IP Library Granted Patent US 9,752,983
Granted Patent B2
US 9,752,983 · App. 14/271,859 · Granted Sep 5, 2017

Optical density monitor and comparator systems and methods

Inventors: Jennifer Godwin Pagan (Charlotte, NC); Edward Brittain Stokes (Charlotte, NC); Paolo Batoni (Charlotte, NC)
Assignees: AquiSense Technologies LLC; The University of North Carolina at Charlotte
G01N21/5907A61L9/205G01N21/031G01N21/33A61L2209/11C02F1/32C02F2209/11C02F2303/04G01N2201/065
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Quick Facts
Patent No.
US 9,752,983
App. No.
14/271,859
Granted
Sep 5, 2017
Kind
B2
Abstract

The present disclosure relates generally to systems and methods for determining the absorption coefficient and the optical density of a fluid as they relate to the wavelength of incident radiation. Specifically, ultraviolet light-emitting diodes (UV LEDs) or the like that emit ultraviolet (UV) radiation or the like are used as sources for irradiating the interior of an integrating chamber that is designed to increase the path length of the radiation through the fluid, thus enhancing the detection limits of the absorption coefficient and the optical density according to Beer's Law.

Claims (26)

1. A system for determining the absorption coefficient and/or the optical density of a fluid and/or organic/inorganic particles disposed in the fluid, comprising:

an integrating flow cell configured to contain a fluid sample within substantially an entire interior portion thereof;

one or more point radiation sources disposed about an interior periphery of the integrating flow cell, wherein the one or more point radiation sources are operable for delivering radiation of a predetermined wavelength to the fluid sample; and

one or more radiation detectors operable for detecting radiation within the interior portion of the integrating flow cell;

wherein the integrating flow cell comprises an integrating sphere having an interior surface operable for reflecting the radiation delivered to the fluid sample by the one or more point radiation sources such that a radiation intensity is uniform throughout the interior portion of the flow cell; and

wherein a path length of the radiation delivered to the fluid sample and reflected is maximized by the fluid sample occupying substantially the entire interior portion of the integrating flow cell.

2. The system of claim 1 , wherein the absorption coefficient and/or the optical density of the fluid and/or organic/inorganic particles disposed in the fluid is determined utilizing the predetermined wavelength of the delivered radiation and a characteristic of the detected radiation.

3. The system of claim 1 , wherein the determined absorption coefficient and/or optical density of the fluid and/or organic/inorganic particles disposed in the fluid is measured at one or more predetermined wavelengths of delivered radiation and a ratio of measured values is used to identify the fluid and/or organic/inorganic particles disposed in the fluid.

4. The system of claim 1 , wherein the one or more point radiation sources comprise a first point radiation source operable for delivering radiation of a first predetermined wavelength to the fluid sample.

5. The system of claim 4 , wherein the one or more point radiation sources further comprise a second point radiation source operable for delivering radiation of a second predetermined wavelength to the fluid sample.

6. The system of claim 1 , wherein the one or more point radiation sources comprise one or more ultraviolet (UV) point radiation sources and/or one or more visible point radiation sources.

7. The system of claim 1 , wherein the one or more point radiation sources comprise a point radiation source operable for delivering radiation having a predetermined wavelength of between about 260 nm and about 280 nm to the fluid sample.

8. The system of claim 1 , wherein the one or more point radiation sources comprise one or more semiconductor optical sources, light-emitting diode (LED) optical sources, and ultraviolet (UV) optical sources.

9. A method for determining the absorption coefficient and/or the optical density of a fluid and/or organic/inorganic particles disposed in the fluid, comprising:

providing an integrating flow cell configured to contain a fluid sample within substantially an entire interior portion thereof;

providing one or more point radiation sources disposed about an interior periphery of the integrating flow cell, wherein the one or more point radiation sources are operable for delivering radiation of a predetermined wavelength to the fluid sample; and

providing one or more radiation detectors operable for detecting radiation within the interior portion of the integrating flow cell;

wherein the integrating flow cell comprises an integrating sphere having an interior surface operable for reflecting the radiation delivered to the fluid sample by the one or more point radiation sources such that a radiation intensity is uniform throughout the interior portion of the flow cell; and

wherein a path length of the radiation delivered to the fluid sample and reflected is maximized by the fluid sample occupying substantially the entire interior portion of the integrating flow cell.

10. The method of claim 9 , wherein the absorption coefficient and/or the optical density of the fluid and/or organic/inorganic particles disposed in the fluid is determined utilizing the predetermined wavelength of the delivered radiation and a characteristic of the detected radiation.

11. The method of claim 9 , wherein the determined absorption coefficient and/or optical density of the fluid and/or organic/inorganic particles disposed in the fluid is measured at one or more predetermined wavelengths of delivered radiation and a ratio of measured values is used to identify the fluid and/or organic/inorganic particles disposed in the fluid.

12. The method of claim 9 , wherein the one or more point radiation sources comprise a first point radiation source operable for delivering radiation of a first predetermined wavelength to the fluid sample.

13. The method of claim 12 , wherein the one or more point radiation sources further comprise a second point radiation source operable for delivering radiation of a second predetermined wavelength to the fluid sample.

14. The method of claim 9 , wherein the one or more point radiation sources comprise one or more ultraviolet (UV) point radiation sources and/or one or more visible point radiation sources.

15. The method of claim 9 , wherein the one or more point radiation sources comprise a point radiation source operable for delivering radiation having a predetermined wavelength of between about 260 nm and about 280 nm to the fluid sample.

16. The method of claim 9 , wherein the one or more point radiation sources comprise one or more semiconductor optical sources, light-emitting diode (LED) optical sources, and ultraviolet (UV) optical source.

Assignments (5)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded May 20, 2025
From: AQUISENSE TECHNOLOGIES LLC
To: AQUISENSE INC.
Reel/Frame 071172/0287 →
CONFIRMATORY LICENSE Recorded Aug 1, 2018
From: UNIVERSITY OF NORTH CAROLINA, CHARLOTTE
To: NATIONAL SCIENCE FOUNDATION
Reel/Frame 046530/0012 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Oct 14, 2015
From: DOT METRICS TECHNOLOGIES, INC.
To: AQUISENSE TECHNOLOGIES LLC
Reel/Frame 036820/0539 →
ASSIGNMENT OF PARTIAL INTEREST Recorded Sep 3, 2014
From: THE UNIVERSITY OF NORTH CAROLINA AT CHARLOTTE
To: DOT METRICS TECHNOLOGIES, INC.
Reel/Frame 033684/0273 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded May 7, 2014
From: PAGAN, JENNIFER GODWIN; STOKES, EDWARD BRITTAIN; BATONI, PAOLO
To: UNIVERSITY OF NORTH CAROLINA AT CHARLOTTE
Reel/Frame 032841/0259 →
Continuity (3)
Continuation In Part 13163055 · Jun 17, 2011
Provisional Application 61820204 · May 7, 2013
Related Publication 20140240695A1 · Aug 28, 2014