Evaporative light scattering detectors (ELSDs), mass spectrometers, and charged aerosol detectors are used routinely for Liquid Chromatography (LC) analysis. In such a device, a liquid sample is converted to droplets by a nebulizer. A carrier gas carries the droplets through a nebulizing cartridge, an impactor, and a drift tube. Conventional devices place the impactor in the path of the droplets to intercept large droplets, which are collected and exit the drift tube through an outlet drain. The remaining appropriately-sized sample droplets pass through the drift tube, which may be heated to aid in evaporation of a solvent portion of the droplets. As the solvent portion of the droplets evaporates, the remaining less volatile analyte passes to a detection cell, or detector, for detection according to the type of device utilized. In the detection cell of an ELSD, for example, light scattering of the sample is measured. In this manner, ELSDs, mass spectrometers, and charged aerosol detectors can be used for analyzing a wide variety of samples.
Conventional detection devices suffer from various drawbacks, including relatively high levels of jagged peak noise detected by the detection cell. Such excessive jagged peak noise can hamper the ability of the detection device to accurately measure the properties of the sample droplets and can decrease sensitivity overall. One conventional strategy for addressing the baseline noise issue of conventional detection devices is to include a diffuser trapping device for preventing large particles, which can increase background noise, from traveling through the drift tube to the detector. Such diffusers, however, are not capable of eliminating all noise. In addition, such diffusers may cause condensation in the drift tube and peak broadening under operating conditions of the detection device. Peak broadening is particularly troublesome for sharp peaks generated from Ultra Performance Liquid Chromatography (UPLC) where the width of a typical peak is between about 0.8 second and about 1.0 second. Therefore, such conventional detection devices with diffusers are unable to adequately reduce noise and increase sensitivity.
The following simplified summary provides a basic overview of some aspects of the present technology. This summary is not an extensive overview. It is not intended to identify key or critical elements or to delineate the scope of this technology. This Summary is not intended to be used as an aid in determining the scope of the claimed subject matter. Its purpose is to present some simplified concepts related to the technology before the more detailed description presented below.
Aspects of the invention relate to new flow controller and impactor technology for liquid chromatography detectors. The flow controller and impactor technology described herein substantially eliminates the jagged peak noise of conventional detection methodologies and significantly reduces the baseline noise for all three detectors mentioned above. Accordingly, aspects of the invention provide a flow controller for a detection device that reduces pressure fluctuations in the droplet flow for decreasing noise and increasing sensitivity. The flow controller includes a flow channel having a cross-sectional area smaller than a cross-sectional area of the drift tube to decrease noise and increase sensitivity, while maintaining adequate signal strength. By reducing such noise, the detection device is capable of achieving a higher level of sensitivity.
Corresponding reference characters indicate corresponding parts throughout the drawings.
As the carrier gas 106 and droplets flow through the nebulizing cartridge 107 and the drift tube 108, which can be heated, evaporation of the mobile phase 102 (solvent) occurs and the size of the droplets decreases. The gas stream continues by entering a detection cell 110 (e.g., an optical cell), which is the detection module of the unit. The stream passes through the detection cell 110 and out an exit port 112 as a waste gas steam 114. The detection cell 110 is adapted for receiving the droplets for analysis, as would be readily understood by one skilled in the art.
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As would be readily understood by one skilled in the art, the specific shape, position, size, and configuration of the impactor 118 can be altered to control what size droplets are intercepted by the impactor and what portion of the droplet flow is allowed to pass through the open areas. Once intercepted, the collected droplets exit the nebulizing cartridge 107 through an outlet drain 120, which can be positioned either upstream or downstream from the impactor 118. As would be understood by one skilled in the art, any material may be used for the impactor.
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The inlet portion 132A includes a tapered inlet sidewall 138 extending from an open mouth 140 of the flow controller 130 and narrowing to the size and shape of the cross-section of the control channel portion 132B. In the embodiment shown, the tapered inlet sidewall 138 is substantially conical in shape and extends at an angle α measured between opposite sides of the tapered inlet sidewall. In one exemplary embodiment, angle α is between about 30 degrees and about 120 degrees. In other exemplary embodiments, the angle α is one of about 30 degrees, about 60 degrees, about 82 degrees, about 90 degrees, about 100 degrees, about 110 degrees, and about 120 degrees. Other α angles between about 30 degrees and about 120 degrees not specifically mentioned here may also be utilized without departing from the scope of the present invention. As would be readily understood by one skilled in the art, different α angles may provide different levels of noise reduction, depending upon other parameters of the ELSD 90. As such, modeling and/or experimentation may be required to optimize noise reduction for a particular ELSD apparatus 90.
The control channel portion 132B of the flow controller 130 comprises a generally cylindrical passage 150. In the embodiment shown, the cylindrical passage 150 is substantially circular. Other cross sectional shapes for the cylindrical passage 150 (e.g., elliptical) are also contemplated as within the scope of the present invention. The length L and width W, or diameter, of the control channel portion 132B may be selected to change the flow dynamics of the droplets as they pass through the flow controller 130. In one exemplary embodiment, the length L of the control channel portion 132B is sized between about 13 millimeters (0.5 inch) and about 25 millimeters (1 inch). In another exemplary embodiment, the width W, or diameter, of the control channel portion 132B is sized between about 3 millimeters (0.1 inch) and about 10 millimeters (0.4 inch). Other lengths L and widths W not specifically mentioned here may also be utilized without departing from the scope of the present invention. As would be readily understood by one skilled in the art, different combinations of lengths L and widths W may provide different amounts of noise reduction, depending upon the other parameters of the ELSD 90. As such, some modeling and/or experimentation may be required to optimize noise reduction for a particular ELSD apparatus 90.
The control channel portion 132B can also be defined according to the ratio of the length L to the width W. In one exemplary embodiment, the L/W ratio of the control channel portion 132B is between about 1.5 and about 20. In another exemplary embodiment, the L/W ratio of the control channel portion 132B is between about 2 and about 5. The control channel portion 132B of the flow controller 130 can also be defined according to the ratio of the cross-sectional area of the control channel portion 132B to the cross sectional area of the drift tube 108. When expressed as a percentage, this ratio indicates the flow area of the flow controller 130 as a percentage of the flow area of the drift tube 108. In one exemplary embodiment, this ratio is between about 2 percent and about 20 percent. In other words, the cross-sectional area of flow of the flow controller 130 is between about 2 percent and about 20 percent the size of the flow area of the drift tube 108. In another exemplary embodiment, the cross-sectional area of flow of the flow controller 130 is between about 3 percent and about 10 percent the size of the flow area of the drift tube 108. In still another exemplary embodiment, where the drift tube 108 has an inside diameter of about 22 millimeters (0.9 inch) and the control channel portion 132B of the flow controller 130 has an inside diameter of about 5 millimeters (0.2 inch), the cross-sectional area of flow of the flow controller is about 5 percent the size of the flow area of the drift tube.
The outlet portion 132C of the flow controller 130 also includes a tapered outlet sidewall 160 extending from the cross-section of the control channel portion 132B to an open exit 164 of the flow controller. In the embodiment shown, the tapered outlet sidewall 160 is substantially conical in shape and extends at an angle β measured between opposite sides of the tapered outlet sidewall. In one exemplary embodiment, angle β is between about 30 degrees and about 120 degrees. In other exemplary embodiments, the angle β is one of about 30 degrees, about 60 degrees, about 82 degrees, about 90 degrees, about 100 degrees, about 110 degrees, and about 120 degrees. Other β angles between about 30 degrees and about 120 degrees not specifically mentioned here may also be utilized without departing from the scope of the present invention. As would be readily understood by one skilled in the art, different β angles may provide different levels of noise reduction, depending upon the other parameters of the ELSD 90. As such, some modeling and/or experimentation may be required to optimize noise reduction for a particular ELSD apparatus 90. It should also be noted that the angle α and the angle β of the flow controller 130 may be different from one another without departing from the scope of the embodiments of the present invention.
The flow controller 130 is adapted to reduce pressure fluctuations and turbulence in the droplet flow, which is believed to be a substantial cause of noise observed by the detection cell 110. Such noise is exhibited as jagged Gaussian peak shape in chromatographs, as will be explained in detail below with respect to
Without being bound to a particular theory, it is believed that a low pressure region forms adjacent (e.g., above) the nebulizer 104 when a significant liquid flow is introduced into the nebulizer 104. It is believed that this low pressure region adjacent the nebulizer 104 causes an oscillation, or fluctuation, or turbulence, in the droplet flow. The pressure oscillation, or fluctuation, or turbulence, disturbs the laminar flow of the droplet flow. This disturbance can be reduced by changing the boundary condition of the droplet stream. In particular, it is believed that the flow controller 130 changes the boundary condition of the droplet stream, thereby reducing the signal noise detected by the detection cell 110. It is also believed that the flow controller 130 focuses the droplets of the droplet stream into the center of the control channel portion 132B of the flow controller, as at least a portion of the droplet flow fluctuation is believed to be spatial in nature. By focusing the droplets toward the center of the control channel portion 132B, this spatial component of fluctuation can be reduced. Moreover, it is also believed that increasing the length L of the control channel portion 132B will further focus the droplets toward the center of the flow channel 132, thereby further reducing the pressure fluctuation.
In addition to reducing turbulence and peak jaggedness, the flow controller 130 also acts as a secondary impactor and further splits a higher percentage of the mobile phase 102. Both the impactor 118 and the flow controller 130 cause the splitting. Thus, a significant amount of the sample with the mobile phase 102 can drain out of the ELSD apparatus 90. To minimize this loss of mobile phase 102, the size of the impactor 118 may be reduced (e.g.,
Over time, liquid can accumulate in the drift tube 108 between the flow controller 130 and the detection cell 110. To address this liquid accumulation, a drain channel 170 formed along the underside of the flow controller 130 extends the length of the flow controller and through the flange 131. This allows the accumulated liquid to flow past the flow controller 130 and flange to the drain 120 located between the nebulizer 104 and the flow controller. As will be explained in greater detail below with respect to the examples of
In one exemplary embodiment, the flow controller 130 is removable from at least one of the nebulizing cartridge 107, the impactor 118, and the drift tube 108, such as for inspection, cleaning, and/or replacement. In another exemplary embodiment, the flow controller 130 may be integrally formed with at least one of the nebulizing cartridge 107, the impactor 118, and the drift tube 108.
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The control channel portion 132B of the flow controller 130 comprises a generally cylindrical passage 150. In the illustrated embodiments, the cylindrical passage 150 is substantially circular. Other cross sectional shapes for the cylindrical passage 150 (e.g., elliptical) are also contemplated as within the scope of the present invention. The length Lc and diameter (e.g., width) Wc of the control channel portion 132B may be selected to change the flow dynamics of the droplets as they pass through the flow controller 130. In an exemplary embodiment, the length Lc of the control channel portion 132B is about 0.5 inches and the diameter (e.g., width) Wc of the control channel portion 132B is between about 0.125 about 0.1875 inches. In the flow controller illustrated in
The outlet portion 132C of the flow controller 130 also connects the control channel portion 132B to an open exit of the flow controller. The outlet portion 132C of the flow controller 130 has a diameter (e.g., width) Wo which is smaller than the diameter (e.g., width) Wi of the inlet portion 132A of the flow controller 130. In particular, the diameter (e.g., width) Wo of the outlet portion 132C of the flow controller 130 may be substantially equivalent to the diameter (e.g., width) Wc of the control channel portion of the flow controller 130. In an exemplary embodiment, the diameter (e.g., width) Wo of the outlet portion 132C of the flow controller 130, is between about 0.125 about 0.1875 inches. In the flow controller illustrated in
The flow controller 130 has a total length Lt which is a function of the selected dimensions (e.g., Wi, α, Lc, Wc, Wo) of the inlet portion 132A, the control channel portion, 132B, and the outlet portion 132C. For example, in the illustrated embodiments, the length Lt of the flow controller 130 is about 2.25 inches.
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Aspects of the present invention are applicable to numerous detection methodologies and systems, including but not limited to Liquid Chromatography Detectors such as ELSDs, Charged Aerosol Detectors, and Mass Spectrometers. The new flow controller technology increases sensitivity, reduces noise, and produces better peak shape for three LS detectors mentioned above. This will translate into higher quality data, better quality control (QC) and higher productivity for customers. This new design also provides reduced manufacturing costs (e.g., reduced by more than $120 per unit compared to a conventional ELSD) by eliminating the need for a impactor. Moreover, implementation of embodiments of the present invention in combination with an improved laser (e.g., a new 20 mW 635 nm laser) provides even greater manufacturing cost reductions (e.g., reduced by more than $200 per unit), and with a much smaller baseline offset, lower baseline noise, better peak shape, and much better reproducibility. As demonstrated herein, the baseline is extremely stable over day to day operation.
Aspects of the improved flow controller are contemplated for implementation into a Flash ELSD system to reduce the effect of drift tube temperature on peak shape.
When introducing elements of the present invention or the embodiment(s) thereof, the articles “a,” “an,” “the,” and “said” are intended to mean that there are one or more of the elements. The terms “comprising,” “including,” and “having” are intended to be inclusive and mean that there may be additional elements other than the listed elements.
As various changes could be made in the above products and methods without departing from the scope of the invention, it is intended that all matter contained in the above description and shown in the accompanying drawings shall be interpreted as illustrative and not in a limiting sense.
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/US09/47029 | 6/11/2009 | WO | 00 | 12/9/2010 |
Number | Date | Country | |
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61060804 | Jun 2008 | US |