Digital Signal Processing Reference
In-Depth Information
Appendix A
Solving Bloch Equation with ADvsinc ð Dvt Þ
Envelope
Rewriting ( 2.21 ) and ( 2.23 ) with ADvsinc ð Dvt Þ envelope as follows with the
condition Dv\\ B 0 c
2p .
dM xy ð t Þ
dt
¼ jcADvsinc ð Dvt Þ M 0 cos ð a Þ e j ð cB 0 t þ h Þ
ð A : 1 Þ
dM z ð t Þ
dt
ð A : 2 Þ
¼ cADvsinc ð Dvt Þ M 0 sin ð a Þ E 0 sin ð h / Þ
Since sinc ð Dvt Þ is almost one for all t with Dv\\ B 0 c
2p , we treat sinc ð Dvt Þ as the
constant in both the equations and solution is obtained as follows
M xy ð t Þ¼ 2M 0 sin ð a Þ e j ð cB 0 t þ / Þ
ð A : 3 Þ
M z ð t Þ¼ cM 0 sin ð a Þ ADvsinc ð Dvt Þ sin ð h / Þ t þ 2M 0 cos ð a Þ
ð A : 4 Þ
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