A core body temperature measurement device includes a plurality of electronic temperature sensors (12, 12f, 12b, 132) operatively coupled with or near a surface (STA, PAA, BTT) having a surface temperature approximating the core body temperature, and a readout controller (10, 48, 68, 90, 124) including a maximum temperature reading selector (14). The readout controller is configured to acquire temperature readings using the plurality of temperature sensors and to output a core body temperature based on a highest usable temperature reading of the acquired temperature readings as determined by the maximum temperature reading selector. A core body temperature measurement method includes: acquiring a plurality of temperature readings at and near a surface (STA, PAA, BTT) having a surface temperature approximating the core body temperature; generating a highest usable temperature reading from the acquired temperature readings; and outputting a core body temperature based on the highest usable temperature.
1. A core body temperature measurement device comprising:
a plurality of electronic temperature sensors operatively coupled with or near a surface having a surface temperature approximating the core body temperature; and a readout controller including a maximum temperature reading selector (14), the readout controller configured to acquire temperature readings using the plurality of temperature sensors and to output a core body temperature based on a highest usable temperature reading of the acquired temperature readings as determined by the maximum temperature reading selector. 2. The core body temperature measurement device as set forth in 3. The core body temperature measurement device as set forth in a head-mountable mechanical frame or pad configured to operatively couple the electronic temperature sensors with or near said surface having a surface temperature approximating the core body temperature. 4. The core body temperature measurement device as set forth in an interpolator that spatially interpolates temperature readings of the plurality of electronic temperature sensors to generate an interpolation; and a peak detector that detects the highest usable temperature reading of the acquired temperature readings as a peak of the interpolation. 5. The core body temperature measurement device as set forth in 6. The core body temperature measurement device as set forth in 7. The core body temperature measurement device as set forth in an oral thermometer body containing the readout controller and defining a neck terminating in a generally spherical sensors head supporting the plurality of sensors. 8. A core body temperature measurement device comprising:
at least one electronic temperature sensor operatively coupled with or near a surface having a surface temperature approximating the core body temperature; and a readout controller configured to acquire an input temperature reading from the at least one electronic temperature sensor and to obtain a core body temperature therefrom, the readout controller including a temperature corrector that increases the input temperature reading to account for a temperature difference between the input temperature reading and the core body temperature. 9. The core body temperature measurement device as set forth in a heat flux sensor associated with the at least one electronic temperature sensor, the heat flux sensor acquiring a measurement used to determine a heat flux, the temperature drop being determined based on the heat flux. 10. The core body temperature measurement device as set forth in a capacitance meter configured to measure a mutual capacitance of the two conductive bodies separated by the insulating material, the temperature difference being derived from the mutual capacitance and one or more temperature readings acquired by the at least one electronic temperature sensor. 11. The core body temperature measurement device as set forth in 12. The core body temperature measurement device as set forth in a blood oxygen sensor configured to acquire a blood oxygenation measurement, an optical source of the blood oxygen sensor additionally being used to generate variable heating from which the temperature corrector derives the increase of the input temperature reading. 13. A core body temperature measurement method comprising:
acquiring a plurality of temperature readings at and near a surface having a surface temperature approximating the core body temperature; generating a highest usable temperature reading from the acquired temperature readings; and outputting a core body temperature based on the highest usable temperature. 14. The core body temperature measurement method as set forth in 15. The core body temperature measurement method as set forth in 16. The core body temperature measurement method as set forth in spatially interpolating the plurality of temperature readings to generate an interpolation; and detecting the highest usable temperature reading of the acquired temperature readings as a peak of the interpolation. 17. The core body temperature measurement method as set forth in selecting the highest usable temperature reading as a highest of the acquired plurality of temperature readings. 18. The core body temperature measurement method as set forth in correcting an input temperature or input temperatures selected from the group consisting of (i) the acquired plurality of temperature readings and (ii) the generated highest usable temperature reading for a temperature drop between the body core and said surface to generate the core body temperature. 19. The core body temperature measurement method as set forth in providing a temperature sensor including spaced-apart conductive bodies with one conductive body in thermal contact at or near said surface; measuring a mutual capacitance of the spaced-apart conductive bodies; and estimating a heat flux between the conductive bodies based on the mutual capacitance. 20. The core body temperature measurement method as set forth in providing a temperature sensor including spaced-apart conductive bodies with one conductive body in thermal contact at or near said surface; variably heating the temperature sensor; acquiring temperatures and a temperature derivative for the conductive bodies at a plurality of different heating levels; and deriving the core body temperature from the acquired temperatures and temperature derivatives at the plurality of different heating levels. 21. The core body temperature measurement method as set forth in operating an optical source of a blood oxygen sensor at different power levels to provide variable heating.
The following relates to the medical arts. It finds particular application in measuring core body temperature, and is described with particular reference thereto. However, the following finds more general application in measuring core body temperature-related values suitable for use in medical diagnostic, treatment monitoring, and related medical applications. Core body temperature is an important medical vital sign. Unlike other vital signs such as heart rate or blood pressure, core body temperature is relatively insensitive to variations due to psychological or emotional state. Thus, core body temperature can be a good indicator of a medical problem. Moreover, a shift in core body temperature of only a few degrees Celsius away from the typical range can be life-threatening in and of itself, providing further motivation for monitoring this critical vital sign. Unfortunately, core body temperature has heretofore been more difficult to measure than other vital signs such as heart rate or blood pressure. The core body temperature is defined as the temperature of blood flowing through the heart. However, for clinical purposes the core body temperature is typically taken as the brain temperature, since this value is typically close to the cardiac core temperature, and elevated brain temperature is a clinically serious condition that would be useful to monitor in clinical settings. As used herein, core body temperature is taken to correspond to the brain temperature. A rectal thermometer is also sometimes used to measure core body temperature, under the assumption that the rectal temperature is a suitable surrogate for the core body temperature. However, rectal temperature may differ substantially from core body temperature of the heart or brain. Insertion of a rectal thermometer is also uncomfortable for the patient, and rectal thermometry is not well-suited for extended monitoring over a period of hours, days, or longer. To precisely measure core body temperature, a temperature sensor can be inserted into brain vasculature using a suitable catheter instrument. Although precise, this approach is clinically problematic because it is invasive and can produce disadvantageous side effects such as infection, vascular clotting, or so forth. Core body temperature can also be estimated by measuring forehead temperature. This is the basis for the home diagnostic of placing a hand over the forehead of the patient to determine whether a fever is present. As a measure of core body temperature, this technique is inexact at best. A more precise core body temperature estimate can be obtained by placing a thermocouple, thermistor, or other electronic temperature sensor into contact with the forehead. However, the temperature acquired by such sensors can differ substantially from the core body temperature due to temperature drop across the skin and other intervening tissue. This temperature drop is not constant, but varies significantly as a function of sweat, room temperature, and other factors. The acquired temperature can also vary depending upon at what position on the forehead the sensor is placed. Core body temperature is also sometimes estimated using an oral thermometer. It is known that placement of the thermometer in a posterior sublingual pocket provides a relatively accurate estimate of core body temperature, as this region is close to substantial arterial structure. However, even small errors in the positioning of the oral temperature can result in a substantial error in the temperature reading. Respiration, ingestion, or other oral activities can also adversely affect the temperature reading. Thermometers are also known which are inserted into the ear canal to contact the tympanic membrane, also known colloquially as the ear drum. The tympanic membrane has relatively close proximity to the brain and reflects the core body temperature relatively accurately. However, the shape of the ear canal varies from person to person, and in some instances access to the tympanic membrane may be impeded or blocked by curvature of the ear canal. Another potential source of error is wax buildup in the ear canal. Physical contact with the tympanic membrane by the thermometer can also promote ear infection, which can be a serious medical condition. Core body temperature measurement via the tympanic membrane is also not well suited for extended monitoring over a period of hours, days, or longer. Abreu, U.S. Published Application 2004/0059212, discloses a recently developed technique for measuring core body temperature that overcomes some of these difficulties. The approach of Abreu is based on identification of a thermally conductive pathway to the brain, called a “brain tunnel” in US 2004/0059212, located between the eyes proximate to an orbit or eye socket. By using contact thermometry at the location of this “brain tunnel,” a relatively accurate core body temperature reading can be non-invasively obtained. Unfortunately, the identified brain tunnel has a small external cross-section near the eye orbit, which makes the accuracy of the core body temperature measurement strongly dependent upon precise placement of the temperature sensor. Positional deviations of as little as one or two millimeters can adversely affect the core body temperature measurement via the brain tunnel. While acquisition of an accurate core body temperature reading is difficult, extended monitoring of this vital sign is more difficult still. As noted above, suitable sites for measuring core body temperature, such as the posterior sublingual pocket and the “brain tunnel” identified by Abreu, are typically small. As a result, shift or movement of the temperature sensor over time during extended monitoring is problematic. The following provides new and improved apparatuses and methods which overcome the above-referenced problems and others. In accordance with one aspect, a core body temperature measurement device includes a plurality of electronic temperature sensors operatively coupled with or near a surface having a surface temperature approximating the core body temperature, and a readout controller including a maximum temperature reading selector. The readout controller is configured to acquire temperature readings using the plurality of temperature sensors and to output a core body temperature based on a highest usable temperature reading of the acquired temperature readings as determined by the maximum temperature reading selector, optionally also including a correction for the temperature drop through the skin as will be described in more detail in the sequel. In accordance with another aspect, a core body temperature measurement device includes at least one electronic temperature sensor operatively coupled with or near a surface having a surface temperature approximating the core body temperature, and a readout controller configured to acquire an input temperature reading from the at least one electronic temperature sensor and to obtain a core body temperature therefrom. The readout controller includes a temperature corrector that increases the input temperature reading to account for a temperature difference between the input temperature reading and the core body temperature. In accordance with another aspect, a core body temperature measurement method includes: acquiring a plurality of temperature readings at and near a surface having a surface temperature approximating the core body temperature; generating a highest usable temperature reading from the acquired temperature readings; and outputting a core body temperature based on the highest usable temperature. One advantage resides in providing an accurate non-invasive core body temperature measurement. Another advantage resides in providing a non-invasive core body temperature measurement that is relatively insensitive to the precise positioning of the temperature measurement device. Another advantage resides in providing a non-invasive core body temperature measurement that is corrected for a temperature difference between the surface at which the temperature is measured and the body core. Still further advantages of the present invention will be appreciated to those of ordinary skill in the art upon reading and understand the following detailed description. With reference to With continuing reference to While With reference to Using the plurality of temperature sensors 12 accommodates such individual variation. A maximum reading selector 14 selects the highest temperature measurement acquired by the plurality of temperature sensors 12 as a highest usable temperature reading 15 for determining the core body temperature. This approach relies on the recognition made herein that the measured temperature should be highest at that point where the skin temperature most closely approximates the core body temperature. Lower temperature measurements generally reflect higher thermal losses away from the surface having a surface temperature approximating the core body temperature. Lower temperature measurements may also reflect inaccurate temperature readings due to poor thermal contact of the temperature sensor with the skin or other measurement errors. Thus, by using the plurality of temperature sensors 12 and employing the maximum reading selector 14 to select the highest temperature measurement, such difficulties are alleviated. With brief reference to With returning reference to On the other hand, if multiple peaks are located (that is, if ∇TS=0 at more than one position) then the highest interpolated temperature of the multiple peaks is suitably defined as Tmax. For example, if ∇TS(x1,y1)=0 and TS(x1,y1)=37.4° C., while ∇TS(x2,y2)=0 and TS(x2,y2)=37.1° C., then selection of Tmax=37.4° C. is appropriate. In the embodiments described with reference to Still further, the maximum reading selector 14 With returning reference to Optionally the temperature measurement device includes sensors to acquire other physiological parameters besides temperature. For example, a blood oxygen sensor 20, such as an SpO2sensor or an StO2sensor, acquires a measurement (typically an optically based measurement in the case of an SpO2or StO2sensor) that is converted into a blood oxygenation level reading and a pulse reading by a pulse/oxygen extractor 22. Different or additional sensors can be included, such as a blood pressure sensor. The resulting information including the core body temperature and optional other readings such as blood oxygenation and pulse are output by a suitable output path such as a built-in display (not shown in As mentioned previously, the optional skin temperature corrector 16 in some embodiments employs an estimated skin temperature drop correction, such as a 1° C. temperature drop correction. This approach is computationally straightforward, but can lead to some error since the actual skin temperature drop varies based on factors such as moisture (e.g., sweat), ambient temperature, air convection, and so forth. To accommodate such factors, in some embodiments the skin temperature corrector 16 employs a more complex corrective approach based on feedback. Some suitable temperature correction algorithms are disclosed in Fox et al., U.S. Pat. No. 3,933,045 which is incorporated herein by reference; Heikkilä et al, U.S. Pat. No. 5,816,706 which is incorporated herein by reference; and Tokita et al., U.S. Pat. No. 6,886,978 which is incorporated herein by reference. One suitable temperature correction algorithm operates in conjunction with the one or more skin temperature sensors 12 each configured to include parallel conductive plates or films spaced apart by a distance that is adjustable using inchworm actuators, MEMS actuators, or so forth. These temperature sensors are in effect combination temperature/heat flux sensors, because by acquiring temperature measurements across the two plates at different plate separations, the heat flux can be determined, from which the skin temperature drop can in turn be estimated. Designating the temperatures of the two conductive plates as T1and T2, respectively, and the core body temperature as Tcore, the following expression holds: where α=λ/ρcP, λ denotes thermal conductivity, ρ denotes density, and cPdenotes specific heat. In a suitable coordinate system, x denotes depth with x=0 corresponding to a point inside the body at temperature Tcoreand x=hscorresponding to the surface of the skin. The boundary conditions for Equation (1) include the core body temperature Tcore(to be determined) at x=0, and the measured temperature Tsat x=hs, that is, at the surface of the skin. If the conductive plate at temperature T2is contacting or otherwise in good thermal communication with the skin, then Ts=T2to a good approximation. The heat flux out of the skin is denoted qsherein. Assuming the skin 33 can be represented as a plane of thickness hsand thermal conductivity λs, the heat flux out of the skin qs(that is, heat transfer rate on a per-unit area basis) can be written as: and a solution of Equation (1) can be approximated as: At equilibrium, Equation (3) reduces to: which demonstrates that the core body temperature Tcoreis higher than the skin temperature by a temperature drop across the skin corresponding to (hs/λs)·qs. By using feedback control of actuators separating the parallel conductive plates or films, the values of the quantities Ts, qs, and can be measured for different moments in time ti={t1, . . . , tn}toproduce a matrix of coupled equations: in which the unknown quantities are Tcore, and where: It is assumed here that Tcore, are time-independent during the time interval {t1, . . . , tn} over which the set of measurements are acquired. The system of Equations (5) can be solved by the temperature corrector 16 using a least squares minimisation procedure or other suitable coupled equations solver to provide the body core temperature Tcore, and also the heat flux qsthrough the surface of the skin. The sampling moments tiare suitably chosen such that to ensure that the system of Equations (5) is well-conditioned. In some embodiments, the heat flux across the parallel conductive plates of a parallel-plate temperature/heat flux sensor is determined by a combination of thermal and electrical measurements. This approach makes use of a formal correspondence identified herein between the electrostatic potential distribution given by Poisson's equation (ε·∇2φ=0) and the expression for temperature distribution (k·∇2T=0). Comparing these equations and using the boundary conditions φ|Ω where ηTis the thermal conductance between the two spaced-apart conductive plates, C is the mutual capacitance of the two spaced-apart conductive plates, k is the thermal conductivity of the dielectric material spacing apart the conductive plates, and ε is the dielectric constant of the dielectric material spacing apart the conductive plates. In deriving this relationship between thermal conductance ηTand mutual capacitance C, it is assumed that the ratio k/ε is a constant. This assumption holds sufficiently for air, foam, polyethylene, and numerous other common dielectric spacers. The dielectric constant or permittivity ε of the dielectric spacer is related to the vacuum permittivity εo≈8.8542×10−12F/m by the relative dielectric constant εraccording to the relationship ε=εr·εo. The relationship enables the heat flux f across the parallel plates 30, 31 to be determined for the known (measured) T1and T2by a straightforward mutual capacitance measurement using a capacitance meter, from which the heat flux across the skin can be estimated. Advantageously, the geometrical assumptions going into derivation of the relationship are limited—for example, spaced apart conductive bodies that are not parallel plates can be used. In the combination temperature/heat flux sensor of As another approach, the temperature corrector 16 can make a skin temperature drop correction determined based on physiological measurements such as the ambient temperature (suitably acquired using a temperature sensor that is not in contact with or close to the skin), skin sheet resistance or conductivity (measurable using a first electrode pair driving a small current and a second electrode pair measuring voltage generated by the drive current), or so forth. A lookup table or empirical formula suitably relates the skin temperature drop correction to the measured ambient temperature, skin sheet resistance, or other parameters. In some contemplated embodiments of the temperature corrector 16, the corrective approach of Tokita et al, U.S. Pat. No. 6,886,978 is used, in which a variable heater provides a perturbation of the temperature distribution from which the core body temperature can be estimated. In this approach, the temperature distribution can be written for the sensor of is used to derive the heat flux between the plates 30, 31 from which along with T1and T2the derivative dT2/dx is determined Additionally, the actuators 34 can be omitted in these embodiments in which thermal (i.e., heating) perturbation is used instead of mechanical perturbation. With the actuators 34 omitted, the spacing of the conductive layers or plates 30, 31 is not modifiable. With reference to The mechanical frames illustrated in With reference to The provision of a plurality of temperature sensors 132 (represented by filled circles in The invention has been described with reference to the preferred embodiments. Modifications and alterations may occur to others upon reading and understanding the preceding detailed description. It is intended that the invention be construed as including all such modifications and alterations insofar as they come within the scope of the appended claims or the equivalents thereof.