Login / Signup

Metabolic activity diffusion imaging (MADI): I. Metabolic, cytometric modeling and simulations.

Charles S SpringerEric M BakerXin LiBrendan MoloneyGregory J WilsonMartin M PikeThomas M BarbaraWilliam D RooneyJeffrey H Maki
Published in: NMR in biomedicine (2022)
Evidence mounts that the steady-state cellular water efflux (unidirectional) first-order rate constant (k io [s -1 ]) magnitude reflects the ongoing, cellular metabolic rate of the cytolemmal Na + , K + -ATPase (NKA), c MR NKA (pmol [ATP consumed by NKA]/s/cell), perhaps biology's most vital enzyme. Optimal 1 H 2 O MR k io determinations require paramagnetic contrast agents (CAs) in model systems. However, results suggest that the homeostatic metabolic k io biomarker magnitude in vivo is often too large to be reached with allowable or possible CA living tissue distributions. Thus, we seek a noninvasive (CA-free) method to determine k io in vivo. Because membrane water permeability has long been considered important in tissue water diffusion, we turn to the well-known diffusion-weighted MRI (DWI) modality. To analyze the diffusion tensor magnitude, we use a parsimoniously primitive model featuring Monte Carlo simulations of water diffusion in virtual ensembles comprising water-filled and -immersed randomly sized/shaped contracted Voronoi cells. We find this requires two additional, cytometric properties: the mean cell volume (V [pL]) and the cell number density (ρ [cells/μL]), important biomarkers in their own right. We call this approach metabolic activity diffusion imaging (MADI). We simulate water molecule displacements and transverse MR signal decays covering the entirety of b-space from pure water (ρ = V = 0; k io undefined; diffusion coefficient, D 0 ) to zero diffusion. The MADI model confirms that, in compartmented spaces with semipermeable boundaries, diffusion cannot be described as Gaussian: the nanoscopic D (D n ) is diffusion time-dependent, a manifestation of the "diffusion dispersion". When the "well-mixed" (steady-state) condition is reached, diffusion becomes limited, mainly by the probabilities of (1) encountering (ρ, V), and (2) permeating (k io ) cytoplasmic membranes, and less so by D n magnitudes. Importantly, for spaces with large area/volume (A/V; claustrophobia) ratios, this can happen in less than a millisecond. The model matches literature experimental data well, with implications for DWI interpretations.
Keyphrases