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“Modeling of Electric Field and Joule Heating in
Breast Tumor during Electroporation”
Departamento de Ingeniería Eléctrica, CINVESTAV
Sección Bioelectrónica.
CONACYT Instituto Nacional de Rehabilitación Subdivisión de Investigación
Biotegnológica
Instituto de Enfermedades de la Mama- FUCAM, Mexico City, Mexico.
2016 13th International Conference on Electrical Engineering, Computing Science and
Automatic Control (CCE), Mexico, City. Mexico. September 26-30, 2016.
C. A. Ramírez Martínez*, A. L. Vera Tizatl, C. E. Vera Tizatl, P. R. Hernández Rodríguez, A. Vera
Hernández, L. Leija Salas, M. I. Gutiérrez Velasco, S. A. Rodríguez Cuevas
• Introduction
• Methodology
• Results
• Conclusion
2016 13th International Conference on Electrical Engineering, Computing Science and Automatic Control (CCE), Mexico, City. Mexico. September 26-30, 2016.
2
Contents
• In this work, it is presented a simulation of a breast carcinoma
embedded in healthy tissue under an electric field exposure through
steel electrodes.
• These work seeks to observe the current density and the
temperature rise in both tissues.
Introduction
𝛁 𝛔 + 𝛆
𝛛
𝛛𝐭
𝛁𝚿(𝐱, 𝐲, 𝐳, 𝐭) = 𝟎 (𝟏)
Fig. 1. Exposure of a spherical cell with
radius R, thickness membrane d within an
electric field.
∆𝚿 𝐦 = 𝛂𝐄𝐑𝐜𝐨𝐬𝛉 (𝟐)
𝛂 =
𝟑𝛔 𝐞 𝟑𝐝𝐑 𝟐
𝛔𝐢 + (𝟑𝐝 𝟐
𝐑 − 𝐝 𝟑
) 𝛔 𝐦 − 𝛔𝐢
𝟐𝐑 𝟑 𝛔 𝐦 + 𝟐𝛔 𝐞 𝛔 𝐦 +
𝟏
𝟐
𝛔𝐢 − 𝟐 𝐑 − 𝐝 𝟑(𝛔 𝐞−𝛔 𝐦)(𝛔𝐢−𝛔 𝐦)
(𝟑)
The spatial and temporal distribution of the electrical potential in a medium, is given by Eq. 1 [Tizatl, A.L.V., et al. 3D model and
simulation of electroporation application on healthy and tumoral breast tissue. in Electrical Engineering, Computing Science and
Automatic Control (CCE), 2013 10th International Conference on. 2013..].
Methodology
2016 13th International Conference on Electrical Engineering, Computing Science and Automatic Control (CCE), Mexico, City. Mexico. September 26-30, 2016.
4
𝒒
~
==
𝑬 𝟐
𝑳 𝟐
𝝈
𝝈 𝟎 𝑽𝒂 𝟐
(𝟕)
𝜵 𝟐
𝑻 − 𝒘 𝒃
𝒄𝑳 𝟐
𝒌
𝑻 + 𝒒
~
=
𝜹𝑻
𝜹𝒕
(𝟖)
2016 13th International Conference on Electrical Engineering, Computing Science and Automatic Control (CCE), Mexico, City. Mexico. September 26-30, 2016.
5
Figure 2. A tumor tissue of 1 cm in diameter (1), inside
healthy tissue of 8 cm diameter is proposed (2). Two
stainless steel electrodes 1.2 mm diameter (3).
The joule heating energy term is given by Eq. 7 [Van Gemert, M.J., et al., Irreversible electroporation: just another form of thermal therapy? Prostate, 2015.
75(3): p. 332-5.]. The heat transfer in tissue is given by Eq. 8 [Becker, S.M. and A.V. Kuznetsov, Thermal damage reduction associated with in vivo skin
electroporation: A numerical investigation justifying aggressive pre-cooling. International Journal of Heat and Mass Transfer, 2007. 50(1-2): p. 105-116.]
Material
Health
tissue
Tumoral
tissue
Units
Electrical
conductivity
0.5 0.03 S/m
Relative
permittivity
123 80 1
Thermal
conductivity
0.49 0.5 W/(m*K)
Density 1090 1000 kg/m^3
Heat capacity 3421 4000 J/(kg*K)
Table 1 Material proprieties in adiabatic form [2].
1 2
3
The initial conditions to the phenomena were in
37-celsius degrees and the boundaries of the
health tissue are in 25-celcius degrees.
MESHING GEOMETRY
6
Figure 3. The solver used was adjusted to display the electric field distribution applied by the boundary electrodes
inside the both kinds of tissue .
,
2016 13th International Conference on Electrical Engineering, Computing Science and Automatic Control (CCE), Mexico, City. Mexico. September 26-30, 2016.
Results
7
Figure 4. Electrical Potential thought tumoral tissue. Figure 5 . Electric field distribution and current
density in breast tissue.
,
2016 13th International Conference on Electrical Engineering, Computing Science and Automatic Control (CCE), Mexico, City. Mexico. September 26-30, 2016.
8
Figure 7. Isothermal distribution of electric field.
,
2016 13th International Conference on Electrical Engineering, Computing Science and Automatic Control (CCE), Mexico, City. Mexico. September 26-30, 2016.
Conclusions
• The electroporation caused by potential induced by the electrodes, increase in
temperature due to the distribution of current.
• The distribution of electric potential inside the tissues was lower within the tumor
tissue compared to healthy tissue.
• The current distribution through the tissues was higher in the tissue healthy that in
tumor tissue.
• We must pay attention to prevent the electrodes from touching the healthy tissue at
least possible because the electroporation is not needed in this area, neither the
current distribution in this tissue.
9
,
2016 13th International Conference on Electrical Engineering, Computing Science and Automatic Control (CCE), Mexico, City. Mexico. September 26-30, 2016.

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Modeling of Electric Field and Joule Heating in Breast Tumor during Electroporation

  • 1. “Modeling of Electric Field and Joule Heating in Breast Tumor during Electroporation” Departamento de Ingeniería Eléctrica, CINVESTAV Sección Bioelectrónica. CONACYT Instituto Nacional de Rehabilitación Subdivisión de Investigación Biotegnológica Instituto de Enfermedades de la Mama- FUCAM, Mexico City, Mexico. 2016 13th International Conference on Electrical Engineering, Computing Science and Automatic Control (CCE), Mexico, City. Mexico. September 26-30, 2016. C. A. Ramírez Martínez*, A. L. Vera Tizatl, C. E. Vera Tizatl, P. R. Hernández Rodríguez, A. Vera Hernández, L. Leija Salas, M. I. Gutiérrez Velasco, S. A. Rodríguez Cuevas
  • 2. • Introduction • Methodology • Results • Conclusion 2016 13th International Conference on Electrical Engineering, Computing Science and Automatic Control (CCE), Mexico, City. Mexico. September 26-30, 2016. 2 Contents
  • 3. • In this work, it is presented a simulation of a breast carcinoma embedded in healthy tissue under an electric field exposure through steel electrodes. • These work seeks to observe the current density and the temperature rise in both tissues. Introduction
  • 4. 𝛁 𝛔 + 𝛆 𝛛 𝛛𝐭 𝛁𝚿(𝐱, 𝐲, 𝐳, 𝐭) = 𝟎 (𝟏) Fig. 1. Exposure of a spherical cell with radius R, thickness membrane d within an electric field. ∆𝚿 𝐦 = 𝛂𝐄𝐑𝐜𝐨𝐬𝛉 (𝟐) 𝛂 = 𝟑𝛔 𝐞 𝟑𝐝𝐑 𝟐 𝛔𝐢 + (𝟑𝐝 𝟐 𝐑 − 𝐝 𝟑 ) 𝛔 𝐦 − 𝛔𝐢 𝟐𝐑 𝟑 𝛔 𝐦 + 𝟐𝛔 𝐞 𝛔 𝐦 + 𝟏 𝟐 𝛔𝐢 − 𝟐 𝐑 − 𝐝 𝟑(𝛔 𝐞−𝛔 𝐦)(𝛔𝐢−𝛔 𝐦) (𝟑) The spatial and temporal distribution of the electrical potential in a medium, is given by Eq. 1 [Tizatl, A.L.V., et al. 3D model and simulation of electroporation application on healthy and tumoral breast tissue. in Electrical Engineering, Computing Science and Automatic Control (CCE), 2013 10th International Conference on. 2013..]. Methodology 2016 13th International Conference on Electrical Engineering, Computing Science and Automatic Control (CCE), Mexico, City. Mexico. September 26-30, 2016. 4
  • 5. 𝒒 ~ == 𝑬 𝟐 𝑳 𝟐 𝝈 𝝈 𝟎 𝑽𝒂 𝟐 (𝟕) 𝜵 𝟐 𝑻 − 𝒘 𝒃 𝒄𝑳 𝟐 𝒌 𝑻 + 𝒒 ~ = 𝜹𝑻 𝜹𝒕 (𝟖) 2016 13th International Conference on Electrical Engineering, Computing Science and Automatic Control (CCE), Mexico, City. Mexico. September 26-30, 2016. 5 Figure 2. A tumor tissue of 1 cm in diameter (1), inside healthy tissue of 8 cm diameter is proposed (2). Two stainless steel electrodes 1.2 mm diameter (3). The joule heating energy term is given by Eq. 7 [Van Gemert, M.J., et al., Irreversible electroporation: just another form of thermal therapy? Prostate, 2015. 75(3): p. 332-5.]. The heat transfer in tissue is given by Eq. 8 [Becker, S.M. and A.V. Kuznetsov, Thermal damage reduction associated with in vivo skin electroporation: A numerical investigation justifying aggressive pre-cooling. International Journal of Heat and Mass Transfer, 2007. 50(1-2): p. 105-116.] Material Health tissue Tumoral tissue Units Electrical conductivity 0.5 0.03 S/m Relative permittivity 123 80 1 Thermal conductivity 0.49 0.5 W/(m*K) Density 1090 1000 kg/m^3 Heat capacity 3421 4000 J/(kg*K) Table 1 Material proprieties in adiabatic form [2]. 1 2 3 The initial conditions to the phenomena were in 37-celsius degrees and the boundaries of the health tissue are in 25-celcius degrees.
  • 6. MESHING GEOMETRY 6 Figure 3. The solver used was adjusted to display the electric field distribution applied by the boundary electrodes inside the both kinds of tissue . , 2016 13th International Conference on Electrical Engineering, Computing Science and Automatic Control (CCE), Mexico, City. Mexico. September 26-30, 2016.
  • 7. Results 7 Figure 4. Electrical Potential thought tumoral tissue. Figure 5 . Electric field distribution and current density in breast tissue. , 2016 13th International Conference on Electrical Engineering, Computing Science and Automatic Control (CCE), Mexico, City. Mexico. September 26-30, 2016.
  • 8. 8 Figure 7. Isothermal distribution of electric field. , 2016 13th International Conference on Electrical Engineering, Computing Science and Automatic Control (CCE), Mexico, City. Mexico. September 26-30, 2016.
  • 9. Conclusions • The electroporation caused by potential induced by the electrodes, increase in temperature due to the distribution of current. • The distribution of electric potential inside the tissues was lower within the tumor tissue compared to healthy tissue. • The current distribution through the tissues was higher in the tissue healthy that in tumor tissue. • We must pay attention to prevent the electrodes from touching the healthy tissue at least possible because the electroporation is not needed in this area, neither the current distribution in this tissue. 9 , 2016 13th International Conference on Electrical Engineering, Computing Science and Automatic Control (CCE), Mexico, City. Mexico. September 26-30, 2016.

Editor's Notes

  1. Saluda GOOD MORNING Presenta  Buenas tardes mi nombre es carlos ramires y vengo a presentarles el trabajo enviado al CCE titulado Simulacion de la distribucion del cmapo electrico y el efecto del calentamiento de Joule en tumor de mama.
  2. van de 100 a 1m Se desprecia la dependencia temporal Al ser el fenómeno pulsante de campo eléctrico dentro del rango de 100us a 1ms y comando en cuenta que la carga de la membrana celular al esta comportarce como un capacitor, es del orden de 1us, se desprecia la parte temporal y solo queda la parte espacial con respecto a la conductividad Existe una relación directamente entre la permeablilidad y la conductividad Cito transformación de coordenandas de cartecianas a esféricasGeometria asimotal debido a la orientación del campo eléctrico Quedando solo con la dependencia de dos variables.
  3. van de 100 a 1m Se desprecia la dependencia temporal Al ser el fenómeno pulsante de campo eléctrico dentro del rango de 100us a 1ms y comando en cuenta que la carga de la membrana celular al esta comportarce como un capacitor, es del orden de 1us, se desprecia la parte temporal y solo queda la parte espacial con respecto a la conductividad Existe una relación directamente entre la permeablilidad y la conductividad Cito transformación de coordenandas de cartecianas a esféricasGeometria asimotal debido a la orientación del campo eléctrico Quedando solo con la dependencia de dos variables.