Dylan Archer Dingwell1,2 and Charles H Cunningham1,2
1Medical Biophysics, University of Toronto, Toronto, ON, Canada, 2Physical Sciences Platform, Sunnybrook Research Institute, Toronto, ON, Canada
Synopsis
Keywords: Signal Modeling, Hyperpolarized MR (Non-Gas), 13C Signal Dynamics, 13C MRI, Enzyme Kinetics, Reaction Kinetics, Metabolism
In this study,
we used a particle-based Brownian dynamics simulator with concurrent MR modeling
to characterize diffusion-related effects on 13C signal dynamics. We
conducted a spectrophotometric lactate dehydrogenase (LDH) activity assay with
and without the presence of glass beads to measure the influence of diffusion
constraints and spatial compartmentalization on the reaction kinetics of
LDH-mediated conversion of pyruvate to lactate. We also investigated the relationship
between diffusion and RF refocusing in a typical fast GRE sequence by comparing
simulated signal intensities for RF spoiled and non-spoiled GRE sequences applied under
varying diffusion conditions.
Introduction
Hyperpolarized (HP) carbon-13 MRI is a
powerful tool for metabolic imaging, but interpretation of in vivo
results is challenging due to the complexity of 13C signal dynamics, especially
the variety of factors which affect metabolic reaction kinetics.1,2 Reaction rates involving 13C
metabolites are influenced by diffusion, transport, and uptake processes, which
vary regionally and locally due to differences in cellular microstructure and
metabolite compartmentalization.1–5 Characterizing the interplay between
microstructural and biochemical influences on reaction rates is made even more
difficult by the non-recoverable nature of hyperpolarized signal, which limits
HP 13C MRI scans to a relatively narrow time window. Gradient-echo (GRE)
pulse sequences are useful for applications where rapid acquisition is
important, such as in 3D imaging;6 however, if the repetition time of a GRE
sequence is short relative to relaxation time, then successive acquisitions are
affected by transverse coherences.6,7 Fast GRE sequences without RF
spoiling are often used for HP 13C data acquisition,8–11 resulting in a contribution
from refocused transverse magnetization that is diffusion-weighted and may
contribute significantly to the metabolite signal.Methods
To assess reaction kinetics of LDH-mediated
conversion of pyruvate to lactate, a standard LDH activity assay protocol was used with a
range of LDH concentrations.13 For each assay, 0.5 mL of
sodium pyruvate in phosphate buffer (pH 7.3) was added to a polystyrol cuvette,
followed by 0.5 mL of reduced nicotinamide adenine dinucleotide (NADH), for
final concentrations of 2 mM and 1 mM respectively. Lastly, LDH was added to
concentrations from 0.8-2.8 units/mL, and decrease in absorbance at 340 nm was
monitored at 1 s intervals to determine the maximum reaction rate (Vmax)
for each run. Assays at each concentration of LDH were conducted twice, once
with and once without the presence of glass beads (5 mm diameter) as a model of
structural constraints on diffusion. This system was reproduced in Smoldyn by
generating a cubic volume with 10 mm isotropic length containing either 0 or 8
spherical excluded volumes with 5mm diameter. The lower half of this volume was
populated with 1000 pyruvate particles and the upper half with 500-2000 LDH
particles (shown in Figure 1), with a bidirectional reaction on contact between
particles allowing conversion between pyruvate and LDH. MR spectroscopic
measurements were taken by applying a 90° pulse on pyruvate at 1 s intervals
and reading out the total transverse magnetization.
For RF
refocusing experiments, simulated images were generated in our Smoldyn MR
module using two versions of a 64x64 gradient echo sequence, one with RF
spoiling via a standard phase cycling scheme14 and crusher gradients applied in the
z-direction, and the other with no spoiling (partially shown in Figure 3). In
each simulated scan, 1000 particles were deposited into a rectangular central
volume (dimensions 10 mm x 10 mm x 1 mm) and set to diffuse freely with varying
diffusion coefficients. Signal intensity was calculated from the resulting
images by taking the summed voxel intensity from the region of interest. All
simulations were conducted on 1-4 cores of an AMD Ryzen 9 5900X 12-Core
Processor operating at 4.80 GHz.Results and Discussion
We previously reported
application of a Smoldyn-based MR model to monocarboxylate reaction kinetics, with
close agreement between simulated and in vitro measured results.15 By introducing a structural
constraint on diffusion through addition of glass beads (Figure 1), a
consistent reduction in the reaction rate of LDH-mediated pyruvate to lactate
conversion was observed (Figure 2), with a similar magnitude in vitro
(mean Vmax ratio of 0.624) and in silico (mean Vmax
ratio of 0.762). The higher variability in the in vitro results is
likely primarily due to differences in the bead arrangement, which affects both
the model structure and the effective path length of the spectrophotometric
measurement. Future work will build on these results by using MR phantoms with similar
internal structure to model MR signals expected from different microstructural
conditions.
In
addition to modeling how changes to diffusion conditions influence reaction
kinetics, we investigated how such changes to diffusion rates affect MR signal
intensity in GRE sequences with and without the use of RF spoiling and crusher
gradients to eliminate residual magnetization between successive excitations. As
shown in Figure 4, signal intensities from images acquired with the spoiled GRE
sequence were consistently lower than from the non-spoiled sequence, reflecting
the loss of signal contribution from residual magnetization. Signal intensities
for both spoiled and non-spoiled sequences generally declined sharply with
higher diffusion coefficients; variability in this trend for some data points
was likely a result of the lower particle count (1000 per simulation) used in
this experiment.Conclusions
An in silico
model using particle-based Brownian dynamics and concurrent MR data acquisition
and simulation was compared with spectrophotometric lactate dehydrogenase (LDH)
activity measurements under two different conditions (with and without glass
beads) and was in rough agreement. The in silico model was also shown to
reproduce complex MR signal mechanisms such as the RF refocusing that occurs in
fast gradient-echo sequences. The in
silico model resulting from this work will be useful for designing and predicting
the outcome of future in vivo experiments to understand metabolic
compartmentalization in tissue.Acknowledgements
The authors are grateful for funding from Canadian Institutes for Health
Research grant CIHR PJT152928 and Natural Sciences and Engineering Research
Council grant RGPIN-2016-05566.
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