Magnetic Resonance — Question 9

Section 40-5 · Physics pages 6668–6669

Question 9 A magnetic gradient maps resonance frequency to position A sample sees B(z) = B0 + Gz with G = .0200 T/m. Use γ/(2π) = 42.6 MHz/T. A frequency-selective pulse excites a full bandwidth of ∆f = 1.20 kHz around fc. Ignore nonlinearities and intrinsic linewidth. z f Schematic; labels, not drawing lengths, specify the data. (a) Find the position of the selected slice center. (b) Find its full thickness and the gradient needed to halve it without changing bandwidth.
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Question 9 - Solution A magnetic gradient maps resonance frequency to position z f (a) Method and calculation f(z) = γ 2π(B0 + Gz) ⇒zc = fc −(γ/2π)B0 (γ/2π)G . df dz = (42.6 × 106)(.0200) = 8.52 × 105 Hz/m. (b) Interpretation and further calculation ∆z = ∆f |df/dz| = 1.408 mm . ∆z ∝G−1 ⇒G′ = 2G = .0400 T/m . Physical check The bandwidth and slice thickness are both full widths. The model assumes the selected region is small enough that the local field varies linearly.

Question 9

A magnetic gradient maps resonance frequency to position

A sample sees B(z)=B0+GzB(z)=B_0+Gz with G=.0200T/mG=.0200\,\mathrm{T/m}. Use γ/(2π)=42.6MHz/T\gamma/(2\pi)=42.6\,\mathrm{MHz/T}. A frequency-selective pulse excites a full bandwidth of Δf=1.20kHz\Delta f=1.20\,\mathrm{kHz} around fcf_c. Ignore nonlinearities and intrinsic linewidth.

Diagram shown in the original SVG worksheet.

  1. Find the position of the selected slice center.

  2. Find its full thickness and the gradient needed to halve it without changing bandwidth.

Question 9 - Solution

A magnetic gradient maps resonance frequency to position

Diagram shown in the original SVG worksheet.

(a) Method and calculation

f(z)=γ2π(B0+Gz)⇒zc=fc−(γ/2π)B0(γ/2π)G.f(z)=\frac{\gamma}{2\pi}(B_0+Gz)\Rightarrow\boxed{z_c=\frac{f_c-(\gamma/2\pi)B_0}{(\gamma/2\pi)G}}.dfdz=(42.6×106)(.0200)=8.52×105Hz/m.\frac{df}{dz}=(42.6\times10^6)(.0200)=8.52\times10^5\,\mathrm{Hz/m}.

(b) Interpretation and further calculation

Δz=Δf|df/dz|=1.408mm.\boxed{\Delta z=\frac{\Delta f}{|df/dz|}=1.408\,\mathrm{mm}}.Δz∝G−1⇒G′=2G=.0400T/m.\Delta z\propto G^{-1}\Rightarrow\boxed{G\prime=2G=.0400\,\mathrm{T/m}}.

Physical check

The bandwidth and slice thickness are both full widths. The model assumes the selected region is small enough that the local field varies linearly.