Ramesh Paudyal1, Eve LoCastro1, James Russell1, Ivan Wolansky1, Carl C. Lekaye1, Joseph O. Deasy1, John L. Humm1, and Amita Shukla-Dave1,2
1Medical Physics, Memorial Sloan Kettering Cancer Center, New York, NY, United States, 2Radiology, Memorial Sloan Kettering Cancer Center, New York, NY, United States
Synopsis
Pancreatic
cancer accounts for about 3% of all cancer-related deaths in the US. An
elevation of interstitial fluid pressure (IFP) is a major barrier to drug
delivery in solid tumors. Noninvasive estimation of IFP as a biomarker in
typically inaccessible tumors is a significant step toward assessing tumor
response to therapy. We applied well-recognized fluid flow in porous media to
mouse models of pancreatic ductal adenocarcinoma DCE-MRI data using extended
Tofts' model-derived permeability maps with tumor-appropriate tumor geometry.
Initial results suggest that after validation, IFP can be imaging biomarkers of
early response to therapy.
Purpose
Elevated interstitial fluid pressure (IFP) in solid tumors
can cause a substantial barrier to the fluid and macromolecules delivery [1].The pancreatic ductal adenocarcinoma (PDAC)
microenvironment comprises stromal cells and an extracellular matrix
[2]. The wick-in-needle technique is the
gold-standard, but it is an invasive method of measuring tumors IFP [3]. Dynamic contrast-enhanced magnetic resonance
imaging (DCE-MRI) has been explored as a potential method for the noninvasive
measurement of IFP in preclinical and clinical settings [4-7]. Recently, computational fluid modeling (CFM) method
[8] using DCE data has taken special attention for the estimation
of IFP [9-12]. This study aims to use DCE MRI-based CFM for estimation
of IFP in mouse models of PDAC.Methods
Animals and Tumor Models:
All procedures involving animals were approved by the
Institutional Animal Care and Use Committee of Memorial Sloan Kettering Cancer
Center. Tumors were established by injecting 2×105 KPC 4662 subcutaneously into
the right shoulder region of athymic mice (n=4). The cells were originally
derived from a murine pancreatic tumor, genotype Pdx1-Cre; LSL KRASG12D; Trp53R172H/wt.
The MRI’s were performed 10-12 days after tumor inoculation.
MRI Data Acquisition:
MRI was performed on a 9.4 T (Bruker BioSpin MRI GmbH). T2-weighted
images with TR/ TE= 2092.34/33 ms, FOV=30 ×30 mm2, NA=2, NS=20, slice thickness= 0.7 mm, slice
gap=0.7 mm, and acquisition matrix size (MS)=256×256 were used to locate the
tumor slices for DCE-MRI slices. The DCE-MRI series were acquired using a FLASH
sequence with TR/TE = 54.63/1.29 ms,
NA=1, NS=6, flip angle (FA=15°), MS=132×106, and temporal resolution
5.79 s, resulting in a total acquisition time of 14 min 38 s. For precontrast T10,
T1w images were acquired using four different TR values, i.e. 100
ms, 200 ms, 800 ms, and 2000 ms. Other scanning parameters were the same as
mentioned above.
DCE
Data Analysis: Tumor regions of interest (ROI’s) were contoured
using ITK-SNAP on dynamic images. For estimation of IFP, the volume transfer
constant for CA, Ktrans [min-1], derived from the
extended Tofts model (ETM) and arterial
input function value (obtained from neck artery) were incorporated into the CFM
simulation [9, 12].
Computational
Theory for IFP: The CFM method is based on transport of CA in
porous media providing estimates of IFP [9].
Starling equation of the vascular system consisting of source and sink terms [13] is incorporated into Equation [1] (Figure1), i.e., Darcy velocity, u , and IFP relationship [8 ]. The resulting equation modulated by Ktrans is
applied for CFM simulation (Equation [2]) is shown in Figure 1. CFM simulation was performed
for Equation [2] using the following model parameters: vessel permeability Lp=
2 × 10−11 mPa−1s−1 (in
tumor, t) and 3 × 10−12 mPa−1s−1 (in
normal tissue, n); lymphatic
filtration coefficient LpLSL/V=1 × 10−7 Pa−1 s−1;
tissue hydraulic conductivity KH = 1.9 × 10−12 (t), 3.8 ×
10−13 (n) m2 Pa−1 s−1; microvascular surface
area-to-volume S/V= 2 × 104 (t), 7 × 103 (n) m−1;
microvascular pressure pv= 2300 Pa; osmotic pressure in
microvasculature πv= 2670 Pa; osmatic pressure in interstitial space
πi= 3230 (t), 1330 (n) Pa; and osmotic reflection coefficient for
plasma σ= 0.82 (t), 0.91 (n) (Unitless).
CFM Simulation: Tumor
ROI’s obtained were grayscale-dilated by 20 pixels, forming an extended domain
ROI to incorporate normal tissue around tumor. ROI’s for tumor and extended
domain were resliced 1mm3-isotropic, converted to STL format, and
imported as boundary meshes for the model. The computations use finite element
method in COMSOL Multiphysics software (COMSOL Inc., Stockholm, Sweden).
Results
We developed a noninvasive
DCE method to estimate IFP for PDAC. ETM derived mean Ktrans and CFM-estimated
IFP values from four mice were 0.038±.004 (min -1) and 1.17±0.27 (kPa)
respectively. A representative DCE data fitting with ETM is displayed in Figure 2. Representative T2 weighted image,
ETM derived Ktrans map, and CFM generated IFP map are shown in
Figure 3. Figure 4a shows a scatter plot of total tumor ROI volume vs. IFP. Tumor
heterogeneity leading to the subtle differences in IFP values within the tumor
are visualized in these maps. A weak positive linear relationship is observed
between these metrics (r= 0.31). CFM-estimated IFP exhibited a strong linear
relationship with Ktrans (r= 0.90) (Figure 4b). The leakage space, ve, and
IFP exhibited weak positive correlation (r= 0.28).Discussion
Ktrans and IFP maps
depict heterogeneity within the tumor. IFP is maximum at tumor core and monotonically
decreases outwards to the tumor periphery towards the normal tissue. We
observed a
positive correlation between total tumor volume and IFP, and Ktrans
and ve. Elevation of IFP in tumors are thought to be associated with
the high vessel permeability and impaired lymphatic drainage from the
interstitium. A linear relationship may be highly influenced by the tumor cellularity
and stroma, depending on the tumor types [14].Conclusion
After appropriate validation, non-invasive IFP from DCE MRI-based CFM estimate
can have promising application in the clinics.Acknowledgements
We acknowledge
funding support from NCI R01 CA194321.References
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