ABSTRACT

I. Introduction 303

II. Background 304

A. Overview of Lung Structure 304

B. Techniques for Measuring the Diffusion of 3He 305

GRE Pulse Sequences with Bipolar Gradients 305

Spin-Echo Train Pulse Sequences 308

Magnetic Tag Dissolution 309

C. Quantitative Models of Diffusion in the Lung 310

Spherical Shells 311

Isotropically Distributed Cylinders 311

The Lung as a Porous Medium 312

III. ADC Measurements in Human Subjects 313

A. Studies in Healthy and Diseased Subjects 313

B. Time Dependence 315

C. Directional Dependence 317

D. Dependence on Lung Inflation 319

E. Model-Based Diffusion Results 320

IV. Conclusion 321

References 322

I. Introduction

Since the emergence of hyperpolarized 3He gas as a novel contrast agent for MRI,

there has been substantial interest in exploiting the unique properties of this gas

for evaluating lung structure and function. Of particular relevance for assessing

the microstructure of the lung, 3He has a very high self-diffusion coefficient

(2 cm2/s at body temperature and a pressure of 760 Torr) which, in an unrestricted environment, results in relatively large diffusion-driven displacements of 3He atoms during time periods of relevance for MRI, such as during the echo

time of a gradient-echo (GRE) pulse sequence, as routinely used for hyperpol-

arized 3He imaging. For example, within air in an unrestricted space, the root

mean squared displacement of a 3He atom is 2 mm during 5 ms. A second important characteristic of 3He is its low tissue solubility, which

effectively confines inhaled 3He gas to the airspaces of the lung. When 3He is

confined to relatively small spaces such as the distal airway structures, which

have characteristic lengths on the order of 0.1 mm, its motion is restricted result-

ing in reduced displacements and a decrease in the apparent diffusion coefficient

(ADC) as measured by MRI (1-4). Depending on the parameters of the pulse

sequence, these ADC values may exhibit a complex dependence on a variety

of morphological features of the lung microstructure including the surface-to-

volume ratio, the length scales of the distal airways, the anisotropy of airway

orientation, and the tortuosity of airway connectivity. Application of diffusion

MRI methods to hyperpolarized 3He thus presents the opportunity to create

image contrast on the basis of differences in the morphology of the microstruc-

tural environment between each voxel in the image, yielding a powerful tool

to quantitatively evaluate disease processes that alter the underlying structure

of the lung.