Difference between revisions of "Relaxation of spin 1/2 nuclei: two-state derivation"
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When an NMR sample is placed in a static magnetic field and allowed to come to equilibrium it is found that a net magnetization of the sample along the direction of the applied field (traditionally the z-axis) is developed. Magnetization parallel to the applied field is termed longitudinal. This equilibrium magnetization arises from the unequal population of the two energy levels that correspond to the α and β spin states. In fact, the z-magnetization, M<sub>z</sub>, is proportional to the population difference: | When an NMR sample is placed in a static magnetic field and allowed to come to equilibrium it is found that a net magnetization of the sample along the direction of the applied field (traditionally the z-axis) is developed. Magnetization parallel to the applied field is termed longitudinal. This equilibrium magnetization arises from the unequal population of the two energy levels that correspond to the α and β spin states. In fact, the z-magnetization, M<sub>z</sub>, is proportional to the population difference: | ||
| − | + | M<sub>z</sub>z ∝ (n<sub>α</sub> - n<sub>β</sub>) | |
where n<sub>α</sub> and n<sub>β</sub> are the populations of the two corresponding energy levels. Ultimately, the constant of proportion just determines the absolute size of the signal we will observe. As we are generally interested in the relative size of magnetizations and signals we may just as well write: | where n<sub>α</sub> and n<sub>β</sub> are the populations of the two corresponding energy levels. Ultimately, the constant of proportion just determines the absolute size of the signal we will observe. As we are generally interested in the relative size of magnetizations and signals we may just as well write: | ||
Revision as of 04:50, 12 April 2020
Introduction
When an NMR sample is placed in a static magnetic field and allowed to come to equilibrium it is found that a net magnetization of the sample along the direction of the applied field (traditionally the z-axis) is developed. Magnetization parallel to the applied field is termed longitudinal. This equilibrium magnetization arises from the unequal population of the two energy levels that correspond to the α and β spin states. In fact, the z-magnetization, Mz, is proportional to the population difference:
Mzz ∝ (nα - nβ)
where nα and nβ are the populations of the two corresponding energy levels. Ultimately, the constant of proportion just determines the absolute size of the signal we will observe. As we are generally interested in the relative size of magnetizations and signals we may just as well write:
Mzz = (nα - nβ)
Mathematically this system can be treated similar to chemical kinetics.
