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TRANSCRIPT
Chapter-2
24
2525
INTRODUCTION:
The present chapter comprises two sections. Section-I comprises
characterization techniques used to characterize the produced compounds (shown in
following chapters). and Section-II comprises the synthesis and characterization of
various Schiff bases of NTOH.
2626
SECTION-I
TECHNIQUES USED FOR CHARACTERIZATION OF COMPOUNDS
2727
2.1 Elemental Analysis
The majority of organic compounds are composed of a relatively small
number of elements. The most important ones are: carbon, hydrogen, oxygen,
nitrogen, sulphur, chlorine, etc. Elementary quantitative organic analysis is used to
determine the content of carbon, hydrogen, nitrogen, and other elements in the
molecule of an organic compound.
2.2 Introduction to Spectrometry
In modern era structure determination is very easy by using various
spectroscopy techniques: the study of the interaction of matter and light (or other
electromagnetic radiations). These techniques have been greatly significant to many
areas of science. For example, by help of spectroscopy we exactly know about orbital
and bonding. But spectroscopy is also important to the scientist because it can be used
to determine unknown molecular structures. Although this arrangement of
spectroscopy will spotlight largely on its applications, some fundamentals of
spectroscopy theory must be considered first.
2.3 Infrared Spectroscopy
Infrared spectroscopic technique [1-4] is of an immense importance to organic
chemists for the identification of the presence of functional groups in the organic
compounds although it does not give the fully data with respect to the molecular
constituents of the organic compounds. However it is used for the identification of the
compounds.
Infrared spectroscopic technique gives the information about the molecular
vibrations or large exactly on the transition between vibrational and rotational energy
levels in the molecule and due to this characteristic; it is of immense help to organic
chemists.
When infrared light is approved through a taster, some of the frequencies are
engrossed while other frequencies are transmitted through the sample. The absorption
2828
of infrared radiation depends on increasing the energy of vibration or rotation
associated with co-valent bond in a molecule.
Radiation absorption in the IR region outcome in the bond excitation
deformations, bending or either stretching. Different bending and stretching vibrations
found at fixed quantized frequencies. When IR light of required frequency is pass or
incident on the compound, amplitude of that vibration because of energy is absorbed.
“An IR spectrum are found If the frequency of vibrations of compounds suitable to
the IR frequency radiations absorbed.”
The sample under investigation is largely in the solid state, a solution or neat
liquid. Occasionally, however, a sample is in the vapor or gaseous phase is
investigated. Under this situation, in addition with alteration in vibrational energy,
meanwhile alteration in rotational energy can also observed and as a result few fine
structures may be found in the vibrational band. IR spectrum of a compound
represents its energy absorption pattern in the infrared region and is obtained by
plotting percentage absorbance or transmittance of infrared radiation as a function of
wavelength or wave number over a particular range.
Infrared spectroscopy is usually divided into three regions.
• Near infrared (overtone region) – between 12500cm-1-4000cm-1
• Middle infrared (fundamental vibrational region) – between 4000cm-1-
667cm-1
• Far infrared (pure rotational region) – between 667cm-1-50cm-1
The normal or middle infrared level is specifically meant for organic scientist
therefore the vibrations induced in organic compounds are absorbed within this level.
The fundamental vibrational area is divided into the functional group region (4000cm-
1-1400cm-1) and finger print region (1400cm-1-667cm-1). The normal and far infrared
regions contain absorptions due to fundamental harmonic and combination bands.
The use of linear-in-frequency instruments results in a considerable expansion
of the high frequency end of the infrared region, resulting in an increased ability to
2929
resolve bands and define their positions. The place of absorption observed in the band
is rapidly articulated in form of wave number (cm-1) with respect to absorbed light.
The IR spectrum is the easy, quicker & often more reliable resources for
interoperating a sample to its division. It can also give different information on purity,
symmetry, structure, geometrical and structural isomers & H- bonding.
2.3.1 Anticipated Infrared Frequencies for Heterocyclised products based on
NTOH.
The present thesis comprises the study of following heterocyclized products:
2-(3-flourophenyl)-1,2,4-[3,2-b]-triazolo-Odz-6-thione aceto hydrazide (NTOH)
b) Schiff Bases of AOD
c) 2-Azetidinones
d) 4-Thiazolidinones
e) 2H-Pyrrole-2-Ones
f) 2-Pyrrolidinones
Hence, prior to characterize these compounds by IR spectroscopy it is
necessary to predict the anticipated frequencies of each moiety.
2-(3-flourophenyl)-1,2,4-[3,2-b]-triazolo-Odz-6-thione (NTOH):
NTOH is a heterocyclic compound. It is an aromatic compound thus it
provides the IR frequencies. The bands due to oxadiazole are at 990-1190cm-1 and
1620-1640cm-1 corresponds to C-O-C (str.) and C=N groups. The weak band at 1040
cm-1 is because of N-N of oxadiazole ring. The other band because of aromatic
fragments at 4-place are found at their respective place.
Schiff Bases:
3030
Acyclic unsaturated nitrogen compounds containing C=N bond is most
commonly encountered in oximes and Schiff’s bases. Both the classes absorb in the
region from 1690-1640 cm-1, usually less strongly than carbonyl compounds but the
oximes are distinguished by the presence of O-H stretching(free) absorptions between
3650 and 3600 cm-1 in dilute solution.
2-Azetidinones (β-lactams):
Lactams exhibits the following characteristic absorption bands in their spectra.
Lactams exhibit a strong N-H stretching bonded absorption in the solid state closer to
3200 cm-1 and a weaker band closer 3100 cm-1 resulted due to the grouping of N-H in-
plane bending and C=O stretching absorptions [5,6]. The carbonyl stretching vibration
absorbs near 1650 cm-1 in six or seven membered rings as in the case of acyclic trans
structure. Lactams (five membered ring lactams) absorb near 1750-1700 cm-1.
Unfused β-lactams absorb at 1760-1730 cm-1 while β -lactams fused to unoxidized
thiazolidine rings absorbed at 1780-1710 cm-1 [7,8].
Carbon-Nitrogen symmetrical stretching, Nitrogen-Hydrogen in-plane and out
plane bending, and N-H wagging vibrations: Cyclic mono substituted amide shows
no band in the area from 1600-1500 cm-1 similar to the 1550 cm-1 Carbon-Nitrogen-
Hydrogen in-plane bending band in the trans structure. The in-plane bending vibration
absorbs at 1490-1440 cm-1 for cis N-H & the vibration at 1350 cm-1 C-N stretching
[9]. There is much less interaction between these modes compared to the trans form.
The broad band closer to 800 cm-1 is because of N-H out-of-plane bending (wagging)
vibration appears.
3131
4-Thiazolidinones:
The carbonyl stretching vibration absorbs near 1650 cm-1 in six or seven
membered rings as in the case of acyclic trans structure. Thiazolidinones absorbs at
1730-1700 cm-1[10].
2-Pyrrolidinones:
Carbonyl stretching vibration around 1750-1710 cm-1 because of C=O. the
absorption at 1410 cm-1 because of C-N stretching vibration. N-H stretching vibration
between 3200-2400 cm-1 for saturated heterocycles such as pyrrolidinones and
piperidines. Heterocyclic systems exhibit C-H stretching bands in the usual region
3100-3000 cm-1[11,12].
2H-Pyrrole-2-ones:
Carbonyl group found at stretching vibration 1620-1685 cm-1. The stretching
vibration at 1410 cm-1 due to absorption for Carbon-Nitrogen single pi-bond. In non-
polar solvents it shows a very strong N-H stretching absorption within 3500 & 3450
cm-1. Heterocyclic systems shows C-H stretching vibrations in usual region n 3100-
3000 cm-1. Band because of C=C of the ring stretching around 1615-1565 cm-1. N-H
in-plane bending found closer to 1146 cm-1 and out-of-plane bending is found closer
to 561 cm-1[11,12].
2.4 Proton NMR Spectroscopy
Nuclear resonance (NMR) spectrum analysis is supplementary technique to IR
spectrum analysis to urge details data concerning structure of organic Compounds.
most generally studied nucleus is nucleon and so the technique is named PMR
spectrum analysis [92-93].
IR spectra provide data concerning the purposeful cluster whereas magnetic resonance
spectra give data concerning the precise nature of nucleon and its atmosphere. so this
method is additional helpful within the elucidation of associate degree Comp.. IR
3232
spectra of isomers might seem same however their magnetic resonance spectra can
markedly disagree.
The development of nuclear resonance was 1st rumored severally in 1946. Block and
organist were discovered this innovation and therefore they was awarded in 1952 for
discovery in physics for this. Since from this point, the NMR techniques are widely
useful in chemistry, advance biology for complex structure determination.
The nucleon resonance (PMR) spectrometry is that the most significant technique
used for the characterization of organic Compounds. It gives the information
regarding the proton and give exact idea about the structure. In other words it tells one
regarding completely different forms of environments of the chemical element atoms
within the molecule. PMR also give useful information regarding arrangement of
proton in space, i.e stereochemistry.
It is accepted that each one nuclei carry a charge. Thus, the nucleus behaves sort of a
little magnet. The momentum of the spinning charge is delineating in terms of spin
range (I). The magnitude of generated dipole is expressed in terms of nuclear torque
(µ).
The spinning nucleus of a atom (1H or proton) is that the simplest and is often
encountered in organic Compounds. The chemical element nucleus includes a
twisting, δ= 2.79268 and its spin range (I) is + ½. Hence, in associate applied external
flux, its torque might have 2 attainable alignments.
The orientation within which the torque is aligned with the applied flux is a lot of
stable (lower energy) than within which the torque is aligned against the sector (high
energy). The energy needed for flipping the nucleon from its lower energy level to the
upper energy level depends upon the difference in energy (∆E) between the two
states.
The substance placed in a magnetic flux of constant strength, so the spectrum
obtained similar to infrared or associate spectrum. Those radiations is absorbed b y
passing radiation of different frequency through the substance and perceptive the
frequency. It was found to be a lot of convenient that radiation frequency constant and
vary the strength of the flux. At some worth of the sector strength the energy needed
to flip the nucleon matches the energy of the radiation, absorption happens. Such a
spectrum is named a nuclear resonance (NMR) spectrum.
3333
Nuclear resonance (NMR) spectrum analysis is supplementary technique to IR
spectrum analysis to urge details data concerning structure of organic Compounds.
most generally studied nucleus is nucleon and so the technique is named PMR
spectrum analysis.
IR spectra provide data concerning the purposeful cluster whereas magnetic resonance
spectra give data concerning the precise nature of nucleon and its atmosphere. so this
method is additional helpful within the elucidation of associate degree Comp.. IR
spectra of isomers might seem same however their magnetic resonance spectra can
markedly disagree.
The development of nuclear resonance was 1st rumored severally in 1946. Block and
organist were discovered this innovation and therefore they was awarded in 1952 for
discovery in physics for this. Since from this point, the NMR techniques are widely
useful in chemistry, advance biology for complex structure determination.
The nucleon resonance (PMR) spectrometry is that the most significant technique
used for the characterization of organic Compounds. It gives the information
regarding the
3434
proton and give exact idea about the structure. In other words it tells one regarding
completely different forms of environments of the chemical element atoms within the
molecule. PMR also give useful information regarding arrangement of proton in
space, i.e stereochemistry.
2.4.1 13C NMR spectroscopy
In a current era, most of the structure determinations of organic molecules are
performed by 13CMR spectroscopy. It is more powerful tool to determine the exact
geometry of molecules.
In contrast to 1H spectra, it is not possible to determine the relative ratio of carbon
atoms in a Comp. by integration of the peak areas in the 13C FT-NMR spectrum.
There are two reasons for this. The first result results from the different relaxation
times of carbon atoms in different environments. This means that some atoms with
long relaxation times may still be partly saturated when the next pulse of radiation is
received, and the resulting absorption peak areas will not be proportional to the
different environmental nature of carbon atom. C-H bonds have longer relaxation
times and are therefore likely to give rise to peaks of lower intensity in the spectrum.
The second reason is due to the Nuclear Overhauled Effect (NOE). This is the
enhancement of some signals in the 13C spectrum as a result of the spin-decoupling
process which is used to produce the normal, noise-decoupled spectrum by removing
the interaction between carbon and hydrogen nuclei. The NOE is not the same for all
nuclei. The maximum effect is for carbon atoms with hydrogen attached. The
consequence is that carbon atoms without hydrogen attached appear without any NOE
enhancement. As a result of these two effects, it is often possible to identify b y
inspection, as a result of their lower intensity, those peaks in the 13C spectrum which
result from carbon atoms not attached to hydrogen, including those in aromatic rings
which carry a substituent.
A considerable amount of the data is available which correlates the position of
absorptions in the 13C NMR spectrum with the structure of an organic molecule, and it
is these imperial correlations which provide the main basis for the use of the
technique in structure determination. The values for the chemical shifts are normally
related to the tetramethylsilane carbon absorption, with positive values increasing to
lower field (corresponding to the scale in PMR spectroscopy). The vast majorit y
3535
of absorptions fall in a range of 200 ppm between the carbonyl absorptions at low
field and the methyl absorptions at high field.
The orientation within which the torque is aligned with the applied flux is a lot of
stable (lower energy) than within which the torque is aligned against the sector (high
energy). The energy needed for flipping the nucleon from its lower energy level to the
upper energy level depends upon the difference in energy (∆E) between the two
states.
The substance placed in a magnetic flux of constant strength, so the spectrum
obtained similar to infrared or associate spectrum. Those radiations is absorbed b y
passing radiation of different frequency through the substance and perceptive the
frequency. It was found to be a lot of convenient that radiation frequency constant and
vary the strength of the flux. At some worth of the sector strength the energy needed
to flip the nucleon matches the energy of the radiation, absorption happens. Such a
spectrum is named a nuclear resonance (NMR) spectrum.
3636
2.5 Mass Spectroscopy
It is unlikely that the laboratory organic chemist will be required to record
mass spectra of compounds produced in the laboratory as they will normally be
obtained through a centralized service.
Probably the most common use of mass spectrometry by the organic chemist
is for the accurate determination of molecular weight. A second important use is to
provide information about the structure of compounds by an examination of the
fragmentation pattern.
2.6 General Remarks for the Experimental Techniques
� All the compounds were characterized in terms of Melting points (oC) by open
capillary method and were uncorrected.
� The yields of all compounds reported are of crystallized. All solvents used
were distilled and dried. The cleanliness of the sample was tested by TLC.
� C, H, N and S elemental analysis of all prepared compounds were recorded on
Thermofinigen 1101 Flash elemental analyzer.
� IR data were observed in KBr pellets on Nicolet 760D spectrophotometer.
� CMR and PMR spectra were found on Bruker NMR spectro-photometer.
� LC-MS of selected one sample of each series has been carried out on LC-
MSD Trap-SL 01046 instrument using CH3CN solvent.
3737
SECTION – II
SYNTHESIS AND CHARACTERIZATION OF VARIOUS SCHIFF BA SES OF
NTOH
3838
Theoritical consideration:
Organic chemists are frequently facing the problem of characterizing and
ultimately elucidating the structure of organic compounds. The worker in the region
of natural product has the prospects of isolating such compounds from their sources in
a pure state and then determining their structure. On the other hand the synthetic
organic chemist encounters new or unexpected compounds in the course of
investigations.
All the synthesized are also characterized by its melting point and meting points were
detected by melting point apparatus. All the MPs were uncorrected.
The yields of all Compoundsreported are of crystallized. All solvents used were
distilled and dried. TLC was carried out to determine purity of the Compounds.
Column chromatography technique was employed using silica of 60-120 mesh.
Elemental analysis of all the Compoundswere recorded on Thermofinigen 1101 Flash
elemental analyzer for determining content of C, H, N and S contents.
Infrared spectra were recorded on Nicolet 760 spectrophotometer by preparing KBr
pellets.
1H and 13C NMR were measured on Bruker avance 400 MHz instrument. Chemical
shifts were measured in ppm. Solvent peak were used as a internal standard.
LC-MS of selected one sample of each series has been carried out on LC-MSD Trap-
SL 01046 instrument using CH3CN solvent.
The reagents, the reaction and the conditions of the reaction system are given in the
following scheme 2.1 as follows,
2.7. Synthesis of 2-(5-((naphthalen-1-yloxy)methyl)-1,3,4-oxadiazol-2-thioxo-
3(2H)-yl) acetohydrazide (NTOH).
2-(5-((naphthalen-1-yloxy) methyl)- 1,3,4-oxadiazole-2-thioxo (A) were prepared
by method reported in literature [13].
2-(5-((naphthalen-1-yloxy) methyl)- 1,3,4-oxadiazole-2-thioxo- (A) (0.01 mole)
and 0.01 mole chloro acetic acid in acetone (5 ml) were taken in round bottom flask [100
ml]. Then charge K2CO3 (0.005 mole) and mixture were refluxed for 5-8 hrs. The
3939
solution was drinkable through celite bed and filtrate solution was distilled out to get
crude solid product. This is in turn purified by dissolving in methanol and pure
product fall out by adding water. Which in turn filtered and washed with water and
dried for 12 hrs. at 500-550 C.
The NH2OH (0.02 M), some drops of H2SO4 and title compound (0.01 mol) were
mixed in ethanol. All the liquid mass was refluxed for time mentioned. After the
completion of reaction the solid product was fall out and filtered and dried [14].
2.7.1 Synthesis of Schiff bases of 2-(5-((naphthalen-1- yloxy)methyl)- 1,3,4-
oxadiazol-2-thioxo--3(2H)-yl) acetohydrazide (NTOH). The Schiff bases of NTOH
were synthesized by method reported [15].
Benzaldehyde derivative (2a-h) (0.01mole), NTOH (0.01mole) and ethanol
(20ml) were taken in a beaker [100ml]. The mixture was heated until a pure solution
was obtained. The pure solution was kept overnight when respective Schiff base fall
out which was filtered, washed by petroleum ether and air dried. The resultant Schiff
bases are designated as 2a-h and their details are shown as follows.
4040
O S
O N NH
(A)
2-(5-((naphthalen-1-yloxy) methyl)-2-thioxo-1,3,4-oxadiazole
ClCH2COOH
NH2NH2
O
O N N
S CH2CONHNNH2
(1)
2-(5-((naphthalen-1-yloxy) methyl)-2-thioxo- 1,3,4-oxadiazol-3(2H)-yl) acetohydrazide (NTOH)
Ar-CHO
O
O N N
S CH2CONHN CH Ar
Schiff bases
(2a-h)
OH NO2
Where, Ar = , ,
CH3 OMe
, , , OH
, , O
N
H3C CH3
Scheme 2.1
4141
RESULTS:
2.8 Experimental:
The synthesis of Schiff base derivatives by the earlier described method
resulted in products with good yields.
Compound 2a
O
O N N
S CH2CONH N
N'-arylene-2-(5-((methyl-1-yloxy)naphthalen)-Odz-2-acetohydrazide-3(2H)-thioxoyl)
Molecular Formula : C22H18N4O3S Elemental Analysis
Molecular Weight : 418 %C %H %N %S
Physical state : Off white crystals Theoritical 63.15 4.30 13.39 7.65
Melting point : 152-1540C Found 63.65 4.40 14.50 8.05
Percentage Yield : 87%
Compound 2b
O
O S
N N CH2CONH N
CH3
N'-arylene-2-(5-((methyl-1-yloxy)naphthalen)-Odz-2-acetohydrazide-3(2H)-thioxoyl)
Molecular Formula : C23H20N4O3S Elemental Analysis
Molecular Weight : 432 %C %H %N %S
Physical state : Off white crystals Theoritical 63.88 4.63 12.96 7.40
Melting point : 170-1720C Found 63.80 4.70 13.00 7.50
Percentage Yield : 88%
4242
Compound 2c
O
O N N
S CH2CONH N
OMe
N'-arylene-2-(5-((methyl-1-yloxy)naphthalen)-Odz-2-acetohydrazide-3(2H)-thioxoyl)
Molecular Formula : C23H20N4O4S Elemental Analysis
Molecular Weight : 448 %C %H %N %S
Physical state : Light yellow crystals Theoritical 61.60 4.46 12.50 7.14
Melting point : 160-1620C Found 61.70 4.50 12.50 7.20
Percentage Yield : 89%
Compound 2d
O
O N N
S OH
CH2CONH N
N'-arylene-2-(5-((methyl-1-yloxy)naphthalen)-Odz-2-acetohydrazide-3(2H)-thioxoyl)
Molecular Formula : C22H18N4O4S Elemental Analysis
Molecular Weight : 434 %C %H %N %S
Physical state : White crystals Theoritical 60.82 4.14 12.90 7.37
Melting point : 175-1760C Found 60.70 4.15 12.90 7.40
Percentage Yield : 90%
4343
Compound 2e
O
O
N N
S CH2CONH N
OH
N'-arylene-2-(5-((methyl-1-yloxy)naphthalen)-Odz-2-acetohydrazide-3(2H)-thioxoyl)
Molecular Formula : C22H18N4O4S Elemental Analysis
Molecular Weight : 434 %C %H %N %S
Physical state : Brown crystals Theoritical 60.82 4.14 12.90 7.37
Melting point : 180-1820C Found 60.75 4.15 12.95 7.45
Percentage Yield : 92%
Compound 2f
O
O N N
S CH2CONH N
NO2
N'-arylene-2-(5-((methyl-1-yloxy)naphthalen)-Odz-2-acetohydrazide-3(2H)-thioxoyl)
Molecular Formula : C22H17N5O5S Elemental Analysis
Molecular Weight : 463 %C %H %N %S
Physical state : Brown crystals Theoritical 57.02 3.67 15.12 6.91
Melting point : 180-1820C Found 57.00 3.70 15.15 7.00
Percentage Yield : 85%
Compound 2g
4444
N
CH3
O
O N N
S CH2CONH N
CH3
N'-arylene-2-(5-((methyl-1-yloxy)naphthalen)-Odz-2-acetohydrazide-3(2H)-thioxoyl)
Molecular Formula : C24H23N5O3S Elemental Analysis
Molecular Weight : 461 %C %H %N %S
Physical state : Brown crystals Theoritical 62.47 4.98 15.18 6.54
Melting point : 180-1820C Found 62.50 5.00 15.20 6.60
Percentage Yield : 87%
Compound 2h
O
O N N
S
O CH2CONH N
N'-arylene-2-(5-((methyl-1-yloxy)naphthalen)-Odz-2-acetohydrazide-3(2H)-thioxoyl)
Molecular Formula : C20H16N4O4S Elemental Analysis
Molecular Weight : 408 %C %H %N %S
Physical state : Light pink crystals Theoritical 58.82 3.92 13.72 7.84
Melting point : 120-1220C Found 58.90 4.00 13.80 7.90
Percentage Yield : 88%
4545
2.9 Characterization:
Compound 2a
O
O N N
S
CH2CONH N
Infrared Spectral Features in cm-1
3453 cm-1 N-H stretching of amide
1626 C=O stretching of CH2CONHN
1500 cm-1 stretching of C-H
1592 cm-1 stretching of CH=N
1H-NMR spectral Features (δ, ppm)
6.14-8.57 (m, Ar-H & Napthalene +
CH=N proton),
4.2 (s, 2H, OCH2)
2.93 (s, 2H, -CH2CONH)
Mass in m/z
Molecular ion peak was observed at 419.3
13C-NMR spectral Features (δ, ppm)
114-130 Benzene & naphthalene
114-165 oxadiazole
153 C=N
46
Fig. 2.1 IR Spectrum of Compound 2a
Fig. 2.2 1H-NMR Spectrum of Compound 2a
47
Fig. 2.3 13C-NMR Spectrum of 2a
48
Fig. 2.4 Mass Spectrum of 2a
49
Compound 2b
O
O N N
S CH2CONH N
CH3
Infrared Spectral Features in cm-1
3453 cm-1 N-H stretching of amide
1626 cm-1 C=O from CH2CONH
1500 cm-1 stretching of C-H
1592 cm-1 stretching of CH=N
1H-NMR spectral Features (δ, ppm)
6.14-8.57 (m, Ar-H & Napthalene +
CH=N proton)
4.2 (s, 2H, OCH2)
2.95 (s, 2H, -CH2CONH)
2.50 (s, 3H, CH3)
Mass in m/z
Molecular ion peak was observed at 433.3
13C-NMR spectral Features (δ, ppm)
114-130 Benzene & naphthalene
114-165 oxadiazole
153 C=N
50
51
Fig. 2.5 IR Spectrum of Compound 2b
2.6 1H-NMR Spectrum of 2b
52
Fig. 2.7 13C-NMR Spectrum of 2b
53
Fig. 2.8 Mass Spectrum of 2b
54
5555
Compound 2c
O
O
N N
S
C H 2 C O N H N
O M e
Infrared Spectral Features in cm-1
3453 cm-1 N-H of amide stretching
1626 cm-1 C=O of CH2CONH
1500 cm-1 C-H stretching
1592 cm-1 CH=N stretching
1250 cm-1 OCH3 stretching
1H-NMR spectral Features (δ, ppm)
6.14-8.57 (m, Ar-H & Napthalene +
CH=N proton),
2.95 (s, 2H, -CH2CONH)
4.20 (s, 2H, OCH2)
4.30 (s, 3H, OCH3)
Mass in m/z
Molecular ion peak was observed at 449.4
13C-NMR spectral Features (δ, ppm)
114-125 Benzene & naphthalene
114-160 oxadiazole
154 C=N
Compound 2d
O S O H
O N N
CH2 CONH N
Infrared Spectral Features in cm-1
3453 cm-1 N-H of amide stretching
1630 cm-1 C=O of CH2CONH
1500 cm-1 C-H stretching
1595 cm-1 CH=N stretching
3215 cm-1 OH stretching
1H-NMR spectral Features (δ, ppm)
6.14-8.57 (m, Ar-H & Napthalene +
CH=N proton),
11.2 (s, H, OH)
4.2 (s, 2H, OCH2)
2.98 (s, 2H, -CH2CONH)
Mass in m/z
Molecular ion peak was observed at 435.6
13C-NMR spectral Features (δ, ppm)
114-125 Benzene & naphthalene
114-160 oxadiazole
154 C=N
5656
Compound 2e
O S
O N N
CH2CONH N OH
Infrared Spectral Features in cm-1
3453 cm-1 N-H of amide stretching
1626 cm-1 C=O of CH2CONH
1500 cm-1 C-H stretching
1592 cm-1 CH=N stretching
3215 cm-1 OH stretching
1H-NMR spectral Features (δ, ppm)
11.2 (s, H, OH)
6.14-8.57 (m, Ar-H & Napthalene +
CH=N proton),
4.2 (s, 2H, OCH2)
2.92 (s, 2H, -CH2CONH)
Mass in m/z
Molecular ion peak was observed at 435.4
13C-NMR spectral Features (δ, ppm)
114-125 Benzene & naphthalene
114-160 oxadiazole
154 C=N
Compound 2f
O S
O N N
C H2 C O N H N
NO 2
Infrared Spectral Features in cm-1
3453 cm-1 N-H stretching of amide
1626 cm-1 C=O of CH2CONH
1500 cm-1 C-H stretching
1592 cm-1 CH=N stretching
2750 cm-1 N=O stretching of –NO2
1H-NMR spectral Features (δ, ppm)
6.14-8.57 (m, Ar-H & Napthalene +
CH=N proton)
4.23 (s, 2H, OCH2)
2.98 (s, 2H, -CH2CONH)
Mass in m/z
Molecular ion peak was observed at 464.2
13C-NMR spectral Features (δ, ppm)
114-125 Benzene & naphthalene
114-160 oxadiazole
154 C=N
Compound 2g
5757
C H3
O S N C H3
O N N
CH2 CO N H N
Infrared Spectral Features in cm-1
3453 cm-1 N-H stretching of amide
1626 cm-1 C=O of CH2CONH
1500 cm-1 C-H stretching
1592 cm-1 CH=N stretching
1050 cm-1 N-O stretching of –N-(CH3)2
1H-NMR spectral Features (δ, ppm)
6.14-8.57 (m, Ar-H & Napthalene +
CH=N proton)
4.25 (s, 2H, OCH2)
2.95 (s, 2H, -CH2CONH)
2.50 (s, 6H, -N(CH3)2 ) Mass in m/z
Molecular ion peak was observed at 462.5
13C-NMR spectral Features (δ, ppm)
114-125 Benzene & naphthalene
114-160 oxadiazole
154 C=N
Compound 2h
O S
O N N O
CH 2C ON H N
Infrared Spectral Features in cm-1
3453 cm-1 N-H stretching of amide
1626 cm-1 C=O of CH2CONH
1500 cm-1 C-H stretching
1592 cm-1 CH=N stretching
1592 cm-1 C=S stretching of ring
1H-NMR spectral Features (δ, ppm)
6.14-8.57 (m, Ar-H & Napthalene +
CH=N proton+ Furan)
4.2 (s, 2H, OCH2)
2.94 (s, 2H, -CH2CONH)
Mass in m/z
Molecular ion peak was observed at 409.2
13C-NMR spectral Features (δ, ppm)
114-125 Benzene & naphthalene
114-160 oxadiazole
154 C=N
5858
2.10 Results and Discussion:
All the Schiff bases of NTOH are in amorphous form and soluble in polar
organic solvents.
The C, H, N and S elemental of all the Schiff bases are found with the given
structures. The infrared spectral (Typical in Figs. 2.1 and 2.5) data are given in details
of each compound. All the spectra comprises the important IR spectral features of
aromatic, oxadiazole ring and –CH=N- group.
The 1H NMR spectra (Typical in Figs. 2.2 and 2.6) of all Schiff bases shows
the signal for aromatic proton and azo methine proton in the range of 6.1 to 6.8 δ
ppm.
While in 13C-NMR spectra (Typical in Figs. 2.3 to 2.7) signals are observed
which are in the region of 114 to 153 ppm. The assignment of signals is given
individually in each compound.
Finally LC-MS of one of samples spectrum shows peak of (m/z) is good
consistent with the theoretical molecular weight of 2a-h.
5959
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