๐Ÿงฒ MRI / NMR Physics โ€” Bloch Equations (2D)

Magnetisation vector ยท RF pulse excitation ยท T1 & T2 relaxation ยท FID signal

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Parameters

Magnetisation

Mx0.000
My0.000
Mz1.000
|Mxy|0.000
Larmor freq63.9 MHz
Time0 ms

๐Ÿงฒ What It Demonstrates

This 2D companion models nuclear magnetic resonance (NMR) โ€” the physical basis of MRI โ€” by integrating the same Bloch equations as the 3D version, drawn on a flat Canvas 2D projection instead of a WebGL scene. A net magnetisation vector M = (Mx, My, Mz) starts aligned with the static field Bโ‚€ along the z-axis. An RF pulse tips M into the transverse plane, where it precesses at the Larmor frequency and decays through two independent relaxation processes: T1 (spin-lattice, longitudinal recovery) and T2 (spin-spin, transverse decay). The decaying transverse signal is the Free Induction Decay (FID).

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