Three-dimensional impedance imaging processes

• US 5,284,142 A
• Filed: 12/16/1991
• Issued: 02/08/1994
• Est. Priority Date: 12/16/1991
• Status: Expired due to Term

• Current Assignee: Rensselaer Polytechnic Institute
• Original Assignee: Rensselaer Polytechnic Institute
• Inventors: Goble, John C., Isaacson, David, Cheney, Margaret
• Primary Examiner(s): Smith, Ruth S.
• Application Number:
  US07/808,795
• Time in Patent Office: 785 Days
• Field of Search: 128/734, 364/413.13
• US Class Current: 600/547
• CPC Class Codes: A61B 5/0536 Impedance imaging, e.g. by tomography
• CPC Class Codes: G01R 27/26 Measuring inductance or capacitance; Measuring quality factor, e.g. by using the resonance method; Measuring loss factor; Measuring dielectric constants ; Measuring impedance or related variables
• CPC Class Codes: G16H 50/50 for simulation or modelling of medical disorders

Abstract

A method of practicing electrical impedance tomography produces three-dimensional images of a body. First, one applies certain special current patterns to the body through an array of electrodes attached to the surface. For each current pattern, one measures the voltage at each electrode, thus obtaining a corresponding pattern of voltages. These data are then used in a certain special reconstruction process, which enables a full three-dimensional reconstruction to be done in a short time. The result is a display of an approximation to the electric conductivity and/or electric permittivity in the interior of the body.

Claims

1. A method for three-dimensionally imaging the interior of a body having an internal resistivity using electrical impedance tomography, comprising:

applying an electrode array having a first selected number of electrodes (L) to the surface of the body;

applying a second selected number of current patterns to the electrode array;

measuring a number of voltage patterns, which is equal to the second selected number, resulting from application of the current patterns;

reconstructing an approximation of the internal resistivity, in which the resistivity ρ

¹ is expressed in terms of a finite-dimensional basis, and its coefficients in this basis are given by equation (10), F(ρ

⁰) is a known vector given by equation (9), and a matrix F'"'"' is a previously obtained approximation;

##EQU23## where V_l^k is the measured voltage pattern and U_l^k is a predicted voltage pattern, E is an error and ∂

U_l^k /∂

ρ

_n is a change in voltage; and

making a three-dimensional image of the interior of the body based on the approximation of the internal resistivity.

2. A method according to claim 1, wherein the matrix F'"'"' is defined by ##EQU24##

3. A method according to claim 1, wherein the matrix F'"'"' is defined by

4. A method according to claim 1, wherein said current patterns are selected from the group consisting of (a) tensor products of discrete trigonometric functions, (b) the best patterns with which to represent the boundary map (R), and (c) the best patterns with which to distinguish the internal resistivity from an estimate for the internal resistivity.

5. A method according to claim 1, where ρ

⁰ is defined by (17);

##EQU26##

6. A method according to claim 1, including finding and storing a plurality of eigenvectors and a plurality of eigenvalues for the matrix F'"'"', inverting the matrix F'"'"' for forming a matrix inverse wherein the matrix inverse is computed according to a spectral theorem, and so that the matrix inverse is reduced to a computation of a plurality of inner products.

7. A method according to claim 6, wherein the matrix F'"'"' is defined by ##EQU27##

8. A method according to claim 6, wherein the matrix F'"'"' is defined by