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The basis of MRI scanning

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1 The basis of MRI scanning
17/04/2017 NMR SPECTROSCOPY The basis of MRI scanning

2 NUCLEAR SPIN Protons and neutrons can be regarded as spinning about their axis. In many atoms these spins are paired against each other and so the nucleus has no overall spin (e.g. 12C). In some atoms (e.g. 1H and 13C – an odd number of subatomic particles) the nucleus has an overall spin. A nucleus that spins generates a magnetic field i.e. behaves like a small magnet. The direction of the magnetic field depends which way the nucleus spins.

3 Applied magnetic field
NUCLEAR SPIN Usually the two possible spin states of the nucleus have the same amount of energy. However, in a magnetic field, the two spin states have different energies. Energy Magnetic field opposed to applied field Applied magnetic field Energy gap corresponds to frequency of radiowaves Magnetic field in same direction as applied field

4 Different “types of hydrogens”
The frequency absorbed is determined by the environment of the atoms giving the signal Atoms in different environments are sometimes said to be of different types To be of the same type hydrogen atoms must be indistinguishable Example ethane – all hydrogens identical, so one type Propane (2 types) Propan-1-ol (4 types) Notes

5 Example Draw a displayed formula of butanone and decide how many types of hydrogen there are This determines the number of peaks seen in the spectrum

6 butanone 3 3 2

7 EQUIVALENT H ATOMS In a spectrum, there is one signal for each set of equivalent H atoms. i.e. H atoms in an identical situation/environment The intensity of each signal being proportional to the number of equivalent H atoms it represents, so the hydrogen atoms are counted (area under peak) In a real spectrum the relative peak areas is given rather than actual numbers, so 2:1 = 4:2 = 6:3 etc – beware of this!

8 2 sets of equivalent H’s: ratio 6:2 (3:1)

9 For each of the following compounds, predict the number of signals and the relative intensity/area of the signals. a) methylpropene propene 2-chloropropane propanone methylamine ethyl propanoate 1,2-dibromopropane dimethylethyl propanoate but-2-ene

10 2 signals: ratio 6:2 (3:1) 1 signal 3 signals: ratio 2:1:3 2 signals: ratio 3:2 2 signals: ratio 6:1 4 signals: ratio 3:2:2:3

11 3 signals: ratio 2:1:3 3 signals: ratio 3:2:9 2 signals: ratio 6:2 (3:1)

12 SOLVENTS & CALIBRATION
Samples are dissolved in solvents free of 1H atoms, e.g. CCl4, CDCl3. A small amount of TMS (tetramethylsilane) is added to calibrate the spectrum. It is used because: its signal is away from all the others it only gives one signal it is non-toxic it is inert it has a low boiling point so is easy to remove

13 CHEMICAL SHIFT The d is a measure in parts per million (ppm) of how far the magnetic field required for absorption is shifted away from that for TMS. The d depends on what other atoms/groups are near the H – more electronegative groups gives a greater shift.

14 Butanone again – look at the chemical shift this time. See data sheet

15 Note that the signal from each type of hydrogen is seen in this case as a group of lines (still called a “peak”)

16 SPIN-SPIN COUPLING Each signal in the spectrum can be split into further lines due to inequivalent H’s on neighbouring C atoms. NOTE This splitting effect is not observed if adjacent H atoms are in an identical situation/environment Number of lines that the peak is split into = number of inequivalent H’s on neighbouring C atoms + 1 The n+1 rule

17 number of neighbouring inequivalent H atoms
SPIN-SPIN COUPLING signal singlet doublet triplet quartet appearance number of lines 1 2 3 4 number of neighbouring inequivalent H atoms relative size 1:1 1:2:1 1:3:3:1

18 butanone shift (d) assignment relative intensity coupling coupled to
1.0 CH3CH2 3 triplet CH2 2.0 CH3CO singlet 2.4 2 quartet CH3

19 butane shift (d) Assignment relative intensity coupling coupled to 1.3
CH2 2 quartet CH3 0.8 3 triplet

20 SUMMARY Number of signals -radiowave region Position of signals
Relative intensities Splitting how many different sets of equivalent H atoms there are information about chemical environment of H atom gives ratio of numbers of H atoms for the peaks how many H atoms on adjacent C atoms (alcohol OH, [aldehyde H] no splitting) IDENTICAL PROTONS DO NOT CAUSE SPLITTING

21 dimethylethyl propanoate but-2-ene
For each of the following compounds, predict the number of signals, the relative intensity of the signals, and the multiplicity (singlet, doublet etc) of each signal. a) methylpropene propene 2-chloropropane propanone methylamine ethyl propanoate 1,2-dibromopropane dimethylethyl propanoate but-2-ene

22 2 signals: ratio 6 : 2 (3 :1) s s 1 signal 3 signals: ratio 2 : 1 : 3 d m d 2 signals: ratio 3 : 2 t q 2 signals: ratio 6 : 1 d m 4 signals: ratio 3 : 2 : 2 : 3 t q q t

23 3 signals: ratio 2 : 1 : 3 t m d 3 signals: ratio 3 : 2 : 9 t q s 2 signals: ratio 6 : 2 (3 :1) d q

24 Use of deuterium based compounds in NMR
Deuterium is 12H 1.e. 1 proton and 1 neutron in the nucleus Deuterium does not give nmr signal (even number of sub-atomic particles) CDCl3 is one of the standard nmr solvents (the solvent does not interfere with the spectrum) D2O removes peaks due to O-H and N-H from the spectrum As a result of rapid H/D exchange

25 Past paper example

26 Mark scheme (i) carboxylic acid / COOH (protons) NOT just “OH protons” [1] (ii) D replaces protons on OH groups / OH protons are labile 􀀹 peak for (CO)OH protons disappears 􀀹

27 Further example

28 Further example continued

29 Protons on a benzene ring
Need to identify aromatic protons from chemical shift patterns No need to worry about their splitting patterns Signals can appear as one or two complex peaks

30 Example (past paper)

31 Mass spec mol. Ion peak at 86
Pentan-3-one Mass spec mol. Ion peak at 86


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