Edwin J. Baldelomar1, Scott C. Beeman2, Jennifer R. Charlton3, and Kevin M. Bennett4
1Radiology, Washington University in St. Louis, St. Louis, MO, United States, 2Biomedical Engineering, Arizona State University, Tempe, AZ, United States, 3Pediatrics, University of Virginia, Charlottesville, VA, United States, 4Radiology, Washington University in St. Louis, Saint Louis, MO, United States
Synopsis
In this work, we
use contrast agents cationic ferritin and gadolinium-DTPA (Gd-DTPA) to visualize dynamics of macromolecules and freely filtering
particles in individual nephrons throughout entire
perfused rat kidneys. Further, we also look at dynamics in kidneys that
received a vasoconstriction agent, angiotension II (AngII). Voxel time courses were fitted with a bi-exponential model for each experiment (Experiment I, CF
infusion and Experiment II, Gd-DTPA bolus). From fitting we assess CF uptake rates and measure single nephron glomerular
filtration rate (snGFR). CF uptake rates and values of snGFR were mapped
spatially and observed to be heterogeneously distributed throughout the kidney.
Introduction
The kidney serves a
primary role in maintaining osmostic homeostasis, blood pressure, and metabolite
concentrations. Clinical tools to assess kidney function are insensitive to early stages of kidney disease(17). Nephron endowment and function is
heterogeneous within and between individuals(9). Conventional tools can probe function in
individual nephrons, have revealed functional heterogeneity in small subset of
nephrons within the kidney but not in the whole kidney (8, 12, 18). Here we demonstrate MRI to measure and map macromolecular
filtration and single nephron glomerular filtration rates (snGFR) in the intact,
perfused rat kidney, under normal conditions and in a kidney receiving the vasoconstrictor
angiotension II (AngII). This is the first report of whole-kidney measurements
of renal physiology mapped to individual nephrons.Methods
Male Sprague-Dawley
rats (n=4) were anesthetized with ketamine/xylazine for terminal surgery.
Procedure to isolate the right kidney was adapted from (1), and using the organ preservative solution
Lifor(14) to maintain organ function during
transportation (on ice) to MRI. A custom holder and radiofrequency coil were
constructed. To mimic physiological conditions, temperature was maintained at
37oC; a cell-free blood substitute of Krebs-Ringer solution mixed with
Fraction V BSA (5.5g/100mL) and 95/5% O2/CO2 was bubbled
into the solution. Perfusion was 6 mL/min throughout the experiment (15, 16).
We used two
different contrast agents to probe individual glomeruli. Experiment I: Cationic ferritin (CF) visualized the
dynamics of a large particle that does not freely filter through the glomerulus
but binds to the glomerular basement membrane and is detectable by MRI(2, 3). CF was mixed with the perfusate
solution (0.033mg/mL) and 60mL was perfused into the kidney. Experiment II: A bolus of Gd-DTPA, 6.25 uM,
mixed with the perfusate solution was injected into the line. Gd-DTPA was used
to image the dynamics of a freely filtering particle through the individual
glomerulus(5, 6). In a separate experiment, hemodynamics
were modulated with the vasoconstrictor, ANGII (10ng/min throughout)(13).
Imaging was
performed on a Bruker 7T/30 MRI. A T2*-weighted(T2*-w) 3D gradient
recalled echo (GRE) sequence was used for Experiment I with TE/TR = 12.6/45, ϴflip=45,
resolution = 104.2x184.9x220.0 um3, and a temporal resolution of 2.83
minutes between scans with a total of 7 scans.
A T1-weighted(T1-w) 3D
GRE sequence was used for Experiment II with TE/TR = 3.23/22, ϴflip =45,
resolution = 104.2x184.9x220.0 um3, and 1.38 minutes between scans
with a total of 11 scans acquired.
Post processing and analysis were performed
using AFNI and Matlab. Images were first co-registered. Voxel signal in each
experiment was normalized to its mean and time courses were modeled with a
bi-exponential function(4); Sn(t)=Y0+M⋅t+k⋅(e−α1(t−t0) -e−α2(t−t0)).
Here, Y0=Y-Intercept, M=Linear Factor, k = Scale Constant, t0 = Time
Offset, α1 = Phase II Rate, α2 = Phase I Rate. In experiment I, fitting was
performed over the entire time course (Phase I: CF infusion, Phase II: Signal after
CF, in voxels with identified glomeruli). In experiment II, we fitted from the
peak of the Gd-DTPA bolus (Phase I) until ~6 minutes post bolus at the second
peak due to the concentration of filtered Gd-DTPA in the distal tubule (Phase
II). Calculating snGFR - Using α1 from
Experiment II, we first multiplied α1 with the voxel volume. Next, we divided
by a constant to represent the volume fraction occupied by mean tubule diameter
(10) as a scale factor.Results
Experiment I - T2* weighted MRI during CF infusion
into the kidney resolved glomeruli in cortex. Glomerular voxels decreased in
signal with CF infusion (Figure 1,A-E). Experiment
II - T1-weighted MRI after the bolus of Gd-DTPA showed a ~100% spike in
normalized signal at the time Gd-DTPA entered the kidney (t~31min), followed by
a second peak at t~37min in the voxels containing glomeruli (Figure 1, F-J). These
were consistent with an initial delivery of Gd-DTPA to the vasculature and
proximal tubule, movement of filtered Gd-DTPA through the proximal tubule, then
a later rise from concentrated Gd-DTPA in the distal convoluted tubule. Voxels
containing glomeruli were separated into 3 groups based on the shape of their
time course during CF infusion: (1) a ‘Early’ time course where signal begins
to decrease at t~5min, (2) a ‘Normal’ time course where signal decrease begins
at t~10min and decreases rapidly, and (3) a ‘Late’ time course where the
decrease in signal begins at t~10min or later and decreases slowly (Figure 2, Right).
There was no significant difference in average uptake rate of CF between
kidneys with (0.44±0.27 min-1) and without (0.42±0.24min-1
) AngII. Mean snGFR was significantly lower (18.6±18.4 nL/min ) after AngII
compared to no AngII (32.0±28.1 nL/min). Discussion
Contrast enhanced MRI
combined with a custom imaging setup enabled the visualization and measurement
of snGFR and macromolecular dynamics throughout the entire kidney. Values of
snGFR and CF binding rate to the GBM were spatially heterogeneous (Figure 3).
Mean values of snGFR obtained with MRI were consistent with literature values(8). Future work will be aimed at direct validation(11) of MR measurements in the same kidney. Recently
developed imaging protocols and improvements in hardware(7, 19) should increase temporal and spatial resolution. Perfused organ
studies have been critical to understanding renal physiology. This work
establishes a framework for measurements of single nephron physiology by MRI in
the whole, intact kidney. Acknowledgements
We would like to thank the molecular imaging core at the University of Virginia and Jack Roy for his support with this work. References
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