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Conference Paper: Modeling of the subsurface interface radar

TitleModeling of the subsurface interface radar
Authors
Issue Date1990
Citation
Digest - International Geoscience And Remote Sensing Symposium (Igarss), 1990, p. 31 How to Cite?
AbstractSummary form only given. A finite-difference time-domain method is used to solve the problem of the response of an arbitrary source, in particular, an impulsive point source, in a two-dimensional isotropic inhomogeneous medium. In general, a source excites all components of the vector wave field; thus, a scalar solution is incomplete. The field is 3-D, while the inhomogeneity is 2-D. This is called a 2-1/2-D problem. Since the current generated by a point source in a plane is an even function of the coordinate perpendicular to that plane, the field components assume even or odd symmetries correspondingly. Using this fact and taking advantage of the invariance of the geometry in one dimension, cosine and sine transforms are used to eliminate one of the spatial derivatives in Maxwell's equations, thereby reducing the problem to two dimensions. A rectangular staggered grid is used to discretize the differential equations. The complete solution is obtained by linearly superimposing several transformed field components. This provides great savings in terms of computer storage and run time over the three-dimensional finite-difference method. A criterion is given to ensure the stability of this finite-difference scheme, which is a generalized form of Courant-Lewy-Friedrichs stability criterion in two dimensions. Two methods are proposed to treat the source region singularity and the inaccuracy caused by rapidly decaying evanescent waves.
Persistent Identifierhttp://hdl.handle.net/10722/182818

 

DC FieldValueLanguage
dc.contributor.authorChew, WCen_US
dc.contributor.authorMoghaddam, Men_US
dc.contributor.authorYannakakis, Een_US
dc.date.accessioned2013-05-02T05:17:12Z-
dc.date.available2013-05-02T05:17:12Z-
dc.date.issued1990en_US
dc.identifier.citationDigest - International Geoscience And Remote Sensing Symposium (Igarss), 1990, p. 31en_US
dc.identifier.urihttp://hdl.handle.net/10722/182818-
dc.description.abstractSummary form only given. A finite-difference time-domain method is used to solve the problem of the response of an arbitrary source, in particular, an impulsive point source, in a two-dimensional isotropic inhomogeneous medium. In general, a source excites all components of the vector wave field; thus, a scalar solution is incomplete. The field is 3-D, while the inhomogeneity is 2-D. This is called a 2-1/2-D problem. Since the current generated by a point source in a plane is an even function of the coordinate perpendicular to that plane, the field components assume even or odd symmetries correspondingly. Using this fact and taking advantage of the invariance of the geometry in one dimension, cosine and sine transforms are used to eliminate one of the spatial derivatives in Maxwell's equations, thereby reducing the problem to two dimensions. A rectangular staggered grid is used to discretize the differential equations. The complete solution is obtained by linearly superimposing several transformed field components. This provides great savings in terms of computer storage and run time over the three-dimensional finite-difference method. A criterion is given to ensure the stability of this finite-difference scheme, which is a generalized form of Courant-Lewy-Friedrichs stability criterion in two dimensions. Two methods are proposed to treat the source region singularity and the inaccuracy caused by rapidly decaying evanescent waves.en_US
dc.languageengen_US
dc.relation.ispartofDigest - International Geoscience and Remote Sensing Symposium (IGARSS)en_US
dc.titleModeling of the subsurface interface radaren_US
dc.typeConference_Paperen_US
dc.identifier.emailChew, WC: wcchew@hku.hken_US
dc.identifier.authorityChew, WC=rp00656en_US
dc.description.naturelink_to_subscribed_fulltexten_US
dc.identifier.scopuseid_2-s2.0-0025554555en_US
dc.identifier.spage31en_US
dc.identifier.scopusauthoridChew, WC=36014436300en_US
dc.identifier.scopusauthoridMoghaddam, M=7004934627en_US
dc.identifier.scopusauthoridYannakakis, E=6506077215en_US

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