Labib Shahid1, Juan Pablo Gonzalez-Pereira1, Cody Johnson1, and Alejandro Roldán-Alzate1
1University of Wisconsin-Madison, Madison, WI, United States
Synopsis
Studying common urinary conditions
such as BPH/LUTS require measuring urine flow in the urethra by invasive
techniques. We present a method that uses real-time MR images of the bladder
and urethra to quantify urine flow dynamics. Images of the urethra define the
anatomical geometry, while images of the bladder inform the flow rate inside
the urethra. Coupling MRI with CFD allows the urinary flow simulation inside the
urethra providing information about urine velocity, pressure, and wall shear
stress non-invasively.
Introduction
Benign prostatic hyperplasia
(BPH) is the nonmalignant growth of the prostate, commonly observed in aging
men. Lower urinary tract symptoms (LUTS) are the most common manifestation of
BPH. Over 50% of men aged over 60 years suffer from BPH, and 15%-30% of these
men have LUTS1.
Standard imaging techniques to assess urethral abnormalities are retrograde
urethrography (RUG) and voiding cystourethrography (VCUG)2. However, both RUG and VCUG have
become uncommon and the limited exposure of radiologists to these examinations
can make it challenging to interpret results3. Image-based computational fluid
dynamics (CFD) has been used to study biomechanics in cardiovascular diseases4.
Our group has investigated MRI-based CFD, with a focus on cardiac flows as well5.
In this study, we expand the tools we developed and apply them to pathological
urinary flows. The purpose of this study was to develop and implement a non-invasive
MRI-based computational methodology for the simulation of urinary flow inside urethra. Methods
In-vivo MRI study was performed
on four male subjects aged 55 ± 19 years with no history of BPH/LUTS following
an IRB-approved HIPAA-compliant protocol. Subjects were scanned on a clinical
3T scanner (Premier, GE Healthcare, Waukesha, Wisconsin, USA) using 3D
Differential Subsampling with Cartesian Ordering (DISCO) Flex sequence. 15
minutes prior to the start of the imaging session, 1/3 of a single weight-based
dose (0.1 mmol/kg) of gadolinium-based contrast was slowly hand injected
intravenously outside and the subjects were asked to walk around to ensure
enhancement of the urine. Right before the scan, the subject was equipped with
a condom catheter to allow the void event while scanning, and volumetric dynamic
images of the bladder and urethra were collected throughout the void. The MR
images were manually segmented using the semiautomatic segmentation software
packages Mimics
and 3-matic (Materialise NV, Leuven, Belgium).
For the computational simulations, anatomical models of the urethra at
the moment of maximum flow were generated from the segmented images for all
subjects. To determine the inlet boundary conditions, bladder volumes were segmented
and the urinary flow rate in the urethra was calculated as the rate of change
in volume of the bladder over time. The outlet boundary condition was
atmospheric pressure. The urethra geometry was inputted into the CFD software
package CONVERGE 3.1 (Convergent Science, Inc., Madison,
Wisconsin, USA)6. Tecplot 360 EX (Tecplot, Inc.,
Bellevue, Washington, USA) was used to visualize the in-silico results. Subject
demographic information, in-vivo scans, urethra geometries, and flow rates from
bladder volumes are shown in Figure 1.Results
Contrast-enhanced
MRI studies provided real-time anatomies of urethra and bladder during voiding.
The flow rates and geometries extracted from the in-vivo studies were used to
successfully simulate the urine flow inside each subject’s urethra during voiding.
The CFD simulation results are visualized in Figure
2. Figure
1 shows that Subjects 1 and 2 voided the largest
volumes. This is reflected in our CFD results, with Subjects 1 and 2 having the
highest velocities and pressures. In all four subjects, their prostatic/membranous
section were narrower than the penile section of the urethra. In-silico data predicts
wall shear stress to be higher in the prostatic/membranous region. Pressure
drops across the prostatic, membranous, and penile urethra were calculated and
are plotted in Figure
3. In Subjects 1 and 4, the pressure drop across
membranous urethra is larger than pressure drop across prostatic urethra. It is
the opposite in Subjects 2 and 3. For all four subjects, the pressure drop in
the penile urethra is the smallest, corresponding to the thickest section of
the urethra.Discussion
Real-time MRI data alone do not
provide any insight into the flow dynamics of urine. Our method combines MRI of
the urinary system with CFD to present a computational methodology that quantitatively
and qualitatively characterizes urine flow in the urethra. Furthermore, the
MRI-based CFD simulation calculates the pressure required at the bladder neck
(start of the urethra) to flow urine at a prescribed rate. Information on the
pressure at the bladder neck is useful because it can be imposed as the outlet
boundary condition when simulating the bladder voiding process. Unlike the
current procedures used to measure urine flow in the urethra, namely RUG and
VCUG, our MRI-based approach is non-invasive and provides not only anatomical
but functional information not available with any other diagnostic method. Conclusion
This study shows that MRI-based
CFD can be expanded to study pathological flows in the urinary system. Our
simulations assumed the urethra to be rigid, which is anatomically inaccurate.
Future studies should include the motion of the urethra wall in their model
extracted from the real time MRI images. Further studies should compare results
from our method with results from benchmark clinically used techniques.Acknowledgements
The authors acknowledge support
from the NIH (R01 DK126850-01).
GE Healthcare, which provides
research support to the University of Wisconsin.
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