Solutions of the Bloch equations for MRT

In summary, the conversation is about the relationship between the upper equations and the Bloch equations. It is confirmed that the upper equations are special solutions of the Bloch equations and they apply when there is no RF being transmitted. It is also clarified that the upper equations are valid after the end of a 90° excitation pulse as long as no further RF pulse is irradiated. The lower three solutions are the magnetization component from the perspective of the detector coil and have slight differences compared to the upper equations. These differences include assuming that the spins are on-resonance and the phase of the transverse component is constant, as well as assuming a longitudinal magnetization of 0 at t=0.
  • #1
Derbyshire
4
0
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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  • #2
Yes, those are the free precession equations. They apply when there is no RF being transmitted.
 
  • #3
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?
 
  • #4
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
 
  • #5
Thanks Dale,

one more question: i assume that the lower three solutions are the magnetization component from "view" of the detector coil, right?
 
  • #7
Thanks!
 

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