MR Contrast Due to Microscopically Heterogeneous Magnetic Susceptibility: Numerical Simulations and Applications to Cerebral Physiology

We calculate the effects of subvoxel variations in magnetic susceptibility on MR image intensity for spin‐echo (SE) and gradient‐echo (GE) experiments for a range of microscopic physical parameters. The model used neglects the overlap of gradients from one magnetic inclusion to the next, and so is valid for low volume fractions and weak perturbations of the magnetic field. Transverse relaxation is predicted to deviate significantly from linear exponential decay in both SE and GE at a particle radius of 2.5 μm. Calculated changes in transverse relaxation rates for SE and GE increase linearly with volume fraction of high‐susceptibility regions of 5 μm diameter, but increase with about the 3/2 power of volume fraction of regions with 15 μm spacing between centers. This sensitivity to the actual size and spacing of magnetized regions may allow them to be measured on the basis of contrast, without being resolved in images. GE and SE decay rates are approximately twice as sensitive to long cylinders of 5 μm diameter than to spheres of the same size, for diffusion constants of 2.5 μm2/ms. Calculated changes in transverse decay rates increase with approximately the square of field and susceptibility variation for 5‐μm spheres and a diffusion constant of 2.5 μm2/ms. This exponent is smaller for cylindrical magnetized regions of the same size, and also depends on the diffusion constant. We discuss possible applications of our theoretical results to the analysis of the effects of high‐susceptibility contrast agents in brain. Experimental data from the literature are compared with calculated signal changes according to the model. The monotonic dependence of decay rates on the volume of distribution of the contrast agent suggests that cerebral blood volume and flow could be measured using MR contrast. © 1991 Academic Press, Inc.

[1]  L. Josephson,et al.  The effects of iron oxides on proton relaxivity. , 1988, Magnetic resonance imaging.

[2]  John C. Gore,et al.  Studies of diffusion in random fields produced by variations in susceptibility , 1988 .

[3]  R B Buxton,et al.  Susceptibility induced MR line broadening: applications to brain iron mapping. , 1988, Journal of computer assisted tomography.

[4]  B. Rosen,et al.  Dynamic imaging with lanthanide chelates in normal brain: Contrast due to magnetic susceptibility effects , 1988, Magnetic resonance in medicine.

[5]  S. H. Koenig,et al.  Transverse relaxation of solvent protons induced by magnetized spheres: Application to ferritin, erythrocytes, and magnetite , 1987, Magnetic resonance in medicine.

[6]  Alan H. Morris,et al.  A mathematical model of diamagnetic line broadening in lung tissue and similar heterogeneous systems: Calculations and measurements , 1987 .

[7]  T J Brady,et al.  Ferrite particles: a superparamagnetic MR contrast agent for the reticuloendothelial system. , 1987, Radiology.

[8]  G M Bydder,et al.  Clinical magnetic susceptibility mapping of the brain. , 1987, Journal of computer assisted tomography.

[9]  R R Edelman,et al.  Contrast in rapid MR imaging: T1- and T2-weighted imaging. , 1987, Journal of computer assisted tomography.

[10]  Z H Cho,et al.  An improved nuclear magnetic resonance diffusion coefficient imaging method using an optimized pulse sequence. , 1986, Medical physics.

[11]  P. Grenier,et al.  MR imaging of intravoxel incoherent motions: application to diffusion and perfusion in neurologic disorders. , 1986, Radiology.

[12]  R R Edelman,et al.  MR of hemorrhage: a new approach. , 1986, AJNR. American journal of neuroradiology.

[13]  D Matthaei,et al.  Dynamic digital subtraction imaging using fast low-angle shot MR movie sequence. , 1986, Radiology.

[14]  P. Lauterbur,et al.  Ferromagnetic particles as contrast agents for magnetic resonance imaging of liver and spleen , 1986, Magnetic resonance in medicine.

[15]  P. Röschmann,et al.  Susceptibility artefacts in NMR imaging. , 1985, Magnetic resonance imaging.

[16]  P C Lauterbur,et al.  Nuclear magnetic resonance technology for medical studies. , 1984, Science.

[17]  W. T. Dixon Simple proton spectroscopic imaging. , 1984, Radiology.

[18]  R. Sepponen,et al.  A Method for Chemical Shift Imaging: Demonstration of Bone Marrow Involvement with Proton Chemical Shift Imaging , 1984, Journal of computer assisted tomography.

[19]  B. Rosen,et al.  Nuclear magnetic resonance: in vivo proton chemical shift imaging. Work in progress. , 1983, Radiology.

[20]  G. Pawlik,et al.  Quantitative capillary topography and blood flow in the cerebral cortex of cats: an in vivo microscopic study , 1981, Brain Research.

[21]  B. Siesjö,et al.  Cerebral Blood Flow and Oxygen Consumption in the Rat Brain during Extreme Hypercarbia , 1979, Anesthesiology.

[22]  J. Freed Dynamic effects of pair correlation functions on spin relaxation by translational diffusion in liquids. II. Finite jumps and independent T1 processes , 1978 .

[23]  O B Paulson,et al.  Filtration and diffusion of water across the blood-brain barrier in man. , 1977, Microvascular research.

[24]  M E Raichle,et al.  Evidence of the Limitations of Water as a Freely Diffusible Tracer in Brain of the Rhesus Monkey , 1974, Circulation research.

[25]  K. J. Packer The effects of diffusion through locally inhomogeneous magnetic fields on transverse nuclear spin relaxation in heterogeneous systems. Proton transverse relaxation in striated muscle tissue , 1973 .

[26]  Baldwin Robertson,et al.  Spin-Echo Decay of Spins Diffusing in a Bounded Region , 1966 .

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

[28]  H. Pfeifer Der Translationsanteil der Protonenrelaxation in wäßrigen Lösungen paramagnetischer Ionen , 1961 .

[29]  E. Purcell,et al.  Effects of Diffusion on Free Precession in Nuclear Magnetic Resonance Experiments , 1954 .