Vocab 6 Flashcards

1
Q

Units used in MS to express atomic or molecular masses; defined relative to the mass of the carbon isotope 12/6 , so 1/12 the mass of one neutral 12/6 C atom

A

Atomic Mass Unit (amu) / Dalton (Da).

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2
Q

Refers to the rounded, whole-number precision of an amu measurement

A

nominal mass

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3
Q

Naturally occurring mass of an element in nature

A

Chemical Atomic Mass / Average Atomic Weight (A).

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4
Q

Common abscissa units used for plotting mass spectra; obtained by dividing the atomic or molecular mass of an ion (m) by the number of charges the ion carries

A

mass-to-charge ratio

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5
Q

Method of introducing gaseous or liquid samples directly into MS ionization chamber without the need for preliminary separation stages; usually accomplished by direct injection of small gaseous or liquid volumes into ionization chamber with continuous vacuum; heated inlets are sometimes used to volatilize the sample.

A

Batch Inlet Sample Introduction

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6
Q

Method of introducing solid samples into the MS ionization chamber; direct insertion probe is used where the sample is held onto the end of the probe; probe and sample are introduced into the MS and vacuum then introduced; inlet can be heated to help volatilize the sample.

A

Direct Probe INlet Sample Introduction

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7
Q

Method of introducing gaseous samples into the MS ionization chamber by interfacing the output of a gas chromatograph to the MS ionization chamber

A

gas chromatographic inlet sample introduction

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8
Q

Method of introducing liquid samples into the MS ionization chamber by interfacing the output of a liquid chromatograph to the MS ionization chamber

A

liquid chromatographic inlet sample introduction

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9
Q

Relatively simple MS detector; uses an aligned or tilted collector electrode that is connected to ground through a resistor; voltage drop is amplified using high impedance amplifier

A

Faraday Cup

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10
Q

Most common MS detector; analogous to a photomultiplier tube; ions strike cathode, emitting multiple electrons; each secondary electron strikes a series of intermediate dynodes held at successively higher voltages

A

electron multiplier

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11
Q

MS detector that uses microchannel plate and image intensifier; individual elements in microchannel plat act as electron multipliers; electrons emitted from microchannel plate can be captured and directed to two-dimensional optical array detector

A

Electro-optical Ion Detector

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12
Q

MS source in which the sample is first volatilized into the gas phase, then ionized.

A

Gas-Phase Ionization Source

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13
Q

MS source in which the sample is not first volatilized; rather, the sample probe is used to ionize the sample directly from a liquid or solid state into the gaseous ionic state.

A

Desorption Ionization Source

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14
Q

Highly energetic MS source that imparts large energies to the analyte molecule, resulting in bond cleavage and extensive fragmentation; molecular ion peak may be reduced or absent.

A

Hard Ionization Source

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15
Q

Less energetic MS source that produces simpler spectra with relatively little fragmentation; molecular ion peak predominates.

A

Soft Ionization Source

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16
Q

Most common MS ionization method; hard, gas phase source that ionizes molecules due to electrostatic repulsion; primary products are singly charged positive ions; not an efficient ionization process

A

Electron Ionization Source

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17
Q

radical ion that corresponds to the same molecular weight as the parent molecule

A

Molecular Ion

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18
Q

The largest abundance peak, or the one with the highest response, in the mass spectrum.

A

base peak

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19
Q

Large numbers of positive ion peaks that have m/z values less than that of the molecular ion

A

daughter ions

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20
Q

Peaks in the mass spectrum that occur at m/z values greater than that of the molecular ion; these peaks are attributable to ions having the same chemical formula as the molecular ion, but with different isotopic compositions.

A

Isotope Peaks

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21
Q

Peaks in the mass spectrum due to ion-molecule collisions; most common is the peak that gives the protonated molecular ion due to hydrogen ion exchange.

A

Collision Product Peaks

22
Q

Second most common MS ionization method; gas phase and soft source; ionization process based on gas phase ion-molecule reactions; most commonly used reagent gases are methane, isobutane, and ammonia; main ionization reactions occur in CI through proton transfer (most common), adduct formation, or charge transfer; CI is much gentler ionization source than EI; less fragmentation seen, simpler spectra, much stronger molecular ion peak.

A

Chemical Ionization Source

23
Q

type of gas phase solvation mechanism used by polar molecules in chemical ionization, in which ions can result from association of analyte molecule M with reagent gas RH+, resulting in (R + M)+, with protonated molecular ion MH+, resulting in (2M + H)+, or with a fragment ion F+, resulting in (F + M)+.

A

Adduct Formation

24
Q

Chemical ionization mechanism that uses gases with high ionization potential, e.g. rare gases (Xe), N2 or CO as the reagent gas; reaction occurs by charge transfer; less commonly used ionization method.

A

Charge Transfer

25
Q

Most common mechanism in chemical ionization; gas phase acid-base reaction with reagent ion RH+ (acid) and analyte molecule MH (base) resulting in R and MH2+; results in peak (M + 1)+.

A

Proton Transfer

26
Q

Gas phase acid-base reaction mechanism seen in chemical ionization with reagent ion RH+ (base) and analyte molecule MH (acid) resulting in M+ and RH2; results in peak (M – 1)+.

A

Hydride Transfer

27
Q

Gas phase, soft ionization method in which the ions are formed under the influence of a large electric field; special fine tungsten wires with carbon dendrites are used as electron emitters; results in very little fragmentation, mostly forms molecular ions

A

Field Ionization Source

28
Q

Ionization method in which sample solution is pumped at atmospheric pressure through stainless steel capillary needle at a rate of 1-10 μL min-1; needle is maintained at 3-6 kV with respect to surrounding electrode (electric fields of ~10e6 V m-1); high electric field results in charge accumulation in droplet spray of molecules; as solution droplets become smaller as a consequence of solvent evaporation, charge density becomes greater and desorption of ions into ambient gas phase occurs; ions formed are multiply charged so that their m/z values are small enough to detect with analyzers such as quadrupoles; little fragmentation occurs, application to large biomolecules.

A

Electrospray Ionization (ESI)

29
Q

Desorption method very similar to field ionization, except that it is applicable to more than just gas phase samples; electrode is mounted on a probe that is removed from sample compartment and coated with the sample, which can be either liquid or solid; electrode is then replaced in MS; application of high electrical potential leads to sample desorption; good technique for high MW non- polar species.

A

Field Desorption Source

30
Q

Desorption technique in which condensed-phase sample is bombarded with energetic (keV) Ar0 atoms; sample is typically in form of glycerol mull; used for high molecular weight (10 kDa) polar samples, especially good for biomolecules and polymers.

A

Fast Atom Bombardment (FAB)

31
Q

Desorption technique in which sample is mixed into a UV- absorbing organic matrix and applied to the surface of a metallic probe; probe surface is exposed to UV (250 – 350 nm) excimer laser pulses; matrix absorbs laser pulses causing rapid heating and sublimation of matrix along with ionization of analyte; ion is directed into TOF MS for analysis; spectrum is recorded between laser pulses; little fragmentation occurs, molecular ion peak predominates; very useful for large (>100 kDa) polymers and biomolecules.

A

Matrix Assisted Laser Desorption (MALDI)

32
Q

High vacuum surface analysis technique in which surface is bombarded with high energy (5 – 20 keV) ions (e.g. Ar+); impact of primary Ar+ ions hitting surface causes surface layer of atoms to be stripped or sputtered off; these secondary ions are then directed into a mass spectrometer; very surface sensitive – samples only the first few atomic or molecular layers.

A

Secondary Ion Mass Spectrometry (SIMS)

33
Q

The ratio of the velocities of two molecules in the gas phase is inversely proportional to the square root of the ratio of their masses

A

Graham’s Law

34
Q

The ability of a mass analyzer to yield distinct signals for two ions with a small m/z difference.

A

Mass Resolution, R

35
Q

Single-focusing mass analyzer that uses a permanent magnet or electromagnet to steer the beam of ionized molecules from the MS source; magnet causes ion beam to travel in a circular path of 60° / 90° /180°; ions of different mass are scanned by varying the field strength of the magnet; ions are separated spatially, i.e. sorted in space.

A

Magnetic Sector Mass Analyzer

36
Q

The product of the mass and velocity of a molecule

A

Momentum

37
Q

The circular path that ions travel in the magnetic field of a magnetic sector MS instrument; most common values are 60°, 90°, or 180°

A

degree of deflection

38
Q

Single-focusing mass analyzer that uses a pulsed ionization source (e.g. a laser) to generate ions and accelerates them in an electrostatic field to constant kinetic energy; after leaving source, ions enter a field-free drift tube; since all ions entering the drift tube have the same kinetic energy, their velocities vary inversely with their masses; lighter masses reach detector first, heavier masses later; ions are sorted temporally, i.e. sorted in time.

A

Time-of-Flight Mass Analyzer

39
Q

Electric- and magnetic-field free region of length L in a time-of-flight mass spectrometer; section of TOF MS in which ion separation takes place

A

Drift Tube

40
Q

Type of TOF MS that incorporates a static or time-dependent electric field as an ion mirror to reverse the direction of travel of the ions entering the TOF drift tube; substantially diminishes the spread of flight times of all ions with the same m/z caused by the spread in kinetic energy of these ions, thereby increasing resolution.

A

Reflectron Time-of-Flight Mass Analyzer

41
Q

Refers to the use of two types of mass analyzers in series – electrostatic analyzer followed by a magnetic analyzer – that takes into account both the directional and kinetic energy distributions of the ions to increase resolution; ion beam passes first through electrostatic analyzer, which limits the kinetic energy of ions reaching the magnetic sector analyzer to a small range; magnetic sector analyzer then provides a homogeneous B-field to directionally focus a given mass by momentum & radius of curvature onto the detector; resolution can be up to R ~ 10e5 in some instruments.

A

Double-Focusing Mass Analyzer

42
Q

consists of 4 parallel metal rods that serve as electrodes; these 4 rods are held at a DC voltage, and modulated with AC RF frequencies; At any given set of AC/DC operating conditions, it will transmit only ions within a narrow range of m/z; all other ions are neutralized and carried away as uncharged molecules; mass is tuned by tuning the AC RF frequency; varying the electrical signals to the quadrupole makes possible the variation of the range of m/z values transmitted, therefore spectral scanning is possible.

A

Quadrupole Mass Analyzer / Mass Filter

43
Q

usually 3 quadrupole mass analyzers placed in series; first quadrupole : output is largely molecular ions; serves to separate parent ions by mass selection; second quadrupole : introduce collision gas here (e.g. N2 or He) to fragment parent ions selected by first quadrupole; third quadrupole : allows mass selective detection of daughter ion fragments, provides a spectrum rich in structure.

A

Tandem Mass Spectrometer

44
Q

Device in which ions can be formed and confined for extended periods by electric and/or magnetic fields; formed from central doughnut-shaped ring electrode and pair of end-cap electrodes; ions confined between electrodes of a particular shape that resembles operation of a quadrupole; analyte ions admitted to cell through grid in upper end cap; RF voltage applied to ring electrode: confines ions in trap; variable RF voltages applied to ring electrode: destabilizes lighter ions; lighter ions swept from cell, pass through lower end cap into detector; mass spectrum obtained by increasing RF amplitude, which destabilizes ions of increasing mass

A

Ion Trap Mass Spectrometer

45
Q

Determines m/z of ions based on the cyclotron resonance frequency of ions in a fixed magnetic field; uses trapped ion analyzer cell; gaseous molecules in cell are ionized by pulsed electron beam from source filament; ions held in place by 1 - 5 V potential applied to trap plate; ions are accelerated by RF-frequency pulse applied to transmitter plate; after RF pulse, image current is detected as FID; time domain FID is then Fourier transformed into mass domain spectrum; very high resolution MS technique that can determine masses with high accuracy.

A

Fourier Transform Mass Spectrometer

46
Q

Phenomena related to the motion of gaseous ions in a magnetic field; path of these ions becomes circular in a plane perpendicular to the B field direction

A

Ion Cyclotron Resonance (ICR)

47
Q

Angular frequency of the motion of gaseous ions in a magnetic field perpendicular to the field direction; depends inversely on the m/z value

A

Cyclotron Resonance Frequency ωc

48
Q

Result of the coherent motion of all resonant ions with a particular cyclotron resonant frequency ; induced by circular motion of charged ions interacting with detector plates in ICR cell; coherent character of circulating ions eventually lost due to collisions; decay provides time domain signal detected by detector plates in ICR cell.

A

Image Current

49
Q

FT-MS ICR cell which is conceptually similar to an ion trap; ion source, analyzer and detector are all incorporated into the same cell; gaseous molecules in the cell are ionized by pulsed electron beam from source filament; ions held in place by 1 – 5 V potential applied to trap plates; ions accelerated by RF pulse applied to transmitter plate; ions circulate for extended periods; after RF pulse, image current detected by detector plates.

A

Trapped Ion Analyzer Cell

50
Q

Time domain representation of the intensity decay of the image current as detected by the trapped ion ICR cell; Fourier transform of the FID provides the frequencies, and therefore the m/z values, of the ions that are present in the cell.

A

Free Induction Decay