2020
DOI: 10.17576/jsm-2020-4912-04
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Rapid ESKAPE Pathogens Detection Method using Tapered Dielectrophoresis Electrodes via Crossover Frequency Analysis

Abstract: This paper introduces the versatile of an electrokinetic technique by using the non-uniform electric field for dielectrophoresis (DEP) application. This technique is defined as electromicrofluidics. The potential application for portable and real time detection method of Enterococcus faecium (EF), Staphylococcus aureus (SA), Klebsiella pneumoniae (KP), Acinetobacter baumannii (AB), Pseudomonas aeruginosa (PA) and Enterobacter aerogenes (EA), which are the (ESKAPE) bacteria. The MATLAB analytical modelling was … Show more

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Cited by 2 publications
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“…The particles are temporarily polarized and move toward increasing or decreasing field intensity based on permittivity and conductivity differences between the particles and medium. In general, the DEP force (F DEP ) is determined by the physical and electrical properties of the particles and the medium and described by the following equation [24, 25]: 0.28emFDEPbadbreak=0.28em2πrext3ε0εm0.28emRe[]fCME2$$\begin{equation}{\rm{\;}}{{\rm{F}}_{{\rm{DEP}}}} = \;2\pi r_{ext}^3{\varepsilon _0}{\varepsilon _m}\;Re\left[ {{f_{CM}}} \right]\nabla {E^2}\end{equation}$$where rext${r_{ext}}$ is the particle radius, ε 0 is the permittivity for vacuum (8.854 × 10 –12 F/m), εm${\varepsilon _m}$ is the relative permittivity of the suspending medium, Refalse[fCMfalse]$Re[ {{f_{CM}}} ]$ is the real part of the Clausius–Mossotti factor (CMF) of the particle, and E2$\nabla {E^2}$ defines the gradient of the external field magnitude square. The real part of fCM${f_{CM}}$ for a spherical particle is described by the following equation, which depends on medium complex permittivity, εm$\varepsilon _m^*$, and the second effective complex permittivity of the particle, εeff2$\varepsilon _{eff2}^*$ [25]: Re0.28em[]fCMbadbreak=0.28emRe[]εeff2εmεeff...…”
Section: Dep Theorymentioning
confidence: 99%
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“…The particles are temporarily polarized and move toward increasing or decreasing field intensity based on permittivity and conductivity differences between the particles and medium. In general, the DEP force (F DEP ) is determined by the physical and electrical properties of the particles and the medium and described by the following equation [24, 25]: 0.28emFDEPbadbreak=0.28em2πrext3ε0εm0.28emRe[]fCME2$$\begin{equation}{\rm{\;}}{{\rm{F}}_{{\rm{DEP}}}} = \;2\pi r_{ext}^3{\varepsilon _0}{\varepsilon _m}\;Re\left[ {{f_{CM}}} \right]\nabla {E^2}\end{equation}$$where rext${r_{ext}}$ is the particle radius, ε 0 is the permittivity for vacuum (8.854 × 10 –12 F/m), εm${\varepsilon _m}$ is the relative permittivity of the suspending medium, Refalse[fCMfalse]$Re[ {{f_{CM}}} ]$ is the real part of the Clausius–Mossotti factor (CMF) of the particle, and E2$\nabla {E^2}$ defines the gradient of the external field magnitude square. The real part of fCM${f_{CM}}$ for a spherical particle is described by the following equation, which depends on medium complex permittivity, εm$\varepsilon _m^*$, and the second effective complex permittivity of the particle, εeff2$\varepsilon _{eff2}^*$ [25]: Re0.28em[]fCMbadbreak=0.28emRe[]εeff2εmεeff...…”
Section: Dep Theorymentioning
confidence: 99%
“…The first effective complex permittivity, εeff1$\varepsilon _{eff1\;}^{*\;}$, depends on the permittivity of the bacteria core, inside of the cytoplasmic region, εc$\varepsilon _c^*$, and the permittivity of the inner shell, εs1$\varepsilon _{s1\;}^{*\;}$, as described by the following equation [24, 25]: εeff10.28em0.28em0.28embadbreak=0.28emεs10.28em0.28em0.28emr2r13+20.28emεcεs1εc2εs1r2r130.28emεcεs1εc+2εs1$$\begin{equation}\varepsilon _{eff1\;}^{*\;}\; = \;\varepsilon _{s1\;}^{*\;}\;\frac{{{{\left( {\frac{{{r_2}}}{{{r_1}}}} \right)}^3} + 2\;\frac{{{\varepsilon _c}^* - {\varepsilon _{s1}}^*}}{{{\varepsilon _c}^* - 2{\varepsilon _{s1}}^*}}}}{{{{\left( {\frac{{{r_2}}}{{{r_1}}}} \right)}^3} - \;\frac{{{\varepsilon _c}^* - {\varepsilon _{s1}}^*}}{{{\varepsilon _c}^* + 2{\varepsilon _{s1}}^*}}}}\end{equation}$$where r 1 and r 2 are the inner and outer shells of the bacteria. The second effective complex permittivity, εeff2$\varepsilon _{eff2\;}^{*\;}$, is then derived by considering the first effective complex permittivity, εeff1…”
Section: Dep Theorymentioning
confidence: 99%
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