2021
DOI: 10.1109/tpwrd.2020.3009656
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Segmented Sampling Least Squares Algorithm for Green's Function of Arbitrary Layered Soil

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Cited by 6 publications
(4 citation statements)
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“…The size of current measurement electrodes is much smaller than the entire soil space, C 1 and C 2 can be approximated as the point sources. The position of C 1 is taken as the origin and a cylindrical coordinate system is established, the apparent soil resistivity is ρm=4πD1+2DD2+4h02DD2+h02()φ()D,h0φ()2D,h0 ${\rho }_{\mathrm{m}}=\frac{4\pi D}{1+\frac{2D}{\sqrt{{D}^{2}+4{h}_{0}^{2}}}-\frac{D}{\sqrt{{D}^{2}+{h}_{0}^{2}}}}\left(\varphi \left(D,{h}_{0}\right)-\varphi \left(2D,{h}_{0}\right)\right)$ where ρ m is the measured apparent soil resistivity, φ()D,h0 $\varphi \left(D,{h}_{0}\right)$ and φ()2D,h0 $\varphi \left(2D,{h}_{0}\right)$ are the measured potential of electrodes P 1 and P 2 [20]. Besides, the h 0 is usually much less than D , so the Equation () can be further simplified as: ρm=2πD(φ(D,0)φ(2D,0)) ${\rho }_{\mathrm{m}}=2\pi D(\varphi (D,0)-\varphi (2D,0))$ …”
Section: Basic Theory Of Grounding Parameter Calculation In Horizonta...mentioning
confidence: 99%
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“…The size of current measurement electrodes is much smaller than the entire soil space, C 1 and C 2 can be approximated as the point sources. The position of C 1 is taken as the origin and a cylindrical coordinate system is established, the apparent soil resistivity is ρm=4πD1+2DD2+4h02DD2+h02()φ()D,h0φ()2D,h0 ${\rho }_{\mathrm{m}}=\frac{4\pi D}{1+\frac{2D}{\sqrt{{D}^{2}+4{h}_{0}^{2}}}-\frac{D}{\sqrt{{D}^{2}+{h}_{0}^{2}}}}\left(\varphi \left(D,{h}_{0}\right)-\varphi \left(2D,{h}_{0}\right)\right)$ where ρ m is the measured apparent soil resistivity, φ()D,h0 $\varphi \left(D,{h}_{0}\right)$ and φ()2D,h0 $\varphi \left(2D,{h}_{0}\right)$ are the measured potential of electrodes P 1 and P 2 [20]. Besides, the h 0 is usually much less than D , so the Equation () can be further simplified as: ρm=2πD(φ(D,0)φ(2D,0)) ${\rho }_{\mathrm{m}}=2\pi D(\varphi (D,0)-\varphi (2D,0))$ …”
Section: Basic Theory Of Grounding Parameter Calculation In Horizonta...mentioning
confidence: 99%
“…The solution method of φ(D,0) $\varphi (D,0)$ is φ(D,0)=ρ12π0α1J0(λD)normaldλ $\varphi (D,0)=\frac{{\rho }_{1}}{2\pi }\int \nolimits_{0}^{\infty }{\alpha }_{1}{J}_{0}(\lambda D)\mathrm{d}\lambda $ where, α1 ${\alpha }_{1}$ is the integral coefficient that is related to the soil parameters ρ1,,ρn,h1,,hn1 ${\rho }_{1},{{\cdots}},{\rho }_{n},{h}_{1},{{\cdots}},{h}_{n-1}$, the detailed solution process of α1 ${\alpha }_{1}$ is shown in Ref. [20, 21]. The complex image method is used to process Equation (), and the processed results are substituted into Equation () [22]: ρc0.25em=0.25emρ1Dj=12naj2bj2+D212 ${\rho }_{\mathrm{c}}{\,=\,\rho }_{1}D\sum\limits _{j=1}^{2n}{a}_{j}^{2}{\left({b}_{j}^{2}+{D}^{2}\right)}^{-\tfrac{1}{2}}$ where ρc ${\rho }_{\mathrm{c}}$ is the calculated apparent soil resistivity, a j and b j are coefficients of the complex image method, and n is the number of soil layers.…”
Section: Basic Theory Of Grounding Parameter Calculation In Horizonta...mentioning
confidence: 99%
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