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1 llows analysis of complicated changes of the equivalent circuits.
2 observed impedimetric effect we performed an equivalent circuit analysis as well as analyzed the role
3                                              Equivalent circuit analysis indicated that electron tran
4         The proposed methodology requires no equivalent circuit analysis or data fitting and is equal
5 lified) and non-faradaic assays, requires no equivalent circuit analysis or prior assumption of respo
6        By using a one-dimensional capacitive equivalent circuit and a resonant tunneling model, this
7 e fitting in order to obtain electrochemical equivalent circuit and corresponding circuit parameters
8 ad to cancer are abstracted as faults in the equivalent circuit and the Boolean circuit model is then
9 , it allows for the analysis of more complex equivalent circuits as associated with the presence of n
10                    As a result, functionally equivalent circuits can produce similar activity despite
11 ional resistance of the Butterworth-Van Dyke equivalent circuit) can be measured simultaneously.
12 ental viewpoint, the direct applicability of equivalent circuit concepts borrowed from microwaves is
13         The impedance data were fitted to an equivalent circuit consisting of a series resistor (R(S)
14 d the behavior of the IDA microelectrode, an equivalent circuit, consisting of an ohmic resistor of t
15  emitter excited state produce an optical ac equivalent circuit current, I(o) = qomega|x(o)|/d, feedi
16 s modeled with either a Helmholtz or Randles equivalent circuit (depending on the SAM used) in which
17 aic contributions present within an improved equivalent circuit description of such interfaces, it is
18                                    A network equivalent circuit element is derived to include the eff
19                        The variable topology equivalent circuit element model of the nanocapillary is
20  Our model consists of a Hodgkin-Huxley-type equivalent circuit for the sarcolemma, coupled with a fl
21                                           An equivalent circuit for the SECM cell and membrane is pro
22 f the electrical parameters that define this equivalent circuit in bulge, transition and mature RGCs.
23                                An electrical equivalent circuit is derived for the electrospray proce
24                                     Using an equivalent circuit mimicking simultaneous whole-cell vol
25                                We develop an equivalent circuit model and introduce a mutual inductan
26 imulating the photocurrent responses with an equivalent circuit model containing a chemical capacitan
27 model for the sensor surface and the Randles equivalent circuit model for interfacial impedance.
28                                          The equivalent circuit model for tissue resistance between t
29 ement with the theoretical analysis using an equivalent circuit model of the new FBAR structure.
30         The macroscopic model consists of an equivalent circuit model of the tethered membrane, and a
31 The obtained EIS spectra were fitted with an equivalent circuit model successfully explaining the imp
32 ent model of the nanocapillary is used in an equivalent circuit model that included contributions fro
33                                We present an equivalent circuit model to describe resistive component
34                 Moreover, we used an adapted equivalent circuit model to get a deeper understanding f
35                                We propose an equivalent circuit model to minimize electrode polarizat
36 t, and in so doing, a full validation of the equivalent circuit model utilized, but also facilitates
37                                           An equivalent circuit model was developed to simulate this
38 d from impedance measurements, an electrical equivalent circuit model was developed.
39     By fitting the data to an electronically equivalent circuit model, cell-related parameters (cell
40 are generated and automatically fit into the equivalent circuit model, which is established using ele
41  response is readily understood via a simple equivalent circuit model.
42                  We derive a lumped-element, equivalent-circuit model for the thickness-shear mode (T
43 the measured frequency responses based on an equivalent-circuit model.
44 n in the impedance data obtained by EIS, and equivalent circuit modeling of the electrodes composed o
45                                           An equivalent circuit modeling-based approach indicates tha
46 V, and kinetic parameters based on electrode-equivalent circuit models are obtained as functions of C
47                 CPEs have been introduced in equivalent circuit models, sometimes without solid justi
48 e impedance data are interpreted by designed equivalent circuit models.
49 y fitting the impedance spectra to a Randles equivalent circuit, one can demonstrate that the charge-
50 t of the impedance minimum of the electrical equivalent circuit or of the corresponding frequency.
51 on pores during degranulation, tracking many equivalent circuit parameters simultaneously.
52 t during the behavior, and assessment of the equivalent circuit, reveal the effectiveness of the beha
53                                           An equivalent circuit that models the impedance response of
54 pproach with point-contact loading and Mason equivalent circuit theory.
55     The results allowed each variable in the equivalent circuit to be estimated.
56                                          The equivalent circuit used for fitting the EIS spectra prov
57 s were interpreted on the basis of a Randles equivalent circuit where the binding of hydrophobic elec
58 ce in impedance was analyzed using a derived equivalent circuit, which is similar to that of open fin
59 ce in impedance was analyzed using a derived equivalent circuit, which is similar to that of open fin
60 ease gap were modeled with a simple Thevenin equivalent circuit, which satisfactorily predicted the e

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