Electrical Resistivity of K12/TRb Tumors vs. Normal Liver Tissue

Slides:



Advertisements
Similar presentations
A study of the electrical bio-impedance of tumors, Morimoto (1993) Measurement System: Three-electrode method, frequency range 0-200kHz, a thin coaxial.
Advertisements

5 Current Field Measurement 5.1Alternating Current Field Measurement 5.2Direct Current Potential Drop 5.3Alternating Current Potential Drop.
CHAPTER TWO POWER SEMICONDUCTOR DIODES AND CIRCUITS DESIGNED BY DR. SAMEER KHADER PPU “E-learning Project”
Developing New Technology for Local Tumor Control: A Bioengineering Approach Andrew Wright MD Department of Surgery 1/25/02.
“Finite Element Modeling of Radiofrequency Cardiac and Hepatic Ablation” SUPAN TUNGJITKUSOLMUN “Finite Element Modeling of Radiofrequency Cardiac and.
Electrical Techniques MSN506 notes. Electrical characterization Electronic properties of materials are closely related to the structure of the material.
Introduction to Finite Element Modeling in Biomechanics Dr. N. Fatouraee Biomedical Engineering Faculty December, 2004.
High Frequency Ultrasonic Characterization of Carrot Tissue Christopher Vick Advisor: Dr. Navalgund Rao Center for Imaging Science Rochester Institute.
ET 332a Dc Motors, Generators and Energy Conversion Devices Lesson 2: Magnetic Circuits- Quantities and Definitions 1.
Genomics Lecture 7 By Ms. Shumaila Azam. Tumor Tumor – abnormal proliferation of cells that results from uncontrolled, abnormal cell division A tumor.
Living Longer: Colon Cancer Patients Gain Time With Radiofrequency Ablation Treatment CT Sofocleous, EN Petre, M Gonen, KT Brown, RH Thornton, AM Covey,
John G. Webster Department of Biomedical Engineering University of Wisconsin Madison WI USA Supported by NIH grant HL56143.
Cancer A Disease of Mitosis.
EE513 Audio Signals and Systems Noise Kevin D. Donohue Electrical and Computer Engineering University of Kentucky.
Chris Roy September 28 th 2010 MBP 1028 Optical, Thermal and Radiation Biophysics Principles of Radiofrequency and Microwave Heating.
High frequency ultrasound in monitoring organ viability for transplantation Roxana Vlad 1, Anoja Giles 1, 2, G.J Czarnota 1, 2, J.W. Hunt 1, 2, M.D. Sherar.
Integrated Fluorescent Probe and Radiofrequency Ablator Rachel Riti and Alex Walsh Advisers: Bart Masters and Anita Mahadevan-Jansen Department of Biomedical.
PSST 10819_11/2008 Arrhythmia in Practice Today ™ Content provided by Boston Scientific September 2008 Lessons in Lesions.
Microwave Radiometry Microwave Radiometry. The RTM-01-RES radiometer receives and evaluates the natural electromagnetic radiation (temperature) from the.
Basic Probability (Chapter 2, W.J.Decoursey, 2003) Objectives: -Define probability and its relationship to relative frequency of an event. -Learn the basic.
Near Field Antenna Measurements for Cellular Phone Certification Ahlia M. Tillman, John Rzasa, Bandar Hakim, Quirino Balzano, and Christopher C. Davis.
I n s t i t u t e of H i g h E n e r g y P h y s i c s И н с т и т у т Ф и з и к и В ы с о к и х Э н е р г и й Influence of cooling on the working parameters.
HYDRAULICS of steady and pulsatile flow in systemic circulation Motivation Experimental techniques for measurement pressure and flowrate How to calculate.
Cauterization Catheter – An Advancement in Conductive Biomaterials and Medicine C. Blyth 1, C. Fernandez 1, S. Hittinger 1, C. Jones 1, B. McGee 1, B.
Objective 8: TSWBAT explain how cancerous cell division is different from normal cell division.
Laser Treated Metallic Probes for Cancer Treatment in MRI Systems July 08, Advance Materials Processing and Analysis Center (AMPAC) Department of.
Multiscale Modeling of Avascular Tumor Growth Jelena Pjesivac-Grbovic Theoretical Division 7, LANL Ramapo college of New Jersey University of Tennessee,
Project Update Explore the effects of blood vessels in thermal ablation using sensitivity analysis Cliff Zhou CBC Lab Meeting August 5th, 2013.
Multiprobe RF ablation: A Feasibility Study Fred T. Lee Jr., MD Dieter Haemmerich, MS Andrew S. Wright, MD David M. Mahvi, MD John G. Webster, PhD University.
Cauterization Catheter – An Advancement in Conductive Biomaterials and Medicine C. Blyth 1, C. Fernandez 1, S. Hittinger 1, C. Jones 1, B. McGee 1 Advisors:
Monday, April 23, PHYS , Spring 2007 Dr. Andrew Brandt PHYS 1444 – Section 004 Lecture #19 Monday, April 23, 2007 Dr. Andrew Brandt Inductance.
Chapter 10 – Cell Size, Mitosis and Cancer. Cells come in a variety of sizes… Red blood cells = 9 micrometers Nerve cells (large animals) = 1m (with small.
CLIC workshop 2015 EXTRACTION KICKER STRIPLINE MEASUREMENTS C. Belver-Aguilar (IFIC) On behalf of: A. Faus-Golfe (IFIC), F. Toral (CIEMAT), M.J. Barnes.
Closed Circuits In applications requiring the use of current, electrical components are arranged in the form of a circuit. A circuit is defined as a path.
The current density at each interfacial layer. The forward voltage is continuous at every point inside the body. A Layered Model for Breasts in Electrical.
1 Modeling of heat transfer in an accelerator superconducting coil with a ceramic insulation in supercritical helium S. Pietrowicz, B. Baudouy, CEA Saclay/
Ultrasound Learning Objectives: Describe the properties of ultrasound;
Noise propagation issues in complex power cables for HEP detectors M. Iglesias, I. Echeverria,F. Arteche 12 th Meeting of the Spanish Network for future.
LONGITUDINAL COUPLED-BUNCH OSCILLATIONS IN THE RECYCLER RING PRESENTED BY: MUHED RANA UNIVERSITY OF MARYLAND, BALTIMORE COUNTY (UMBC), BALTIMORE, MD SUPERVISOR:
Date of download: 6/23/2016 Copyright © ASME. All rights reserved. From: Design of Bioimpedance Spectroscopy Instrument With Compensation Techniques for.
Chapter 12 Therapeutic Heating Applications of Radio Frequency Energy C-K. Chou.
LC Circuit Section 22.5 There is a characteristic frequency at which the circuit will oscillate, called the resonance frequency.
DIATHERMY Diathermy was once one of the most popular modalities used in rehab. Became less popular with development of more modern tech like US and because.
Contents: Computer Code
Audio Power Amplifier Detailed Design
How does an electrical circuit work?
The Benefits of Microwave Ablation
Medical Laboratory Instrumentation
Date of download: 10/17/2017 Copyright © ASME. All rights reserved.
Radio Coverage Prediction in Picocell Indoor Networks
M. Migliorati, C. Vaccarezza INFN - LNF
Applied Electricity and Magnetism
Cells.
Date of download: 11/15/2017 Copyright © ASME. All rights reserved.
Abstract Langmuir probes in low-density RF plasmas sometimes show peculiar I-V characteristics with no electron saturation. This is due to the space potential.
Dynamically Shaped Magnetic FieldsClinical Perspective
Lecture 1 - Introduction to Electrical Engineering
Andrew Wright MD, Chris Johnson, Fred Lee Jr. MD, and David Mahvi MD
Physics 114: Exam 2 Review Material from Weeks 7-11
Esther Bridges, Adrian L. Harris  Cancer Cell 
Volume 148, Issue 1, Pages (January 2012)
HYDRAULICS of steady and pulsatile flow in systemic circulation
Andrew Wright MD, Chris Johnson, Fred Lee Jr. MD, and David Mahvi MD
Duplex ultrasound changes in the great saphenous vein after endosaphenous laser occlusion with 808-nm wavelength  Leonardo Corcos, MD, Sergio Dini, MD,
Biomedical analysis using Smart algorithms
C.A. Bertrand, D.M. Durand, G.M. Saidel, C. Laboisse, U. Hopfer 
Applied Electromagnetic Waves
Chapter 32 Problems 6,7,9,16,29,30,31,37.
Pairing-Induced Changes of Orientation Maps in Cat Visual Cortex
Two-Microelectrode Voltage Clamp of Xenopus Oocytes: Voltage Errors and Compensation for Local Current Flow  W. Baumgartner, L. Islas, F.J. Sigworth 
Presentation transcript:

Electrical Resistivity of K12/TRb Tumors vs. Normal Liver Tissue Dieter Haemmerich S. Tyler Staelin Supan Tungjitkusolmun Jang-Zern Tsai Omer R. Ozkan David Mahvi John G. Webster This research has been supported by NIH grant #1R01 HL56143-01

Motivation Liver is second most common site of metastases next to lymph nodes Usage of resistivity data: Detect tumors via bio-impedance measurements Radio Frequency ablation as treatment: Determine distribution of absorbed electromagnetic energy No known studies on in-vivo tumor resistivity at audio and radiofrequencies We tried to model liver metastases in animal (rat) Explain RF ablation: catheter is inserted into tissue; current flows from catheter to groundpad (placed on back) -> surrounding tissue is heated. Dieter Haemmerich, Univ. Wisconsin-Madison email: haemmeri@cae.wisc.edu

Experimental Details K12/TRb is a colon cancer line with histologic characteristics similar to human colon cancer Liver tumors were initiated in 40 rats by injecting 106 cells intrahepatically (n=20) or 8·106 cells intraspleenically (n=20) Rats were opened 6 – 9 weeks after injections 24 tumors in 18 rats were measured Cell line used to model liver metastases Intraspleenic injections -> metastases developed in liver Dieter Haemmerich, Univ. Wisconsin-Madison email: haemmeri@cae.wisc.edu

Tumor resistivity was measured over 4 weeks in 1-week intervals Tumors were 1cm – 2 cm in diameter Normal liver tissue was measured for control Animals were sacrificed after measurement Tumor volume was estimated Histologic slides were created of each tumor % Necrosis and % Fibrosis were estimated at measurement site Dieter Haemmerich, Univ. Wisconsin-Madison email: haemmeri@cae.wisc.edu

Current-to-voltage converter Experiment Setup Tissue Function RS232 generator Amplifier Current-to-voltage converter Channel 1 RS232 Oscilloscope Channel 2 Computer Probe 4-terminal method minimizes errors from electrode polarization Probe has silver electrodes, 0.38 mm diameter, 1.5 mm apart, 5 mm long, covered with AgCl We measured at 8 frequencies from 1 Hz to 1 MHz Dieter Haemmerich, Univ. Wisconsin-Madison email: haemmeri@cae.wisc.edu

Resistivity: Tumor vs. Normal Dieter Haemmerich, Univ. Wisconsin-Madison email: haemmeri@cae.wisc.edu

Current paths in tissue Current paths at DC and low frequencies Current paths at high frequencies It is generally agreed upon… Applies to most types of tissue Why different in tumor? I’ll come back to that later. Dieter Haemmerich, Univ. Wisconsin-Madison email: haemmeri@cae.wisc.edu

Approximation Equation Resistivity curves approximated by: A ... Resistivity at low frequencies Q = A / (1+eB)... Resistivity at high frequencies C ... Controls rate of decrease Parameters A, Q, C were fit for each tumor and control Dieter Haemmerich, Univ. Wisconsin-Madison email: haemmeri@cae.wisc.edu

Sample Tumor Resistivity Data and Approximation A = 397, Q = 211, C = -1.01 Dieter Haemmerich, Univ. Wisconsin-Madison email: haemmeri@cae.wisc.edu

Spearman`s correlation coefficients were determined between each of the parameters (A, Q, C) and: Tumor Volume Tumor Age % Necrosis at measurement site % Fibrosis at measurement site How did we know where measurement site is? Dieter Haemmerich, Univ. Wisconsin-Madison email: haemmeri@cae.wisc.edu

Probe tracts -> measurement site can be determined Dieter Haemmerich, Univ. Wisconsin-Madison email: haemmeri@cae.wisc.edu

Typical Tumor Compared to normal liver cells: Cells are very unordered, very diverse, not well differentiated, multiple nuclei Dieter Haemmerich, Univ. Wisconsin-Madison email: haemmeri@cae.wisc.edu

Tumor-Liver Interface Ordered vs. unordered Liver parenchyma compressed at border Very few blood vessels inside tumor Dieter Haemmerich, Univ. Wisconsin-Madison email: haemmeri@cae.wisc.edu

Necrosis and Fibrosis Tumor gets blood support from tumor-liver-boundary As tumor grows, inner regions get depleted of nutrients and waste products accumulate This leads to necrosis (cell death), preferably at the tumor center After cells die, (tumor) tissue gets replaced with fibroblastic tissue Blood brings nutrients to the cells and carries metabolic waste products away from cells Fibrosis depends on regenerative capabilities of cell type Dieter Haemmerich, Univ. Wisconsin-Madison email: haemmeri@cae.wisc.edu

Tumor with Necrosis & Fibrosis Dieter Haemmerich, Univ. Wisconsin-Madison email: haemmeri@cae.wisc.edu

Central Necrosis Dieter Haemmerich, Univ. Wisconsin-Madison email: haemmeri@cae.wisc.edu

Significance Probabilities (P-values) Tumor Parameters Age Volume Fibrosis Necrosis A 0.2085 0.0161 0.3527 0.0031  0.900 0.1815 0.9198 0.0018 C 0.5355 0.3416 0.2748 0.0116 Significance probabilities calculated from Spearman’s Correlation Coefficients P-values are underlined where significance is reached Dieter Haemmerich, Univ. Wisconsin-Madison email: haemmeri@cae.wisc.edu

Parameter A vs. Necrosis Dieter Haemmerich, Univ. Wisconsin-Madison email: haemmeri@cae.wisc.edu

Parameter Q vs. Necrosis Dieter Haemmerich, Univ. Wisconsin-Madison email: haemmeri@cae.wisc.edu

Conclusions Results strongly support theory that necrosis is responsible for drop in resistivity: When cells are intact, current is restricted to extracellular room at low frequencies During cell necrosis cell membrane loses integrity. Resistivity drops. Difference in resistivity at frequencies below 100 kHz can be exploited to increase efficacy of electromagnetic tumor heating (RF ablation) Currently RF ablation uses frequ. Around 500 kHz Dieter Haemmerich, Univ. Wisconsin-Madison email: haemmeri@cae.wisc.edu

Model Geometry Dieter Haemmerich, Univ. Wisconsin-Madison email: haemmeri@cae.wisc.edu

Temp. distribution Current density Parameter Case 1 Case 2 Case 3 Liver resistivity 102.7 cm 308.0 cm 924.0 cm Tumor resistivity Total energy 574 J 974 J 1732 J Red: 50C-boundary Dieter Haemmerich, Univ. Wisconsin-Madison email: haemmeri@cae.wisc.edu

Acknowledgements Web Site Glen Leverson Thomas F. Warner Web Site Acknowledge two people who had significant contribution to study http://rf-ablation.engr.wisc.edu Dieter Haemmerich, Univ. Wisconsin-Madison email: haemmeri@cae.wisc.edu