Investigating 3He diffusion NMR in the lungs using finite difference simulations and in vivo PGSE experiments.

Finite difference simulations have been used to model (3)He gas diffusion in simulated lung tissue. The technique has the advantage that a wide range of structural models and diffusion-sensitizing gradient waveforms can be investigated, for which analytical methods would otherwise be virtually impossible. Results from simulations and in vivo pulsed-gradient-spin-echo (PGSE) experiments show that the apparent diffusion coefficient (ADC) is a function of diffusion time and gradient strength, and suggests diffusion is locally anisotropic. The simulations have been compared to recent work on an analytical model that characterizes lung tissue as a series of independent cylinders. The results presented may have clinical implications for (3)He ADC measurements in assessing lung diseases such as chronic-obstructive-pulmonary-disease.

[1]  Eiichi Fukushima,et al.  The Narrow-Pulse Criterion for Pulsed-Gradient Spin-Echo Diffusion Measurements , 1995 .

[2]  Bengt Jönsson,et al.  Predictions of pulsed field gradient NMR echo-decays for molecules diffusing in various restrictive geometries. Simulations of diffusion propagators based on a finite element method. , 2003, Journal of magnetic resonance.

[3]  N. Galiè Do we need controlled clinical trials in pulmonary arterial hypertension? , 2001, The European respiratory journal.

[4]  Gary P. Zientara,et al.  Spin‐echoes for diffusion in bounded, heterogeneous media: A numerical study , 1980 .

[5]  J. Liner,et al.  Determination of the Temperature Dependence of Gaseous Diffusion Coefficients Using Gas Chromatographic Apparatus , 1972 .

[6]  Dmitriy A Yablonskiy,et al.  Quantitative in vivo assessment of lung microstructure at the alveolar level with hyperpolarized 3He diffusion MRI , 2002, Proceedings of the National Academy of Sciences of the United States of America.

[7]  John P Mugler,et al.  Emphysema: hyperpolarized helium 3 diffusion MR imaging of the lungs compared with spirometric indexes--initial experience. , 2002, Radiology.

[8]  Scott N. Hwang,et al.  Biexponential diffusion attenuation in the rat spinal cord: Computer simulations based on anatomic images of axonal architecture , 2002, Magnetic resonance in medicine.

[9]  M. H. Blees,et al.  The Effect of Finite Duration of Gradient Pulses on the Pulsed-Field-Gradient NMR Method for Studying Restricted Diffusion , 1994 .

[10]  Eduard E de Lange,et al.  MRI of the lungs using hyperpolarized noble gases , 2002, Magnetic resonance in medicine.

[11]  Schwartz,et al.  Short-time behavior of the diffusion coefficient as a geometrical probe of porous media. , 1993, Physical review. B, Condensed matter.

[12]  P. Callaghan Principles of Nuclear Magnetic Resonance Microscopy , 1991 .

[13]  J. E. Tanner,et al.  Spin diffusion measurements : spin echoes in the presence of a time-dependent field gradient , 1965 .

[14]  D. Yablonskiy,et al.  MR imaging of diffusion of 3He gas in healthy and diseased lungs , 2000, Magnetic resonance in medicine.

[15]  S. Patz,et al.  Probing porous media with gas diffusion NMR. , 1999, Physical review letters.

[16]  John Crank,et al.  The Mathematics Of Diffusion , 1956 .

[17]  C. Kittel Introduction to solid state physics , 1954 .

[18]  D G Cory,et al.  The narrow pulse approximation and long length scale determination in xenon gas diffusion NMR studies of model porous media. , 2002, Journal of magnetic resonance.

[19]  E J van Beek,et al.  Pulmonary ventilation imaged by magnetic resonance: at the doorstep of clinical application. , 2001, The European respiratory journal.

[20]  T. L. James,et al.  CHAPTER 2 – PRINCIPLES OF NUCLEAR MAGNETIC RESONANCE , 1975 .

[21]  C. H. Neuman Spin echo of spins diffusing in a bounded medium , 1974 .