Brain Topography

, Volume 3, Issue 1, pp 143–150 | Cite as

Do optimal Dipoles obtained by the Dipole Tracing Method slways suggest true source locations?

  • Toshimitsu Musha
  • Saburo Homma
Article

Summary

Scalp potentials generated by a concentrated electric source in the brain are very similar to potentials generated by an electric dipole at the source position. In this sense a concentrated source in the brain is modelled as an electric dipole. When the source is diffuse such a dipole which best approximates the scalp potential is called an optimal dipole. Its position is calculated by the Dipole Tracing Method based on a realistic head model with homogeneous electric conductivity. There are 2 major difficulties inherent in this method: (1) The low electric conductivity of the skull causes systematic shifts of the optimal dipole positions from the true positions of concentrated sources; (2) the optimal dipoles cannot specify diffuse source positions. The first difficulty is overcome by using the numerical correction obtained by comparing the known dipole positions generated within a human head with their optimal ones. The second difficulty is removed to a certain extent by comparing the optimal dipole positions obtained with the 1-dipole and 2-dipole models together with their dipolarity. We have obtained criteria for the validity of the dipole approximation and source concentration.

Key words

Dipole tracing method Realistic head model Optimal dipole Dipole Subdural electrode Inhomogeneous conductivity 

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References

  1. Ary, J.P., Klein, S.A. and Fender, D.H. Location of sources of evoked potentials: corrections for skull and scalp thickness. IEEE Trans. Biomed. Eng., 1981, BME-28: 447–452.Google Scholar
  2. He, B., Musha, T., Okamoto, Y., Homma, S., Nakajima, Y. and Sato, T. Electric dipole tracing in the brain by means of the boundary element method and its accuracy. IEEE Trans. Biomed. Eng., 1987, BME-34: 406–414.Google Scholar
  3. He, B. and Musha, T. Effects of cavities on EEG dipole localization and their relations with surface electrode positions, Int. J. Biomed. Comput., 1989, 24: 269–282.PubMedGoogle Scholar
  4. Homma, S. and Musha, T. New imaging method of brain functions- Evoked potentials in human brain. Nakayama Shoten. In: Taisha, 1989, 26: 67–72.Google Scholar
  5. Homma, S., Nakajima, Y., Musha, T., Okamoto, Y., Hagbarth,K.-E., Blom, S. and Flink, R. Generator mechanism of epileptic potentials analyzed by dipole tracing method, Neuroscience Letters, 1990, 113: 181–186.PubMedGoogle Scholar
  6. Homma, S., Nakajima, Y., Musha, T., He, B. and Okamoto, Y. Dipole-tracing of ‘awareness’ attenuating the cortical components of somatosensory evoked potentials. Neuroscience Letters, 1988, 88: 257–262.PubMedGoogle Scholar
  7. Musha, T. and Takakura, K. Diagnosis of epileptic focus by means of the dipole tracing (DT) method. In: K. Takakura (Ed.), Recent Examinations for Neurological Disorders. Gendai Iryousha, Tokyo, 1989: 183–192.Google Scholar
  8. Nakajima, Y., Homma, S., Musha, T., Okamoto, Y., Ackerman, R.H., Correia, J.A. and Alpert, N.M. Dipole tracing of abnormal slow brain potentials after cerebral stroke-EEG, PET, MRI correlations. Neuroscience Letters, 1990, 112: 59–64.PubMedGoogle Scholar
  9. Rush, S. and Driscoll, D.A. Current distribution in the brain from surface electrodes. Anesthesia and Analgesia, Current Researches, 1968, 47: 717–723.Google Scholar
  10. Rush, S. and Driscoll, D.A. EEG electrode resistivity - An application of reciprocity. IEEE Trans. Biomed. Eng., 1969, BME-16: 15–22.Google Scholar

Copyright information

© Human Sciences Press 1990

Authors and Affiliations

  • Toshimitsu Musha
    • 1
  • Saburo Homma
    • 2
  1. 1.Department of Applied ElectronicsTokyo Institute of TechnologyNagatsuta, Midoriku, YokohamaJapan
  2. 2.Department of PhysiologySchool of Medicine, Chiba UniversityChibaJapan

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