IP Library › Granted Patent US 8,996,338
Granted Patent B2
US 8,996,338 · App. 12/996,089 · Granted Mar 31, 2015

Method of component concentration detection based on reference wavelength

Inventors: Kexin Xu (Tianjin, CN); Wenliang Chen (Tianjin, CN)
Assignee: Tianjin Sunrise Technologies Development Co., Ltd.
G01N21/359A61B5/14532
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Quick Facts
Patent No.
US 8,996,338
App. No.
12/996,089
Granted
Mar 31, 2015
Kind
B2
Abstract

A method of detecting a concentration of a target component by using a reference wavelength includes: defining a wavelength at which a light intensity is insensitive to the variation of the target component concentration as a reference wavelength for the target component; detecting spectra at both the reference wavelength and a further measuring wavelength; processing the spectrum detected at the further measuring wavelength, with the spectrum detected at the reference wavelength as an inner reference, to obtain a characteristic spectrum including specific information of the target component; building a calibration model between the characteristic spectrum and the concentration of the target component; and determining the concentration of the target component based on the calibration model.

Claims (198)

1. A method of detecting a concentration of a target component in a sample, including steps of:

1) defining a wavelength at which a light intensity is insensitive to variation of the target component concentration as a reference wavelength for the target component;

2) detecting spectra at the reference wavelength and a further measuring wavelength;

3) processing the spectrum detected at the further measuring wavelength, with the spectrum detected at the reference wavelength as an inner reference, to obtain a characteristic spectrum including specific information of the target component;

4) building a calibration model between the characteristic spectrum and the concentration of the target component; and

5) determining the concentration of the target component based on the calibration model,

wherein the reference wavelength λ r is defined as follows:

for a pure absorption sample, α g (λ r )+α w (λ r )·k=0; and

for a scattering sample,

6.44

*

10

-

5

*

r

2.37

*

ρ

s

*

n

s

*

(

n

s

-

n

w

)

1.09

λ

r

0.37

*

n

w

3.09

*

1

1

-

g

⁡

(

λ

r

)

=

α

g

⁡

(

λ

r

)

+

α

w

⁡

(

λ

r

)

·

k

,

wherein α w and α g are absorption coefficients of the water molecule and the target component molecule respectively, k is a replacement coefficient between the water and the target component, g is an anisotropic factor of the scattering sample, n s is a refractive index of scattering particles of the scattering sample, n w is the refractive index of the water, r is a radius of the scattering particles, ρ s is the number of scattering particles per unit volume of the sample (nm −3 ).

2. The method according to claim 1 , wherein the reference wavelength for the glucose in the aqueous glucose solution is 1525 nm.

3. The method according to claim 1 , wherein a wavelength at which light intensity is most sensitive to the variation of the target component concentration is selected as the measuring wavelength.

4. The method according to claim 1 , wherein in step 3), the specific information of the target component is obtained as follows:

for a pure absorption sample, the specific information including the variation of the target component concentration is:

A

G

⁡

(

λ

)

=

-

Ln

⁡

(

I

s

⁡

(

λ

)

I

b

⁡

(

λ

)

·

I

b

⁡

(

λ

r

)

I

s

⁡

(

λ

r

)

)

;

for a scattering sample, the specific information including the variation of the target component concentration is:

A

G

⁡

(

λ

)

=

Ln

⁢

I

b

⁡

(

λ

)

·

I

s

⁡

(

λ

r

)

I

s

⁡

(

λ

)

·

I

b

⁡

(

λ

r

)

+

K

Δ

⁢

⁢

c

·

Ln

⁡

(

I

b

⁡

(

λ

)

I

b

⁡

(

λ

r

)

·

I

0

⁡

(

t

b

,

λ

r

)

I

0

⁡

(

t

b

,

λ

)

)

,

where I s (λ r ) and I b (λ r ) are intensities of the transmitted light from the sample and a background sample at the reference wavelength respectively, I s (λ) and I b (λ) are intensities of the transmitted light from the sample and the background sample at the measuring wavelength respectively, I 0 (t b , λ r ) and I 0 (t b , λ) are intensities of the light incident to the background sample at the reference wavelength and the measuring wavelength respectively, and K Δc is a percentage coefficient of the light path length variation caused by the concentration change of the target component of Δc.

5. The method according to claim 1 , wherein the calibration model is built by the Partial Least Squares (PLS) method or the net analyte signal method.

Assignments (2)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Apr 21, 2011
From: TIANJIN SUNSHINE OPTICS TECHNOLOGIES CO., LTD.
To: TIANJIN SUNRISE TECHNOLOGIES DEVELOPMENT CO., LTD.
Reel/Frame 026165/0276 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Feb 11, 2011
From: XU, KEXIN; CHEN, WENLIANG
To: TIANJIN SUNSHINE OPTICS TECHNOLOGIES CO., LTD.
Reel/Frame 025793/0552 →
Priority Claims (1)
CN 2008 1 0053456 · Jun 6, 2008 · national
Continuity (1)
Related Publication 20110131021A1 · Jun 2, 2011