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By Dr. N. Bloembergen (auth.)

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Extra resources for Nuclear Magnetic Relaxation

Sample text

If the saturation term is taken into account. on elimination of z the locus is found to be an ellipse the eccentricity of which de~ pends on H I • Now it has to be remembered. that the receiver detects only changes in amplitude of the input voltage. If the balance were complete. the output of a square law detector would be proportional to 16. V 12 • Under operation conditions the balance is never made com~ plete and the situation is represented by fig. 3. 11. OA is the unbalanced signal. BO is the signal coming through the dummy circuit.

2Q, of which any part could be shorted by a sliding contact. 05 Q manganin resistance in the magnet circuit. 3. 2. The radio signal caused by nuclear resonance. We shall assume that the amplitude and frequency of the modulation sweep are so small. that the solutions obtained in chapter 2 for a time independent field Hg remain valid. In section 3. 7 we shall indicate some violations of the results. if the rate of change of the magnetic field is too fast. Since the condensor Cl in 6g. 9. being driven by a constant current The aequivalent diagram of the nuc1ear generator io i W Cl VI' where VI resonance circuit.

Iz. + I I) ! ,0. ,0. J sm Vij eos vije ! ' ,

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