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preface to fifteenth edition

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SPECTROSCOPY 7.89<br />

7.7 NUCLEAR MAGNETIC RESONANCE<br />

TABLE 7.41<br />

Nuclear Properties of the Elements<br />

In the following table the magnetic moment is in multiples of the nuclear magne<strong>to</strong>n N (eh/4Mc) with<br />

diamagnetic correction. The spin I is in multiples of h/2, and the electric quadrupole moment Q is in multiples<br />

of 10 28 square meters. Nuclei with spin 1<br />

⁄2 have no quadrupole moment. Sensitivity is for equal numbers of<br />

nuclei at constant field. NMR frequency at any magnetic field is the entry for column 5 multiplied by the value<br />

of the magnetic field in kilogauss. For example, in a magnetic field of 23.490 kG, pro<strong>to</strong>ns will process at 4.2576<br />

23.490 kG 100.0 MHz. Radionuclides are denoted with an asterisk.<br />

The data were extracted from M. Lederer and V. S. Shirley, Table of Iso<strong>to</strong>pes, 7th ed., Wiley-Interscience,<br />

New York, 1978; A. H. Wapstra and G. Audi, “The 1983 A<strong>to</strong>mic Mass Evaluation,” Nucl. Phys. A432:1–54<br />

(1985); V. S. Shirley, ed., Table of Radioactive Iso<strong>to</strong>pes, 8th ed., Wiley-Interscience, New York, 1986; and<br />

P. Raghavan, “Table of Nuclear Moments,” At. Data Nucl. Data Tables, 42:189 (1989).<br />

Nuclide<br />

Natural<br />

abundance,<br />

% Spin I<br />

Sensitivity at<br />

constant field<br />

relative <strong>to</strong><br />

1<br />

H<br />

NMR<br />

frequency<br />

for a 1-kG<br />

field, MHz<br />

Magnetic<br />

moment<br />

/ N ,<br />

J·T 1<br />

Electric<br />

quadrupole<br />

moment Q,<br />

10 28 m 2<br />

1<br />

n * 1<br />

⁄2 0.321 39 2.916 39 1.913 043<br />

1<br />

H 99.985<br />

1⁄2 1.000 00 4.257 64 2.792 847<br />

2<br />

H 0.015 1 0.009 65 0.653 57 0.857 438 0.002 860<br />

3<br />

H * 1<br />

⁄2 1.213 54 4.541 37 2.978 963<br />

3<br />

He 0.0001 1<br />

⁄2 0.442 12 3.243 52 2.127 624<br />

6<br />

Li 7.5 1 0.008 50 0.626 60 0.822 047 0.000 82<br />

7<br />

Li 92.5 3<br />

⁄2 0.293 55 1.654 78 3.256 427 0.040 1<br />

9<br />

Be 100<br />

3⁄2 0.013 89 0.598 6 1.177 9 0.052 88<br />

10<br />

B 19.9 3 0.019 85 0.457 51 1.800 645 0.084 59<br />

11<br />

B 80.1 3<br />

⁄2 0.165 22 1.366 26 2.688 649 0.040 59<br />

13<br />

C 1.10 1<br />

⁄2 0.015 91 1.070 81 0.702 412<br />

14<br />

N 99.634 1 0.001 01 0.307 76 0.403 761 0.020 2<br />

15<br />

N 0.366 1<br />

⁄2 0.001 04 0.431 72 0.283 189<br />

17<br />

O 0.038 5<br />

⁄2 0.029 10 0.577 41 1.893 80 0.025 58<br />

19<br />

F 100 1<br />

⁄2 0.834 00 4.007 65 2.628 867<br />

21<br />

Ne 0.27 3<br />

⁄2 0.002 46 0.336 30 0.661 797 0.101 55<br />

22<br />

Na * 3 0.018 1 0.443 4 1.745<br />

23<br />

Na 100<br />

3⁄2 0.092 70 1.126 86 2.217 522 0.108 9<br />

25<br />

Mg 10.00 5<br />

⁄2 0.002 68 0.260 82 0.855 46 0.199 4<br />

27<br />

Al 100 5<br />

⁄2 0.206 89 1.110 28 3.641 504 0.140 3<br />

29<br />

Si 4.67<br />

1⁄2 0.007 86 0.846 53 0.555 29<br />

31<br />

P 100 1<br />

⁄2 0.066 52 1.725 10 1.131 60<br />

33<br />

S 0.75 3<br />

⁄2 0.002 27 0.327 16 0.643 821 0.067 8<br />

35<br />

S * 3<br />

⁄2 0.008 50 0.508 1.00 0.045<br />

35<br />

Cl 75.77 3<br />

⁄2 0.004 72 0.417 64 0.821 874 0.081 65<br />

36<br />

Cl * 2 0.012 1 0.489 3 1.283 8 0.016 8<br />

37<br />

Cl 24.23 3<br />

⁄2 0.002 72 0.347 64 0.684 124 0.064 35<br />

37<br />

Ar * 3<br />

⁄2 0.012 76 0.581 8 1.145<br />

39<br />

K 93.258 3<br />

⁄2 0.000 51 0.198 93 0.391 466 0.060 1<br />

40<br />

K 0.0117 4 0.005 23 0.247 37 1.298 099 0.074 9<br />

41<br />

K 6.730 3<br />

⁄2 0.000 084 0.109 19 0.214 870 0.073 3<br />

43<br />

Ca 0.135<br />

7⁄2 0.006 42 0.286 88 1.317 26 0.0408<br />

45<br />

Sc 100 7<br />

⁄2 0.302 44 1.035 88 4.756 483 0.22<br />

47<br />

Ti 7.3 5<br />

⁄2 0.002 10 0.240 40 0.788 48 0.29<br />

49<br />

Ti 5.5 7<br />

⁄2 0.003 78 0.240 47 1.104 17 0.24<br />

50<br />

V 0.250 6 0.055 71 0.425 04 3.345 689 0.21

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