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Electrochemical Theory. Kinetics of Activation Controlled Reactions. M M n+ + ne - rate of reaction depends on potential according to the Tafel equation:. Tafel’s Law. Slope . Slope b. b =2.303 . Potential. E 0 a. i 0,a. ln | i |. log | i |. Charge Transfer Resistance.
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Kinetics of Activation Controlled Reactions M Mn+ + ne- • rate of reaction depends on potential according to the Tafel equation:
Tafel’s Law Slope Slope b b=2.303 Potential E0a i0,a ln |i| log |i|
Charge Transfer Resistance • Charge transfer resistance = local slope of i versus E curve (not log i)
Charge Transfer Resistance • Note that charge transfer resistance is not a constant, but depends on the applied current density • If we could measure the charge transfer resistance, we could determine the current density
Dependence of Kinetics on Reactant Concentration • More reactant allows reaction to go faster, hence rate is proportional to reactant concentration • e.g. oxygen reduction Surface concentration of oxygen Minus sign because thisis a cathodic reaction(and c is taken as positive)
[O2] [O2] [O2] Tafel’s Law Cathodic reaction - rate increases withdecreasing potential Rate with constantsurface concentrationof oxygen Rate with surface concentration of oxygen varying E0c Potential i0,c ln |i| log |i| ilim
Mixed Potential Theory • Net current density on freely-corroding electrode must be zero. • Therefore potential (Ecorr) will be that at which anodic and cathodic current densities are equal and opposite. • Called a mixed equilibrium (not a true electrochemical equilibrium)
Tafel’s Law Potential log |i|
Tafel’s Law E0c Potential i0,c ln |i| log |i| ilim
Charge • Results from inbalance between electrons and protons in a metal, or between anions and cations in a solution • Unit the coluomb, C • Charge on the electron = 1.6 x 10-19 C
Current • Flow of charge past a point in a conductor (either electron or ion) • Unit the Amp, A
Conservation of Charge • Charge can be neither created nor destroyed • Hence, the currents into and out of a point in an electrical circuit must add up to zero (Kirchoff’s Law)
Potential • The potential at a point in space is the work done in moving a unit charge to that point from infinity. • Units of volts, V (=J/C)
Potential Difference (or Voltage) • The potential difference or voltage is the difference between the potentials at two points, and hence the work done in moving a unit charge from one point to the other. • Units of Volts
Resistance • A resistor (conventional symbol R) is a device that produces a voltage across its terminals when a current passes through it • Ohm’s Law V=IR • R is the resistance of the resistor • Units Ohms, • 1 V is produced by a current of 1 A through a resistance of 1
Capacitance • A capacitor (conventional symbol C) is a device that stores charge when a current is applied to it • Units of capacitance Farads, F • I = C dV/dt • A 1 F capacitor will produce a voltage increase of 1 V/s when a current of 1 A flows into it
Rct Metal Solution Cdl Equivalent Circuits • An electrical circuit with the same properties as a metal-solution interface • The simplest circuit is a resistor, corresponding to the polarization resistance, in parallel with a capacitor, corresponding to the double layer capacitance
Rct Metal Rct Solution Cdl Equivalent Circuits • An electrical circuit with the same properties as a metal-solution interface • The Randles equivalent circuit adds a series resistor, corresponding to the solution resistance
Electrode Potential • The potential of a metal electrode with respect to a solution. • BUT the charge carriers in a metal are electrons, while the charge carriers in a solution are ions. • So how do we measure it?
Measurement of Electrode Potential • Use arbitrary reference electrode to convert from ion current to electron current. • Conventional standard reference electrode is based on the reaction Hydrogen ions in solution at unit activity Electrons in the metal Hydrogen gas in solution at unit activity
Secondary Reference Electrodes • Reference electrodes of the first kind, a metal in equilibrium with a soluble salt: Potential controlled by Cu2+ concentration
Secondary Reference Electrodes • Reference electrodes of the second kind, a metal in equilibrium with a sparingly soluble salt and a solution containing anions of the salt: Ag+ concentration controls equilibrium potential Chloride concentration controls Ag+ concentration [Ag+][Cl-] = const
Potential Measurement Requirements - Input Resistance • High input resistance to minimize errors due to source resistance. • For most corrosion work 107 ohm is sufficient, but for high resistance systems (paints, passive metals etc.) 109 ohm or more may be better.
Potential Measurement Requirements - Frequency Response • Frequency response (ability to detect rapid changes). Often not important for corrosion measurements. • Measurements at around 1 Hz are quite easy • Measurements above 1kHz are rather more difficult • Measurements at around 50 Hz are difficult (due to mains frequency interference).
Potential Measurement Requirements - Resolution • Resolution is the ability to detect small changes in a large value • for most corrosion measurements 1 mV is adequate • for electrochemical noise and similar studies, 1mV may be necessary
Potential Measurement Requirements - Sensitivity • Resolution is the ability to detect small changes in a large value • Sensitivity is the ability to measure small values • e.g. it is relatively easy to obtain a sensitivity of 1 mV when measuring 1 mV, but it is very difficult to obtain a resolution of 1 mV when measuring a 10 V signal • not usually a problem for corrosion measurements
Potential Measurement Requirements - Precision • Resolution is the ability to detect small changes in a large value • Sensitivity is the ability to measure small values • Precision or accuracy is the ability to measure the ‘true’ value
Potential Measurement Methods • Analogue meter (moving coil) • low impedance (typically 20 kohm/V) • poor frequency response (~1 Hz) • low sensitivity (~1 mV) • low resolution (~1%) • low precision (~3%)
Potential Measurement Methods • Analogue meter (electronic) • high impedance (typically 10 Mohm) • poor frequency response (~1 Hz) • possibly high sensitivity (~1mV) • low resolution (~1%) • low precision (~3%)
Potential Measurement Methods • Digital meter • high impedance (typically 10 Mohm or more) • poor frequency response (around 3 Hz) • high sensitivity (10 mV to 100 nV) • high resolution (0.1% to 0.0001%) • high precision (0.1% to 0.0001%)
Potential Measurement Methods • Electrometer (digital) • very high impedance (~1014 ohm) • poor frequency response (<1 Hz) • high sensitivity (1 mV to 100 nV) • high resolution (0.1% to 0.001%) • high precision (0.1% to 0.001%)
Potential Measurement Methods • Chart recorder • impedance depends on instrument (from 103 to 107 ohm) • moderate frequency response (~10 Hz) • moderate sensitivity (~10mV) • moderate resolution (~0.1%) • moderate precision (~0.1%)
Potential Measurement Methods • Oscilloscope • high impedance (106 to 107 ohm) • high frequency response (10 MHz or more) • moderate sensitivity (~100mV) • poor resolution (~1%) • poor precision (~1%)
Potential Measurement Methods • Computer data acquisition • high impedance (~107 ohm) • variable frequency response (10 Hz to 1 MHz or more) • moderate to good sensitivity (~10 mV) • moderate to good resolution (0.5 to 0.01%) • moderate to good precision (0.5 to 0.01%) • facilitates subsequent plotting and analysis
Current Measurement Requirements - Input Resistance • Low input resistance to minimize errors due to voltage drop across measuring device. • For most corrosion work 1 mV voltage drop will have little effect. • A wide dynamic range (ratio of largest current to smallest current) is required for many corrosion measurements.
Current Measurement Methods • Analogue meter (moving coil) • usually poor input resistance (~ 75 mV drop at full scale) • poor frequency response (around 1 Hz) • low resolution (around 1%) • low precision (around 3%) • dynamic range acceptable using range switching
Current Measurement Methods • Analogue meter (electronic) • usually poor input resistance (~100 mV drop at full scale) • poor frequency response (around 1 Hz) • low resolution (around 1%) • low precision (around 3%) • dynamic range acceptable using range switching
Current Measurement Methods • Digital multimeter • often poor input impedance (~100 mV drop at full scale) • poor frequency response (around 3 Hz) • high resolution (0.1% to 0.0001%) • high precision (0.1% to 0.0001%) • often poor sensitivity (100 mA to 1 mA) • dynamic range acceptable using autoranging
Current Measurement Methods • Electrometer (digital) • essentially zero input impedance • poor frequency response (<1 Hz) • high resolution (0.1% to 0.001%) • high precision (0.1% to 0.001%) • good dynamic range using range switching or autoranging
Current Measurement Methods • Chart recorder • resistor used to convert current to voltage, hence voltage drop depends on sensitivity • moderate frequency response (~10 Hz) • moderate resolution (~0.1%) • moderate precision (~0.1%) • acceptable dynamic range providing range switching is used
Current Measurement Methods • Oscilloscope • resistor used to convert current to voltage, hence voltage drop depends on sensitivity • high frequency response (10 MHz or more) • poor resolution (~1%) • poor precision (~1%) • poor dynamic range
Current Measurement Methods • Computer data acquisition • resistor used to convert current to voltage, hence voltage drop depends on sensitivity • variable frequency response (10 Hz to 1 MHz or more) • moderate to good resolution (0.5 to 0.01%) • moderate to good precision (0.5 to 0.01%) • dynamic range often limited • facilitates subsequent plotting and analysis