The magnetic field shift within cylindrical blood vessels can be used to estimate venous oxygen saturation, based on the magnetic susceptibility of deoxyhemoglobin. However, conduit veins in the periphery are often surrounded by fat, which has a larger magnetic susceptibility than water and the venous blood pool. It is shown that the magnetic susceptibility effects of fat can confound estimation of venous oxygen saturation. A new method to correct for these effects is described with
Background: Imaging of venous oxygen saturation enables non-invasive study of oxygen consumption/metabolism. The magnetic susceptibility of blood (χBlood) is linearly related to oxygen saturation (SvO2), χBlood=χdo*Hct*(1-SvO2), where χdo=4π*0.27 ppm for fully deoxygenated blood, Hct=hematocrit. For cylindrical vessels at an angle of θ to B0, χBlood shifts the magnetic field (ΔBO2) in relation to the venous oxygen saturation, SvO2(%)=100*{1-2*ΔBO2/(γ*χdo*Hct*B0*(cos2θ-1/3))}.1, 2 Additional static field inhomogeneities are removed by estimation and subtraction of a background field, ΔBBackground.3 For applications in skeletal muscle oxygen consumption4, 5, the conduit veins of interest (e.g. popliteal/ femoral vein) are commonly surrounded by fat (χFat=0.65 ppm), particularly where smaller veins converge to the larger targeted veins. The potentially complex magnetic field perturbation from the fat (ΔBFat) may extend into the vein and the surrounding muscle reference tissue, potentially confounding estimation of the targeted ΔBO2 (i.e. the measured magnetic field, ΔBMeasured, will be the sum of ΔBO2, ΔBBackground and ΔBFat).
Approach: Part 1 - We propose that Dixon fat-water separated imaging (multi-echo acquisitions)6 can be used to quantify fat/water distributions, which can be used to generate a susceptibility model of the fat (for the estimation of ΔBFat), and to quantify off-resonance frequency (ΔBMeasured) to estimate SvO2. ΔBBackground can be measured using a low spatial frequency fit of the off-resonance field from the reference tissues surrounding the targeted vein.3 Part 2 - We further propose that the measured ΔBFat can be used in subsequent single-slice time-resolved studies of SvO2, in conjunction with isolated muscle exercise.
MRI Acquisition: Imaging studies (3T PRISMA; Siemens Healthcare; Erlangen, Germany) of the popliteal vein (i.e. venous return from lower leg) were performed in 10 healthy individuals. Part 1 - A slice interleaved multi-echo gradient echo sequence provided spatial coverage from the knee to lower thigh (TE=[2.44,4.26,6.08,8.90,9.72,11.54] ms, TR=700ms, flip=30°, 192x102 matrix, 49x4mm slice thickness) (Fig 1). Part 2 - a single slice version of the sequence from Part 1 (TR = 18.9 ms,flip=20°) was used for dynamic studies with exercise (3.75 sec/image, 50 time-points). Flow-encoding gradients were added to the single-slice sequence to enable phase-contrast evaluation of venous blood flow in the same acquisition.4, 5
Exercise: All subjects performed incremental plantar flexion exercise targeting the gastrocnemius (4-9 Watts, increasing 1 Watt/minute) for 3-6 minutes, to a perceived level of 75% of maximum (Ergospect; Austria). Exercise imaging started within 1 second of the completion of exercise (to capture peak and recovery dynamics).
Analysis: The VARPRO method was used to calculate water, fat and off-resonance (ΔBMeasured) maps6 for both multi-slice (3D) and post-exercise time-resolved acquisitions. Volumetric susceptibility maps were calculated using fat-fraction from the VARPRO analysis (Fig. 2a), for calculation of ΔBFat7 (Fig. 2b). Venous field shift was calculated according to ΔBO2=ΔBMeasured -ΔBFat-ΔBBackground for both multi-slice acquisitions (at rest), and time-resolved single-slice dynamic data, to calculate dynamic SvO2. VO2 = blood flow*Ca*Hgb*(SaO2-SvO2), where Ca=1.34ml O2/g of Hb, and hemoglobin was assumed to 14.6 g/dL (with Hct=0.43). Arterial blood oxygen (SaO2) was measured with a pulse oximeter.
The magnetic susceptibility of fat gives rise to potentially complex variations in the static magnetic field in skeletal muscle, which was shown to give rise to errors in the estimated venous oxygen saturation. On a subject-by-subject basis, Dixon fat-water separated imaging can be used to measure the magnitude of (and to correct) these effects (ΔBFat), while also measuring the targeted magnetic field, ΔBMeasured, used to estimate SvO2. These methods are compatible with the targeted dynamic exercise applications, which are essential for the study of the mechanisms of reduced exercise capacity (e.g. reduced oxygen extraction, blood flow or delayed recovery following exercise).8
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Figure 1: Spatial coverage and slice prescription of fat, water and off-resonance images, showing the popliteal vein locations (3 sample slices shown). Water, fat, and off-resonance maps were calculated using a multi-echo DIXON acquisition with VARPRO processing.
Figure 2: Measurement of and correction for the magnetic field shift from fat. The fat-fraction map (a) is used to generate a fat-susceptibility map (b) and to calculate a resulting field shift (c). The measured magnetic field (d) is corrected for the fat-induced field shift from c to yield the final venous oxygen field shift (e), for calculation of SvO2.