Volume 75, Issue 1 pp. 363-371
Full Paper

The effect of dissolved oxygen on the susceptibility of blood

Avery J.L. Berman

Corresponding Author

Avery J.L. Berman

McConnell Brain Imaging Centre, Montreal Neurological Institute, McGill University, Montreal, Quebec, Canada

Department of Radiology and Hotchkiss Brain Institute, University of Calgary, Calgary, Alberta, Canada

Correspondence to: Avery Berman, 3330 Hospital Drive NW, HMRB Room 193, Calgary, AB Canada T2N 4N1. E-mail: [email protected]Search for more papers by this author
Yuhan Ma

Yuhan Ma

McConnell Brain Imaging Centre, Montreal Neurological Institute, McGill University, Montreal, Quebec, Canada

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Richard D. Hoge

Richard D. Hoge

Institut de génie biomédical, Département de physiologie, Université de Montréal, Montréal, Québec, Canada

Unité de neuroimagerie fonctionelle, Centre de recherche de l'institut de gériatrie de Montréal, Montreal, Quebec, Canada

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G. Bruce Pike

G. Bruce Pike

Department of Radiology and Hotchkiss Brain Institute, University of Calgary, Calgary, Alberta, Canada

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First published: 06 March 2015
Citations: 13

Abstract

Purpose

It has been predicted that, during hyperoxia, excess O2 dissolved in arterial blood will significantly alter the blood's magnetic susceptibility. This would confound the interpretation of the hyperoxia-induced blood oxygenation level-dependent signal as arising solely from changes in deoxyhemoglobin. This study, therefore, aimed to determine how dissolved O2 affects the susceptibility of blood.

Theory and Methods

We present a comprehensive model for the effect of dissolved O2 on the susceptibility of blood and compare it with another recently published model, referred to here as the ideal gas model (IGM). For validation, distilled water and samples of bovine plasma were oxygenated over a range of hyperoxic O2 concentrations and their susceptibilities were determined using multiecho gradient echo phase imaging.

Results

In distilled water and plasma, the measured changes in susceptibility were very linear, with identical slopes of 0.062 ppb/mm Hg of O2. This change was dramatically less than previously predicted using the IGM and was close to that predicted by our model. The primary source of error in the IGM is the overestimation of the volume fraction occupied by dissolved O2.

Conclusion

Under most physiological conditions, the susceptibility of dissolved O2 can be disregarded in MRI studies employing hyperoxia. Magn Reson Med 75:363–371, 2016. © 2015 Wiley Periodicals, Inc.

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