special one dimensional, and two …...two aromatc rings for 7 index of hydrogen deficiency; one...
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SPECIAL ONE DIMENSIONAL, AND TWO DIMENSIONAL NMR
A method which simplifies NMR spectrum
- Determine the exact frequency of HA or HX- Irradiate the system at the resonance frequency of HAinduces transitions between the two spin states of HA- Signal for HA disappears- HX can not distinguish the two spin states of HAand ‘sees’ a time average orientation of HA and a singlet for HX appears instead of a doublet.
A
B
Useful to simplify complex spectra and identify coupling partners
Signal for HA disappears
Signal for HX disappears
CHO
CH3
dd, H2
d, H3qdd
dqd
dd
H3qd, H2
qddqd
Only the threeMethyls can beidentified
1
2
3
4,56,7
8,9 10
R4C > R3CH > R2CH2 > RCH3
g-steric effectis shielding
Broad Band 1H decoupled 13C NMR Spectrum
Entire 1H range is irradiated as the 13C is observed
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Off Resonance Decoupled 13C Spectrum
Irradiation if 1H out side but near its resonance frequency (1000-3000 Hz)2J and above coupling removed1J coupling constant reducedPeak height increased
DEPT/INEPT SPECTRA
However, using DEPT/INEPT spectra we can ascertain how many protons are attached to each carbon.
The standard 13C NMR spectra are proton broadband decoupled.Each non-equivalent carbon appears as a single peak
DEPT (Distortionless Enhancement by Polarization Transfer)
INEPT (Insensitive Nuclear Enhancement by Polarization Transfer)
Multiplicity can be obtained from: 1) 1H Coupled 13C NMR Spectrum2) Off Resonance Decoupled 13C Spectrum3) DEPT/INEPT Spectrum
Run first the normal Broad band 1H decoupled13C NMR spectrum
1
2
3
4,56,7
8,9 10
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INEPT SPECTRUM OF CAMPHOR
Quaternary signals are not observed5
13C NMR SPECTRUM OF IPISENOL (75 MHz, CDCl3)
9
10
sp2 hybridized carbon atoms
sp3 hybridized carbon atoms
CDCl3
DEPT SPECTRUM OF IPSENOL
13C NMRALL SHOWN
↑ CH,CH3
↓ CH2
↑ CH
6
CDCl38,93,5
74 2 1,10
10
9
C
TWO DIMENTIONAL NMRThis is actually a misnomer because the plot is3-dimensional with the tops of the signals cut off to yield a 2-D contour plot.
HOMONUCLEAR CORRELATION SPCECTROSCOPY (H,H-COSY)
1D 1H NMR spectra are shown on both axesHelps to identify coupling partners2D contours are shown as diagonal peaks on a diagonal line at the intersection points when lines are drawn from peaks in the 1D spectra.Where coupling occurs among nuclei,contours (cross peaks, correlation peaks) occur as pairs outside the diagonal line.
1H NMR spectrum of ethyl acetate
2H3H3H
CH3 O
O
CH3
HH
Diagonal line
Diagonal peak
Cross peak
Cross peak(correlation peak)
CH3 O
O
CH3
HH
12
3
4.654.28 4.00
3.96 3.65 3.42
s
C13H12O310
.23
1H NMR spectrum (CDCl3, 300 MHz)
2.75
2.
64
17.3
3
CHCl3
7.49
07.
463
7.43
7
6.84
86.
845
7.05
77.
054
6.97
46.
971
7.08
47.
081
6.87
76.
819
1H NMR spectrum (CDCl3, 300 MHz)
1H NMR spectrum (CDCl3, 300 MHz)
2.74
6
2.64
12.
642
13C NMR spectrum (CDCl3, 75 MHz)20
4.91
8
32.1
75
25.2
29
168.
568
158.
319
13C NMR spectrum (CDCl3, 75 MHz)13
8.33
6
133.
259
132.
735 12
1.83
9
117.
452
113.
605
112.
962
111.
139
COSY spectrum
COSY spectrum
C13H12O3
[(2X13)+2]-12
2= 16
2= 8
Two aromatc rings for 7 index of hydrogen deficiency;one double bond for 1 index of hydrogen deficiency
Accounts for 10 C atoms
C=O (d 204.9) from 13C NMR2XAr-O- (d 168.6 & 158.3) from 13C NMR
2XCH3: dC 32.2 & 25.2; dH 2.75 &2.64 from NMR
C13H12O3
OH or COH10.230
1H NMR spectrum (CDCl3, 300 MHz)
2XCH32.75 & 2.64
17.3
31
CHCl3
HH
HOH
A B
AM
X
AMX spin system
8.1 Hz 7.8 Hz
0.9 Hz
8.1 Hz0.9 Hz7.
490
7.46
37.
437
6.84
86.
845
7.05
77.
054
6.97
46.
971
7.08
47.
081
6.82
26.
819
1H NMR spectrum (CDCl3, 300 MHz)
7.490-7.463=0.027ppm=0.027X3008.1 Hz
7.084-7.057=0.027ppm=0.027X3008.1 Hz
7.463-7.069 =0.394x300=118.2/8.1=14.527.069 – 6.835 =0.234x300=70.2/0.9=78
OH
HH
H
HH
HOH
A B
7.46 (t, J = 8 Hz)
6.86 (dd, J = 8, 1 Hz)
7.07 (dd, J = 8, 1 Hz)
CH3
OCH3
H
X
X
XX
J = 0.6 HzB
C=O 2XAr-OH
CH3
O
Ar-CH3
4X Ar-H
HH
HOH
HOH
CH3
COCH3A B
4X Ar --C
HH
HOH
HOH
CH3
COCH3A B
OH OHCH3
H
CH3 O
OH OH
HCH3
CH3
O
OH OH
CH3
O
CH3
C=O at d 204.9 ppm
No conjugation with aromatic ring
OH OH
CH3
CH3 O
1H NMR signals at d10.23 (s)17.33 (s)
OH OH
CH3
O
HCH3
HH
H
coupling
C=O at d 204.9 ppm:pushed out of plane;no conjugation with the ring
H,H-COSY Spectrum
OH OH
CH3
O
HCH3
OH OH
CH3
O
HCH3
HH
H
10.23 (s)17.33 (s)
2.75 (s)
2.64 (d, J =0.6 Hz )
OH OH
CH3
O
HCH3
HH
H
10.23 (s)17.33 (s)
2.75 (s)
2.64 (d, J =0.6 Hz )
6.97 (br d or m)7.07 (dd, J = 8.1, 0.9 Hz )
6.83 (dd, J = 8.1, 0.9 Hz )
7.46 (t, J = 8.1 Hz )
OH OH
CH3
O
HCH3
HH
H 1
2
45
8
9
10 36
7 11
13
12
1H,13C-COSY (HETROCOSY, HETCOR)1D 1H NMR spectrum is shown on one axis.1D 13C NMR spectrum is shown on the other axis.1J coupling correlation peaks (cross peaks) are shownat the intersection of 1H and 13C peaks.Helps to assign 1H data if 13C value is known. or to assign 13C data if 1H value is known.NO diagonal peaks are shown here.The modern method for observing correlation between1H and 13C peaks are called HMQC and HSQC(Heteronuclear Multiple Quantum Coherence).The sensitivity of 13C nuclei is increase 64 times.HSQC (Heteronuclear Single Quantum Coherence)HSQC better resolution along 13C axis, but the experiment involves more complex pulse sequence.
13
12
CD(H)Cl3
7
45
6
Quaternary carbon atoms can not be assigned from HMQC (or HSQC) spectrum
13127456
CHCl3
OH OH
CH3
O
HCH3
HH
H ?
?
121.8117.5
?
?
? ?
132.7
111.1 ?
25.2
32.1
13C ASSIGNMENT FROM HMQC SPECTRUM
LONG RANGE H,C-COSY SPECTRUMYields information on all kinds of carbon atoms,including quaternary carbons.
The term long range in H-C coupling applies for 2JCH and above.1JCH =125-250 Hz,2JCH is between -6 to 65 Hz
In the long range H,C-COSY, the experiment is optimized to observe only long range coupling.mainly 2JCH and 3JCHDirect C-H coupling may not entirely be eliminated.
NO diagonal peaks
HMBC (Heteronuclear Multiple Bond Connectivity).
11
134
1
OH OH
CH3
CH3 O
HX813
12
X X
12
HMBC (Heteronuclear Multiple Bond Connectivity)8-OH
8
103
6 547
6
45
7 2,9
Optimized for J=10 Hz
12 13
OH OH
CH3
O
HCH3
HH
H
HMBC CORRELATIONSOH OH
CH3
CH3 O
OH OH
CH3
O
HCH3
HH
H 168.6
113.6
121.8117.5
158.3
113.0
138.3 133.2
132.7
111.1 204.9
25.2
32.1
17.33 (s)
C=O at d 204.9 ppm
10.23 (s) Not observed
SCoAO
O
O O O O
O
OH OH
CH3
O
CH3
It is a natural product and the structure should be biogenetically explained
THE NUCLEAR OVERHAUSER EFFECT (NOE)
Spin-spin coupling takes place through bonds.The information is relayed by bonding electrons,leading to signal splitting.Magnetic nuclei can also interact through space,but the interaction does not lead to signal splitting.For protons close in space (2-4Å),when one is irradiated at its resonance frequencythe signal intensity of the other will either,increase (most of the time) or decrease.This is called the Nuclear Overhauser Effect (NOE)NOE falls rapidly as the inverse sixth power of distance between two nuclei.
1H COUPLED 13C NMR SPECTRUM
DOUBLE RESONANCE 13C NMR SPECTRUM
AN INCREASE IN INTENSITY IS DUE TO:i) Collapse of multiplets into singletsii) Nuclear Overhauser Effect (NOE)
Higher noise level
Lower noise level
Irradiation of protons increases the intensities of carbons in the neighborhood
APPLICATION
1H NMR spectrum of dimethylformamideThe methyl protons appear as two singlets at 20ºC
H N
O
CH3
CH3H N
+
O
CH3
CH3
A B
As the temperature gradually increased the two singlets coalesce into one singlet
H N
O
CH3
CH3
H-C=O
N+
CH3
CH3
How can we assign these two signals at room temp.?
H N+
O
CH3
CH3
B
Cis-CH3
trans-CH3
H-C=O
N+
CH3
CH3
a a
a b b a
b b1
4
2
3
H1
H2
W0W2Irr.
Irradiation of H1 (2→1,4→3)Population at levels 2 and 4 will be reducedPopulation at levels 1 and 3 will be increasedEquilibrium state is disturbed and relaxation (W) will take placePath W2 increases the population of 4 and decrease 1Population in 4 higher than 2 and 3 higher than 1Signal intensity of H2 will increase (Positive NOE)
H1 H2 -D
-D
+D
+D
SOURCE OF NOE
Path W0 increases the population of 2 and decrease 3population in 4 lower than 2 and 3 lower than 1Signal intensity of H2 will decreased (negative NOE)
Path W0 increases the population of 2 and decrease 3population in 4 lower than 2 and 3 lower than 1Signal intensity of H2 will decreased (negative NOE)
Relaxation by W2 is preferred by molecules with molecular weight between 100-400Relaxation by W0 is preferred by large molecules with molecular weight above 600Molecules with molecular weight between 400-600 may not show NOE, because both pathways take place, cancelling each other
NOE enhancement can reach up to 200%in 1H decoupled (broad band) 13C NMR spectra.In 1H NMR the maximum enhancement is 50%But usually between 1-20%.NOE is weak in CH3 group because each H can be relaxed by the other two nuclei.NOE is most easily detected by methine groups.
NOEs can be measured by integrating signals with the irradiation on and off, and measuring the difference in integration values.This can be measured if the enhancement is above 10%.
NOE DIFFERENCE SPECTRANOEs are more easily detected by subtracting in a computerThe normal spectrum from a spectrum taken with the irradiation signal on.All the unaffected signals simply disappear.The enhancement will be shown, and alsoan intense negative signal at the irradiating frequency.
H1 H2 H1 H2 H1 H2
=minus
NOE NOE differenceNormal spectrumH3 H4H4H3
Me
Me Me O
H
H
Me
H H
H
H
HH
1
2
34
5
67
8
910
Irr.NOE 5.5% 12.9%
irr2.9%
7.2%
5.0%
9.8%irr
8.7%
5.2%
S-cis rotamer
Me
Me Me CH3
H
H
O
H H
H
H
HH
More prominent rotamer
S-trans rotamer
Me
Me Me O
H
H
Me
H H
H
H
HH
S-cis rotamer
NUCLEAR OVERHAUSER AND EXCHANGE SPECTROSCOPY (NOESY)
NOE in two dimension. In NOESY The NOE between all protons can be observed simultaneously.NOESY resembles COSY, 1D 1H NMR spectrum is shown on one axis.1D 1H NMR spectrum is shown on the other axis.Diagonal peaks occur.Spatially close protons can be seen as a cross peaks.
abc
Me
Me Me O
H
H
Me
H H
H
H
HH 1
2
34
5
6
78 9 10
3, 2
From NOESY Spectrum
abc
Me
Me Me O
H
H
Me
H H
H
H
HH 1
2
34
5
6
78 9 10
3
4
1
2
3
4
1
2
3
4
1
2
+ve J -ve J -ve J
3+41+212 214 3 43
+VE AND –VE J VALUES
+ve J
1H 13C 13C 13C
AA
A
BB
BCC
C
DD
D