Kyeongseon Min1, Tan Toi Phan2,3, Sungkwon Chung4, Jongho Lee1, Seung-Kyun Lee2,3, and Jang-Yeon Park2,3
1Laboratory for Imaging Science and Technology, Department of Electrical and Computer Engineering, Seoul National University, Seoul, Korea, Republic of, 2Department of Biomedical Engineering, Sungkyunkwan University, Suwon, Korea, Republic of, 3Center for Neuroscience Imaging Research, Institute for Basic Science, Suwon, Korea, Republic of, 4Department of Physiology, Samsung Biomedical Research Institute, Sungkyunkwan University School of Medicine, Suwon, Korea, Republic of
Synopsis
In this
study, the effects of membrane potential on T1 and T2 were examined using Jurkat T lymphocytes. We applied tetraethylammonium
ion (TEA) to depolarize
Jurkat cell membrane potential. Significant changes in T1 and T2, which were measured to be -10.39 ms/mM and 0.920 ms/mM, respectively, were observed.
One potential explanation for the changes of T1 and T2 is
the depolarization of membrane potential, while the underlying mechanism needs
to be explored. Further studies are expected to utilize the membrane potential
as a new contrast mechanism for MRI.
Introduction
Direct
detection of neuronal activity in MRI has the potential to
provide better spatiotemporal localization of neuronal activity than
conventional fMRI which utilizes hemodynamic response. While it has been
studied by many groups, most works focused on the locally induced magnetic
field by the neuronal current.1-3 Recently,
studies by Lee et al.4 and Phan et al.5 demonstrated that a line-scanning FLASH sequence with
a very high temporal resolution (~5 ms) enables direct detection of neuronal
activity. While the contrast mechanism is not fully elucidated, the authors
suggested that T1 and/or T2 change during action
potential might be responsible for these observations. This
study aims to investigate the changes in T1 and/or T2
could be explained by the change in the cell membrane potential.Method
Cell culture preparation. We
used Jurkat cells (immortalized human T lymphocyte cells) as the experiment
model. The
Jurkat cells were cultured in RPMI 1640 medium with 10% fetal bovine serum and
1% penicillin/streptomycin (denoted as RPMI medium hereafter) at 37 °C and 5% CO2 in the air. Immediately before MRI acquisition, the cell density of the suspension was adjusted to 2.1 × 107 cells/ml.
Resting potential manipulation. We applied a few concentrations of tetraethylammonium ion (TEA; i.e., 0, 10, 20, 30
mM) on the Jurkat cell suspension to depolarize the membrane potential of
Jurkat cells. For a control test, the RPMI media of the same TEA concentrations
were prepared, assessing the effect of TEA on T1 and/or T2
change. The cell
suspensions were kept at a stable temperature of 34 °C in the MRI scanner. The experimental
specifications are detailed in Fig. 1a.
MRI acquisition and analysis. Experiments were performed on a Bruker
9.4 T animal MRI scanner. For T1 estimation, a RARE sequence with
varying TR was used. Voxel-wise T1 values were obtained by fitting
magnitude data to a mono-exponential recovery function. For T2
estimation, a multi-echo spin-echo sequence was used. Voxel-wise T2
values were obtained by fitting magnitude data to an extended phase graph (EPG)
corrected6 exponential decay curve. Fig. 1b lists all the relevant
scan parameters. The regions of interest (ROIs) were set as circles at the center of each tube containing Jurkat cell suspension or RPMI medium. Since there is no available theoretical prediction of the
relationship between the relaxation times and TEA concentration, the linear
fitting was performed.Results
T1
and T2 maps at varying TEA concentrations from 0 to 30 mM were
displayed in Figs. 2a and b. Their averages and standard deviations in the
ROIs were presented in Figs. 3a and b. As shown in Fig. 3, T1 showed a negative linear
correlation with TEA concentration (red line, R2 = 0.72, slope =
-10.39 ms/mM), whereas T2 showed a positive linear correlation (red
line, R2 = 0.73, slope = 0.920 ms/mM). In the case of the RPMI
medium itself (blue lines), no significant change in T1 but a slight
increase of T2 was observed (R2 = 0.50, slope = 0.557
ms/mM). The difference in the slopes of T2 versus TEA concentration was
0.363 ms/mM.Discussion
Relaxation times of the Jurkat cell
suspension without TEA. The
Jurkat cell suspension with no TEA had longer T1 and shorter T2
than the RPMI medium, implying that the addition of the Jurkat cells into the
RPMI medium increased T1 but decreased T2. The increased
T1 was somewhat counter-intuitive as the presence of cells might
decrease T1 due to the interaction. This observation may indicate
that the intracellular water of the Jurkat cells has longer T1 and
shorter T2 than those of the RPMI medium.
Interpretation of the TEA effects on the
relaxation times. Our
hypothesis for the results is that the depolarization of the membrane potential
could result in decreased T1 and increased T2. According
to the recent work by Tarun et al.7, a change
in the membrane potential can induce a change in the amount of the membrane
water molecules, which are anisotropically oriented by the membrane potential. If such a change of membrane water is
measurable in MRI, it could be measured in terms of the
relaxation times. Another possibility is osmosis, which would act to cause the
net efflux of the intracellular water to the extracellular medium, resulting in
decreased T1 and increased T2.Conclusion
The
motivation of this study was to examine the effects of the cell membrane potential on the relaxation times.
According to our study, a significant change in T1 and T2
of the Jurkat cell suspension was observed when TEA was applied to the cell
suspension. A further study is warranted for elucidating the underlying
mechanism of the relaxation-time change due to the depolarization of the
membrane. It is expected that the new contrast mechanism introduced here, which
seems to be related to the membrane potential, might open up a new opportunity
for functional MRI that allows direct detection of the neuronal activity with a
high spatial and temporal resolution.Acknowledgements
This
research was supported by the Brain Research Program through the National Research
Foundation of Korea (NRF) funded by the Ministry of Science, ICT & Future
Planning (NRF-2019M3C7A1031993, NRF-2019M3C7A1031994).
This work
was supported by the Brain Korea 21 Plus Project in 2019.
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