Electrical capacitance tomography (ECT) is a low-cost, high-speed imaging technique useful in many industrial settings. ECT is predicated on the knowledge of sensitivity maps between capacitance electrodes that blanket the imaging domain. The simultaneous activation of multiple electrodes can be advantageous to manipulate the resulting field distributions and capture additional spatial information for imaging purposes. However, conventional methods for sensitivity map computation in ECT are not adequate in the presence of multielectrode activation because the mutual coupling between electrodes is not properly accounted for. This coupling becomes especially critical in adaptive electrical capacitance volume tomography (AECVT) sensors, where signals from many small electrode segments are combined into synthetic electrodes. A more general approach is presented for sensitivity map computation in AECVT based on the actual posteriori (induced) charge distributions rather than the conventional approach based on boundary conditions with no account for electrode interactions.
[1]
M. S. Beck,et al.
Capacitance-based tomographic flow imaging system
,
1988
.
[2]
S. Mylvaganam,et al.
Electrical Capacitance Tomography—Sensor Models, Design, Simulations, and Experimental Verification
,
2006,
IEEE Sensors Journal.
[3]
V. H. Rumsey,et al.
Reaction Concept in Electromagnetic Theory
,
1954
.
[4]
Liang-Shih Fan,et al.
Electrical Capacitance Volume Tomography
,
2007,
IEEE Sensors Journal.
[5]
Fernando L. Teixeira,et al.
Adaptive Electrical Capacitance Volume Tomography
,
2014,
IEEE Sensors Journal.
[6]
F. Teixeira,et al.
Sensitivity matrix calculation for fast 3-D electrical capacitance tomography (ECT) of flow systems
,
2004,
IEEE Transactions on Magnetics.
[7]
V. Rumsey.
A short way of solving advanced problems in electromagnetic fields and other linear systems
,
1963
.