Abstract
The relationship between fat thickness tfat and current density magnitude |iφ| has been clarified by coupling of electromagnetic simulation and electrical impedance tomography (ES-EIT) under electrical muscle stimulation (EMS) in three responsive calf muscle compartments which are called M1 compartment of gastrocnemius muscle, M2 compartment of tibialis anterior, extensor digitorum longus, and peroneus longus muscles, and M3 compartment of soleus muscle. ES-EIT images the current density magnitude |iφ| from the conductivity distribution σ reconstructed by EIT for the decision of optimum voltage intensity \({\boldsymbol{\varphi }}_{\mathbf{O}\mathbf{V}\mathbf{I}}^{\mathbf{i}}\) of EMS. As a result, the highest sensitivity of |iφ| to fat thickness tfat is M1, the physiological-induced conductive response in M2 depends not only on the |iφ|, but also on the muscle mechanical motion. The Pearson correlation coefficient (PCC) r between spatial-mean current density magnitude <|iφ|> and spatial-mean conductivity difference Δ < σφ−pre> in M1, M2 and M3 shows high correlation under EMS. The tfat and |iφ| are negatively correlated in muscle compartments of each subject. The individual tfat and |iφ| are negatively correlated in muscle compartments of each subject because the fat layer becomes an obstacle against |iφ| from the skin to the subcutaneous tissue. As a discussion, the optimum voltage intensity \({\boldsymbol{\varphi }}_{\mathbf{O}\mathbf{V}\mathbf{I}}^{\mathbf{i}}\) and \({\boldsymbol{\varphi }}_{\mathbf{O}\mathbf{V}\mathbf{I}}^{{\varvec{\upsigma}}}\) of M1 are defined as the highest point of second-order difference of spatial-mean current density magnitude \(\langle {\left.\frac{{\partial }^{2}\left|{\mathbf{i}}_{\boldsymbol{\varphi }}^{{\varvec{M}}1}\right|}{\partial {\boldsymbol{\varphi }}^{2}}\right|}_{\boldsymbol{\varphi }}\rangle\) and spatial-mean conductivity \(\langle {\left.\frac{{\partial }^{2}{{\varvec{\upsigma}}}_{\boldsymbol{\varphi }}^{{\varvec{M}}1}}{\partial {\boldsymbol{\varphi }}^{2}}\right|}_{\boldsymbol{\varphi }}\rangle\) under EMS, which are increased with the increase in tfat. The absolute difference |ΔφOVI| between \({\boldsymbol{\varphi }}_{\mathbf{O}\mathbf{V}\mathbf{I}}^{\mathbf{i}}\) and \({\boldsymbol{\varphi }}_{\mathbf{O}\mathbf{V}\mathbf{I}}^{{\varvec{\upsigma}}}\) is decreased with increasing tfat, which is due to the fact that the effect of EMS loading voltage on muscle diminishes with increasing tfat, thus reducing the effect of muscle quality on the results of optimum voltage intensity calculations.
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Acknowledgements
This work was supported by JST SPRING, Grant Number JPMJSP2109. This work was partly supported by JSPS under postdoctoral fellowship of Japan society for the promotion of science (JSPS). The authors would like to thank Dr. Marlin Ramadhan Baidillah and Mr. Prima Asmara Sejati of Chiba University for suggestion and assistance with the experiments.
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According to Chiba University ethical code, all subjects gave written informed consent for the study after receiving a detailed explanation for the purposes, potential benefits, and risks associated with participation. All study procedures were conducted in accordance with the Declaration of Helsinki and research code of ethics of Chiba University, and were approved by the Committee for Human Experimentation of Chiba University. The number of ethical approvals for our experiments by the committee of human experimentation of Chiba University is 29–13.
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Sun, B., Darma, P.N., Ikeda, K. et al. Relationship between fat thickness and current density magnitude in calf muscles compartments under electrical muscle stimulation (EMS) by coupling of electromagnetic simulation and electrical impedance tomography (ES-EIT). J Vis 26, 1375–1388 (2023). https://doi.org/10.1007/s12650-023-00932-4
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DOI: https://doi.org/10.1007/s12650-023-00932-4