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Direct imaging of glymphatic transport using H217O MRI
Mohammed S. Alshuhri, Lindsay Gallagher, Lorraine M. Work, William M. Holmes
Mohammed S. Alshuhri, Lindsay Gallagher, Lorraine M. Work, William M. Holmes
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Resource and Technical Advance Development Neuroscience

Direct imaging of glymphatic transport using H217O MRI

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Abstract

The recently proposed glymphatic pathway for solute transport and waste clearance from the brain has been the focus of intense debate. By exploiting an isotopically enriched MRI tracer, H217O, we directly imaged glymphatic water transport in the rat brain in vivo. Our results reveal glymphatic transport that is dramatically faster and more extensive than previously thought and unlikely to be explained by diffusion alone. Moreover, we confirm the critical role of aquaporin-4 channels in glymphatic transport.

Authors

Mohammed S. Alshuhri, Lindsay Gallagher, Lorraine M. Work, William M. Holmes

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Figure 2

Effect of inhibiting AQP4 channels on glymphatic water flow.

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Effect of inhibiting AQP4 channels on glymphatic water flow.
(A and B) S...
(A and B) Serial sagittal MRI revealing the temporal evolution of H217O tracer for vehicle-treated rats (upper panel, n = 6) (A) and rats treated with AQP4 inhibitor (lower panel, TGN 020, n = 6) (B). Pseudocolor scaling illustrates the distribution of H217O throughout the brain over 80 minutes of recording, with AQP4 inhibition resulting in substantially reduced H217O transport compared with the vehicle. (C) Summary data showing the percent signal change as a function of time for the vehicle (blue circles) and AQP4 inhibitor–treated (red circles) groups in the frontal cortex, cerebellum, and cisterna magna. Artificial CSF (aCSF; i.e., without 17O-enriched H217O) was used as a negative control. Blue shading on graphs indicates period of contrast agent infusion. (D) Representative images of H217O transport at different time points. The red rectangle has been magnified to better show the actual penetration of H217O, with the top of the red rectangle position on the cerebral cortex. The theoretically calculated displacements of H217O due to diffusion only are 0.53 mm, 0.75 mm, and 0.91 mm at times 231, 459, and 665 seconds, respectively. It is clear that the rapid H217O penetration of the parenchyma cannot be explained by diffusion alone, indicating the presence of convective ISF flow. *P < 0.05, **P < 0.01, ***P < 0.001, ****P < 0.0001. Data are presented as mean ± SEM.

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