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1H and 13C NMR Spectroscopy in Organic Chemistry

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Presentation on theme: "1H and 13C NMR Spectroscopy in Organic Chemistry"— Presentation transcript:

1 1H and 13C NMR Spectroscopy in Organic Chemistry
Basics, Parameters, Internuclear Interaction and Applications Helmut Duddeck Institute of Organic Chemistry

2 Contents Basics The NMR Parameters Stereochemistry
Internuclear Connectivity Exercises

3 Basics

4 The NMR Experiment Excitation: DE = E1 – E0 DE = h · n = h · c/l
with c = n · l

5 Electromagnetic Spectrum

6 The Spin Some nuclei have a mechanical spin P, i.e. the sum
of all spins of the nucleons in the nucleus is not equal to zero. This results in a magnetic moment m. The relation between those properties is: m = g · P When such nucleus is placed into a static homogeneous magnetic field B0, is can adopt several orientations the number of which is given by the spin quantum number I. In the case of 1H and 13C: I = ½ i.e. those nuclei can adopt two orientations.

7 How Do Spins React to B0? The interaction between
two vectors is described by the vector product. This results in a rotation of m about B0: d m /dt = m x B0 ( Bloch equations)

8

9 How Do Spins React to B0? Precession w0 = 2 p n0 = - g · B0
(Larmor Equation) Bruker Avance 400 Hannover [ g(1H)  4 · g(13C) ]

10 Excitation of an Individual Spin
Boltzmann distribution: N1/N0 = e-DE/kT

11 M = Macroscopic magnetization
The Vector Model M = Macroscopic magnetization

12 Rotating Frame and Irradiation
a = g · B1 · tp

13 Longitudinal (Spin-Lattice) Relaxation, T1
dMz/dt = -(Mz – M0)/T1

14 Longitudinal Relaxation
M M0

15 Transversal (Spin-Spin) Relaxation, T2
dMx´/y´/dt = -Mx´/y´/T2 T2  T1

16 “Real“ T2 Times NMR Line Widths
1/T2* = 1/T /T2(inhom) NMR Line Widths w1/2 = 1/(2pT2*)

17 „Classical“ PFT-NMR Experiment

18 Pulse and FID resonance range

19 Transversal Magnetization My‘
Dn = n0 - n1 = 0 ; 900 pulse (p/2) y´-Magnetization decays exponentially.

20 Free Induction Decay

21 Fourier Transformation of an FID
FT of an exponentially decaying curve gives a Lorentzian. analytical form: However: the freq.-domain spectrum consists of two sections: (1) real part (see curve); (2) imaginary part)

22 Transversal Magnetization My‘
Dn = n0 - n1 > 0

23 FID as Function of Dn Dn = 15 Hz Dn = 65 Hz and 114 Hz, resp.

24 FID as Superposition

25 Digitization dwell time td
number of data points is mostly a multiple of 1 K (kilo) = = (nearly 1000)

26 Digital Resolution Examples: 13C NMR, resonance frequency 100.6 MHz,
typical d range of 250 ppm 250 ppm is ca Hz = 25 kHz, FID collected with 32 K data points; in the real spectrum 16 K = Digital resolution = 1.5 Hz/point (= ppm)! Good enough for chemical shifts but not for coupling constants. 1H NMR, resonance frequency MHz, typical d range of 10 ppm; 10 ppm is ca Hz = 4 kHz. FID collected with 64 K data points; in the real spectrum 32 K = Digital resolution = 0.12 Hz/point (= ppm)! Very good for chemical shifts but not for coupling constants: Precision > 0.2 Hz!

27 Spectral Window; Nyquist-Frequency
Given a data point train; <2 points per period => ambiguity !

28 Spectral Window; Nyquist-Frequency
Given a data point train; <2 points per period => ambiguity !

29 Spectral Window; Nyquist-Frequency
Given a data point train; <2 points per period => ambiguity !

30 Which is the Folded Signal?
Quadrature detection

31 Data Manipulation Akkumulation
Signal-to-noise ratio after n accumulations: S/N = n / n = n 13C signals of a phenyl group: NS = 4 NS = 16 NS = 64

32 Data Manipulation Exponential Multiplication
FID: FID + exponential multiplication:

33 Data Manipulation Exponential Multiplication

34 Data Manipulation Exponential Multiplication
13C signals of a phenyl group:

35 Data Manipulation Resolution Enhancement
FID and spectrum before (left) and after Lorentzian-Gaussian transformation (right)

36 Data Manipulation Resolution Enhancement
Example: 13C-Signal () of 1-trifluoromethyladamantane: plus Lorentz-Gauß- transformation from the original FID

37 Data Manipulation Resolution Enhancement
Sucrose mind the wiggles (apodization)!

38 Data Manipulation Truncation
What happens when FID are truncated after decaying to zero ? Signal is not affected and S/N ratio is improved.

39 Data Manipulation Truncation
What happens when FID are truncated before decaying to zero (apodization) ? Signal is affected by wiggles.

40 Data Manipulation Zero Filling
What happens when a fully decayed FID is supplemented by zeros (data points with zero information)? Better digital resolution without loss of signal information.


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