Apparatus and method for measuring concentrations of components

Claim 1

An apparatus for measuring concentrations of components comprising a light irradiator for projecting pulse light of different wavelengths toward an object, a photodetector for performing a time resolved measurement of the quantity of light with respect to at least one of reflected light and transmitted light from the object which is subject to changes with lapse of time after the generation of the pulse light, and an arithmetic unit for calculating a component concentration in the object and outputting the calculation result such that the relationship between time lapse and measured quantity of light is converted into a relationship between an optical path length representing the distance of light travel within the object and a change in the measured quantity of light relative to a change in unit concentration so that the optical path length and the quantity of light which is measured when the change in the quantity of light is at a peak are stored in memory to enable selection of an optimum optical path length for each wavelength, with the quantity of light for the optimum optical path length being used as a basis for the calculation.

Claim 4

A method for measuring concentrations of components which comprises projecting pulse light of a selected wavelength from a light irradiator toward an object; causing a photodetector to perform a time resolved measurement of the quantity of light with respect to at least one of reflected light and transmitted light from the object which is subject to changes with lapse of time after the generation of the pulse light; storing the measured data in an arithmetic unit; and repeating the foregoing steps for different wavelengths of pulse light in such a manner that the arithmetic unit converts the relationship between time lapse and measured quantity of light into a relationship between an optical path length representing the distance of light travel within the object and a change in the measured quantity of light relative to the change in unit concentration so that the optical path length and the quantity of light which is measured when the change in the quantity of light is at a peak are stored in memory for each wavelength to enable selection of an optimum optical path length for each wavelength, whereby concentrations of components in the object is calculated on the basis of the quantity of light for the optimum optical path length, the calculated result being then output.

Claim 5

A method for measuring concentrations of components which comprises the steps of: (i) generating pulse light of a selected wavelength from a light irradiator and causing a photodetector to perform a time resolved measurement of the quantity of received light I R from an object which serves as a reference and is subject to changes with lapse of time t; (ii) projecting pulse light of the selected wavelength from the light irradiator toward the object and causing the photodetector to perform a time resolved measurement of the quantity of transmitted light I t from the object which is subject to changes with lapse of time t; (iii) with respect to the measured quantity of received light I R (L) and measured quantity of transmitted light I t (L) which are subject to changes with an optical path length L corresponding to lapse of time t, selecting a reference quantity of received light I R (L o ) and a reference quantity of transmitted light I t (L o ) at a reference optical path length L o corresponding to a certain reference lapse of time t o ; (iv) calculating value γ o for γ at reference optical path length L o from equation I t (L) = I R (L)tγ (where, t: transmittance of light relative to the object); (v) calculating optical path length ratio k p corresponding to an optical path length L p which gives a maximum sensitivity for quantity-of-light measurement, from an equation k = -1/log₁₀γ o which expresses the relationship between optical path length ratio k = L/L o and γ o at reference optical path length L o ; (vi) calculating an optimum lapse of time t p corresponding to the optimum optical path length L p from equation L = Ct which expresses the relationship between optical path length L and lapse of time t; (vii) calculating the quantity of transmitted light I tp (t p ) from the object for a certain wavelength λ at optimum lapse of time t p ; (viii) calculating, on the basis of the quantity of received light I RP and quantity of transmitted light I tp at the optimum lapse of time and from equation A = log₁₀ (I R /I t ) for absorbance A, an absorbance A p corresponding to I RP and I tp ; and (ix) repeating the foregoing steps for plural wavelengths, whereby on the basis of respective calculated absorbances are carried out multivariate analyses to calculate the concentrations of the components in the object, the calculated results being then output.

Claim 6

A method for measuring concentrations of components which comprises the steps of: (i) generating pulse light of a selected wavelength from a light irradiator and causing a photodetector to perform a time resolved measurement of the quantity of received light I R from an object which serves as a reference and is subject to changes with lapse of time t; (ii) projecting pulse light of the selected wavelength from the light irradiator toward the object and causing the photodetector to perform a time resolved measurement of the quantity of reflected light I r from the object which is subject to changes with lapse of time t; (iii) with respect to the measured quantity of received light I R (L) and measured quantity of reflected light I r (L) which are subject to changes with an optical path length L corresponding to lapse of time t, selecting a reference quantity of received light I R (L o ) and a reference quantity of reflected light I r (L o ) at a reference optical path length L o corresponding to a certain reference lapse of time t o ; (iv) calculating value γ o for γ at reference optical path length L o from equation I t (L) = I R (L)tγ (where, t: transmittance of light relative to the object); (v) calculating optical path length ratio k p corresponding to an optical path length L p which gives a maximum sensitivity for quantity-of-light measurement, from an equation k = -1/log₁₀γ o which expresses the relationship between optical path length ratio k = L/L o and γ o at reference optical path length L o ; (vi) calculating an optimum lapse of time t p corresponding to the optimum optical path length L p from equation L = Ct which expresses the relationship between optical path length L and lapse of time t; (vii) calculating the quantity of reflected light I rp (t p ) from the object for a certain wavelength λ at optimum lapse of time t p ; (viii) calculating, on the basis of the quantity of received light I RP and quantity of reflected light I rp at the optimum lapse of time and from equation A = log₁₀ (I R /I r ) for absorbance A, an absorbance A p corresponding to I RP and I rp ; and (ix) repeating the foregoing steps for plural wavelengths, whereby on the basis of respective calculated absorbances are carried out multivariate analyses to calculate the concentrations of the components in the object, the calculated results being then output.

Claim 7

A method for measuring concentrations of components which comprises the steps of: (i) generating pulse light of a selected wavelength from a light irradiator and causing a photodetector to perform a time resolved measurement of the quantity of received light I R from an object which serves as a reference and is subject to changes with lapse of time t; (ii) projecting pulse light of the selected wavelength from the light irradiator toward the object and causing the photodetector to perform a time resolved measurement of the quantity of transmitted light I t and quantity of reflected light I r from the object which are subject to changes with lapse of time t; (iii) with respect to the measured quantity of received light I R (L), measured quantity of transmitted light I t (L) and measured quantity of reflected light I r (L) which are subject to changes with an optical path length L corresponding to lapse of time t, selecting a reference quantity of received light I R (L o ), a reference quantity of transmitted light I t (L o ), and a reference quantity of reflected light I r (L o ) at a reference optical path length L o corresponding to a certain reference lapse of time t o ; (iv) calculating value γ o for γ at reference optical path length L o from equation I t (L) = I R (L)tγ (where, t: transmittance of light relative to the object); (v) calculating optical path length ratio k p corresponding to an optical path length L p which gives a maximum sensitivity for quantity-of-light measurement, from an equation k = -1/log₁₀γ o which expresses the relationship between optical path length ratio k = L/L o and γ o at reference optical path length L o ; (vi) calculating an optimum lapse of time t p corresponding to the optimum optical path length L p from equation L = Ct which expresses the relationship between optical path length L and lapse of time t; (vii) calculating the quantity of transmitted light I tp (t p ) and quantity of reflected light I rp (t p ) from the object for a certain wavelength λ at optimum lapse of time t p ; (viii) calculating, on the basis of the quantity of received light I RP , quantity of transmitted light I tp , and quantity of reflected light I rp at the optimum lapse of time and from equation A = log₁₀ (I R /I r ) for absorbance A, an absorbance A p corresponding to I RP , I tp and I rp ; and (ix) repeating the foregoing steps for plural wavelengths, whereby on the basis of respective calculated absorbances are carried out multivariate analyses to calculate the concentrations of the components in the object, the calculated results being then output.