrared stretching absorptions. Carbonyl groups absorb at frequencies around 1700 cm-1, but the exact frequency depends on the specific functional group and the rest of the molecule. Some carbonyl groups absorb at frequencies higher than 1710 cm-1. For example, simple carboxylic esters absorb around 1735 cm-1. These higher-frequency absorptions are also seen in strained cyclic ketones (in a fivemembered ring or smaller). In a small ring, the angle strain on the carbonyl group forces more electron density into the C=O double bond, resulting in a stronger, stiffer bond. 60 The normal base values for the C=O stretching vibrations for the different carbonyl groups are: 1810 Anhydride 1 1800 Acid chloride 1760 Anhydride2 1735 Ester 1725 Aldehyde 1715 Ketone 1710 Carboxylic acid 1690 Amide cm-1 61 Factors that influence the C=O stretching vibrations: 1- Resonance lowering of Carbonyl Frequencies: Delocalization of the pi electrons reduces the electron density of the carbonyl double bond, weakening it and lowering the stretching frequency from about 1710 cm- 1 to about 1685 cm- 1 for conjugated ketones, aldehydes, and acids. The C=C absorption of a conjugated carbonyl compound may not be apparent in the IR spectrum because it is so much weaker than the C=O absorption. The presence of the C=C double bond is often inferred from its effect on the C=0 frequency and the presence of unsaturated =C-H absorptions above 3000 cm-1. 62 Often, two closely spaced C=O absorption peaks are observed for these conjugated systems, resulting from two possible conformations, the s-cis and s-trans. The s-cis conformation absorbs at a frequency higher than the s-trans conformation. In some cases, the C=O absorption is broadened rather than split into the doublet. 63 2- Ring-Size Effects: Six-membered rings with carbonyl groups are unstrained. Decreasing the ring size increases the frequency of the C=O absorption. For ketones and esters, there is often a 30 cm−1 increase in frequency for each carbon removed from the unstrained six-membered ring values. 64 3- α-Substitution Effects: When the carbon next to the carbonyl is substituted with a chlorine (or other halogen) atom, the carbonyl band shifts to a higher frequency. 4- Hydrogen-Bonding Effects: Hydrogen bonding to a carbonyl group lengthens the C=O bond and lowers the absorption frequency. 65 Simple Ketones, Aldehydes, and Acids: The C=O stretching vibrations of simple ketones, aldehydes, and carboxylic acids occur at frequencies around 1710 cm-1. These frequencies are higher than those for C=C double bonds because the C=0 double bond is stronger and stiffer. 66 Infrared spectra of (a) 2-heptanone and (b) butyraldehyde. Both the ketone and the aldehyde show intense carbonyl absorptions near 1710 cm-1. In the aldehyde spectrum, there are two peaks (2720 and 2820 cm-1) characteristic of the aldehyde C-H stretch. 67 A carboxylic acid produces a characteristic broad 0-H absorption in addition to the intense carbonyl stretching absorption. Because of the unusually strong hydrogen bonding in carboxylic acids, the broad 0-H stretching frequency is shifted to about 3000 cm-I, centered on top of the usual C-H absorption. This broad 0-H absorption gives a characteristic overinflated shape to the peaks in the C-H stretching region. Participation of the acid carbonyl group in hydrogen bonding frequently results in broadening of the strong carbonyl absorption as well. 68 Problem: Determine the functional group(s) in the compound whose IR spectrum appears here. A weak peak around 3400 cm-1, a strong peak about 1720 cm-1, and an unusual C-H stretching region. The C-H region has two additional peaks around 2720 and 2820 cm-1. The strong peak at 1725 cm-1 must be a C=0, and the peaks at 2720 and 2820 cm-1 suggest an aldehyde. The weak peak around 3400 cm-1 might be mistaken for an alcohol 0-H. 69 Problem: Spectra are given for three compounds. Each compound has one or more of the following functional groups: alcohol, amine, ketone, aldehyde, and carboxylic acid. Determine the functional group(s) in each compound. 70 Amides: The carbonyl groups of amides absorb at particularly low IR frequencies: about 1640 to 1680 cm-1. The dipolar resonance structure places part of the pi bond between carbon and nitrogen, leaving less than a full C=0 double bond. Like primary amines, most primary amides show two spikes in the N–H stretching region (about 3300 cm-1) Secondary amides (like secondary amines) generally show one N–H spike. The very low frequency of the amide carbonyl might be mistaken for an alkene C=C stretch. So, how can we distinguish between C=O and C=C absorptions, even when they appear in the same region of the spectrum?! 71 In the spectra of butyramide (C=O about 1640 cm-1) and 1-methylcyclopentene (C=C at 1658 cm-1) we can see three differences: 1. The amide carbonyl absorption is much stronger than the absorption of the alkene double bond. 2. There are prominent N-H stretching absorptions in the amide spectrum. 3. There is an unsaturated C-H stretching (just to the left of 3000 cm-1 ) in the alkene spectrum. 72 Conjugation does not reduce the C=O frequency in amides. The introduction of α,β, unsaturation causes an increase in frequency from the base value given. Apparently, the introduction of sp2-hybridized carbon atoms removes electron density from the carbonyl group and strengthens the bond instead of interacting by resonance as in other carbonyl examples. Since the parent amide group is already highly stabilized, the introduction of the C=C unsaturation does not overcome this resonance. Cyclic amides (lactams) give the expected increase in C=O frequency for decreasing ring size. 73 Esters: 74 Examples: 75 76 Conjugation with a Carbonyl Group (α,β Unsaturation or Aryl Substitution): The C=O stretching vibrations are shifted by about 15 to 25 cm−1 to lower frequencies with α,β unsaturation or aryl substitution. Conjugation with the Ester Single-Bonded Oxygen: Conjugation involving the single-bonded oxygen shifts the C=O vibrations to higher frequencies. 77 Examples: 78 Hydrogen-Bonding Effects: When intramolecular (internal) hydrogen bonding is present, the C=O is shifted to a lower frequency. Cyclic Esters (Lactones): The C=O vibrations are shifted to higher frequencies with decreasing ring size. 79 80 α-Halo Effects: Halogenation on the carbon leads to an increase in the C=O frequency. α-Keto Esters: In principle, one should see two carbonyl groups for a compound with “ketone” and “ester” functional groups. Usually, one sees a shoulder on the main absorption band near 1735 cm−1 or a single broadened absorption band. β-Keto Esters: Although this class of compounds exhibits tautomerization less evidence exists for the enol form because β-keto esters do not enolize to as great an extent. 81 β-Keto esters exhibit a strong-intensity doublet for the two carbonyl groups at about 1720 and 1740 cm−1 in the “keto” tautomer, presumably for the ketone and ester C=O groups. Evidence for the weak-intensity C=O band in the “enol” tautomer (often a doublet) appears at about 1650 cm−1. Because of the low concentration of the enol tautomer, one generally cannot observe the broad O-H stretch that was observed in β-diketones 82 C-O Stretching Vibrations in Esters: Two (or more) bands appear for the C-O stretching vibrations in esters in the range from 1300 to 1000 cm−1. The C-O stretch next to the carbonyl group (the “acid” side) of the ester appears between 1300 and 1150 cm−1 for most common esters. The C-O stretch for the “alcohol” part of the ester may appear as a weaker band in the range from 1150 to 1000 cm−1. In analyzing the 1300- to 1000-cm−1 region to confirm an ester functional group, do not worry about fine details. It is usually sufficient to find at least one very strong and broad absorption to help identify the compound as an ester. 83 Acid Chlorides: C=O Stretching Vibrations Acid chlorides show a very strong band for the C=O group that appears in the range of 1810–1775 cm−1 for aliphatic acid chlorides. Conjugation lowers the frequency. The strong carbonyl absorption appears at a characteristically high frequency of about 1800 cm−1 for saturated acid chlorides. Conjugated acid chlorides absorb at a lower frequency (1780 to 1760 cm−1). C-Cl Stretching Vibrations These bands, which appear in the range from 730 to 550 cm−1, are best observed if KBr plates or cells are used. 84 85 Anhydrides: Anhydrides show two strong bands for the C=O groups. Simple alkyl-substituted anhydrides generally give bands near 1820 and 1750 cm−1. Conjugation shifts each of the bands to lower frequencies (about 30 cm−1 each). Simple five-membered ring anhydrides have bands at near 1860 and 1780 cm−1 Anhydrides and acid chlorides are the most common functional groups that have a C=O peak appearing at such a high frequency. 86 87 The characteristic pattern for noncyclic and saturated anhydrides is the appearance of two strong bands, not necessarily of equal intensities, in the regions from 1830 to 1800 cm−1 and from 1775 to 1740 cm−1. The two bands result from asymmetric and symmetric stretch. Conjugation shifts the absorption to a lower frequency, while cyclization (ring strain) shifts the absorption to a higher frequency. The strong and broad C-O stretching vibrations occur in the region from 1300 to 900 cm−1. 88 ETHERS Simple aliphatic ethers can be distinguished from alkanes by the presence of the C-O band. The most prominent band is that due to C-O stretch, 1300–1000 cm−1. Absence of C=O and O-H is required to ensure that C-O stretch is not due to an ester or an alcohol. Phenyl alkyl ethers give two strong bands at about 1250 and 1040 cm−1, while aliphatic ethers give one strong band at about 1120 cm−1. 89 Dialkyl Ethers: The asymmetric C-O-C stretching vibration leads to a single strong absorption that appears at about 1120 cm−1, as seen in the spectrum of dibutyl ether. The symmetric stretching band at about 850 cm−1 is usually very weak. The asymmetric C-O-C absorption also occurs at about 1120 cm−1 for a six-membered ring containing oxygen. 90 Aryl and Vinyl Ethers: Aryl alkyl ethers give rise to two strong bands: an asymmetric C-O-C stretch near 1250 cm−1 and a symmetric stretch near 1040 cm−1, as seen in the spectrum of anisole. Vinyl alkyl ethers also give two bands: one strong band assigned to an asymmetric stretching vibration at about 1220 cm−1 and one very weak band due to a symmetric stretch at about 850 cm−1. 91 The shift in the asymmetric stretching frequencies in aryl and vinyl ethers to values higher than were found in dialkyl ethers can be explained through resonance. 92 Nitriles: Stretch is a medium-intensity, sharp absorption near 2250 cm−1. Conjugation with double bonds or aromatic rings moves the absorption to a lower frequency. 93 The C≡N group in a nitrile gives a medium-intensity, sharp band in the triple-bond region of the spectrum (2270 to 2210 cm−1). The C≡C bond, which absorbs near this region (2150 cm−1), usually gives a weaker and broader band unless it is at the end of the chain. Aliphatic nitriles absorb at about 2250 cm−1, whereas their aromatic counterparts absorb at lower frequencies, near 2230 cm−1. C=N: The C=N bond absorbs in about the same range as a C=C bond. Although the C=N band varies in intensity from compound to compound, it usually is more intense than that obtained from the C=C bond. An oxime (R-CH=N-O-H) gives a C=N absorption in the range from 1690 to 1640 cm−1 and a broad O-H absorption between 3650 and 2600 cm−1. An imine (R-CH=N-R) gives a C=N absorption in the range from 1690 to 1650 cm−1. 94 95 96 97 98 99 100 Infrared Spectroscopy Lecture 3 101 APPLICATION OF IR SPECTROPHOTOMETRY IN STRUCTURE ELUCIDATION EXAMPLES OF IR SPECTRA OF DRUG MOLECULES Infrared spectrum of paracetamol as a KBr disc. The infrared spectrum of aspirin as a KBr disc. The infrared spectrum of dexamethasone obtained as a KBr disc. IR spectrum of Phenoxymethyl penicillin potassium. Obtained as a KBr disc. IR spectrophotometry as a fingerprint technique