Abstract: A method for monitoring fuel quality of a power system used in transport is provided. The method includes a controller of the power system determining that the prime mover is actively running. The method also includes the controller monitoring an output of a water-in-fuel (WIF) sensor configured to measure an amount of water accumulated in a water collection reservoir of a fuel/water separator that separates water from fuel passing there through. Also, the method includes the controller determining an amount of fuel passing through the fuel/water separator. Further, the method includes the controller calculating a fuel quality score of the fuel based on the output of the WIF sensor and the amount of fuel having passed through the fuel/water separator. The method further includes the controller triggering different alerts based on the calculated fuel quality score.

Abstract: The invention provides a dry electroblotting system for dry blotting gels, in which the system includes an electroblotting transfer stack that comprises an analysis gel and a blotting membrane, an anode, a body of anodic gel matrix juxtaposed with the anode between the anode and the transfer stack, a cathode, and a body of cathodic gel matrix juxtaposed with the cathode between the cathode and the transfer stack, in which the anodic gel matrix and the cathodic gel matrix each comprise an ion source for electrophoretic transfer. The dry electroblotting system does not use any liquid buffers that are added to the system just before electroblotting (such as when the transfer stack is being assembled). The anode, the cathode, or both can be separate from a power supply and provided as part of a disposable electrode assembly that also includes a body of gel matrix that includes ions for electrophoretic transfer.

Abstract: Control of an amplitude of a signal applied to rods of a quadrupole is described. In one aspect, a mass spectrometer includes an amplifier circuit that causes a radio frequency (RF) signal to be applied to the rods of the quadrupole. A controller circuit can determine that the actual amplitude of the RF signal differs than the expected amplitude and, in response, identify current and past environmental and performance parameters to adjust the amplitude.

Abstract: An ion guide is provided for a spectrometer. The ion guide comprises a first electrode assembly, comprising a plurality of guide electrodes aligned along a central axis. Each guide electrode comprises an aperture. The apertures define an ion channel from a first end of the first electrode assembly to a second end of the first electrode assembly. The ion channel is configured to receive an ion beam at the first end. The guide electrodes are configured to receive RF voltages to define a confinement volume for the ion beam, wherein the confinement volume is centred about the central axis. The ion guide comprises a second electrode assembly adjacent to the first electrode assembly, wherein the second electrode assembly is configured to receive a DC voltage, such that a centre of the ion beam is deflected to be off the central axis.

Abstract: A Liquid Chromatography Mass Spectrometry system comprises: a chromatograph; a mass spectrometer configured to ionize separated fractions of a sample received from the chromatograph; and a programmable processor operable to repeatedly execute the steps of: (i) causing the mass spectrometer to perform a data-independent analysis of the precursor ion species using a mass analyzer of the mass spectrometer; (ii) calculating one or more degree-of-matching scores that relate to detection of an internal standard; and (iii) if each of the degree-of-matching scores meets a respective degree-of-matching condition, performing a quantitative tandem mass spectrometric analyses of both the internal standard and the analyte; the programmable processor further operable to calculate a quantity of the analyte in the sample by comparison between intensities of one or more mass spectral signals generated by the quantitative tandem mass spectrometric analyses of the analyte and the internal standard.

Abstract: A method of determining an expected response to injecting a beam of ions of a species of interest into a static field mass filter of a mass spectrometer including a mass analyser is provided. The method includes: measuring an intensity of ions injected into the static field mass filter for various combinations of test ion species, test magnetic field strengths, and test electric field strengths; determining electric field strengths corresponding to an intensity equal to a first and a second fraction of the measured peak intensity; based on a predetermined relationship between magnetic field strength, electric field strength and centre mass of the static field mass filter, determining mass values corresponding to the determined electric field strengths; and interpolating, from said mass values and for each ion species and for at least one of the test magnetic field strengths, expected mass values for an ion species of interest.

Abstract: An analytical instrument comprises a mass analyser and first and second ion traps coupled to the mass analyser. A method of operating the instrument comprises operating the first ion trap in a mode of operation in which the first ion trap confines ions within a first mass-to-charge ratio (m/z) range, storing first ions in the first ion trap, operating the second ion trap in a mode of operation in which the second ion trap confines ions within a second different mass-to-charge ratio (m/z) range, and storing second ions in the second ion trap. The method further comprises ejecting the first ions from the first ion trap into the mass analyser, ejecting the second ions from the second ion trap into the mass analyser, and mass analysing the first ions and the second ions.

Abstract: A method of tuning a static field mass filter of a mass spectrometer, the static field mass filter having a first Wien filter and a second Wien filter. The method comprises injecting a beam of ions into the static field mass filter, applying a magnetic and an electric field in the first and second Wien filters, adjusting a second lens of the filter.

Abstract: A computer-implemented method of simulating a mass filter, which has a bandpass characteristic, of a mass spectrometer includes: receiving a first candidate magnetic field strength and a first candidate electric field strength of the mass filter; based on the received first candidate magnetic and electric field strengths, determining a corresponding centre mass of the mass filter; based on the received first candidate magnetic and electric field strengths, determining the width of a passband of the bandpass characteristic; and determining at least one of a lower or an upper bound of the passband of the bandpass characteristic of the mass filter, the determining of the upper bound including adding a first predetermined fraction of the determined width of the passband to the determined centre mass and the determining of the lower bound comprising subtracting a second predetermined fraction of the determined width of the passband from the determined centre mass.

Abstract: A method of analysing a field of a mass spectrometer comprising a mass analyser and a static field mass filter having a first Wien filter and a second Wien filter is provided. The method includes, for each of a plurality of predetermined strengths of one of an electric field or a magnetic field of the first and second Wien filters: setting the one of the electric field or the magnetic field of the first and second Wien filters to the predetermined strength; causing a beam of ions comprising one or more ion species to be injected through the static field mass filter; and measuring, using the mass analyser, a respective intensity of ions of each of the one or more ion species in the beam.

Abstract: Methods for acquiring mass spectral data comprise determining first and second sets of m/z sub-ranges comprising respective first and second m/z sub-ranges. A sample is mass filtered to isolate ions in the first and second sets of m/z sub-ranges using respective mass filters. Mass analysis is performed to obtain first and second partial mass spectral data sets, the first and second mass filters having first and second response profiles having respective relatively high transmission regions and one or more relatively low transmission regions. The first and second sets of m/z sub-ranges are determined such that relatively high transmission regions of the first response profile and the second response profile at least partially overlap.

Abstract: A method of performing mass spectrometry includes accessing a series of mass spectra of detected ions derived from components eluting from a chromatography column; obtaining, based on the series of mass spectra, an elution profile including a plurality of detection points representing intensity of at least a set of the detected ions as a function of time; and determining, based on a set of detection points included in the plurality of detection points, a predicted next detection point of the elution profile to be obtained based on a next mass spectrum to be acquired subsequent to acquisition of the series of mass spectra.

Abstract: A method for preparing a protein-containing sample for analysis by mass spectrometry includes introducing the sample into a reaction vessel. The reaction vessel contains a reagent mixture including pre-measured quantities of an immobilized proteolytic enzyme, a reducing agent and an alkylating agent. The contents of the reaction vessel are activated by heating or by sonication.

Abstract: A low friction wear film includes a chromium layer provided on a surface of a metal substrate, a tungsten carbide layer provided on a surface of the chromium layer, and a diamond-like carbon layer as a top layer provided on a surface of the tungsten carbide layer. The tungsten carbide layer includes a chromium-tungsten carbide gradient layer and a tungsten carbide uniform layer. In the tungsten carbide layer, a tungsten-concentrated layer in which a tungsten simple substance is present is not provided at a boundary between the chromium-tungsten carbide gradient layer and the tungsten carbide uniform layer.

Abstract: Methods for acquiring mass spectral data of a sample across at least a portion of an m/z range comprise receiving mass spectral data across the m/z range and partitioning the m/z range into one or more sets of m/z sub-ranges, each set comprising one or more m/z sub-ranges, by dividing the m/z range into a plurality of m/z bins, determining an indication of ion abundance for each m/z bin, based on the mass spectral data, and forming an m/z sub-range of the one or more sets of m/z sub-ranges by assigning m/z bins having ion abundances that correspond to at least a threshold degree to the formed m/z sub-range. A mass analysis is performed on the sample for each set of m/z sub-ranges, thereby acquiring one or more partial mass spectral data sets.

Abstract: Methods for acquiring mass spectral data of a sample across at least a portion of an m/z range include receiving mass spectral data of the sample across the m/z range. The m/z range is partitioned into one or more sets of m/z sub-ranges, each set comprising one or more m/z sub-ranges, by dividing the m/z range into a plurality of m/z bins, determining an indication of ion abundance for each m/z bin, based on the mass spectral data, and forming an m/z sub-range of the one or more sets of m/z sub-ranges by assigning m/z bins having ion abundances that correspond to at least a threshold degree to the formed m/z sub-range. A mass analysis is performed on the sample for each set of m/z sub-ranges, thereby acquiring one or more partial mass spectral data sets.

Abstract: A Time of Flight (TOF) mass analyser comprises an ion source, a detector, an electrode, and a resistive divider comprising first and second resistors. The ion source and the detector define an ion flight path from the ion source to the detector. The electrode is arranged along the ion flight path and receives an output voltage. Thermal expansion produces a first mass shift/Kelvin of detected ions. The resistive divider is thermally coupled to the TOF mass analyser to receive an input voltage and output an output voltage to the electrode. The first and second resistors have respective first and second temperature coefficients that provide a voltage shift/Kelvin to the output voltage to the electrode producing a second mass shift/Kelvin of detected ions, compensating for the first mass shift/Kelvin.