Model Selection in Magnetic Resonance Imaging Measurements of Vascular Permeability: Gadomer in a 9L Model of Rat Cerebral Tumor

Author:

Ewing James R12,Brown Stephen L3,Lu Mei4,Panda Swayamprava1,Ding Guangliang1,Knight Robert A1,Cao Yue5,Jiang Quan1,Nagaraja Tavarekere N6,Churchman Jamie L1,Fenstermacher Joseph D6

Affiliation:

1. Department of Neurology, Henry Ford Health Systems, University of Michigan, Detroit, Michigan, USA

2. Department of Radiology, Henry Ford Health Systems, University of Michigan, Detroit, Michigan, USA

3. Department of Radiation Oncology, Henry Ford Health Systems, University of Michigan, Detroit, Michigan, USA

4. Department of Biostatistics and Research Epidemiology, Henry Ford Health Systems, University of Michigan, Detroit, Michigan, USA

5. Departments of Radiation Oncology and Radiology, Henry Ford Health Systems, University of Michigan, Detroit, Michigan, USA

6. Department of Anesthesiology, Henry Ford Health Systems, University of Michigan, Detroit, Michigan, USA

Abstract

Vasculature in and around the cerebral tumor exhibits a wide range of permeabilities, from normal capillaries with essentially no blood-brain barrier (BBB) leakage to a tumor vasculature that freely passes even such large molecules as albumin. In measuring BBB permeability by magnetic resonance imaging (MRI), various contrast agents, sampling intervals, and contrast distribution models can be selected, each with its effect on the measurement's outcome. Using Gadomer, a large paramagnetic contrast agent, and MRI measures of T1, over a 25-min period, BBB permeability was estimated in 15 Fischer rats with day-16 9L cerebral gliomas. Three vascular models were developed: (1) impermeable (normal BBB); (2) moderate influx (leakage without efflux); and (3) fast leakage with bidirectional exchange. For data analysis, these form nested models. Model 1 estimates only vascular plasma volume, vD, Model 2 (the Patlak graphical approach) vD and the influx transfer constant K1- Model 3 estimates vD, Ki and the reverse transfer constant, kb, through which the extravascular distribution space, ve, is calculated. For this contrast agent and experimental duration, Model 3 proved the best model, yielding the following central tumor means (±s.d.; n = 15): vD = 0.07±0.03 for Ki = 0.0105±0.005 min −1 and ve = 0.10±0.04. Model 2 Ki estimates were approximately 30% of Model 3, but highly correlated ( r 0.80, P<0.0003). Sizable inhomogeneity in vD, Ki and kb appeared within each tumor. We conclude that employing nested models enables accurate assessment of transfer constants among areas where BBB permeability, contrast agent distribution volumes, and signal-to-noise vary.

Publisher

SAGE Publications

Subject

Cardiology and Cardiovascular Medicine,Neurology (clinical),Neurology

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