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. Author manuscript; available in PMC: 2016 Jul 1.
Published in final edited form as: Magn Reson Imaging. 2014 Dec 6;33(6):829–839. doi: 10.1016/j.mri.2014.11.003

Table 5.

Comparisons of magnetic susceptibility measurements between MRI and SQUID. The first column lists the diameters of glass beads. The second column lists calculated susceptibilities (Δχ) from magnetic moments of glass beads obtained at TE =15 ms in Table 2 and from volumes V0′ in Table 4. The uncertainties of susceptibility values were calculated through the error propagation method. These are results from MRI. The third column lists the absolute susceptibility value of each bead, by adding −9.05 ppm (which is the absolute susceptibility of water) to each value shown in the second column. We assume no uncertainty of the water susceptibility value. The fourth column lists measured susceptibility of each bead from SQUID. Measurements between our CISSCO method from MRI and SQUID agree within uncertainties. However, different sizes of beads seem to have slightly different susceptibility values.

Beads MRI MRI + water SQUID
2 mm −2.23 ± 0.32 ppm −11.3 ± 0.3 ppm −11.1 ± 0.7 ppm
3 mm −2.01 ± 0.13 ppm −11.1 ± 0.1 ppm −10.8 ± 0.2 ppm
5 mm −1.82 ± 0.11 ppm −10.9 ± 0.1 ppm −10.1 ± 0.7 ppm
6 mm −1.68 ± 0.09 ppm −10.7 ± 0.1 ppm −11.2 ± 0.6 ppm