I Solutions of the Bloch equations for MRT

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The discussion centers on the relationship between specific equations and the Bloch equations in the context of magnetic resonance technology. The upper equations represent free precession solutions applicable after a 90° excitation pulse when no further RF pulses are transmitted. The lower solutions relate to the magnetization components as perceived by the detector coil, assuming spins are on-resonance and the longitudinal magnetization is zero immediately after the RF pulse. Clarifications confirm that the upper equations hold under specific conditions, emphasizing their relevance in MRI applications. Understanding these relationships is crucial for accurate interpretation of MRI signals.
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Hello all,

I have a question about the relationship between
1691101354726.png

1691101337116.png

resp.
1691101317270.png


and the Bloch equations
1691101375370.png
.

Are these upper equations special solutions of the Bloch equations? If yes, under what condition(s) do the solutions hold?

Thanks in advance for helpful support!
 
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Yes, those are the free precession equations. They apply when there is no RF being transmitted.
 
Thank you. So the upper 5 equations are valid e.g. after the end of a 90° excitation pulse as long as no further RF pulse is irradiated?
 
Derbyshire said:
Thank you. So the upper 5 equations are valid e.g. after the end of a 90° excitation pulse as long as no further RF pulse is irradiated?
Yes, that is right
 
Thanks Dale,

one more question: i assume that the lower three solutions are the magnetization component from "view" of the detector coil, right?
 
Thanks!
 

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