NMR Spectroscopy Lecture

basic H NMR Spectroscopy

1. Nuclear Magnetic Resonance
Spectroscopy

(
1
H NMR or PMR)
For M. Sc. I Chemistry
Shaikh Siraj Babulal

2. 1937 Rabi predicts and observes nuclear magnetic resonance
1946 Bloch, Purcell first nuclear magnetic resonance of bulk sample
1953 Overhauser NOE (nuclear Overhauser effect)
1966 Ernst, Anderson Fourier transform NMR
1975 Jeener, Ernst 2D NMR
1984 Nicholson NMR metabolomics
1985 Wüthrich first solution structure of a small protein (BPTI)
from NOE derived distance restraints
1987 3D NMR +
13
C,
15
N isotope labeling of recombinant proteins (resolution)
1990 pulsed field gradients (artifact suppression)
1996/7 residual dipolar couplings (RDC) from partial alignment in
liquid crystalline media
TROSY (molecular weight > 100 kDa)
2000s Dynamic nuclear polarisation (DNP) to enhance NMR sensitivity

5 Nobel prizes for NMR field
1944 Physics Rabi (Columbia)
1952 Physics Bloch (Stanford), Purcell (Harvard)
1991 Chemistry Ernst (ETH)
2002 Chemistry Wüthrich (ETH)
2003 Medicine (MRI) Lauterbur (University of Illinois in Urbana),
Mansfield (University of Nottingham)
NMR History
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3. NMR
•The NMR deals with the nucleus of the atom that
posses a magnetic moment.
•The nucleus being positively charged and spin
about its axis generate a magnetic field directed
along the axis of spin. Thus the nucleus behaves
as a tiny magnet.
•Nuclear magnetic resonance is defined as a
condition when the frequency of the rotating
magnetic field becomes equal to the frequency of
the processing nucleus.
Spinning charged
particle is a magnet
Spinning charged
particle is a magnet
3 SIRaJ/MSc/NMR

4. Sample at
Equilibrium
Radiation
Excited State
Spectrum
Relaxation
Observation
Spectroscopy
UV-Visible: Presence of chromophoric system / conjugation in the
molecules

IR Spectroscopy: Presence of Functional Groups in the molecules

1
H NMR Spectroscopy:
The number of different types of Hydrogens in the molecules
The relative numbers of different types of Hydrogens in the molecules
The electronic environment of different types of Hydrogens in the molecules
The “neighbours to the neighbours” of the functional group

These spectroscopic techniques are mutually complimentary and a
combination of these three-along with a Mass Spectroscopy form a
powerful device in the determination of structures of organic molecules.
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5. NMR Spectroscopy
•NMR uses energy in the radio frequency range.
•This energy is too low to cause changes in electron energy levels or
in the vibrations of molecules.
•NMR can cause changes in the spin of particles in the nucleus of
some atoms.
•Nuclear magnetic resonance (NMR) is a physical phenomenon in
which nuclei in a magnetic field absorb and re-emit electromagnetic
radiation.
•This energy is at a specific resonance frequency which depends on
the strength of the magnetic field and the magnetic properties of
the isotope of the atoms; in practical applications, the frequency is
similar to VHF and UHF television broadcasts (60–1000 MHz).
•NMR allows the observation of specific quantum mechanical
magnetic properties of the atomic nucleus.

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6. Nucleus
•The atomic nucleus is the small, dense region
consisting of protons and neutrons at the
center of an atom.
•Protons and Neutrons form the nucleus of the
atom, electrons orbit the nucleus in electron
shells.
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7. •All nucleons, that is neutrons and protons,
composing any atomic nucleus, have the
intrinsic quantum property of spin.
•The overall spin of the nucleus is determined
by the spin quantum number S / I.
•The spinning charged nucleus generates a
magnetic field.

7 SIRaJ/MSc/NMR

8. The nuclei of some atoms have a property called “SPIN”.
NUCLEAR SPIN
These nuclei behave as if they were spinning.
This is like the spin property of an electron,
which can have two spins: +1/2 and -1/2 .
Each spin-active nucleus has a number of spins defined by its spin quantum number, I.
….. we don’t know if they actually do spin!
8 SIRaJ/MSc/NMR

9. l
Nucleii
spin +charge
l
Nucleii
spin +charge
ll
Nucleii
spin +charge Spinning charged
particle is a magnet
Spinning charged
particle is a magnet Magnetic Properties of Nuclei The spinning of positively charged particle produces:
(1) Spin angular momentum or Spin quantum number (I)
(2) Magnetic moment (m) along the axis of spin
(3) Electric quadrupole moment (Q)
(as a result of non-spherical distribution of nuclear charge)
9 SIRaJ/MSc/NMR

10. The spin state of a nucleus is affected by an applied magnetic field
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11. Behavior of Magnetic Nuclei Randomly oriented nuclear
spins of equal energy in the
absence of any magnetic field 1
2
_
1
2
+
E
P
1
2
_
1
2
+
ElectromagneticRadiation in
R F range with energy E = Ep
Ho
Precisely oriented nuclear spins
in the presence of Magnetic field
For nuclei with spin I = ½
Two possible orientations
as per equation 2I + 1
In NMR, we are measuring the energy required for the flipping of the nucleus
11 SIRaJ/MSc/NMR

12. Nuclear spins are oriented randomly in the absence (a) of an external magnetic
field but have a specific orientation in the presence (b) of an external field, B
0
•Some nuclear spins are aligned parallel to the external field
–Lower energy orientation
–More likely
•Some nuclear spins are aligned antiparallel to the external field
–Higher energy orientation
–Less likely


Nuclear Magnetic Resonance Spectroscopy

13. In the presence of a strong magnetic field,
the tiny magnetic field due to spinning
charged particles aligns to be either with or
against the magnetic field.
13 SIRaJ/MSc/NMR

14. •More nucleons will be in the lower energy
state aligned with the magnetic field.
•A nucleon can absorb a quantum of energy in
the radio frequency range and align against
the magnetic field.
•It emits a radio frequency when it drops back
to its original position.
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15. NUCLEAR SPIN STATES - HYDROGEN NUCLEUS
+ 1/2 - 1/2
The two states
are equivalent
in energy in the
absence of a
magnetic or an
electric field.
+ +
The spin of the positively
charged nucleus generates
a magnetic moment vector, m.
m
m
TWO SPIN STATES
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16. Is all nuclei are NMR active?
•The angular momentum of spinning nucleus is described in terms of spin quantum no.I
•The spin quantum no. I is a characteristic constant of a nucleus, and is dependent on the
number of protons and neutrons.

•In general three rules apply to the nuclear spins.
1)Nuclei with odd mass number and odd or even no. of protons have half – integral spin
such as 1/2, 3/2, 5/2 etc.

2)Nuclei with even mass number and odd no. of protons have integral spin such as 1, 2, 3

3) Nuclei with even mass number and even no. of protons always have zero spin (Due to
pairing of oppositely directed spins in the nucleus)
(Mass Number:-the total number of protons and neutrons in a nucleus.)
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17. Requirements of nuclei to be NMR active
Three important characteristics:
o Nuclei should have Spin no. I > 0 and magnetic momemtum m > 0
o Nuclei should have even charge distribution that is nucleus should be
spherical in shape so as Q = 0.
o Nuclei should have high % of natural abundance
1
H,
13
C,
19
F and
31
P nuclei have I = 1/2 and m > 0
These nuclei are spherical in shape (even charge
distribution) and Q = 0
So observed by NMR technique.
1
H,
19
F and
31
P have high % abundance
12
C and
16
O nuclei are also spherical in shape Q = 0; but
I = 0 and m = 0
So non-magnetic and not observed by NMR
17 SIRaJ/MSc/NMR

18. Nucleus No. of
Proton
No. of
Neutron
Mass
No.
Spin No.
(I)
Natural
% Abundance
1
H 1 0 1 1/2 99.98
2
H 1 1 2 1 00.0156
12
C 6 6 12 0 98.80
13
C 6 7 13 1/2 01.108
14
N 7 7 14 1 99.635
15
N 7 8 15 1/2 00.365
16
O 8 8 16 0 99.95
17
O 8 9 17 5/2 00.037
19
F 9 10 19 1/2 100.00
29
Si 14 15 29 1/2 04.70
31
P 15 16 31 1/2 100.00
Nuclear Properties of Important Nuclei
The number of spin states is 2I + 1,
where I is the spin quantum number.
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19. Basic NMR Equation For proton spin no. I = ½. Therefore, there are (2I + 1) two possible orientations.
The energy of orientation is a product of magnetic moment m and strength of the applied
Field Ho (E = mHo).
At resonance:
h = 2 m Ho

= 2mHo / h
The Larmor Frequency equation is
rewritten as

=  Ho /2

Where  = 2.m / h.I
It is a proportionality constant
between m and I.
Also called as Gyro magnetic ratio.
It is constant for a particular nuclei
but different for different nuclei. 

H
O
E
2 = + m H
O
E
1 =  m H
O
Aligned with the field
Low  energy orientation
Aligned against the field
High  energy orientation
E = 2 m H
O
E = h
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20. Gyromagnetic ratio ()

related to the relative sensitive of the NMR signal
magnetic moment (m) is created along axis of the nuclear spin



where:
p – angular momentum
 – gyromagnetic ratio (different value for each type of nucleus)

IIh 
mm
 ==
2 pm=
In physics, the gyromagnetic ratio (also sometimes known as the magnetogyric ratio) of a
particle or system is the ratio of its magnetic moment to its angular momentum, and it is
often denoted by the symbol γ, gamma.
20 SIRaJ/MSc/NMR

21. The mechanism of absorption
(Resonance)
Nuclear Spin
Energy Levels
B
o
+1/2
-1/2
In a strong magnetic
field (B
o) the two spin
states differ in energy.
aligned
unaligned
N
S 21

22. THE “RESONANCE” PHENOMENON
•Absorption of energy by the spinning nucleus.
•When proton kept external magnetic field, it
align to magnetic filed and undergo precess
rotation.
•If we irradiate the sample with radio waves
(MHz) the proton can absorb the energy and be
promoted to the less favorable higher energy
state. This absorption is called resonance
because the frequency of the applied radiation
and the precession coincide or resonate.
22 SIRaJ/MSc/NMR

23. 23 SIRaJ/MSc/NMR

24. Precessional motion
Precession is a change in direction of the axis, but without a change in tilt.
The axis of the nuclear magnet is oriented
exactly parallel or anti parallel with applied
magnetic field, there will be a certain force by
the external field to so oriented it.
But because the nucleus is spinning the
effect is that its rotation axis draws out a
circle perpendicular to the applied field. This
motion is called precession (example is the
gyroscopic motion of the spinning top)
The precessional frequency of the nucleus
depends upon the strength of the applied
magnetic field and the nature of the nucleus.
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25. Precessional
orbit
Nuclear magnet
H
O
H The behavior of a nuclear magnet in a magnetic field
w
o
m
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26. a-spin states b-spin states
absorb E
release E
Signals detected by NMR
RF
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27. Absorption of Energy
B
o
+1/2
-1/2
+1/2
-1/2
E = h
E
Quantized ???
Radiofrequency
Applied
Field
Aligned
Opposed
27 SIRaJ/MSc/NMR

28. B
o
E
+ 1/2
- 1/2
= kB
o = h
degenerate
at B
o = 0
increasing magnetic field strength
THE ENERGY SEPARATION DEPENDS ON B
o
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29. Is all Hydrogen proton absorb or release same
amount of energy in the same magnetic field?
CH
3-CH
2-OH

is all H proton absorb at same frequency?
Magnetic field -same
Energy gap between to spin??
29 SIRaJ/MSc/NMR

30. The absorption frequency is not the same for all
1
H or
13
C nuclei
–Nuclei in molecules are surrounded by electrons
–Electrons set up tiny local magnetic fields that act in
opposition to the applied field, shielding the nucleus from the
full effect of the external magnetic field
–The effective field actually felt by the nucleus is the applied
field reduced by the local shielding effects

B
effective = B
applied – B
local
The Nature of NMR Absorptions
When an atom is placed in a magnetic field, its electrons circulate about the direction of
the applied magnetic field. This circulation causes a small magnetic field at the nucleus
which opposes the externally applied field 30
SIRaJ/MSc/NMR

31. Different types of protons precess at
different rates in the same magnetic field.
N
S CH
2C
O
CH
3
59.999995 MHz
59.999820 MHz
59.999700 MHz
h
60 MHz
To cause absorption of the
incoming 60 MHz the
magnetic field strength, B
o ,
must be increased to a
different value for each type
of proton.
B
o = 1.41 Tesla
Differences are very small,
in the parts per million range.
EXAMPLE:
31
SIRaJ/MSc/NMR

32. Instrumentation
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33. A Simplified 60 MHz
NMR Spectrometer (continuous wave Instrument)
Transmitter
Receiver
Probe
h
S N
RF
Detector
Recorder
RF (60 MHz)
Oscillator
~ 1.41 Tesla
(+/-) a few ppm
absorption
signal
MAGNET MAGNET
33 SIRaJ/MSc/NMR

34. Magnet Legs
NMR Magnet Cross-Section
34 SIRaJ/MSc/NMR

35. NMR Sample tube & Probe Coil
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36. Magnetic field and RF required to
hydrogen nuclei absorb such field
Magnetic field and Resonance Frequency required to hydrogen nuclei can be
calculated by Larmor equation
Nuclei T
-1
S
-1
MHz/T
1
H 26.75 x 10
8
42.58
13
C 6.73 x 10
8
10.71
ω
0 = ϒB
0
in a field (Bo) of 1.41T, the resonance
frequency of ¹H would be

(42.58 MHz/T) x (1.415T) = 60.0378 MHz.

i.e at magnetic field B0 1.41 T, the resonance
frequency (radio frequency radiation require
to change spin) for hydrogen is 60.03 MHz
Gyromagnetic tation (ϒ)
Or
 =  Ho / 2
36 SIRaJ/MSc/NMR

37. The energy difference between the two spin states depends on the strength of the
magnetic field
Energy

Applied Magnetic field B
0
14.092
7.046
1.41
β spin state
α spin state
60 MHz
300 MHz
600 MHz
37
SIRaJ/MSc/NMR

38. 1
H Vs
13
C
Magnetic field and Resonance frequency
38
SIRaJ/MSc/NMR

39. c. The
1
H NMR spectrum of toluene shows that it has two peaks because of methyl and
aromatic protons recorded at 60 MHz and 1.41 T. Given this information, what would be
the magnetic field at 400 MHz?
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40. NMR Sensitivity
But at a significant cost!
~$800,000 ~$2,00,000 ~$4,500,000
40 SIRaJ/MSc/NMR

41. Two ways of doing NMR experiment
Sweeping – change
magnetic field
Keep constant
frequency
Change the frequency
Keep magnetic field
constant
 =  Ho / 2
Commonly Used method
41 SIRaJ/MSc/NMR

42. NMR Signal (sensitivity)

•The applied magnetic field causes an energy difference between the
aligned (a) and unaligned (b) nuclei

•NMR signal results from the transition of spins from the a to b state

•Strength of the signal depends on the population difference between the a
and b spin states








•The population (N) difference can be determined from the Boltzmann
distribution and the energy separation between the a and b spin states:
N
a / N
b = e
E / kT
B
o = 0
B
o > 0
E = h 
a
b
Low energy gap
42
SIRaJ/MSc/NMR

43. Information from
1
H-NMR spectra:

1.Number of signals: How many different types of hydrogens in the
molecule.

2.Position of signals (chemical shift): What types of hydrogens.

3.The chemical shift (δ, in ppm) gives a clue as to the type of hydrogen
generating the peak (alkane, alkene, benzene, aldehyde, etc.)

4.Relative areas under signals (integration): How many hydrogens of
each type. (number of Hydrogens)

5.Splitting pattern: How many neighboring hydrogens.
43 SIRaJ/MSc/NMR

44. Chemical equivalent and non-
equivalent protons
•
1
H NMR spectroscopy determines how many
kinds of electronically nonequivalent
hydrogens are present in a molecule
•Chemically equivalent proton resonance at
same frequency and gives one signal peak.
•Numbers of peaks in NMR gives different sets
of protons
•Symmetric molecules have equivalent protons
on each side of symmetry

44 SIRaJ/MSc/NMR

45. Chemical Equivalence
 Chemically equivalent protons H
3C CH
3
O
O
H
3C CH
3H
3CO OCH
3
O
X Y Z
X, Y, and Z have one set of equivalent protons.
 Chemically non-equivalent protons
CH
3CH
2Cl CH
3CH
2OCH
2CH
3 CH
3CH
2OH

2 signals 2 signals 3 signals
45 SIRaJ/MSc/NMR

46. Examples on
Types of protons / sets of protons
46 SIRaJ/MSc/NMR

47. Symmetric nature
47 SIRaJ/MSc/NMR Cl
Cl
Cl Cl
Cl
Cl CH
3
CH
3
CH
3
CH
3
CH
3
CH
3 O
O
O
O

48. Spectra
An NMR spectrum is a plot of the magnetic field applied (or radio frequency
applied) against absorption.
A signal in the spectrum is referred to as a resonance.
The frequency of a signal is known as its chemical shift, δ
48 SIRaJ/MSc/NMR

49. Integration
•The process of excitation in NMR involves the flipping of
the nucleus. This process of transition and the probability of
the transition is same for all the protons, irrespective of the
electronic environment. As a result, the area under the NMR
resonance is proportional to the number of hydrogens which
that resonance represents.
•In this way, by integrating the different NMR resonance,
information regarding the relative numbers of chemically
distinct hydrogens can be found.
•The integrals will appear as a line over the NMR spectrum.
Integration only gives information on the relative number of
different hydrogens, not the absolute number.

49 SIRaJ/MSc/NMR

50. The area under each
1
H NMR peak is proportional to the number of
protons causing that peak
•Integrating (electronically measuring) the area under each peak makes it
possible to determine the relative number of each kind of proton in a molecule
•Integrating the peaks of 2,2-dimethylpropanoate in a “stair-step” manner
shows that they have 1:3 ratio, corresponding to the ratio of the numbers of
protons (3:9)
Integration of
1
H NMR Absorptions:
Proton Counting

51. Solvents for NMR
D
3COOD
2.02, 11.53

D
3CCOCD
3 2.05

D
3CCN 1.95

C
6D
6 7.20

CDCl
3
7.25

CD
2Cl
2 5.35

D
3C-SO-CD
3 2.50

F
3C.COOD
10-11

A satisfactory solvent should be
 It should be chemically inert
 It should not contain protons
 It should be non – polar and should have low – boiling point
 It should have low viscosity
51 SIRaJ/MSc/NMR

52. Scale
Scale

•Narrow NMR absorption range
•0 to 15  for
1
H NMR

52 SIRaJ/MSc/NMR

53. Requirements for a reference standard in NMR

A good standard should meet the following requirements:
•It should be chemically inert (non-reactive).
•It should give a single sharp line.
•It should be magnetically isotropic.
•It should have unique line position.
•It should be Miscible with organic solvents.
•It should be readily volatile to allow recovery of the compound.
TetraMethylSilane
Silicon is more electro-positive than carbon. Therefore, pushes
electron density towards carbon and thus to hydrogen-making
methyl protons strongly shielded. H
3C
Si
CH
3
C
CH
3
H
H
H
53 SIRaJ/MSc/NMR

54. Reference compound for chemical shift
TMS
• TetraMethylSilane (TMS) used as
reference compound or internal
standard for NMR
•It fulfill all the conditions
•it is the reference peak / calibration
peak for chemical shift.
•Peak of TMS is considered as 0.0 
•In NMR spectra is plotted by
considering TMS as 0.0  on scale

54 SIRaJ/MSc/NMR

55. Chemical Shift
•The chemical shift in absolute terms is defined by
the frequency / magnetic field of the resonance
expressed with reference to a standard
compound which is defined to be at 0 ppm.
•The change in resonance frequency (or field) is
very very low for proton i.e. ppm,
•The scale is made more manageable by
expressing it in parts per million (ppm) and
is independent of the spectrometer frequency.
55 SIRaJ/MSc/NMR

56. SIRaJ/MSc/NMR 56

57. Chemical shift are also expressed in  (ppm)



=
Shift in frequency from TMS (Hz)
X 10
6
Frequency of spectrometer (Hz)

 is dimensionless and is NOT PROPORTIONAL to Ho or Osc.
frequency.
 value is same in all the different instruments
Universal scale in NMR
Higher the value of chemical shift in Hz or   deshielded is the proton.
Lower the value chemical shift in Hz or   shielded is the proton.
Units of Chemical shift
57 SIRaJ/MSc/NMR

58. •Position on NMR chart at which a nucleus
absorbs
–The chemical shift of TMS is set as zero point
–Other absorptions normally occur downfield
–NMR charts calibrated using delta () scale
•1  = 1 part per million of operating frequency



–Chemical shift of an NMR absorption in  units is
constant, regardless of the operating frequency of the
spectrometer
Chemical shift (number of Hz downfield from TMS)
δ =
Spectrometer frequency in MHz
Chemical Shifts
58 SIRaJ/MSc/NMR

59. The NMR Chart
The downfield, deshielded side is on the left, and requires a lower
field strength for resonance
The upfield, shielded side is on the right, and requires a higher
field strength for resonance
The tetramethylsilane (TMS) absorption is used as a reference point
Chemical Shifts
59 SIRaJ/MSc/NMR

60. Low field (Downfield ) & High field (Upfield)
60 SIRaJ/MSc/NMR
Magnetic field increase
High field
Low field
More electron density,
Electron oppose the
external magnetic field
(shield) hence these
proton require higher
external field to come in
resonance
Less electron density or
anisotropic effect,
Electron not oppose the
external magnetic field
(deshield) hence these
proton require lower
external field to come in
resonance

61. Downfield and Up field
•The downfield, deshielded side is on the left, and requires a lower magnetic
field strength for resonance
•The upfield, shielded side is on the right, and requires a higher field strength
for resonance

•More the electron density – more is the shielding - up field - high field

•Less the electron density – more is the deshielding – downfield – low field
61 SIRaJ/MSc/NMR
Downfield
Upfield

62. Shielding
•Shielded mean that “A nucleus whose chemical shift has been
decreased due to more electron density, magnetic induction, or
other effects.”
•shielded proton is surrounded by electrons which oppose the
external magnetic field.
•Due to opposing of external magnetic field, it require high magnetic
strength to bring proton in resonance.
•Shielding decrease the  value i.e. require high field strength

SIRaJ/MSc/NMR 62

63. Deshielding
•Deshielding is the opposite of shielding.
•When we say that an atom is deshielded, we
mean that “A nucleus whose chemical shift
has been increased due to removal of electron
density, magnetic induction, or other effects.”
•In deshieded proton is not surrounded by
electrons or due to other effect
•Deshielding increase the  value ie require low
field strength
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64. Value chart
64 SIRaJ/MSc/NMR

65. Most
1
H NMR chemical shifts occur within the 0 to 10  range except
for carboxylic acid O-H absorptions which usually occur within the 11-
12  range
Chemical Shifts in
1
H NMR Spectroscopy

66. SIRaJ/MSc/NMR 66

68. Factor affecting chemical shift
•Electronegativity
•Conjugation
•Resonance effect Aromatic rings
•Diamagnetic Anisotropic effect
•Hydrogen bonding
•solvent effect-Polar and non polar solvent
68 SIRaJ/MSc/NMR

69. Electronegativity
•Electron withdrawing inductive effect is one of
the parameter that affects the chemical shift
•Stronger the electron withdrawing group –
decrease the electron density.
•As electron density decrease, there is low /
no opposing induced magnetic field.
•more is the deshielding

69 SIRaJ/MSc/NMR

70. Electron withdrawal causes NMR signals to appear at higher frequency (at larger  values)
When an atom is placed in a magnetic field, its electrons circulate about the direction of the applied
magnetic field.
This circulation causes a small magnetic field at the nucleus which opposes the externally applied field
Electronegative atoms pull the eletron from Hydrogens……………………………….
70 SIRaJ/MSc/NMR

71. SIRaJ/MSc/NMR 71

72. SIRaJ/MSc/NMR 72

73. Resonance effect
 Electron donating
resonance effect increases
electron density at the carbon
and in turn to hydrogen –
Shielding of proton.



Electron withdrawing
resonance effect decreases
electron density at carbon
and in turn to hydrogen –
Deshielding of proton. OCH
3
H
H
H
a
b
a-H-deshielded due to -I effect
b-H-shielded due to +M effect
OCH
3
H
H
H
a
b
C
H
H
H
a
b
O
CH
3
C
H
H
H
a
b
O
CH
3
a-H-deshielded due to small -I effect
b-H-deshielded due to strong -M effect
6.38
3.85
5.85
6.40
OCH
3
H
H
H
a
b
6.38
3.85
C
H
H
H
a
b
O
CH
3
5.85
6.40
73 SIRaJ/MSc/NMR

74. Conjugation or Resonance
74 SIRaJ/MSc/NMR O
a
b
H
H
Deshielded proton
Positive charge
High 

Not Deshielded proton
No Positive charge
Low  O
O

75. Explain following
observation
SIRaJ/MSc/NMR 75 a
b
O
H
H
shielded proton
Nigative charge
Low 
Not shielded proton
No negative charge,
-I effect, high  O O

76. SIRaJ/MSc/NMR 76
Conjugation or Resonance
Explain following observation

77. Resonance effect- Aromatic protons
 Electron donating resonance effect increases electron density at the carbon and
in turn to hydrogen – Shielding of proton.
Electron withdrawing resonance effect decreases electron density at carbon and
in turn to hydrogen – Deshielding of proton.

77 SIRaJ/MSc/NMR OR
6.77
7.15
6.82
7.15
6.77 7.26
7.26
7.26
7.26
7.26
7.26 N
+
O-
O
8.19
7.52
7.65
7.52
8.19

78. ED ED ED EW EW EW OCH
3 - 0.43 - 0.09 - 0.37
OH - 0.5 - 0.14 - 0.40
OAc - 0.2 - 0.02 -
NH
2 - 0.75 - 0.24 - 0.63
NMe
2
- 0.64 - 0.10 - 0.60
SubstituentOrtho Meta Para SubstituentOrthoMeta Para
NO
2 + 0.95+ 0.17+ 0.23
CHO
+ 0.58+ 0.21+ 0.27
CN + 0.27+ 0.11+ 0.30 Chemical Shift: Resonance effect
78 SIRaJ/MSc/NMR

79. Diamagnetic anisotropic effect
•Anisotropic induced magnetic field effects are
the result of a local induced magnetic field
experienced by a nucleus resulting from
circulating π electrons that can either be
paramagnetic when it is parallel to the applied
field or diamagnetic when it is opposed to it.
79 SIRaJ/MSc/NMR

80. SIRaJ/MSc/NMR 80 Shielded
Region
Shielded
Region
Deshieded
Region

+
+
Deshieded
Region

B
0
If Hydrogen proton come in this region
The induced magnetic field generated by
electrons is reinforce or same direction of
applied magnetic field (Bo).
Protons are deshielded.
Hence the magnetic strength required to
resonate these proton is lower by induced
magnetic field. Shift of these protons on
downfield or low field.
 is High

B
resonance = B
induced + (B
0- B
induced)
If Hydrogen proton come in this region
The induced magnetic field generated by
electrons is opposite direction of applied
magnetic field (Bo). Protons are shielded.
Hence the magnetic strength required to
resonate these proton is higher due to oppose
of induced magnetic field. Shift of these
protons on upfield or High field
 is low
B
resonance = (B
0+ B
induced) - B
induced
Induced magnetic field current

81. Alkene C=C-H
81 SIRaJ/MSc/NMR H
R
1
R
H
Shielded
Region
Shielded
Region
Deshieded
Region

+
+
Deshieded
Region

Olefinic Protons at  4.5-6.0 Circulation of electrons
perpendicular to Ho Induced Magnetic
Field Ho
It is observed in alkenes where the double bond is oriented perpendicular to the external field
with pi electrons likewise circulating at right angles.
The induced magnetic field lines are parallel to the external field at the location of the alkene
protons which therefore shift downfield to a 4.5 ppm to 7.5 ppm range

82. Alkyne -C≡C-H
82 SIRaJ/MSc/NMR H
R
Shielded
Region
Shielded
Region
+
+
Deshieded
Region

Deshieded
Region

Acetylenic Protons at  2.5-3.0 Ho Circulation of electrons
perpendicular to Ho Induced Magnetic
Field
Alkyne protons by contrast
resonate at high field in a 2–
3 ppm range. For alkynes the
most effective orientation is
the external field in parallel
with electrons circulation
around the triple bond. In this
way the acetylenic protons are
located in the cone-shaped
shielding zone hence the
upfield shift

83. SIRaJ/MSc/NMR 83

84. Benzene ring protons (=6.5-8.0)
84 SIRaJ/MSc/NMR
In benzene rings there are six pi electrons
The protons in aromatic compounds are shifted
downfield even further with a signal for benzene at
7.73 ppm as a consequence of a diamagnetic ring
current.

85. SIRaJ/MSc/NMR 85

86. Aldehydes -CH=O
86 SIRaJ/MSc/NMR

87. Other protons due to anisotropic
effect
87 SIRaJ/MSc/NMR

88. H
C
H
O
H
O
H
H
H
CH
3
CH
3
H
H
H
H
H
H
H H
H
H
H
H
HH
H
H
H
H
H OH HO H
HH
O
O
O
O
OCH
3
H
3CO H
H
3CO
H
O
O
O
O
OCH
3
H
3CO H
H
H
3CO
 8.99
 6.42  5.48
 (Ring) 8.14 - 8.64
 (CH
)  4.25
 3.53  3.75
 (Ring) 7.27; 6.95
 (CH
2)  0.51
  0.42  .42
 (H outer) 9.28  (H inner) 2.99
   0 88 SIRaJ/MSc/NMR

89. SIRaJ/MSc/NMR 89

90. Hydrogen bonding

SIRaJ/MSc/NMR 90

91. Spin Spin splitting
•The 1H-NMR spectra, each set of protons generates a
single NMR signal. In fact, the 1H-NMR spectra of most
organic molecules contain proton signals that are 'split'
into two or more sub-peaks. Rather than being a
complication, however, this splitting behavior actually
provides us with more information about our sample
molecule.
•The source of signal splitting is a phenomenon
called spin-spin coupling, a term that describes the
magnetic interactions between neighboring, non-
equivalent NMR-active nuclei.
91 SIRaJ/MSc/NMR

92. 92
Spin-Spin Splitting in
1
H NMR Spectra
Peaks are often split into multiple peaks due to magnetic interactions between
nonequivalent protons on adjacent carbons, The process is called spin-spin splitting.
The splitting is into one more peak than the number of H’s on the adjacent carbon(s), This
is the “n+1 rule”
The relative intensities are in proportion of a binomial distribution given by Pascal’s
Triangle
The set of peaks is a multiplet (2 = doublet, 3 = triplet, 4 = quartet, 5=pentet, 6=sextet,
7=heptet…..)

93. SIRaJ/MSc/NMR 93

94. Spin Spin Coupling / splitting
•In the simplest case we expect to see a single peak for each type of
proton in a molecule. But consider what happens if a proton that
we are looking at (HA) is near another nonequivalent proton (HB).
In half of the molecules the HA proton will be adjacent to an HB
aligned with the field and in the other half the HA proton will be
adjacent to an HB aligned against the field. Thus, half the HA's in
the sample will feel a slightly larger magnetic field than they would
in the absence of HB and half will feel a slightly smaller magnetic
field. Thus, we will observe two absorptions for the HA proton. (Of
course we would also observe the same thing for HB.) This splitting
of the HA resonance into two peaks is termed "spin-spin coupling"
or "spin-spin splitting" and the distance between the two peaks (in
Hz) is called the "coupling constant" (usually represented by the
symbol J). The spin-spin coupling is transmitted through the
electrons in the bonds and so depends on the bonding relationship
between the two hydrogens.
SIRaJ/MSc/NMR 94

95. SIRaJ/MSc/NMR 95

96. Rules of coupling

The number and nature of multiplets in NMR

Equivalent protons do not couple with each other.
A hydrogen does not cause splitting with itself, but only with
neighboring hydrogens
If you have N number of magnetically equivalent hydrogens causing
the splitting then you have N+1 peaks in the spectrum
Must be within a short distance to allow the small magnetic field of one
hydrogen to affect the magnetic field around another
Splitting is observed if the protons are separated by more than three s
bonds
Spliting of signal depend on neighboring proton
Signal split according to 2nI+1 where I = ½ for proton ie by n+1
Where n = number of neighboring proton

96 SIRaJ/MSc/NMR

97. N+1 rule
SIRaJ/MSc/NMR 97

98. SIRaJ/MSc/NMR 98

99. 05/03/2018 Chapter 19 99

100. Signal
•Signal full form (n+1) n
S singlet one line 0
d doublet two line 1
t triplet three line 2
q quartet four line 3
quent. Quintet five line 4
Sextet sextet six line 5
Sept. Septet seven line 6
m multiplet mix or more line ?
bs broad singlet one broad line 0
100 SIRaJ/MSc/NMR

101. Intensity of splitting
101 SIRaJ/MSc/NMR

102. Pascal’s Triangle

Relative intensities of first order multipletes 1
1 1
1 2 1
1 3 3 1
1 4 6 4 1
1 5 10 10 5
1 6 15 20 15 6 1
1 7 21 35 35 21 7 1
1 8 28 56 70 56 28 8 1
1
n = number of equivalent nuclei Relative Intensity
0
1
2
3
4
5
6
7
8
102 SIRaJ/MSc/NMR

103. C C
H
A
No adjacent proton
C C
H
AH
B
One adjacent non-equivalent
proton
C C
H
AH
B
H
B
Two adjacent nonequivalent
protons
C C
H
AH
B
H
B
H
B
Three adjacent non-equivalent
protons
Structure Spin States
Signals 103 SIRaJ/MSc/NMR

104. Broad peak in NMR (bs-broad singlet)
•In NMR spectra, we get a sharp peak line for
splitting as s,d,t etc
•But some peaks are not sharp
•They show as broad peak
•Protons which are exchangble shows such
peaks or protons which attached to –OH, -NH
2
104 SIRaJ/MSc/NMR

105. Protons Bonded to Oxygen and Nitrogen
These protons can undergo proton exchange
They always appear as broad signals
The greater the extent of the hydrogen bond, the greater the chemical shift
105 SIRaJ/MSc/NMR

106. SIRaJ/MSc/NMR 106
Protons Bonded to Oxygen and Nitrogen will
not spilt even they have neighboring proton

107. SIRaJ/MSc/NMR 107

108. 05/03/2018 Chapter 19 108
Spectra Involving Chemical Exchange Processes
The observed signal is the result of the
weighted average of the nucleus in its
different magnetic environments.

Fast exchanges show up as sharp
signals.

Exchanges on the NMR timescale
(“intermediate”) show up as broad
signals. (presence of acid/base catalyst,
temperature, nature of the solvent, etc.)

Slow exchanges will show two separate
lines.

109. D
2O exchangeable protons
•Protons attached to O, N, S are resonating anywhere between 1 to 15 .
•The position depends on a) substrate b) solvent c) concentration d)
temperature.

•The best method to detect these protons is to re-run the spectra on
addition of drop of D
2O, wherein these protons will change their position.
109 SIRaJ/MSc/NMR

110. 1
H NMR spectra of cyclohexane-d
11 at various temperatures H
H
H
H
axial
equatorial
axial
equatorial
the rate of
chair–chair
conversion is
temperature
dependent
110 SIRaJ/MSc/NMR

111. Coupling constant (J)
•The coupling constant (J) is the distance
between two adjacent peaks of a split NMR
signal in hertz
•Generally fall into range 0 to 18 Hz
111 SIRaJ/MSc/NMR

112. SIRaJ/MSc/NMR 112

113. Types of coupling

SIRaJ/MSc/NMR 113

114. 114
Typical coupling constant

115. Vicinal coupling
115 SIRaJ/MSc/NMR

116. 05/03/2018 Chapter 19 116
An important factor in vicinal coupling is the angle a between the C-H
sigma bonds and whether or not it is fixed.
Coupling is a maximum when a is 0° and 180°; it is a minimum when a
is 90°

117. Geminal coupling
•Nonequivalent H on the same carbon will
couple and cause signal splitting, this type
of coupling is called geminal coupling

117 SIRaJ/MSc/NMR

118. Cis and Trans coupling
118 SIRaJ/MSc/NMR

119. Aromatic coupling constant
119 SIRaJ/MSc/NMR
8 Hz



2 Hz



Not coupling

120. Heterocyclic coupling constant
120 SIRaJ/MSc/NMR

121. Write the splitting pattern in given compounds
121 SIRaJ/MSc/NMR O
O
O
O
O
O
O O
O
O O
O
Cl
Cl H
CH
3
H
H
3C
O
H
H
H
H
3C
O

122. How will differentiate following pair by PMR

SIRaJ/MSc/NMR 122

123. Assign the signals for following compounds

SIRaJ/MSc/NMR 123

124. Deduce the structure from following data

SIRaJ/MSc/NMR 124