Myelin Water Imaging: Multiple Compartmental Model
Irene Vavasour1
1University of British Columbia, Canada

Synopsis

Myelin is composed of alternating layers of lipid bilayers with water in between. The multiple proton compartments in white matter can be modeled as four pools (myelin water, intra/extracellular water, myelin non-aqueous and non-myelin non-aqueous) which have different exchange properties. The water within the myelin bilayers can be measured using its shorter T1 and T2 relaxation time.

Target Audience

Clinicians and imaging scientists interested in myelin water imaging.

Highlights

- White matter can be modeled with 4 proton pools
- The water pools can be separated based on their relaxation times
- There is exchange between the proton pools which may affect the myelin water fraction

White Matter Models

Myelin water imaging (MWI), as the name implies, refers to imaging the signal from water associated with myelin. Myelin itself is a complex system consisting of alternating lipid bilayers and water, termed “myelin water” (Figure 1). White matter also contains water in other physical spaces, for example inside and outside of axons, termed “intra/extracellular (IE) water.” Because multiple water reservoirs exist in white matter, the MR relaxation signal cannot be accurately fit by a single exponential component. Many studies have employed a 4 pool- model (Figure 2) which includes 2 water pools (myelin water and IE water) and 2 non-aqueous proton pools (myelin and non-myelin)1, each with their own relaxation times. These pools exchange magnetisation with one another either through diffusion or cross relaxation. Due to myelin water’s close interaction with non-aqueous protons, it has a shorter T2 than IE water­­­­2. Using MWI, we can quantify this water pool thereby obtaining an in vivo measure of myelin2-5.

MWI techniques

Excellent reviews of MWI techniques can be found in 6,7. Some of the most common approaches include:

Multi spin-echo T2 relaxation2 - Multi spin-echo T2 is often considered the “gold standard” MWI technique. It consists of a modified Carr-Purcell-Meiboom-Gill (CPMG) sequence, typically including 32 echoes with 10ms echo spacing. At each voxel, the T2 decay curve is fit by multiple exponential components using non-negative least squares (NNLS) with stimulated echo correction. For in-vivo measurements at 3T, the myelin water fraction (MWF) is defined as the area under the T2 distribution between 0-40ms divided by the total area (Figure 3).

Combined GRAdient and Spin Echo (GRASE)8 - By collecting higher order k-space lines with gradient echoes, the CPMG sequence is accelerated.

T2 Preparation methods9,10- The signal is “prepared” with a particular T2-weighting before full-volume sampling, allowing for efficient data acquisition at selected TE times.

Multi-gradient echo (MGRE)11,12 - Decay curves are generated from T2* instead of T2 decays. T2* can be collected with shorter echo spacing allowing for more data points at early times when fast relaxing myelin water still has signal.

mcDESPOT13 - Steady state imaging is used with a variety of flip angles to characterise T1 and T2 for different water pools using a complex model.

Multi-component T114,15 / ViSTa16 - By careful sequence preparation, it is possible to extract multiple T1 components in white matter. A short T1 component has been attributed to myelin water; this component may be probed by supressing the IE water using a double inversion recovery such as the direct visualization of short transverse relaxation time component (ViSTa) approach.

Some limitations of MWI techniques

Stimulated echoes – if refocusing pulses are not 180°, some magnetisation becomes trapped along the longitudinal axis until a later pulse transfers it back into the transverse plane; this effect leads to stimulated echoes which corrupt the exponential signal decay. Stimulated echo artifacts can be corrected17.

T1 weighting – insufficient delay between excitation pulses results in T1 weighting. If TR is too short, then the measured MWF may be artificially increased18.

Magnetisation transfer effects – multi-slice acquisition techniques may result in magnetisation transfer effects due to off-resonance pulses from other slices, complicating signal decay.

Iron – the removal of iron from post-mortem samples leads to a decrease in the MWF. If iron removal beyond that contained within myelin decreases MWF, it may be possible that MWF is related to more than just myelin19.

Model limitations – assumptions about the number of water pools, expected relaxation time ranges, exchange between water pools, and Rician/Gaussian noise, all have an effect on estimated MWFs.

Further exploring white matter models with NMR experiments

The non-aqueous proton signal is MRI invisible since it decays within 100µs. However, using an NMR spectrometer, it is possible to measure the signal from both aqueous and non-aqueous protons. Two studies fitted the 4 pool model to T1 and T2 results from ex-vivo bovine brain15,20. The water signal exhibited 4 components corresponding to the 4 pools but with different weightings due to exchange15. The two shortest T1 times were close to the T2 times for myelin water and intra/extracellular water, suggesting that the T2 relaxation of myelin water and IE water is largely driven by magnetisation exchange with the corresponding non-aqueous pools.

Probing proton pool exchange in vivo

To explore exchange between the proton pools in human white matter in vivo, multi-echo T2 has been combined with an MT prepulse. Since myelin water is in close contact with the non-aqueous myelin pool, the MT effect was larger for myelin water21. By varying the time between the prepulse and the multi-echo sequence, the exchange rate between the water pools can be estimated22. Exchange modelling can also be achieved by modulating the amplitude of the MT pulse as well as changing the saturation pulse duration1. Evidence that exchange rates between the water pools is influenced by myelin thickness was found by comparing rat optic nerve and sciatic nerve23,24. If the exchange rate is fast, then the MWF will be reduced. For in-vivo MWI on white matter, the effect of exchange on the MWF is still being debated.

Conclusions

White matter can be modeled as 4 pools, each with unique relaxation times and exchange rates. The myelin water pool is assigned to water trapped between myelin bilayers and can be measured using many different MR techniques. By measuring the myelin water, we are able to gain insight into tissue microstructure which is invaluable in the study of development and many neurological diseases. For further discussion on the use of relaxation in characterising brain tissue microstructure refer to this review paper25.

Acknowledgements

I would like to thank the UBC MRI Research Centre.

References

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Figures

Figure 1: Schematic representation of myelin structure including an EM image of a myelinated axon (C Laule and GRW Moore, Brain Pathology 2018)

Figure 2: Four-pool model for white matter with arrows indicating magnetisation exchange between compartments

Figure 3: T2 distribution from white matter and an example myelin water fraction image

Proc. Intl. Soc. Mag. Reson. Med. 28 (2020)