4D-flow-MRI enables the non-invasive assessment of cardiovascular pressure drops; however, estimation accuracy depends on vascular topology and acquisition noise. Here, we present a method that minimizes the impact of these by using virtual fields to isolate and probe hemodynamic pressure drops. We show that, in-silico, the method accurately assesses pressure drops over multiple segments of a patient-specific co-arcted aorta (average error below 22%), independent of anatomical bifurcations. Additionally, the method compares successfully against catheter measurements, using 4D-flow-MRI in-vivo (average error at peak systole below 15%). With this, the method represents a refined tool for hemodynamic analysis of cardiovascular flow.
The proposed method originates from a work-energy formulation assessing relative pressure drops from a flow field, $$$v$$$6. Here we propose an alteration by introducing a virtual field, $$$w$$$, analyzing the virtual work of $$$w$$$ within a vascular domain in order to isolate the pressure drop, $$$\Delta p$$$. By so, influence from measurement inaccuracies, low flow magnitudes or bifurcations associated with $$$v$$$ are minimized.
Here, $$$w$$$ is chosen as the solution to a Stokes flow boundary value problem, with flow permitted over the inlet and outlet of the desired pressure drop, and with flow restricted at any other surface (vascular wall or secondary bifurcations). Using our previously proposed derivation6 in conjuction with $$$w$$$, $$$\Delta p$$$ can be identified by:
$$ \Delta p=-\frac{1}{Q_w} \left(\frac{\partial}{\partial t}K_w + A_w + V_w \right) $$
with $$$K_w$$$, $$$A_w$$$, and $$$V_w$$$ being the kinetic, advective, and viscous energy components when using $$$w$$$ as the weighting velocity field, and $$$Q_w$$$ being the flow of $$$w$$$ over the domain inlet (for details, see6).
To assess method performance, two setups are evaluated. First, a challenging patient-specific in-silico model of a co-arcted aorta9 is used to generate simulated image data (spatial/temporal resolution: 2 mm3, 43 ms, SNR: 10 and 30), with temporal pressure drops compared to the simulated pressure fields. Second, 4D-flow-MRI (Philips Achieva, 1.5T, spatial/temporal resolution: 2.1 mm3, 31 ms) is acquired from 6 adolescent Fontan patients, with $$$v$$$ reconstructed and corrected using GTFlow (GyroTools). Flow-field-based pressure drop estimates are compared against invasive catheter measurements acquired during the same imaging session. $$$w$$$ is solved using a finite-difference scheme on the vascular segment of interest using a right-preconditioned iterative GMRES-solver and a BFBT-preconditioner10-11. Spatial and temporal noise filtering is introduced by polynomial interpolation and frequency-domain low-pass filtering, respectively.
Figure 1 shows the results of the in-silico setup. The method estimation follows the true pressure drop throughout the cardiac cycle, with minor noise-levels differences. Specifically, the pressure drop is captured with an average error of 22%, equaling 1.9 mmHg at peak systole. Importantly, the strength of the method is shown in the preserved accuracy from aortic inlet to coarctation, unaffected by the bifurcations along the aortic arch, or of the diastolic low-magnitude-flows.
Figure 2 summarizes the results of the in-vivo setup. Again, the method captures temporal changes in relative pressure, with the virtual field isolating the vascular region-of-interest. The peak systolic pressure is captured with an average error of 15%, corresponding to an accuracy of 1.3 mmHg. The method seems robust to anatomical bifurcations or low-magnitude-flows, even though minor fluctuations seem visible in certain phases.
For both setups, our method performs favorable to conventional Bernoulli-based estimates as well as to previous work-energy based measures6 (average error above 200%), in part due to that these methods are not developed to handle vascular bifurcations or diastolic flow-magnitudes.
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