Olga Schimpf1, Stefan Hindel1, and Lutz Lüdemann1
1Strahlenklinik, Med. Physik, Universitätsklinikum Essen, Essen, Germany
Synopsis
Compartmental models for evaluation of dynamic contrast-enhanced
magnetic resonance imaging (DCE-MRI) datasets assume a homogeneous
interstitital volume distribution and homogeneous contrast agent
(CA) distribution within each compartment, neglecting effects of CA
diffusion within the compartments. When necrotic or
micronecrotic tumor tissue is present, these assumptions may no longer be
valid. Therefore, the present study investigates the validity of three
compartmental models in assessing tumors with necrotic components.
Introduction
Dynamic contrast-enhanced
magnetic resonance imaging (DCE-MRI) typically uses low-molecular-weight
contrast agents (LMWCAs). These LMWCAs extravasate instantaniously into the
interstitial space, also known as the extravascular extracellular space. To
assess enhancement after contrast agent administration, several pharmacokinetic
compartmental models are used [1,2]. The most
popular pharmacokinetic compartmental model is the so-called Tofts model [3], which uses a transfer constant to assess contrast enhancement.
All of these models assume a homogeneous tracer concentration within each
compartment and do not take diffusion effects into account.
Compartmental models for evaluation of dynamic contrast-enhanced
magnetic resonance imaging (DCE-MRI) datasets assume a homogeneous
interstitital volume distribution and homogeneous contrast agent
(CA) distribution within each compartment, neglecting effects of CA
diffusion within the compartments. When necrotic or
micronecrotic tumor tissue is present, these assumptions may no longer be
valid. Therefore, the present study investigates the validity of three
compartmental models in assessing tumors with necrotic components.Material and Methods
The general diffusion equation for inhomogeneous tissue was used to simulate
the extravasation of a low-molecular-weight contrast agent from a feeding
vessel into the interstitial space. The simulation was performed in 2D assuming
cylindrical symmetry (see Fig.1). Two tissue slices with lengths of L=100μm and L=150μm were
investigated. Local fractional interstitial volumes of 5%, 10%, 15%, 20%, and 25%
were simulated for viable tissue and volumes of 50% and 100% for necrotic
tissue. The radius of the necrotic area was varied between 10μm and 70μm for L=100μm
and between 10μm and 100μm for L=150μm in steps of 10μm. The simulated concentration-time
curves were evaluated using the extended Tofts model, a parallel 3-compartment model,
and a sequential 3-compartment model.
Results
The permeability and Ktrans calculated by using the Tofts model in a homogen tissue underestimates the actual input by more than a decade (see Fig. 2). For the simulations in inhomogen tissue with L=100μm, the extended Tofts-model and the parallel
3-compartment model failed to provide an interstitial volume fraction of less than
100% in 11% of cases, while the sequential 3-compartment model provided
interstitial volume fractions of less than 100% for all concentration-time
curves. The extended Tofts model overestimated the interstitial volume fraction
by a median of 6.9%, the parallel 3-compartment model by 8.6%, and the
sequential 3-compartment model by 0.2%. For the simulations with L=150μm, the
extended Tofts model failed in 26% of cases to provide an interstitial volume
fraction of less
than 100%, the parallel 3-compartment model in 25%, and the sequential
3-compartment model in 7%. The extended
Tofts model overestimated the interstitial volume fraction by a median of 10.0%
and the parallel 3-compartment model by 15.5%, while the sequential
3-compartment model underestimated it by 18.8%. Overall, the sequential
3-compartment
model provided more reliable results both for the total fractional
interstitial volume and for the interstitial subcompartments.
Conclusions
Our results show that the sequential 3-compartmental model is more
suitable than the other two models for assessing contrast medium
dynamics in inhomogeneous tissues such as tumors, having the lowest
relative and absolute error rates in determining interstitial volume.
The F-test has shown that the sequential model significantly
better fits the concentration–time curve in heterogeneous tissue than
the other two models. The
sequential 3-compartment model yields smaller absolute deviations in
determining the rapidly and slowly equilibrating interstitial components
compared with the parallel 3-compartment model. Thus, the sequential
model has the greatest potential to separate the fast and slow
interstitial volumes in dynamic magnetic resonance imaging. On the other
hand the current study shows that the sequential 3-compartment model is
only a rough approximation and has to be improved.Acknowledgements
No acknowledgement found.References
- Sourbron S.P., Buckley D.L. Classic models for dynamic contrast-enhanced MRI. NMR Biomed. 2013;26(8):1004–1027
- Bergamino M., Bonzano L.,
Levrero F., Mancardi G.L., Roccatagliata L. A review of technical
aspects of T1-weighted dynamic contrast-enhanced magnetic resonance
imaging (DCE-MRI) in human brain tumors. Phys Med. 2014;30(6):635–643
- Tofts P.S., Brix G., Buckley
D.L., Evelhoch J.L., Henderson E., Knopp M.V. Estimating kinetic
parameters from dynamic contrast-enhanced T1-weighted MRI of a diffusable tracer: standardized quantities and symbols. J Magn Reson Imaging. 1999;10:223–232