METHOD FOR THE CONTINUOUS NON-INVASIVE DETERMINATION OF THE CONCENTRATION OF BLOOD CONSTITUENTS

• US 20100331636A1
• Filed: 03/20/2008
• Published: 12/30/2010
• Est. Priority Date: 03/23/2007
• Status: Abandoned Application

• Current Assignee: enverdis GmbH
• Original Assignee: enverdis GmbH
• Inventors: Alt, Michael, Hübner, Thomas
• Application Number:
  US12/532,726
• Publication Number:
  US 20100331636A1
• Time in Patent Office: Days
• US Class Current: 600/310
• CPC Class Codes: A61B 5/0059 using light, e.g. diagnosis by transillumination, diascopy, fluorescence A61B5/0093, A61B5/1455, A61B5/02416 and A61B5/0261 take precedence
• CPC Class Codes: A61B 5/14546 for measuring analytes not otherwise provided for, e.g. ions, cytochromes
• CPC Class Codes: A61B 5/1455 using optical sensors, e.g. spectral photometrical oximeters

Abstract

The invention relates to a method for the non-invasive determination of the concentration of blood constituents, in which a radiation source (12) emits several radiation beams (14), each with a different wavelength. A first photo detector (18) receives the measurement radiation (14) of each wavelength that is reflected by a body part (16) to be examined. A second photo detector (22) receives the measurement radiation (24) of each wavelength that is transmitted by the body part (16) to be examined. The measurement radiation (14) of each wavelength that is absorbed by the body part (16) to be examined is then determined on the basis of the measurement of the reflected radiation (20) by the first radiation receiver (18) and the measurement of the transmitted radiation (24) by the second radiation receiver (22). The concentration of the different constituents is calculated from the absorption of the measurement radiation (14) that has been determined for each wavelength.

Claims

1. A method for the non-invasive determination of the concentration of blood constituents, comprising:

radiating a plurality of measurement radiations with respectively different wavelengths by means of a radiation source;

receiving the measurement radiation of a plurality of said wavelengths, as reflected by the body part to be examined, by means of a first light receiver;

receiving the measurement radiation of a plurality of said wavelengths, as transmitted through the body part to be examined, by means of a second light receiver; and

determining the absorption of the measurement radiation of each wavelength, as caused by the body part to be examined, on the basis of the measurement of said reflected radiation by means of the first radiation receiver and the measurement of said transmitted radiation by means of the second radiation receiver

wherein that an absorption Ag_R is determined by the first radiation receiver on the basis of the measurement of the reflected radiation of a first portion r to r_i of the wavelengths, and an absorption Ag_T is determined by the second radiation receiver on the basis of the measurement of the transmitted radiation of a second portion 1 to r of the wavelengths, wherein, for at least one wavelength r, the reflected as well as the transmitted radiation fraction is measured, comprising the further step of;

determining the n concentrations C_b1 to C_bn of blood constituents on the basis of said determined absorptions Ag_R and respectively Ag_T of the measurement radiation at each wavelength 1 to n, the computation of the concentrations being performed according to the following equation system;

A_T(λ

₁)=E(λ

₁,b₁)*C_b1+ . . . +E(λ

₁,b_n)*C_bn

Ag_T(λ

_T)=E(λ

_r,b₁)*C_b1+ . . . +E(λ

_r,b_n)*C_bn

Ag_R(λ

_r)=(K_T/K_R)*{E(λ

_r,b₁)*C_b1+ . . . E(λ

_r,b_n)*C_bn}

Ag_R(λ

_n)=(K_T/K_R)*{E(λ

_n,b₁)*C_b1+ . . . +E(λ

_n,b_n)*C_bn}

2. The method according to claim 1, wherein said method steps are repeated a plurality of times and the respective absorption values for each wavelength of the measurement radiation are stored for each repetition cycle.

3. The method according to claim 2, wherein the stored absorption values for each wavelength are combined into a representation of the temporal development of the absorption for each wavelength of the measurement radiation.

8. The method according to claim 1, wherein the preceding step:

determining a normalization factor for the light intensity of the radiation source.

9. The method according to claim 1, wherein, at least once per measurement, the constant component of the obtained development of the absorption is determined for each wavelength.

10. The method according to claim 9, wherein the determined alternating component of the development of the absorption for each wavelength is normalized in dependence on the determined constant component for each wavelength.

11. The method according to claim 1, wherein analog and/or digital filters are used for separating the DC and alternating components of the detected developments of the absorption at each wavelength.

12. The method according to claim 1, wherein the detected constant component of the developments of the absorption is included as a correction portion.

13. The method according to claim 1, wherein the said radiating of a plurality of measurement radiations with respectively different wavelengths by means of a radiation source is performed sequentially.

4-7. -7. (canceled)

14-16. -16. (canceled)