spectroscopy measures how electrochemical systems resist alternating current flow. It combines resistance and reactance, allowing us to separate and study different processes happening in the system based on their timing.
Interpreting impedance data involves analyzing Nyquist and Bode plots, which show how the system behaves at different frequencies. We can then model the system using equivalent circuits, helping us understand the physical processes occurring.
Fundamentals of Impedance Spectroscopy
Impedance in electrochemical systems
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Top images from around the web for Impedance in electrochemical systems
The electrical modulus and other dielectric properties by the impedance spectroscopy of LaCrO 3 ... View original
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Frontiers | Capacity Increase Investigation of Cu2Se Electrode by Using Electrochemical ... View original
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Fundamentals and Applications of Electrochemical Impedance Spectroscopy - A Didactic Perspective View original
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The electrical modulus and other dielectric properties by the impedance spectroscopy of LaCrO 3 ... View original
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Frontiers | Capacity Increase Investigation of Cu2Se Electrode by Using Electrochemical ... View original
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Impedance measures the opposition to alternating current (AC) flow in an electrical circuit
Complex quantity consisting of resistance and reactance represented as a vector sum: Z=R+jX, where Z is impedance, R is resistance, and X is reactance
Resistance opposes current flow in an ideal resistor, dissipating energy as heat and is frequency-independent
Capacitance stores electrical charge, with capacitors storing energy in an electric field
Capacitive reactance is frequency-dependent: XC=2πfC1, where XC is capacitive reactance, f is frequency, and C is capacitance
Principles of impedance spectroscopy
Powerful technique for studying complex electrical properties of electrochemical systems
Applies small amplitude AC signal over a range of frequencies to an electrochemical cell and measures current response to applied voltage
Separates different electrochemical processes based on their time constants, such as charge transfer reactions, diffusion processes, and adsorption phenomena
Data represented in Nyquist plots (imaginary vs. real impedance) or Bode plots (log impedance magnitude and phase angle vs. log frequency)
Interpretation of EIS plots
Nyquist plots: each point represents impedance at a specific frequency
High-frequency region (left side) corresponds to charge transfer processes
Low-frequency region (right side) corresponds to mass transfer processes
Phase angle plot: peaks indicate presence of time constants, frequency at peak maximum related to characteristic frequency of the process
Equivalent circuits for EIS
Equivalent circuit models interpret EIS data and relate it to physical processes
Common equivalent circuit elements:
Resistors (R): represent ohmic resistances (solution resistance, charge transfer resistance)
Capacitors (C): represent double-layer or coating capacitance, ideal capacitors have -90° phase angle
Constant Phase Elements (CPE): model non-ideal capacitive behavior due to surface roughness or inhomogeneity, impedance: ZCPE=Q(jω)n1, where Q is CPE coefficient and n is CPE exponent (0 ≤ n ≤ 1)
Warburg elements (W): represent semi-infinite linear diffusion, impedance: ZW=ωσ−jωσ, where σ is Warburg coefficient
Equivalent circuits constructed by combining elements in series or parallel to model the electrochemical system