2006
DOI: 10.2478/s11534-006-0020-3
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A virtual instrumentation based protocol for the automated implementation of the inner field compensation method

Abstract: Abstract:One influential parameter which mediates interactions between many types of molecules and biological membranes stems from the lumped contributions of the transmembrane potential, dipole potential and the difference in the surface potentials on both sides of a membrane. With relevance to cell physiology, such electrical features of a biomembrane are prone to undergoing changes as a result of interactions with the aqueous surrounding. Among the most useful tools devoted to exploring changes of electrica… Show more

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Cited by 3 publications
(4 citation statements)
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References 27 publications
(23 reference statements)
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“…As illustrated in Figure 1A and demonstrated previously [18,19], in assessing the physical response of a lipid membrane to an applied potential difference (Figure 1B), two considerations are crucial: (i) due to electrostriction effects on an equivalent "elastic" capacitor that models to a first approximation a reconstituted lipid membrane, the If for a such model lipid membrane, the externally applied potential difference consists of a constant term (u 0 ) and a sinusoidal component with amplitude (u 1 ) and pulsation (ω) (ΔV ext = u 0 + u 1 sin(𝜔t)), by virtue of elementary circuit analysis, it follows that the resulting time-dependent capacitive current (I C (t)) embodies three harmonics of the fundamental pulsation (ω) (Supporting Information). For our analysis we focused solely on the second harmonic isolated from the power-spectra of the capacitive current (Figure 2A), which in the time-domain and with the notations employed above writes:…”
Section: Physical Principle Of the Detection Systemsupporting
confidence: 79%
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“…As illustrated in Figure 1A and demonstrated previously [18,19], in assessing the physical response of a lipid membrane to an applied potential difference (Figure 1B), two considerations are crucial: (i) due to electrostriction effects on an equivalent "elastic" capacitor that models to a first approximation a reconstituted lipid membrane, the If for a such model lipid membrane, the externally applied potential difference consists of a constant term (u 0 ) and a sinusoidal component with amplitude (u 1 ) and pulsation (ω) (ΔV ext = u 0 + u 1 sin(𝜔t)), by virtue of elementary circuit analysis, it follows that the resulting time-dependent capacitive current (I C (t)) embodies three harmonics of the fundamental pulsation (ω) (Supporting Information). For our analysis we focused solely on the second harmonic isolated from the power-spectra of the capacitive current (Figure 2A), which in the time-domain and with the notations employed above writes:…”
Section: Physical Principle Of the Detection Systemsupporting
confidence: 79%
“…As illustrated in Figure 1A and demonstrated previously [18, 19], in assessing the physical response of a lipid membrane to an applied potential difference (Figure 1B), two considerations are crucial: (i) due to electrostriction effects on an equivalent “elastic” capacitor that models to a first approximation a reconstituted lipid membrane, the membrane capacitance ( C ) depends quadratically upon the sensed voltage difference (Δ V H ) across its hydrophobic core (C0.33em=C0(1+αnormalΔVnormalH2)$C\ = {C_0}( {1 + \alpha \Delta {V_{\rm{H}}}^2} )$ ( C 0 represents for the minimum value of the membrane capacitance at Δ V H = 0 and α [ V −2 ] is a constant (Supporting Information); (ii) the actual Δ V H embodies three main contributions, arising from the externally applied potential difference across the lipid membrane (Δ V ext ), the difference on the lipid membrane surface potentials ( V S ) measured on both sides of the membrane, and respectively the difference in the membrane dipole potentials (Δ V D ) [20–23], as measured between the cis and trans monolayers of the membrane.…”
Section: Resultsmentioning
confidence: 95%
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“…To only monitor how the difference in the dipole potential of the membrane unfolds in time as a result of specific interactions with phlorizin molecules, the dc bias of the applied voltage signal to the membrane ( U = U 0 + U 1 sin (2πυ t ), ν = 220 Hz, U 1 = 50 mV) was kept constant (usually zero, for symmetrical phosphatidylcholine-based membranes), and the time-evolution of the amplitude of the second harmonic component (at the 440 Hz) was recorded . In such experiments, alamethicin monomers were excluded from the interaction with the lipid membrane.…”
Section: Methodsmentioning
confidence: 99%