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Chapter 2

02-01
The Basics

02-02
Magnetic Properties of Nuclei

02-03
The Boltzmann Distribution

02-04
The Larmor Equation

02-05
Resonance

02-06
Magnetization

02-07
The Rotating Coordinate System

02-08
The Magnetic Resonance Signal

02-09
Frequency Analysis: Fourier Transform


02-07 The Rotating Coordinate System

Before we try to explain the effect of a radiofrequency pulse on a spin system, we have to change our way of looking at this system.

It is very difficult to understand the movements within this system because the spin rotates around its own axis and precesses around the axis of the mag­ne­tic field B0 at the Larmor frequency.

The RF pulse adds another movement. To follow these movements requires a lot of imagination (Figure 02-10).


Figure 02-10:
The spiral motion of the tip of the mag­ne­ti­za­tion during RF excitation shown in a sta­ti­o­nary frame. The rotating frame depicts only the blue axes and the green arrows. To distinguish when we are using the ro­ta­ting frame of reference, we denote the x- and y-axes as x' and y'. The same pro­ce­dure can be used for z, but z and z' are iden­ti­cal.


However, if we try to look at the system from the perspective of a coordinate system ro­ta­ting at a frequency equal or close to the Larmor frequency, the si­tu­a­tion become less complicated.

This may not seem obvious, but in fact we are doing this all the time. When a per­son walks by us, it is very easy for us to assess how much faster than us he is wal­king. Yet, if we view the same action from outer space and have to take into account the rotation of the earth the problem would be much more com­pli­ca­ted.

We are, in fact, using a rotating frame of reference since we are rotating at the same rate. In NMR we can achieve this by using a frame of reference which is rotating at the resonance (Larmor) frequency. On resonance, spins will be sta­ti­o­nary in this frame where­as off-resonance spins will rotate at a frequency which is the difference between their frequency and the resonance frequency (Figure 02-11).


Figure 02-11:
Another example of a rotating (coordinate) system: Watching the horses on a merry-go-round from (a) far away and (b), after climbing aboard, from the merry-go-round itself. From outside, the horses look blurred and, if they are moving fast, it is not easy to distinguish them. If one’s point of reference is on the merry-go-round, it is much easier to distinguish the horses and their features.

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