Analytical Exam 2

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169 Terms

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Potentiometry

Use of electrodes to measure voltage and obtain chemical information about analyte activity.

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Indicator (working) electrode

Electrode whose potential responds to analyte activity or concentration.

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Reference electrode

Electrode that maintains a known, stable potential while the indicator electrode responds to the sample.

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Standard hydrogen electrode (SHE)

Primary reference standard assigned E° = 0.000 V; practical measurements often use convenient Ag/AgCl or calomel references.

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Ag/AgCl reference electrode

Half-cell AgCl(s) + e- ⇌ Ag(s) + Cl-; E° = +0.222 V and about +0.197 V in saturated KCl.

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Calomel reference electrode

Half-cell 1/2 Hg2Cl2(s) + e- ⇌ Hg(l) + Cl-; E° = +0.268 V and about +0.241 V in saturated KCl.

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Saturated calomel electrode (SCE)

Calomel electrode containing saturated KCl; its potential is about +0.241 V under the stated conditions.

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Cell potential, Ecell

Difference between the right- and left-electrode potentials under the chosen cell convention; use reduction potentials consistently and account for the reference electrode.

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Nernst equation

Relates electrode potential to activities: E = E° - (RT/nF) ln Q; at 25°C, E = E° - (0.05916 V/n) log Q.

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Metal indicator electrode

Conducting metal surface develops a potential through a redox equilibrium involving the analyte; examples include Pt, Au, and carbon surfaces.

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Platinum indicator electrode

Common relatively inert redox indicator electrode; best response requires a large, clean surface.

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Ion-selective electrode (ISE)

Electrode that responds selectively to an ion by membrane binding/partitioning rather than an analyte redox reaction.

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Ionophore

Ligand in an ISE membrane that selectively binds and carries a target ion through the membrane.

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Liquid-based ISE membrane

Hydrophobic polymer containing viscous organic phase, ionophore, and hydrophobic counterion; target ion can cross while other ions are largely excluded.

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ISE inner filling solution

Contains a fixed target-ion concentration and counterion; its constant activity helps make the inner membrane potential stable.

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Membrane potential

Potential generated by selective ion partitioning/diffusion across an ISE membrane; varies with target-ion activity in the sample.

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Potassium ISE ligand

Valinomycin, selected for high affinity for K+ relative to many other ions.

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ISE response equation

For an ideally selective monovalent cation at 25°C, potential changes by about 59.16 mV per tenfold activity change; slope magnitude is 0.05916/n V per decade for charge n.

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Junction potential

Voltage difference at the boundary between dissimilar electrolyte solutions, caused by ions diffusing at different rates.

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Observed potentiometric voltage

Observed voltage includes cell potential plus liquid-junction contribution: Eobserved = Ecell + Ejunction (with sign set by cell convention).

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Reducing junction potential

Use a salt bridge electrolyte whose ions have similar mobilities, commonly concentrated KCl, to minimize charge separation.

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Glass pH electrode

ISE with a thin hydrated glass bulb whose membrane potential responds mainly to external hydrogen-ion activity.

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Hydrated glass gel layer

Thin water-rich layer on each glass surface where H+ can exchange with metal cations in the glass; inner and outer layers are separated by dry glass.

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Glass membrane ion exchange

H+ from solution replaces mobile metal cations (such as Na+) in the hydrated glass layer; this creates the pH-dependent membrane potential.

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pH electrode reference system

Two Ag/AgCl reference electrodes and fixed internal chloride/hydrogen-ion conditions measure the potential across the glass membrane.

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pH calibration

Measure voltage in at least two standard buffers of known pH to establish the electrode slope/intercept and electromotive efficiency.

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Electromotive efficiency, b

Practical glass-electrode slope relative to the ideal Nernst slope; typically greater than 0.98 and determined by calibration.

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pH measurement errors

Important sources include standards, junction potential and drift, sodium error, acid error, equilibration time, glass hydration, temperature, and cleaning.

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Sodium error

At high pH, glass electrode may respond to Na+ as well as H+, causing the indicated pH to be lower than the true pH.

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Acid error

At very low pH, glass electrode response becomes non-ideal and often indicates a pH higher than the true pH.

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ISE selectivity coefficient

Quantifies an electrode's relative response to an interfering ion compared with the target ion; smaller interference coefficient means better selectivity.

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ISE classes

Glass membrane, solid-state, liquid-based, and compound electrodes.

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Solid-state ISE

Uses an inorganic crystal membrane through which the target ion migrates selectively.

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Fluoride ISE

Uses Eu2+-doped LaF3 crystal; dopant creates anion vacancies that allow F- migration; used to monitor water fluoridation.

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Fluoride electrode filling solution

Typically 0.1 M NaF and 0.1 M NaCl in the described electrode.

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SECTION: CHAPTER 18 - SPECTROPHOTOMETRY

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Spectroscopy

The theoretical study of interactions between matter and radiated energy.

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Spectrometry

The practical measurement/application of spectroscopy using instruments such as spectrometers.

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Spectrophotometry

Quantitative measurement of how much a substance absorbs light as a beam passes through a sample.

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Spectrophotometer

Instrument that measures transmission or reflection as a function of wavelength to produce a spectrum.

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Wavelength, λ

Distance between successive wave maxima or minima; usually measured in m or nm.

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Frequency, ν

Number of oscillations per second; measured in Hz or s-1.

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Speed of light relationship

c = νλ; speed of light c is approximately 3.00 x 10^8 m/s.

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Photon

Particle of electromagnetic radiation with energy E = hν = hc/λ.

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Planck constant, h

6.626 x 10^-34 J s.

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Irradiance, P

Energy per second per unit area carried by a light beam; absorption reduces transmitted irradiance.

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Monochromatic light

Light consisting of one wavelength (ideally); required for Beer’s law in its simple form.

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Transmittance, T

Fraction of incident light transmitted: T = P/P0, where P0 is incident and P is transmitted irradiance.

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Percent transmittance

%T = 100(P/P0).

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Absorbance, A

Logarithmic measure of light absorbed: A = -log10(T) = log10(P0/P).

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Beer-Lambert law

A = εbc; absorbance equals molar absorptivity times pathlength times analyte concentration.

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Molar absorptivity, ε

Proportionality constant in Beer’s law, typically M^-1 cm^-1; depends on analyte and wavelength.

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Pathlength, b

Distance light travels through the sample, usually in cm; common cuvet pathlength is 1.000 cm.

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Chromophore

Part of a molecule responsible for its light absorption.

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Beer’s law assumptions and limits

Best applies to dilute solutions (about ≤0.01 M) and monochromatic light; it can fail with chemical changes, nonlinearity, or other deviations.

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Absorption of light

Analyte absorbs a photon and moves to a higher-energy molecular state; transmitted irradiance decreases.

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Spectrophotometer components

Continuous light source, monochromator to select a narrow wavelength band, sample, and detector for emergent irradiance.

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Cuvet

Transparent sample cell used in UV-visible spectrophotometry; sample and reference cuvets should be matched and positioned consistently.

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Quartz/fused-silica cuvet

Transmits UV and visible light and is suitable for UV-visible measurements.

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Glass cuvet

Suitable for visible light but absorbs UV, so it is unsuitable for many UV measurements.

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IR sample cells

Typically made of NaCl or NaBr, which transmit infrared radiation.

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Mull

Solid sample ground and dispersed in mineral oil (Nujol), then pressed between KBr plates for IR measurement.

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Single-beam spectrophotometer

Measures blank/reference irradiance P0, then replaces the blank cuvet with the sample and measures P.

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Double-beam spectrophotometer

Splits or alternates light between sample and reference cuvets to compare their signals.

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Baseline spectrum

Reference spectrum recorded before the sample; subtracted from the sample spectrum to correct background.

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Wavelength of maximum absorbance, λmax

Chosen for analysis because sensitivity is high and absorbance changes relatively little with small wavelength shifts.

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Useful absorbance range

Approximately 0.4 to 0.9; too much absorption leaves little measurable light, while too little makes sample and blank hard to distinguish.

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Noise and detection

Lower instrumental noise generally allows detection of lower analyte concentrations.

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Good cuvet practice

Use matched cuvets, place them consistently, and wipe fingerprints and dust from optical faces.

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Analyte suitability for spectrophotometry

Analyte must absorb at a measurable wavelength and its absorption should be distinguishable from other sample components.

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Molecular absorption and energy levels

Absorption promotes a molecule to an excited state; emission returns it to a lower-energy state and releases a photon.

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Electronic transition

Transition between electronic energy states; requires more energy than typical vibrational or rotational transitions.

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Vibrational transition

Change in molecular vibrational motion; can be induced by infrared radiation.

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Rotational transition

Change in molecular rotational motion; can be induced by microwave radiation.

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Vibrational relaxation

Nonradiative loss of excess vibrational energy within an electronic state, usually as heat.

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Internal conversion (IC)

Nonradiative transition between electronic states of the same spin multiplicity, such as S1 to S0.

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Intersystem crossing (ISC)

Nonradiative transition between states of different spin multiplicity, such as S1 to T1.

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Singlet state, S

A state in which electron spins are paired; common fluorescent emission occurs from S1 to S0.

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Triplet state, T

A state with parallel electron spins; phosphorescence commonly occurs from T1 to S0.

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Fluorescence

Photon emission from an excited singlet state to a lower singlet state; typical lifetime about 10^-10 to 10^-8 s.

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Phosphorescence

Photon emission from an excited triplet state to a singlet ground state; typical lifetime about 10^-4 to 10^2 s.

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Luminescence

Light emission from an electronically excited molecule, including fluorescence and phosphorescence.

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Nonradiative transition

Relaxation that releases energy without emitting a photon, commonly as heat.

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Stokes shift

Emission occurs at lower energy and longer wavelength than absorption because some energy is lost before emission.

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Emission spectrum

Plot of emitted-light intensity versus emission wavelength, λem.

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Excitation spectrum

Plot of emission intensity versus selected excitation wavelength, λex.

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Emission measurement geometry

Select an excitation wavelength and commonly observe emitted light at 90 degrees to the incident beam to reduce transmitted and scattered excitation light.

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Mirror-image relation

Emission spectrum is often roughly the mirror image of the absorption spectrum, with vibronic structure shifted to longer wavelengths.

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0-0 transition, λ0

Highest-energy emission transition between lowest vibrational levels of excited and ground electronic states; further emission peaks occur at longer wavelengths.

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Emission intensity and concentration

At low concentration, emission intensity is proportional to absorbed irradiance and approximately proportional to analyte concentration.

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SECTION: SENSORS AND ATOMIC SPECTROSCOPY

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Luminescence-quenching sensor

Uses a change in excited-state emission caused by a quencher to measure quencher concentration.

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Excited-state molecule, M*

Molecule after absorbing a photon; it can emit light, lose energy as heat, or transfer energy to a quencher.

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Excitation rate

Rate of excited-state formation by absorption: proportional to ka[M] for incident light of fixed intensity.

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Emission rate

Excited-state loss by photon emission: ke[M*].

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Nonradiative decay rate

Excited-state loss as heat: kd[M*].

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Quenching rate

Excited-state loss by interaction with quencher Q: kq[M*][Q].

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Quantum yield, Φ

Fraction of absorbed photons that produce the specified outcome, such as emitted photons.

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Unquenched emission quantum yield, Φ0

Φ0 = ke/(ke + kd) when no quencher is present.

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Emission quantum yield with quencher, Φ

Φ = ke/(ke + kd + kq[Q]) for the stated dynamic quenching model.