The present application relates to systems and methods for measuring optical properties of liquids, and subsystems and components thereof and therefor, and their operation.
Certain liquids, such as petroleum-based fuels, must meet optical standards and specifications to confirm quality and lack of water and/or particulates within the liquids. Cloudiness and/or haziness in a fuel, which may be caused by the presence of suspended solid particulates and/or water within the fuel, can lead to the fuel not meeting the required optical specifications.
The determination of optical properties, such as haze, clarity, and color allows the quality of petroleum-based fluids, such as fuels and lubricants, to be assessed. Typically, such properties are determined by subjective techniques. For example, the determination of haze in fuels has typically involved the use of subjective, visual techniques, such as that defined by ASTM D4176, Procedure 2. When measurement of optical properties of liquids is reliant upon subjective visual techniques, results vary with operator and lighting conditions.
Current methods for determining the optical properties of certain fuel samples include visual comparison to a standard, which can lead to variations in results. One current method is using bench-top analyzers, which depend on calibration and are sensitive to sample cup properties and other factors. Often, optical property measurement methods require the use of large equipment that is not easily transported, such that samples are analyzed at a remote location rather than on-site where the sample is taken, causing time delays and increasing the risk of errors.
There is a need in the fuel industry for an easy-to-use, hand-held instrument to measure the optical properties of such liquids both quickly and accurately to ensure compliance with standards. There is a need in the fuel industry for a hand-held instrument to measure the optical properties of such liquids at an on-site location (i.e., the location where the sample is taken) rather than a remote lab.
Some embodiments of the present disclosure include a system for measuring optical properties of liquid samples. The system includes a sample inlet, at least one multi-wavelength light source, at least one collimating optical chain, at least one beam-splitter, and at least one light sensor.
Some embodiments of the present disclosure include a method for measuring an optical property of a fluid environment (e.g., liquid or gas) that entails directing a transmitted light through a target environment or an intact and in-situ portion thereof (e.g., a sample) and receiving the directed transmitted light for measurement of the optical property. The system for performing the measurement includes a light source operable to generate and/or a transmit light, and a probe portion adapted for insertion or immersion in the target fluid environment. The probe portion includes a housing for accommodating a light pathway or travel of the transmitted light therethrough, and the housing includes a space that intermediates a proximal (device handle or dry end) and a distal end immersible in the target environment. The system, probe or probe section is configured to include a continuous, solid body with a space intermediate the proximal end and distal end. The space is disposed and configured so as to be substantially in fluid communication with the remainder of the target environment (the remaining volume) and generally in equilibrium therewith. The probe or housing is further configured such that the light path is directed within the housing and through the space, and outside of the probe portion in the manual or dry end. The manual or dry end may house electronics, a central processing unit (CPU), and/or data storage for the optical measurement system. In some embodiments, the space is insertable with the probe portion in the target environment so that the fluid environment occupies the space and, in this way, provides the device or probe a portion or sample of the environment that is spatially and temporally maintained within the target environment during measurement (i.e., when the transmitted light is directed therethrough). In further embodiments, the “sampling space” is provided as or with a window disposed in the housing that is open to and in fluid communication with the target environment outside of the probe portion. In some embodiments, the space is sufficiently sized and configured to readily allow (draw) the fluid therein upon the inserted probe portion displacing fluid in the environment. Care may be taken to minimize disturbance of, and energy transfer with, the fluid environment as may be desirable for measurement purposes.
Another embodiment of the present disclosure includes a spectroscopy method for measuring optical properties of liquid samples. The method includes providing a sample inlet, providing at least one multi-wavelength light source, providing at least one collimating optical chain disposed between the light source and the sample inlet to collimate the light, providing at least one beam-splitter disposed between the light source and the sample inlet to direct the light, and providing at least one sensor to measure the intensity of the light.
Another embodiment of the present disclosure includes a system for measuring optical properties of liquid samples. The system includes a housing. The housing includes or houses a multi-wavelength light source, a collimator, a beam-splitter, and a light sensor. The system includes a probe extending from the housing. The probe includes a sample inlet configured to receive a liquid sample. The multi-wavelength light source is positioned to direct light to the collimator, the collimator is positioned to direct light to the beam-splitter, the beam-splitter is positioned to direct light to the probe, and the light sensor is positioned to receive light transmitted through the probe.
Another embodiment of the present disclosure includes an apparatus for measuring an optical property of a liquid target. The apparatus includes a housing, a collimator supported by the housing, and a beam splitter supported by the housing in optical communication with the collimator.
Another embodiment of the present disclosure includes an apparatus for measuring an optical property of a liquid target. The apparatus includes a housing including a light source and an optical property measuring mechanism. A probe portion extends from the housing and includes a sampler to contact the liquid target.
Another embodiment of the present disclosure includes a method of measuring an optical property of a target liquid. The method includes providing a container of the target liquid, and providing a housing supporting a spectroscopy-based mechanism for measuring the optical property. The housing includes a probe portion having a sampler for contacting a target liquid. The method includes inserting the probe portion into said container such that the probe receives said liquid target. The method includes operating the measuring mechanism, including communicating light to said received liquid target to measure the optical property.
Another embodiment of the present disclosure includes a method of measuring optical properties of a liquid in a local environment. The method includes immersing at least a portion of a probe in the liquid within the local environment such that a sample inlet of the probe is surrounded by the liquid within the local environment and at least a portion of the liquid enters into the sample inlet. The method includes, with the portion of the probe immersed in the liquid within the local environment, transmitting a light along a path within the probe and through a portion of the liquid in the sample inlet and receiving the light at a first sensor. The method includes, with the portion of the probe immersed in the liquid within the local environment, measuring at least one property of the light with the first sensor. The method includes determining at least one property of the liquid using the at least one property of the light.
So that the manner in which the features and advantages of the systems and methods of the present disclosure may be understood in more detail, a more particular description briefly summarized above may be had by reference to the embodiments thereof which are illustrated in the appended drawings that form a part of this specification. It is to be noted, however, that the drawings illustrate only various exemplary embodiments and are therefore not to be considered limiting of the disclosed concepts as it may include other effective embodiments as well.
The present disclosure includes methods, systems, and apparatus for measuring optical properties and, more particularly, measuring the optical properties of a liquid sample within a target environment. As used herein, a “target environment” is an environment in which a liquid sample is present. A target environment may be part of larger environment. In some embodiments, the probe in accordance with the present disclosure is configured to receive and/or isolate a target liquid sample within a target environment. For example, typically a liquid sample is taken from a bulk source of the liquid and is then placed into a measurement device. Embodiments of the present probe-based system are, instead, placed into the bulk source of the liquid. That is, the probe-based system disclosed herein is positioned within the target environment such that the optical properties of the liquid are measured within the target environment, rather than the liquid being transported to a remote location (e.g., a laboratory) for testing. Testing the liquid within the target environment avoids, or at least reduces, errors and disturbances that can occur to a sample during transport (e.g., contamination and temperature changes). When the probe of the probe-based system is inserted into the bulk source of liquid, the probe is within the target environment of the liquid and is surrounded by the liquid, with at least a portion of the liquid entering into a sample inlet of the probe for testing.
The present disclosure includes systems and methods for analyzing liquids. Embodiments include a probe-based, parallel-light spectroscopy system that is configured to perform measurements pursuant to one or more measurement standards. For example, and without limitation, embodiments of the system are configured to perform measurements in accordance with one or more American Society for Testing and Materials (ASTM) standards, Saybolt test standards, Cobalt color test routines, and other standards for measuring haze in liquid samples. In some embodiments, the system is or includes a handheld probe (i.e., a probe that can be operated by hand).
Embodiments of the system include a probe that is configured for in-situ measurements of liquid samples in a target environment (e.g., at the point at which the sample is drawn into a sample container without having to bring a sample to a laboratory or other location). The ability for in-situ measurements facilitates the maintenance of sample integrity; avoiding transportation-related issues including time or temperature impacts on the sample. The probe can include an integrated precision thermocouple that records the temperature at which haze and color testing are performed by the probe. Embodiments of the probe reduce or even eliminate moving parts, such as cuvette sample chamber lids and cooling fans, resulting in a robust system that is less susceptible to mechanical and other failures in comparison to systems with moving parts.
Embodiments of the probe-based system eliminate the need for glass or other sample material cuvettes, which require thorough cleaning and drying, both of which are difficult in some environments. The probe-based system can be cleaned, such as by wiping the surface of the probe (e.g., with a lint-free material and Isopropyl Alcohol).
Rather than using a full-sized spectrophotometer and scattering optics, embodiments of the probe include a compact micro-laser-based spectrophotometer that includes a micro-Peltier Cooling chip and heat sink, which provides for temperature control of the spectrophotometer, minimizes noise, and reduces the variability of results.
The liquid samples measured in accordance with embodiments of the present disclosure include, but are not limited to, petroleum-based liquid samples such as petroleum-based fuels or and petroleum-based lubricants. The petroleum-based liquid may be a liquid middle distillate fuel, such as one blended with synthesized hydrocarbons or biofuels. Liquid middle distillate fuels include refinery products in the middle distillation range of refined products, including fuels having from approximately eleven (11) to approximately eighteen (18) carbons present in each molecule thereof. Liquid middle distillate fuels include heating oil, distillate fuel oil, gas oil, lighting oil, and cooking oil. More particular examples of liquid middle distillate fuels include kerosene, jet fuel, diesel fuel, and marine bunker fuel.
Measurement of the optical properties of the liquid samples can be used to determine if the liquid meets one or more optical standards and specifications to confirm quality and lack of water and/or particulates within the liquids. The liquids can be analyzed to determine the presence and amount of contaminate therein. The contaminate can include particulates in the liquid (e.g., particulates in suspension within the liquid), water, or both.
The optical measurements of the liquid samples can be performed to determine haze, clarity, and/or color of the liquid sample, which can, in-turn, be used to determine the presence and amount (or absence) of contaminate in the liquid. The optical measurements of the liquid samples can be performed in accordance with one or more measurement standards. As would be understood by one skilled in the art, “transmission” through a liquid sample refers to the amount of light that passes through the liquid sample without being scattered; “haze” refers to the amount of light that is subject to wide angle scattering (e.g., at an angle greater than 2.5° from normal (ASTM D1003)); and “clarity” refers to the amount of light that is subject to narrow area scattering (e.g., at an angle less than 2.5° from normal). The “haze” can be measured in accordance with: ASTM D8148 (e.g., ASTM D8148-22), Standard Test Method for Spectroscopic Determination of Haze in Fuels. The liquid samples can be analyzed using spectroscopy to determine the level of suspended water and particulate contamination present therein. Such testing results in the determination of an ordinal, whole-number, Instrument Haze Rating (IHR) of from 1 to 6 and a Haze Clarity Index (HCl) of from 50.0 to 100.0 for a test specimen that is at a specified temperature or range, such as 22.0° C.±2.0° C. As used herein, the “HCl” is a numerical value of from 50.0 to 100.0 that indicates fuel clarity derived from spectroscopic measurements and an algorithm that processes the spectroscopic measurements. The HCl values increase with sample clarity and range from 100.0 HCl for a relatively clear and bright sample to 50.0 HCl for a relatively cloudy and opaque sample. For example, a fuel with an HCl value of 90 has less haze than a fuel with an HCl value of 80. HCl can be used to evaluate haze intensity changes within a given IHR. In accordance with ASTM D4175, Haze Clarity Index (HCl) is an empirical definition of the haze of a middle distillate fuel based on a scale of 50 to 100 as determined by ASTM Test Method D8148. In accordance with ASTM D4176, Haze Clarity Index (HCl) is an empirical definition used to estimate the presence of suspended free water and solid particulate contamination in distillate fuels by generating a numerical value from 50.0 to 100.0 as determined by Test Method D8148. As used herein, the IHR is an ordinal, whole number of from 1 to 6 that corresponds to haze ratings defined in ASTM Test Method D4176—Procedure 2, and is assigned to a test specimen based upon spectroscopic measurements and an algorithm that processes the spectroscopic measurements.
The determination of the color of petroleum products may be used for manufacturing control purposes and provides an indication of the quality characteristics of the liquid, as color is readily observed by the user of the product. In some cases, color may serve as an indication of the degree of refinement of the material. In some aspects, “color”, as used herein, is measured in accordance with any of the following standards: ASTM D156-15, Standard Test Method for Saybolt Color of Petroleum Products (Saybolt Chromometer Method); ASTM D1500-12 (2017), Standard Test Method for ASTM Color of Petroleum Products (ASTM Color Scale); ASTM D6045-12 (2017), Standard Test Method for Color of Petroleum Products by the Automatic Tristimulus Method; ASTM D5386-16, Standard Test Method for Color of Liquids using Tristimulus Colorimetry; and ASTM D1209-05 (2011), Standard Test Method for Color of Clear Liquids (Platinum-Cobalt Scale).
With references to
A multi-wavelength light source 106 is positioned and configured to direct multi-wavelength light into the liquid sample 104. In some embodiments, the light source 106 is a high-intensity, small-spot light source.
A collimating optical chain, collimator 108, is positioned between the light source 106 and the liquid sample 104 for narrowing a beam of light 110 emitted from the light source 106 prior to the beam of light 110 passing though the liquid sample 104. In some embodiments, the collimator 108 includes one or more achromatic doublet lenses 128 and a pinhole 130, as shown in
Light 110 passes from collimator 108 to beamsplitter 118. Beamsplitter 118 directs (e.g., reflects) a portion of light 110, first portion of light 122, to a first light sensor 124 for measurement of an intensity of the light 110 emitted from the light source 106.
The beamsplitter 118 directs the remainder of the light 110, second portion of light 126, through window lens 112 and through the liquid sample 104 within the sample chamber 102. After passing through the liquid sample 104, the second portion of light 126 impacts with a return mirror 114 that is positioned within the sample chamber 102. The return mirror 114 reflects return light 116 back towards the beamsplitter 118. The beamsplitter 118 then directs the return light 116 to a second light sensor 120. The second light sensor 120 measures the intensity of the return light 116 that has passed through the liquid sample 104.
The measurements of intensity taken by the first sensor 124 and the second sensor 120 can be compared, as a function of wavelength, to determine the light-absorbing intensity of the liquid sample 104. The light-absorbing intensity of the liquid sample 104 can then be correlated to an amount of contaminant in the liquid sample 104. The results of the measurements by the first sensor 124 and second sensor 120 can be digitally translated to determine specific optical properties. One or both of the sensors 120 and 124 can be or include a multi-wavelength light sensor having integrated channels for XYZ and NIR measurements. The system 100 can be configured with one or more mirrors or other reflective objects (e.g., mirror 114) to direct light to the desired location(s) and/or imaging lenses or other focusing objects (e.g., lens 112).
With reference to
After passing through the collimator 108, the light 110 is directed to the beamsplitter 118. The beamsplitter 118 splits the light 110 into two portions, including light 122 and light 126. Beamsplitter 118 directs light 122 to a folding mirror 140. Folding mirror 140 directs light 122 to an imaging lens 132. Imaging lens 132 directs light 122 to first sensor 124 for measurement thereof.
The beamsplitter 118 directs light 126 through a sample chamber window lens 112 and into the sample chamber 102 for interaction with the liquid sample therein. After passing through the liquid sample within the sample chamber 102, the light 126 impacts the return mirror 114. The return mirror 114 reflects the light, as return light 116, back through the window lens 112 and to the beamsplitter 118 as return light 116. The beamsplitter 118 directs the return light 116 to folding mirror 136. The folding mirror 136 directs the return light to imaging lens 134. The imaging lens 134 directs the return light 116 to second sensor 120 for measurement thereof. In some embodiments, the light 126 and the return light 116 travel along parallel, but directionally opposite, pathways for at least a distances (e.g., between the beamsplitter 118 and the return mirror 114).
With reference to
In some embodiments, the system 100 includes a beamsplitter and mirror unit 119 that combines the functions of the beamsplitter 118 with the folding mirrors 136 and 140 into a single piece to increase stability of the system 100, as shown in
One skilled in the art would appreciate that the system disclosed herein is not limited to the particular arrangement and number of lenses, mirrors, and other components, as shown in
In one exemplary embodiment, the sensors disclosed herein include a 1 mm2 area detection area and is optimized for diffused light. Using a pinhole camera to image the diffused light source at the sensor can eliminate the stray light from other sources, such as ambient, and other surfaces, such as the walls of the liquid container. The pinhole diameter can be designed to optimize the signal-to-noise selection. The distance can be designed to manage the image size at the detector to select the ROI of the light source.
One skilled in the art would appreciate that the sensors disclosed herein are not limited to the particular embodiment as shown in
In some embodiments, the system disclosed herein is in the form of a probe. With reference to
The housing 158 includes a power butter 162 for turning the system 100 on an off, a USB port 164 for charging the system 100 and/or for transmitting data to and from the system 100, control buttons 166 (here shown as four control buttons) for controlling the functions of the system 100, and an OLED display 168 for displaying data, prompts, and other information. In some embodiments, the OLED display 168 and control buttons 166 are on a top surface 161 of the body 158, the probe 160 extends from a bottom surface 163 of the body 158, and the sample inlet 138 is positioned along the probe 160 between the bottom surface 163 of the body 158 and a bottom surface 165 of the probe 160. The sample inlet 138 can be a void space in the probe 160 that is in optical communication with the light source 106 such that light can pass through the void of the sample inlet 138 and any liquid therein.
The handheld probe embodiment of the system 100 is configured to be used with fuel industry-standard bottles, such as bottle 172 shown in
Embodiments of the present disclosure include methods of measuring optical properties of liquids. The method of testing a liquid sample can include inserting the probe of the system into a container that contains a liquid sample. For example, the liquid sample can be drawn into the container at a pipeline using a sample spigot and letting gravity fill a jar or other type of container. The probe of the system is lowered into the container and inserted into the liquid sample within the container for testing. When the probe is inserted into the liquid sample, a portion of the liquid sample passes into the sample chamber of the probe through the sample inlet. The sample inlet can be precisely designed to maximize required path link between the NIR light and scattering light source and the optical detectors that record the amount of light received or detected. With the probe in the liquid sample, the light source provides light to the optical-lens chain, collimator, to collimate the light from the light source. The beamsplitter then splits the collimated light into reflective light and transmitted light. The reflected light passes to a first light sensor that measures the intensity of the reflective light emitted from the light source. The transmitted light is directed through the liquid sample and is reflected from a return mirror back to the beamsplitter which directs the transmitted light through an imaging lens to a second sensor. The second sensor the measures the intensity of the transmitted light. In some embodiments, instead of being reflected by a return mirror, the transmitted light is directed to a second sensor that is located at an end of the sample inlet. The second sensor detects the intensity, as a function of wavelength, of the light transmitted through the controlled length of the liquid sample. By comparing the intensity of the reflected light and the intensity of the transmitted light, the light-absorbing intensity of the liquid sample is determined. These results can be digitally translated to measure specific optical properties. The data from the sensors can be transmitted to a CPU located in the probe (or external). The CPU computes values received by the sensors into measurements that are used in the industry, such as Haze Clarity Index (HCl), Instrument Haze Rating (IHR) and Saybolt, ASTM and Platinum Cobalt APHA color scales. For example, computer instructions stored in a data storage of the system can instruct the CPU to process the sensor data in accordance with one or more such standards.
In operation, the one or more mirrors can be used to direct the light (either or both the reflective light and the transmitted light) throughout the system to, for example, the sensors. Additionally, one or more imaging lenses can be used to intensify either or both the reflective light and the transmitted light before detection by the sensors. In some embodiments, both the reflective light and the transmitted light are directed from the beamsplitter to a folding mirror, and then through imaging lenses before reaching the sensors.
In some embodiments, the system is designed with one or more mirrors optically aligned and attached to the beamsplitter. Combining the beamsplitter and one or more mirrors into a single, assembled piece increases the stability of the system by reducing the alignment dependency between the beamsplitter and the one or more mirrors when comprised of separate pieces. As a single, combined piece, deviations in the rotation or movement of the beamsplitter and mirror piece will have less effect on the operation of the system.
The system is capable of simultaneously measuring haze and color in a sample, such as by using a broad-spectrum, dual laser-excited light source that emits multiple wavelengths, including both white light and NIR, as well as using a single detector with multiple integrated channels for the measurement of color (X, Y, Z) and NIR for haze. The ability to measure the intensity of the light source with every sample test is more efficient than current techniques in the field. The system is not dependent on test-by-test calibration to set standards, which eliminates the need for empty chamber testing in bench-top analyzers; thereby, greatly reducing testing time. The probe can be inserted directly into a sample, which reduces or eliminates inaccuracies caused by light-absorption and/or refractive properties of sample cups. The measurement of the optical properties of a sample determined by comparative testing of the source light and transmitted light for each test reduces or eliminates differences in the intensity of light source. In some embodiments, a thin-film glass plate is used for absolute calibration for both color and haze. Establishing a digital relationship between the source light and transmitted light to measure optical properties of sample liquids is efficient and reliable.
Collimating the light source improves the signal-to-noise ratio and allows for a smaller light source, which is preferable for a hand-held instrument probe. The system is configured to be independent of the refractive index of the testing sample and the sample holder and reduced or eliminates effects of ambient and divergent light. In a preferred embodiment, the collimator includes a broadband achromatic doublet lenes to account for multiple wavelengths.
The multi-wavelength system disclosed herein enables the effective measurement of small-particle-size contaminants in liquid samples, such as water and wax in petroleum fuels, which have different absorption or scattering effects at different wavelengths.
Some exemplary components and aspects of embodiments of the system are set forth in Table 1, below.
The system disclosed herein can be configured to conduct a single test, multiple tests, timed tests, and/or haze at-temperature tests. The color tests can be in accordance with one or more of: ASTM D6045, Saybolt, and ASTM E313 (D5386). The haze test can be in accordance with one or more of: ASTM D8148; HCl correlation to IHR 1-6. The system can include software configured to process the data collected by the sensors and/or to direct the actions of the system. The software can be resident on the probe and/or external of the probe. Results of the tests performed by the system can be depicted graphically and/or as a numerical output. The data from the system can be transferred to other devices, such as a tablet, through Bluetooth and/or the USB port.
In one example, a haze test can be performed with light that is an 850 nm wavelength (near IR) LED.
In existing systems, light transmits through a parallel glass (or plastic) and the sample at a current cuvette design. If the light is collimated (light transmitted in parallel), the refractive index of glass and sample will not play a role in the image at the detector end. If the light is not collimated, there is a lens effect to focus or diverse the light. The unevenness at the glass or liquid distance will create wavefront distortion to create an uneven image (varying light intensity) at the detector to cause measurement error. This error can occur on existing instruments for both haze and color testing. In contrast, in the present probe-based system, the light path is inside the liquid, eliminating the effect of two glass (or plastic) windows.
CMOS imaging sensors and light sensors were tested as an option for the detector. Light sensors with built-in wavelength filters (colors and near IR on one chip), AD at high resolution (16-bit), and standard serial communication (like I2C) were tested. One light sensor tested had both XYZ and near IR detection capabilities. A sensor with a specific wavelength can also be used for specific enhancement of color detection. At 16-bit on-chip AD, the sensor resolution can be at 1.5 ppm (0.0015%) of the full intensity. The chip can include an LED controller. An exemplary sensor spectrum response curve is shown in
The system can be design such that both the light source and sensor have a stable electrical current to be able to achieve consistent measurements. The LED light can be controlled with PWM (Pulse Width Modulation-rapid switching on/off of the current) or constant current. At the PWM mode, flickering of the light source can occur if the modulation frequency is low. With a higher speed sensor, the frequency requirement will be higher. At the current mode, the light intensity is proportional to the current level and no flickering of the light was observed. The light sensor can have a built-in LED current controller.
Light propagation (image forming at the detector) is consider in the design. Existing instruments have a single element collimating lens in front of the light. A simple test showed that this existing collimating designs was not preferred. A strong lens effect at the haze and color testing was observed. In some embodiments, a collimated light (all in parallel) is used. A diffraction-limited collimating beam with two achromatic lenses and one microscope objective was formed to test this concept. The light beam travelled far without lens effect. The complexity of this design can be cost prohibitive. In another embodiment, a light guide approach can be used. LED light is affordable and can be used to produce substantial amounts of light. The light guide also allows all electrical components to remain above the sample liquid. The design of a light guide can be cost prohibitive. In other embodiments, a pinhole camera and LED illumination film (which provide diffuse, uniform light generation) can be used. The LED illumination film is a preferred embodiment of the light source, is cost-effective, and provides uniformly diffused illumination.
The system disclosed herein is described as a probe-based, parallel-light spectroscopy system to perform the measurements pursuant to, e.g. ASTM, Saybolt, & Cobalt color test routines, as well as haze in liquid samples. However, it would be apparent to one skilled in the relevant chemical, engineering, environmental science, or other technical art, that the system may be applicable to other environments, settings and applications.
The concepts disclosed in the present application can be combined with one or more of the concepts of U.S. Pat. No. 11,619,549 ('549 patent). The system disclosed herein can be used to perform the measurements that are performed by the system disclosed in the '549 patent.
The foregoing description has been presented for purposes of illustration and description of preferred embodiments. This description is not intended to limit associated concepts to the various systems, apparatus, structures, and methods specifically described herein. For example, system and methods described in the context of a probe or manual device or localized environments, may be applicable, in part or in entirety, to other measurement environments or tasks, such as field environments, long-haul trucks or similar powered mobile vehicles. The embodiments described and illustrated herein are further intended to explain the best and preferred modes for practicing the system and methods, and to enable others skilled in the art to utilize same and other embodiments and with various modifications required by the particular applications or uses.
The following exemplary “claims” are provided to set out and describe various aspects of the disclosure. The listing of claims is not intended to be limiting. It should be noted that elements described by the claims may take alternative forms, as may be described above, and various combinations may be implemented (including combinations not described by the dependencies in the claims). For example, the present disclosure extends to methods of operation of any of the systems or apparatus listed, including operation of any subsystem or combination of elements. The disclosure also extends to any system or apparatus described above suitable to perform any methods, process, or operation (and steps) listed below. Such combinations and alternative forms are well within the spirit and scope of the present disclosure.
Although the present embodiments and advantages have been described in detail, it should be understood that various changes, substitutions and alterations can be made herein without departing from the spirit and scope of the disclosure. Moreover, the scope of the present application is not intended to be limited to the particular embodiments of the process, machine, manufacture, composition of matter, means, methods and steps described in the specification. As one of ordinary skill in the art will readily appreciate from the disclosure, processes, machines, manufacture, compositions of matter, means, methods, or steps, presently existing or later to be developed that perform substantially the same function or achieve substantially the same result as the corresponding embodiments described herein may be utilized according to the present disclosure. Accordingly, the appended claims are intended to include within their scope such processes, machines, manufacture, compositions of matter, means, methods, or steps.
The present application claims the benefit of U.S. Provisional Patent Application No. 63/510,017 (pending), having a filing date of Jun. 23, 2023, the entirety of which is incorporated herein by reference. The present application is also a Continuation-in-part of U.S. patent application Ser. No. 18/176,092 (pending), having a filing date of Feb. 28, 2023, the entirety of which is incorporated herein by reference; which is a Continuation of U.S. Pat. No. 11,619,549 (issued), having a filing date of Mar. 1, 2021, the entirety of which is incorporated herein by reference; which is a Continuation of U.S. Pat. No. 10,976,201 (issued), filed on Apr. 26, 2019, the entirety of which is incorporated herein by reference; which claims the benefit of U.S. Provisional Patent Application No. 62/689,726 (expired), filed on Jun. 25, 2018, the entirety of which is incorporated herein by reference, and also claims the benefit of U.S. Provisional Patent Application No. 62/745,187 (expired), filed on Oct. 12, 2018, the entirety of which is incorporated herein by reference.
Number | Date | Country | |
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63510017 | Jun 2023 | US | |
62745187 | Oct 2018 | US | |
62689726 | Jun 2018 | US |
Number | Date | Country | |
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Parent | 17188062 | Mar 2021 | US |
Child | 18176092 | US | |
Parent | 16396287 | Apr 2019 | US |
Child | 17188062 | US |
Number | Date | Country | |
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Parent | 18176092 | Feb 2023 | US |
Child | 18752576 | US |