Geophysical Applications of Electrical Impedance Tomography Ph.D. - - PowerPoint PPT Presentation

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Geophysical Applications of Electrical Impedance Tomography Ph.D. - - PowerPoint PPT Presentation

Geophysical Applications of Electrical Impedance Tomography Ph.D. Defence Alistair Boyle Systems and Computer Engineering Carleton University April 29, 2016 A. Boyle, 2016 Carleton University Ph.D. Defence 1 / 15 Motivation Derailment of


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SLIDE 1

Geophysical Applications of Electrical Impedance Tomography

Ph.D. Defence Alistair Boyle

Systems and Computer Engineering Carleton University

April 29, 2016

  • A. Boyle, 2016

Carleton University Ph.D. Defence 1 / 15

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SLIDE 2

Motivation

Derailment of 39 railway cars carrying crude oil Gogama, ON, Canada (2015)

1

Average 600 derailments per year, 74 with dangerous goods (Canada, 2008-2012)2 Gogama clean-up costs will be “in the millions” – MPP F. Gelinas3

1Transportation Safety Board of Canada, Railway Investigation Report R15H0021, Mar 2015 2Transportation Safety Board of Canada, Statistical Summary - Railway Occurrences 2013, Feb 2014

  • 3M. Stackelberg, CBC News, Ontario bills CN $350K for Gogama derailment clean-up, Dec 2015
  • A. Boyle, 2016

Carleton University Ph.D. Defence 2 / 15

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SLIDE 3

Motivation

Mount Polley mine tailings spill, Likely, BC, Canada (2014)

4

spilled 4.5 mil. m3 of tailings with clean up costs of $200–500 mil.

4CBC News, “Mount Polley mine tailings spill”, Aug 2014

  • A. Boyle, 2016

Carleton University Ph.D. Defence 3 / 15

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SLIDE 4

Motivation

Manage slope stability risks a tool for real-time monitoring of slope movement robust, reliable, informative reconstructions Our tool of choice: Electrical Impedance Tomography Electrical Resistivity Tomography

  • A. Boyle, 2016

Carleton University Ph.D. Defence 4 / 15

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SLIDE 5

Motivation

Manage slope stability risks a tool for real-time monitoring of slope movement electrode movement & resistivity robust, reliable, informative reconstructions algorithm, implementation, data Our tool of choice: Electrical Impedance Tomography Electrical Resistivity Tomography

  • A. Boyle, 2016

Carleton University Ph.D. Defence 4 / 15

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SLIDE 6

Electrical Impedance Tomography

Typical ERT Survey Equipment

ABEM TerrameterLS5

5[http://www.ngi.no/upload/48876/TerrameterLS.jpg]

  • A. Boyle, 2016

Carleton University Ph.D. Defence 5 / 15

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SLIDE 7

Electrical Impedance Tomography

Typical ERT Survey

Pont-P´ ean, France6

6correct electrode wiring

  • A. Boyle, 2016

Carleton University Ph.D. Defence 6 / 15

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SLIDE 8

Electrical Impedance Tomography

Long-term remote monitoring

Hollin Hill, UK7

7Automated Landslide Electrical Resistivity Tomography (ALERT) system

  • A. Boyle, 2016

Carleton University Ph.D. Defence 7 / 15

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SLIDE 9

Methods

Absolute imaging problem; large conductivity contrasts ... a Gauss-Newton nonlinear iterative solver min

x ||Ax − b||2 2

(1) δxn = −(JT

nJn)−1(JT nb)

(2) xn+1 = xn + αn+1 δxn+1 (3)

−1 −0.5 0.5 1 −1 −0.8 −0.6 −0.4 −0.2 0.2 0.4 0.6 0.8 1 −2 −1 1 2

  • A. Boyle, 2016

Carleton University Ph.D. Defence 8 / 15

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SLIDE 10

Methods

Absolute imaging problem; large conductivity contrasts ... a Gauss-Newton nonlinear iterative solver min

x ||Ax − b||2 W + ||λR(x − x∗)||2 2

(1) δxn+1 = −(JT

nWJn + λ2RTR)−1(JT nWb − λ2RTR(xn − x∗))

(2) xn+1 = xn + αn+1 δxn+1 (3)

−1 −0.5 0.5 1 −1 −0.8 −0.6 −0.4 −0.2 0.2 0.4 0.6 0.8 1 −1 1 2

  • A. Boyle, 2016

Carleton University Ph.D. Defence 8 / 15

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SLIDE 11

Methods

δxn+1 = −(JT

nWJn + λ2RTR)−1(JT nWb − λ2RTR(xn − x∗))

Ji,j = δbi

δxj

δx δb W δb δb R x x x

  • A. Boyle, 2016

Carleton University Ph.D. Defence 9 / 15

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SLIDE 12

Methods

Resistivity Ji,j = δbi

δxj

δx δb W δb δb R x x x

  • A. Boyle, 2016

Carleton University Ph.D. Defence 10 / 15

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SLIDE 13

Methods

Resistivity and movement together

electrode # 5 10 15 20 25 30 electrode mvmt [m]

  • 1.5
  • 1
  • 0.5

0.5 upslope downslope 0.2 m

true movement reconstructed

Ji,j = δbi

δxj

δxσ δb W δb δb R xσ xσ δxm xm xm xσ xm

  • A. Boyle, 2016

Carleton University Ph.D. Defence 11 / 15

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SLIDE 14

This Work Addresses

inverse solver improved decision

  • utcomes

boundary/electrode movement more adaptable models fewer artifacts better detectability improved image quality

Background material impedance imaging: fwd problem, hardware (Ch2) rocks and conductivity: a review (Ch3) inverse problems: composing algorithms (Ch4)

  • A. Boyle, 2016

Carleton University Ph.D. Defence 12 / 15

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SLIDE 15

This Work Addresses

inverse solver improved decision

  • utcomes

boundary/electrode movement more adaptable models fewer artifacts better detectability improved image quality

Contributions; with geophysics applications problems with inverse problems: reliable algorithms (Ch5) data quality and model mismatch: reliable data (Ch6) electrode mvmt and modelling errors: reliable Jacobians (Ch7) reconstructing surface movement: [xσ xm]T (Ch8)

  • A. Boyle, 2016

Carleton University Ph.D. Defence 13 / 15

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SLIDE 16

This Work Addresses

inverse solver improved decision

  • utcomes

boundary/electrode movement more adaptable models fewer artifacts better detectability improved image quality

  • A. Boyle, 2016

Carleton University Ph.D. Defence 14 / 15

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SLIDE 17

Thank You

  • A. Boyle, 2016

Carleton University Ph.D. Defence 15 / 15