IP Library Granted Patent US 9,182,363
Granted Patent B2
US 9,182,363 · App. 14/079,968 · Granted Nov 10, 2015

Instrument and method of measuring the concentration of a target element in a multi-layer thin coating

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Quick Facts
Patent No.
US 9,182,363
App. No.
14/079,968
Granted
Nov 10, 2015
Kind
B2
Abstract

An instrument and a method of detecting a target element in a multi-layer thin coating. Lα, Lβ and Lγ x-rays are caused to be emitted from the target element (preferably lead paint) with excitation radiation. Upon detecting the emitted x-rays, an areal concentration of the target element is calculated using Lα and Lβ intensities once, and then using the Lβ and Lγ intensities once, by reference to a single layer model; By combining the two concentrations calculated using single layer model, a more accurate concentration can be calculated for the target element in the multi-layered surface coating.

Claims (38)

1. A method of measuring an areal concentration of a target element coated by more than one layers near the surface of a substrate, the target element capable of emitting La, LI3 and L7 x-rays when suitably excited, the method comprising the steps of:

a) inducing the L α and L β and L γ x-rays to be emitted from said target element with excitation radiation;

b) detecting said L α , L β and L γ x-rays and determining the intensity of the L α , L β and L γ x-rays separately;

c) calculating the areal concentration of said target element by means of the following equations:

m 1 =I Lβ /A 1/ I LβS   Eq. 1

wherein m 1 is the calculated lead concentration based on single layer model using L α and L β intensities; A1 is the absorption factor computed from the L α , L β intensity ratio, wherein during calibration, A1 as a function of L α , L β intensity ratio is fitted as a curve; and this curve is used later to calculate the A1 from measured L α ,L β intensity ratio; I Lβ is the measured L β line intensity of the target element from sample under testing; I LβS is the L β intensity of the target element from a NIST standard without any shielding layers;

m 2 =I Lγ /A 2/ I LγS   Eq. 2

wherein m 2 is the calculated lead concentration based on single layer model using L β and L γ intensities; A2 is the absorption factor computed from the L β , L γ intensity ratio, wherein during calibration, A2 as a function of L β , L γ intensity ratio is fitted as a curve; and this curve is used later to calculate the A1 from measured L α , L β intensity ratio; I Lγ is the measured L γ line intensity of the target element from sample under testing; I LγS is the L γ intensity of the target element from a NIST standard without any shielding layers; and

d) calculating the combine areal concentration of said target element according to:

m z =m 2 +C 3 ( m 2 −m 1 )  Eq. 5

wherein C 3 is a constant determined during an instrument calibration, and m z is the target element concentration emitted from the at least one layer of coating containing the target element.

2. The method of measuring an areal concentration of a target element of claim 1 , wherein the target element is comprised of one or more layers of another material that do not contain the target element.

3. The method of measuring an areal concentration of a target element of claim 1 , wherein the target element is lead paint.

4. The method of measuring an areal concentration of a target element of claim 1 , wherein the Lα, Lβ and Lγ for the target element have x-ray fluorescent lines with an energy of 10.5 keV, 12.6 keV and 14.8 keV, respectively.

5. The method of measuring an areal concentration of a target element of claim 1 , further including using a filter to reduce low energy x-rays associated with the excitation radiation.

6. The method of measuring an areal concentration of a target element of claim 5 , including using a filter wheel to select an optimal filter to reduce the low energy x-rays.

7. The method of measuring an areal concentration of a target element of claim 1 , including using an x-ray tube to generate the excitation radiation.

8. The method of measuring an areal concentration of a target element of claim 1 , including comparing m 1 to m 2 and, if m 1 is substantially equal to m 2 , reporting the areal concentration based on m 1 .

9. The method of measuring an areal concentration of a target element of claim 1 , including carrying out measurements of the areal concentration of the target element in a range from 0 to 2 mg/cm 2 and beyond.

10. An instrument configured as an x-ray fluorescence analyzer for measuring an areal concentration of a target element coated by more than one layers near a surface of a substrate, the target element capable of emitting Lα, Lβ and Lγ x-rays when suitably excited, the instrument comprising:

a) a source of excitation radiation capable of inducing the Lα and Lβ and Lγ x-rays to be emitted from said target element;

b) a detector configured to detect said Lα, Lβ and Lγ x-rays and determine the intensity of the Lα, Lβ and Lγ x-rays separately;

c) a calculating unit configured to calculate the areal concentration of said target element by means of the following equations:

m 1 =I Lβ /A 1/ I LβS   Eq. 1

wherein m 1 is the calculated lead concentration based on single layer model using Lα and Lβ intensities; A1 is the absorption factor computed from the Lα, Lβ intensity ratio, I Lβ is the measured Lβ line intensity of the target element; and I LβS is the lead Lβ intensity based on a NIST (National Institute of Standards and Technology) standard with 1.0 mg/cm 2 lead concentration, recorded during instrument calibration,

m 2 =I Lγ /A 2/ I LγS   Eq. 2

wherein m 2 is the calculated lead concentration based on single layer model using Lβ and Lγ; A2 is the absorption factor computed from the Lβ, Lγ intensity ratio, I Lγ is the measured Lγ line intensity from sample under testing; and I LγS is the lead Lγ intensity from NIST standard with 1.0 mg/cm 2 lead concentration; and

d) further calculating the combined areal concentration of said target element according to:

m z =m 2 +C 3 ( m 2 −m 1 )  Eq. 5

where C 3 is a constant determined during an instrument calibration, m z is the target element concentration emitted from the at least one layer of coating containing the target element.

11. The instrument of claim 10 , wherein the target element is comprised of one or more layers of another material that do not contain the target element.

12. The instrument of claim 10 , wherein the target element is lead paint.

13. The instrument of claim 10 , wherein the Lα, Lβ and Lγ for the target element have x-ray fluorescent lines with an energy of 12.6 keV and 14.8 keV, respectively.

14. The instrument of claim 10 , further including using a filter to reduce low energy x-rays associated with the excitation radiation.

15. The instrument of claim 10 , further including a filter wheel to select an optimal filter to reduce the low energy x-rays.

16. The instrument of claim 10 , including an x-ray tube to generate the excitation radiation.

17. The instrument of claim 10 , wherein the calculating unit is configured to compare m 1 to m 2 and, if m 1 is substantially equal to m 2 , reporting the areal concentration based on m 1 .

18. The instrument of claim 10 , wherein said instrument is configured to carry out measurements of the areal concentration of the target element in a range from 0 to 2 mg/cm 2 and beyond.

Assignments (4)
CONFIRMATORY ASSIGNMENT Recorded Dec 28, 2023
From: OLYMPUS AMERICA INC.
To: EVIDENT SCIENTIFIC, INC.
Reel/Frame 066143/0724 →
MERGER Recorded Mar 16, 2023
From: OLYMPUS SCIENTIFIC SOLUTIONS AMERICAS INC.
To: OLYMPUS AMERICA INC.
Reel/Frame 063112/0940 →
CHANGE OF NAME Recorded Feb 17, 2023
From: OLYMPUS NDT INC.
To: OLYMPUS SCIENTIFIC SOLUTIONS AMERICAS INC.
Reel/Frame 062732/0498 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Nov 14, 2013
From: CHEN, XUNMING
To: OLYMPUS NDT, INC.
Reel/Frame 031602/0616 →