Abstract:
Biochemical components and changes in the components are measured by directing light of several wavelengths into a body at one location, sensing light at the wavelengths emerging from the body at a plurality of distances from the one location, and ascertaining biochemical component characteristics in the body as a function of variations, with respect to distance, of the logarithm of the ratio of the light sensed to the light directed into the body. The variations with respect to distance are in the form of the derivative and square of the derivatives of the logarithm.

Description:
FIELD OF THE INVENTION 
     This invention relates to methods and means for measurement of chemical components, and particularly to non-invasive measurement of biochemical components of a human or animal body. 
     BACKGROUND OF THE INVENTION 
     U.S. Pat. Nos. 4,281,645, 4,223,680, and 5,119,815 describe non-invasive measurement of biochemical components, such as hemoglobin (H), oxyhemoglobin (HbO 2 ), and cytochrome (CyOx) in a human or animal body. These systems introduce a beam of electromagnetic radiation in the form of infra-red light into the body at one point, sense the radiation emerging at another point, process the sensed data in a processor, and display or graph the results. U.S. Pat. No. 4,281,645 involves transillumination across the body from one point to an opposing point on the other side of the body. U.S. Pat. No. 4,223,680 discloses measuring along spaced parts of the body and using two detectors, one located near the light source to correct for light scattered from the skin. U.S. Pat. No. 5,119,815 entails using a pulsed light source. 
     These methods attempt to determine characteristics of such components on the basis of certain assumptions of the correlation between light intensities and the average light paths. However, it is believed that these assumptions lead to inaccuracies that arise from changes in the average light paths with changes in the concentration of the components. 
     An object of the invention is to improve prior art systems. 
     Another object is to overcome the aforementioned problems. 
     Still another object is to provide improved measurement optrode. 
     Yet another object is to provide a measurement system which permits accurate measurement of concentration of biochemical compounds. 
     SUMMARY OF THE INVENTION 
     According to a feature of the invention such results are achieved by directing electromagnetic radiation of several wavelengths into a body at one location, sensing electromagnetic radiation of the several wavelengths emerging from the body at a number of distances from the one location; and ascertaining biochemical component characteristics in the body as a function of variations, with respect to distance, of the negative logarithm of the ratio of the electromagnetic radiation at the wavelengths. 
     According to another feature of the invention, the variations with respect to distance are in the form of the derivative of the logarithm. 
     According to another feature of the invention, ascertaining includes determining concentrations of biochemical components as a function of the square of said variations. 
     According to another feature of the invention, includes determining concentrations of biochemical components as a function of the square of said variations, a scattering coefficient, and an extinction coefficient. 
     According to another feature of the invention, ascertaining includes determining concentrations of biochemical components as a function of the square of said derivative, and an absorption coefficient, composed of a scattering coefficient times an extinction coefficient. 
     According to yet another feature of the invention, each of the steps or functions above are performed by means for performing them. 
    
    
     BRIEF DESCRIPTION OF THE DRAWINGS 
     FIG. 1 is a partial elevation and block diagram of a device embodying features of the invention. 
     FIG. 2 is a plan of a device in FIG. 1 for emitting and sensing light. 
     FIG. 3 is an elevation of FIG. 2. 
     FIG. 4 is a diagram of the device of FIG. 1 and 2 as used on the head of a patient. 
     FIG. 5 is a graph illustrating the emission of light from the device of FIGS. 1 to 4. 
     FIG. 6 is a graph showing the A/D conversion of the graph in FIG. 5. 
     FIG. 7 is a graph of data accumulated from the information in FIG. 6. 
     FIG. 8 is a graph illustrating the variations in optical density at different distances from a light source in the device of FIGS. 1 to 4. 
     FIG. 9 is a diagram illustrating the passage of light from one face to an opposite face, without optical scattering, and the optical density resulting therefrom. 
     FIG. 10 is a section of the average path length of light path between two points along a face when light is subject to optical scattering. 
     FIG. 11 is a graph of the variation of optical density at different distances from the light source along a face. 
     FIG. 12 is a diagram of the absorption coefficient and actual scattering coefficient using the device in FIGS. 1 to 4. 
     FIGS. 13, 14, and 15 are flow charts illustrating operation of the system in FIG. 4. 
    
    
     DETAILED DESCRIPTION OF PREFERRED EMBODIMENTS 
     FIG. 1 illustrates a system embodying the invention. Here, an optrode OP1 connects to a processing and display section SN1 via a cable CA1 and an optical fiber OF1. Details of the optrode OP1 appear in the plan view thereof of FIG. 2, the elevational section of FIG. 3, and the perspective view as placed on a human head in FIG. 4. In the optrode OP1 an elongated, flexible, silicone rubber, holder HO1 carries a light emitter LE1 at one end EN1, and an optical sensor SE1 at another wider end EN2. The holder HO1 spaces the light emitter LE1 about 5 cm away from the sensor SE1. The holder HO1 is thickened at the ends EN1 and EN2 to accommodate the light emitter LE1 and the other end EN2 to accommodate the sensor SE1, while the central portion CE1 between the ends is kept thin to maintain flexibility. 
     The emitter LE1 takes the form of a triangular-crosssectioned prism PM1 which receives light at one face FA1 from the optical fiber OF1. The latter extends, at the prism, in the elongated direction of the optrode OP1. The fiber OF1 receives its light from the section SN1. The prism PM1 internally reflects the light from the fiber OF1 vertically downward in FIG. 3 and transverse to the surface of the head and into the head in FIG. 4. The sensor SE1 is a photo-diode array of n photodiode elements EL1 to ELn aligned in the direction of light entering the prism PM1 of the emitter EM1 from the fiber OF1. The sensor SE1 is a linear sensor and senses light emerging from the head HE1. The sensor SE1 includes n preamplifiers PR1 to PRn, one for each element ELn. Each preamplifier PR1 to PRn accumulates electrons from a corresponding photodiode element ELn and amplifies them. The preamplifiers PR1 to PRn can detect low level signals with good sensitivity and send the detected signals to the section SN1. 
     In FIG. 4 tape or a flexible bandage attaches the optrode OP1 to the head where it is clinically important to know Hb, HbO, CyOx. For convenience, the optrode is attached at a location without hair. Attachment to the head is only an example. The optrode may be used on other parts of the body. 
     In FIG. 1, the section SN1 contains a solid state laser arrangement LA1 which emits repeated cycles of pulses. In each cycle, the laser arrangement LA1 sequentially emits five pulses of light at different wavelengths λ i , where i=1,2,3,4, and 5 (hence λ 1 , λ 2 , λ 3 , λ 4 , and λ 5 ). One cycle of pulses appears in FIG. 5. The light from the laser arrangement LA1 passes through the optical fiber OF1, to the prism PM1 which refracts the light 90 degrees so it is directed transverse to the surface of the head HE1. There it is introduced into the human body. 
     After the light passes into the human body, each of the n elements EL1 to ELn of the sensor SE1 senses each of the i pulses per cycle and the preamplifiers PR1 to PRn transmit the sensed pulses to a sample and hold array SH1 of n sample and hold circuits. An analog to digital converter AD1 digitizes each sampled and held value as shown in the diagram of FIG. 6 and applies it via a bus BU1 to a central processing unit (CPU) CP1 which accumulates and processes the data as shown by the graph of FIG. 7. A read only memory (ROM) RO1 and a random access memory (RAM) RA1 provide required memory for the CPU CP1. A display DI1 displays the output of the CPU CP1 in values of delta HbO 2 , Hb, HbT, CyOx, etc. 
     Analog to digital conversion by the converter AD1 and processing by the CPU CP1 of one cycle of 5 pulses takes about 1 millisecond. The CPU CP1 integrates about 1000 cycles per second. Because the signal obtained by a single emission of light is comparatively weak the CPU CP1 accumulates the data from 5 to 10 seconds, namely for 5,000 to 10,000 cycles. When this accumulation ends, the CPU CP1 performs a log conversion of the data for each wavelength and each pixel and calculates the optical density OD where 
     
         OD=-log (I.sub.o /I.sub.i), 
    
     where I o  is sensed intensity, and I i  is the input intensity. As shown in FIG. 8 it uses the OD from each sensor SE1 to calculate ##EQU1## for each wavelength, λi where d is the distance from the light source. 
     The CPU CP1 then calculates and displays the Oxyhemoglobin saturation ratio SO 2  (%) and the concentrations of Oxyhemoglobin HbO 2 , Hemoglobin Hb, Cytochrome CyOx, changes in concentration of the HbO 2 , Hb, CyOx. The Oxyhemoglobin saturation ratio=HbO 2  /(HbO 2  +Hb) Any or all of these values are also graphed as a function of time to indicate trends. 
     The basis for the operation of the CPU CP1 is described with respect to FIGS. 9 to 12. The operation of the CPU CP1 appears in the flow chart of FIGS. 13 to 15. 
     The invention is based on the Beer-Lambert law, illustrated in FIG. 9. When light passes through an absorbing medium under conditions of no light scattering the light absorption or optical density OD, i.e. the change in light intensity -log(I o  /I i ), is proportional or equal to the product εcd of a known molar extinction coefficient ε, the concentration c of the absorption pigment, and distance d. When there is light scattering, the modification of Beer-Lambert law, 
     
         OD=εcL+X                                           (1) 
    
     has been used as shown in FIG. 10, where L is average light path distance between the position of input light and detecting position, X is the contribution of light which is not picked by detector due to the scattering. Since X is unknown, Equation 1 is unsuitable for accurate measurements. Prior art systems used 
     
         Δ(OD).sub.t =εLΔ(C).sub.t              (2) 
    
     for determining only temporal variation of light absorbance, Δ(OD) t , or measured the concentration variation of each compound or the variation of the Oxygen saturation ratio of Hemoglobin by measuring the difference of OD at two points as shown in FIG. 11, and by using the relation 
     
         Δ(OD).sub.d =εLΔ(L).sub.d              (3) 
    
     These equations assume that the average light path length L is constant. But in reality, L varies depending on the light extinction coefficient μ a  (μ a  =Σε i  c i ) where μ a  is in units of 1/cm. For example, when the absorption increases, the light that travels along a longer trajectory before it reaches the detector is attenuated more than light that travels along a shorter trajectory. Thus the contribution of the detected signal arising from the shorter path is increased relative to the light along the longer path. As result, L becomes shorter, since L is a weighted average of all paths that go to the detector. On the other hand, if the absorption is decreased, L becomes longer. Therefore the light absorption OD is not proportional to the concentration c, and equations 2 and 3 represent broad approximations that can lead to errors. 
     In general, the behavior of light inside an organism can be approximated as a scattering phenomenon, with a diffusion coefficient. D={3(μ a  +μ&#39; s )} -1 , where μ&#39; s  is the actual scattering coefficient in units of 1/cm. In FIG. 12, light is injected at one point and detected a distance d away. In general, μ&#39; s  &gt;&gt;μ a , d&gt;1/μ&#39; s , d&gt;1/√3μ a  μ&#39; s  . For the sake of simplicity the injected light is a pulse of very short duration. Scatter through the organism results in an output of the following response function at distance d: ##EQU2## where the detected photon quantity I(d) is the time-integrated value of the response function. Then, ##EQU3## Since light absorption quantity OD(d) is the minus or negative logarithm of detected light quantity I(d), ##EQU4## (Ordinarily OD is estimated by OD=μ a  L+X where (μ a  =εc)). The invention simplifies the complex relationship between OD and μ a  in the last equation for OD(d) by taking the derivative ##EQU5## 
     Here, the first term is independent of d, when the second term decreases as d increases. For example, using the typical values, μ a  μ&#39; s  ≈0.1 mm -2 , d&gt;40 mm, the second term becomes less than one tenth of the first term and can be approximately by the first term. Therefore: ##EQU6## 
     Thus CPU CP1 employs the latter equation to calculate the concentration of each biochemical j by acquiring ##EQU7## with multiple wavelengths λi using the optrode OP1 and the matrix formula: ##EQU8## where μ ai  is for the wavelength λi and N is at least equal to the number of compounds determined plus 1 for a baseline. 
     The coefficient ##EQU9## that multiples μ a  is independent of μ a . Consequently, the linear dependence of ##EQU10## on μ a  is maintained. Precise measurement of μ a  is possible. The value μ&#39; s , over the appropriate wavelength range can be considered constant. 
     The CPU CP1 measures the biochemical substances HbO 2 , Hb, CyOx, H2O, as well as a baseline where these compounds do not absorb, using the matrix: ##EQU11## 
     The CPU CP1 acquires the relative concentration of each compound j, KCj, by using the aforementioned matrix equation. 
     The CPU CP1 then calculates Hemoglobin Oxygen saturation ##EQU12## which is clinically significant. According to the above method, the CPU CP1 obtains the relative density of all the elements. 
     The measurement accuracy for low concentration CyOx involves a calculation based on the temporal change in ##EQU13## 
     The value ##EQU14## itself includes the absorbance of all the compounds. Therefore solving equation 10 involves including the absorbance of water as well as the baseline contributions from all other substances that absorb in the wavelength range of the measurement. 
     On the other hand, in case of Δ t  ##EQU15## when solving the equation while considering only the element which varies during measurement, HbO 2 , Hb, CyOx, there is no need to consider the influence of things like Offset. The accuracy is greatly improved (even though what is measured is a variation of concentration KΔC). To be precise, CPU CP1 uses the following formula to obtain values of changes with respect to time in concentrations of HbO 2 , Hb, and CyOx. ##EQU16## 
     For measurement value of CyOx, the CPU CP1 obtains the variation of the concentration from matrix equation (11). For Hb and HbO 2 , it compares the variation of KC HbO2 , KC Hb  in the matrix equation (10) and determines KΔ i  C HbO2 , KΔCHb from matrix equation (11). If these are almost the same, it supports the validity of the Hemoglobin concentration calculated by the former of the two matrix equations. 
     As shown above, by measuring ##EQU17## the error generated by μ a  dependence of path length for the current method, which uses OD from equations 1,2, or 3, is improved. The measurement accuracy and reliability also increased by measuring the change of concentration with time, by determining ##EQU18## 
     The system operates as shown in the flow chart of FIGS. 13, 14, and 15. In step 100, the CPU CP1 initializes an accumulation index k=1, and a wavelength index i=0. It then passes to step 104 to actuate laser 0. Such actuation does not actually occur, because there is no laser 0. The step leaves a time slot for detection of background noise. Without a signal from the lasers the fiber OF1 carries no light and the prism PM1 emits no light. However in step 107, the sensor SE1 senses signals s i1 , s i2 , s i3 , and s i4  representing background noise. The preamplifiers PR1 to PRn transmit the signals via the cable CA1 to the sample and hold circuits SH1 to SHn, to the converters AD1, and to the CPU CP1. In step 110, the CPU CP1 accumulates this signal with all previous signals if any. 
     In step 114, the CPU asks whether i=5. If not, the process advances to step 117 to increment i and returns to step 104 to fire laser 1. At step 107 the sensor SE1 detects signals s i1 , s i2 , s i3 , and s i4  from firing of laser 1. In step 110 the sensed signals are accumulated with previously sensed signals. The loop through step 117 repeats until i=5. This then completes one cycle. 
     When i=5 at step 114, the CPU CP1 progresses to step 120 which asks whether k=K (K typically equals 10,000). If not, the system goes on to step 124 to increment k. Such incremental advance occurs once each cycle of i. For each increment of k a new cycle begins for i=0, 1, 2, . . . 5. 
     When k=K, the process goes on to step 130. Here, the CPU CP1 subtracts all background data S o1 (k) from each 1ch, λ i  data S i1 (k), S i2 (k), S i3 (k), and S i4 (k) to obtain values of detected light quantities I i1 , I i2 , I i3 , and I i4 . The relationship between the detected light quantities I i  and the light absorption quantity OD is that the light absorption quantity OD(d) is a minus logarithm of the detected light quantity I(d). Hence, OD(d)=-log I(d), and OD i  =-log (I i  /I.sub.(i-1)). In step 134 the CPU CP1 converts these values to values of light absorption changes OD along the separation, where ##EQU19## 
     The CPU CP1 now determines regression ∂OD/∂d in step 137. In step 140 it calculates the extinction coefficient μ a  for each i. In step 144 it calculates the change in extinction coefficient Δ t  μ a , where 
     
         Δ.sub.t μ.sub.ai =(μ.sub.ai).sub.(t=t) -(μ.sub.ai).sub.(t=0)(12) 
    
     The CPU CP1 now performs the matrix calculation in step 147 and, in step 150, displays the data for SO 2 , ΔHbO 2 , ΔHb, ΔCyOx. 
     According to an embodiment of the invention, laser diodes or LEDs replace the prism PM1, and a cable for energizing the laser diodes or LEDs replaces the optical fiber OF1. 
     The invention permits accurate measurement of concentrations and changes in concentrations of biochemical compounds. 
     Sample values of the known extinction coefficient ε are shown for various wavelengths in the following table: 
     
                       TABLE 1______________________________________Wave-length  Hb           HbO.sub.2  CytOx(mm)    (mM.sup.-1 cm.sup.-1)                (mM.sup.-1 cm.sup.-1)                           (mM.sup.-1 cm.sup.-1)______________________________________800     0.8399       0.8653     2.2619801     0.8338       0.8716     2.2666802     0.8285       0.8780     2.2713803     0.8237       0.8845     2.2762804     0.8190       0.8909     2.2812805     0.8146       0.8973     2.2870806     0.8111       0.9038     2.2927807     0.8075       0.9102     2.2991______________________________________ 
    
     According to an embodiment of the invention, the processor CPU CP1 calculates values of C by the linear least squares method. To start, the measured concentrations are plural (C1,C2, . . . ,Cj) and the general form of equation 10 contains n wavelengths and j components (n≧j) and is ##EQU20## At the left is (nx1)matrix OD. Then (nxj)matrix ε, and (jx1)matrix KC. 
     The general form of the equation, in the next matrix form, is: 
     
         φ=.epsilon slash..Kc/ 
    
     where &#34;.&#34; is matrix multiplication then, where, K¢=.epsilon slash.*. φ.epsilon slash.*=(.epsilon slash. T ..epsilon slash.) -1 ..epsilon slash. T . Here, .epsilon slash. T  : Transpose matrix, .epsilon slash. -1  : square inverse matrix, and (j-n) matrix .epsilon slash.* is the pseudo-inverse matrix of .epsilon slash.. 
     The value ##EQU21## is given by other measurements. Thus the processor CPU CP1 obtains C itself by this linear least squares method in step 147. 
     The laser LA1 and the prism PM direct the wavelengths in a pulse or sine wave form. 
     While embodiments of the invention have been described in detail, it will be evident to those skilled in the art that the invention may be embodied otherwise without departing from its spirit and scope.