US20140140370A1 - Medical thermometer having an improved optics system - Google Patents

Medical thermometer having an improved optics system Download PDF

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Publication number
US20140140370A1
US20140140370A1 US14/082,321 US201314082321A US2014140370A1 US 20140140370 A1 US20140140370 A1 US 20140140370A1 US 201314082321 A US201314082321 A US 201314082321A US 2014140370 A1 US2014140370 A1 US 2014140370A1
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Prior art keywords
radiation
mirror
approximately
medical thermometer
sensor
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Abandoned
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US14/082,321
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English (en)
Inventor
Aleksan Yildizyan
James Christopher Gorsich
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Helen of Troy Ltd
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Kaz USA Inc
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Filing date
Publication date
Application filed by Kaz USA Inc filed Critical Kaz USA Inc
Priority to US14/082,321 priority Critical patent/US20140140370A1/en
Assigned to HELEN OF TROY LIMITED reassignment HELEN OF TROY LIMITED ASSIGNMENT OF ASSIGNORS INTEREST (SEE DOCUMENT FOR DETAILS). Assignors: KAZ USA, INC.
Publication of US20140140370A1 publication Critical patent/US20140140370A1/en
Priority to US15/642,438 priority patent/US20170307445A1/en
Priority to US15/869,259 priority patent/US10054490B2/en
Abandoned legal-status Critical Current

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    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J5/00—Radiation pyrometry, e.g. infrared or optical thermometry
    • G01J5/02—Constructional details
    • G01J5/08—Optical arrangements
    • G01J5/0806—Focusing or collimating elements, e.g. lenses or concave mirrors
    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J5/00—Radiation pyrometry, e.g. infrared or optical thermometry
    • G01J5/0003—Radiation pyrometry, e.g. infrared or optical thermometry for sensing the radiant heat transfer of samples, e.g. emittance meter
    • G01J5/0011—Ear thermometers
    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J5/00—Radiation pyrometry, e.g. infrared or optical thermometry
    • G01J5/02—Constructional details
    • G01J5/06—Arrangements for eliminating effects of disturbing radiation; Arrangements for compensating changes in sensitivity
    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J5/00—Radiation pyrometry, e.g. infrared or optical thermometry
    • G01J5/02—Constructional details
    • G01J5/08—Optical arrangements
    • G01J5/0808—Convex mirrors
    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J5/00—Radiation pyrometry, e.g. infrared or optical thermometry
    • G01J5/02—Constructional details
    • G01J5/08—Optical arrangements
    • G01J5/0831—Masks; Aperture plates; Spatial light modulators
    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J5/00—Radiation pyrometry, e.g. infrared or optical thermometry
    • G01J5/02—Constructional details
    • G01J5/06—Arrangements for eliminating effects of disturbing radiation; Arrangements for compensating changes in sensitivity
    • G01J2005/065—Arrangements for eliminating effects of disturbing radiation; Arrangements for compensating changes in sensitivity by shielding

Definitions

  • the present invention relate generally to devices for measuring temperature, and more specifically to non-contact infrared thermometers for medical applications incorporating mirrors to reduce the effects of stray radiation.
  • thermometer A thermal radiation or infrared (IR) thermometer is a device capable of measuring temperature without physically contacting the object of measurement.
  • thermometers are often called “non-contact” or “remote” thermometers.
  • IR thermometer the temperature of an object is taken by detecting an intensity of the IR radiation that is naturally emanated from the object's surface. For objects between about 0° C. and 100° C., this requires the use of IR sensors for detecting radiation having wavelengths from approximately 3 to 40 micrometers. Typically, IR radiation in this range is referred to as thermal radiation.
  • an IR thermometer is an “instant ear” medical thermometer, which is capable of making non-contact temperature measurements of the tympanic membrane and surrounding tissues of the ear canal of a human or animal.
  • Instant ear thermometers are exemplified by U.S. Pat. No. 4,797,840 to Fraden, which is incorporated by reference herein in its entirety.
  • Other examples include medical thermometers for measuring surface skin temperatures (for example, a skin surface temperature of the forehead) as exemplified by U.S. Pat. No. 6,789,936 to Kraus et al., which is incorporated by reference herein in its entirety.
  • the IR radiation is detected and converted into an electrical signal suitable for processing by conventional electronic circuits.
  • the task of detecting the IR radiation is accomplished by an IR sensor or detector.
  • thermal IR sensors typically include a housing with an infrared transparent window, or filter, and at least one sensing element that is responsive to a thermal radiation energy flux ⁇ emanating from an object's surface that passes through the IR window of the IR sensor and onto the sensing element.
  • the IR sensor functions to generate an electric signal, which is representative of the net IR flux ⁇ existing between the sensing element and the object of measurement.
  • the electrical signal can be related to the object's temperature by appropriate data processing, as is known in the art.
  • Thermal flux ⁇ is a function of two temperatures: a sensing element surface temperature T s and a surface temperature of the object T b (measured in Kelvin).
  • Planck's law describes the amount of electromagnetic energy with a certain wavelength radiated by a black body in thermal equilibrium.
  • T s , T b and the flux ⁇ may be approximated by a fourth-order parabola. This approximation is known as the Stefan-Boltzmann law:
  • ⁇ b and ⁇ s are the surface emissivities of the object and sensing element, respectively
  • ⁇ is the Stefan-Boltzmann constant
  • K is an optical constant which may be determined by measurement during calibration of the IR thermometer.
  • Eq. (1) For a relatively small difference between the object's true temperature T b and sensor's temperature T s , Eq. (1) can be approximated as:
  • An objective of the IR thermometer is to determine the surface temperature of the object, T b , which may be calculated as T bc from inverted Eq. 2:
  • T bc T s + ⁇ 4 ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ b ⁇ ⁇ s ⁇ ⁇ ⁇ ⁇ T s 3 ( 3 )
  • the computed temperature T bc should be equal to the true temperature T b . Practically, these temperatures may differ as the result of, e.g., measurement error or calibration drift. It can be seen from Equation (3) that, in order to calculate temperature T bc , two values need to be determined: the magnitude of the IR flux ⁇ and the IR sensing element's surface temperature T s . The accuracy of the temperature computation depends on the measurement accuracy for all variables on the right side of Eq. (3). The first summand T s can be measured quite accurately by a number of techniques known in the art, for example, by employing a thermistor or RTD temperature sensor.
  • the second summand can be more problematic, especially due to a generally unknown and unpredictable value of the object's emissivity ⁇ b .
  • the emissivity ⁇ b is a skin emissivity that is defined by the skin properties and shape.
  • the skin emissivity may, for example, range from 0.93 to 0.99.
  • Eq. (2) a partial derivative of Eq. (2) may be calculated as:
  • ⁇ ⁇ ⁇ ⁇ b ⁇ 4 ⁇ ⁇ ⁇ ⁇ ⁇ s ⁇ ⁇ ⁇ ⁇ T s 3 ⁇ ( T b - T s ) ( 4 )
  • the partial derivative represents the measurement error due to an unknown emissivity ⁇ b of an object.
  • Eq. (4) shows that the error approaches zero as T s approaches T b . Accordingly, when T b approximately equals T s , the error is small. Thus, to minimize errors, it is desirable to keep the temperature T s of the IR sensor as close as is practical to the object's temperature T b .
  • T s for an instant ear thermometer, for example, U.S. Pat. No. 5,645,349 to Fraden, incorporated by reference in its entirety herein, teaches a heated sensing element for bringing the temperatures T s and T b into proximity of each other.
  • IR thermometer When temperature is measured from a surface, it is important to minimize the amount of radiation received at the IR sensor that emanated from unwanted sources.
  • One way to minimize the chance of picking up unwanted or stray radiation is to narrow the optical field of view of the IR thermometer.
  • One method is to use IR lenses to narrow the optical field of view as exemplified by U.S. Pat. No. 5,172,978 to Nomura et al. (radiant thermometer including a lens barrel mounting a condensing lens at one end and an IR detector at the other end) and U.S. Pat. No. 5,655,838 to Ridley et al. (radiation thermometer with multi-element focusing lens, eye piece, beam splitter and IR detector), each of which is incorporated by reference in its entirety herein.
  • a non-contact IR thermometer includes, among other things, an IR radiation sensor having a sensor surface, which may be coupled to a filter positioned in the sensor's field of view that may be capable of passing only radiation having a desired range of wavelengths; a mirror, which may be parabolic or approximately parabolic in shape and may include surfaces and curvatures based on elliptic paraboloids, the sensor being positioned at or near a focal point of the mirror and the filter being positioned between the sensor and the mirror; and an aperture that is outside the sensor's direct field of view, the mirror providing a radiation path between the filter and the aperture.
  • the senor may be included as a component on a semiconductor device that possesses various additional functionalities as will be understood by those having ordinary skill in the art. Additionally, in various embodiments, the center of the sensor surface may be positioned at or near the focal point of the mirror and the surface of the sensor may be oriented at various angles with respect to the baseline of the mirror to further minimize the amount of stray radiation reaching the sensor, which may be determined or understood as a percentage of total radiation. In various embodiments, the angle between the baseline of the mirror and the normal to the surface of the mirror is between approximately 25° and 35°. In other embodiments, this angle is approximately 31.5°. In various embodiments the aperture may include, be covered by, or have disposed adjacent thereto a protective window and/or filter that can prevent radiation of certain undesired wavelengths from passing therethrough.
  • FIG. 1 is a cross-sectional view of an IR thermometer according to an embodiment of the present invention
  • FIG. 2 is a cross-sectional view of an IR thermometer according to an embodiment of the present invention.
  • FIG. 3 is a cross-sectional view of an IR thermometer according to an embodiment of the present invention.
  • FIG. 4 is a cross-sectional view of an IR thermometer according to an embodiment of the present invention.
  • FIG. 5 is a cross-sectional view of an IR thermometer according to an embodiment of the present invention.
  • FIG. 6 is a cross-sectional view of an IR thermometer according to an embodiment of the present invention.
  • FIG. 7 is a cross-sectional view of an IR thermometer according to an embodiment of the present invention.
  • a remote IR thermometer includes, among other things, a parabolic or approximately parabolic mirror and an IR radiation sensor assembly including a filter component and a sensor component.
  • the sensor component includes a surface with a geometric center point on the surface that is positioned in the vicinity of the mirror's focal point.
  • the sensor component may be oriented about the center point at various angles.
  • FIG. 1 shows a schematic, cross-sectional view of an embodiment of the mirror 20 and sensor assembly 30 inside a remote IR thermometer 10 having a radiation entrance, e.g., aperture 16 that may include, be covered by, or have disposed adjacent thereto a protective window and/or filter 55 .
  • Mirror 20 may be parabolic or approximately parabolic in shape so as to define a focal point 50 near to or along the axis of symmetry 52 , as defined by the mirror's parabolic or approximately parabolic curvature 58 , which is perpendicular to the mirror's baseline 54 , the baseline being a line tangent to the mirror at the base or vertex of the mirror (or the parabolic or approximately parabolic shape thereof).
  • a may be approximately between, e.g., 0.01 and 2.0, or approximately between 0.07 and 0.09, and more particularly, approximately 0.5, 0.08, or 0.0799.
  • b may be approximately between, e.g., ⁇ 2.0 and 2.0, or approximately between ⁇ 0.02 and ⁇ 0.01, and more particularly approximately 1.0, ⁇ 0.02, or ⁇ 0.015.
  • a and b are chosen such that the corresponding focal point may be located on the axis of symmetry, at various positions above the corresponding vertex.
  • axis of symmetry 52 is nominally perpendicular to aperture 16 .
  • axis of symmetry 52 may pass through a lower portion of aperture 16 . In other embodiments, axis of symmetry 52 may pass below aperture 16 .
  • the mirror surface is defined by sweeping or rotating any of the parabolas heretofore described about the axis of symmetry 52 .
  • the mirror may also include curvatures and surfaces that may be described by the equation for an elliptic paraboloid, i.e.,
  • Sensor assembly 30 includes at least a sensor component 32 that includes a detection surface 42 with a geometric center point 44 thereon that is positioned in the vicinity of the mirror's focal point 50 . As shown in FIG. 1 , center point 44 is disposed at focal point 50 .
  • Surface 42 may be oriented at various angles a (formed between the normal to surface 42 and baseline 54 of the mirror) so that surface 42 faces at least a portion of mirror 20 .
  • sensor assembly 30 may also include a filter component 40 adjacent to or abutting sensor component 32 . When a sensor assembly 30 including a filter component 40 is used in IR thermometer 10 , filter component 40 may be disposed between sensor component 32 and mirror 20 .
  • mirror 20 is disposed inside thermometer 10 such that aperture 16 is in the line of sight of mirror 20 . So disposed, mirror 20 may reflect radiation toward sensor assembly 30 that was emitted from a portion of an object 14 in the field of view of aperture 16 and passed through aperture 16 and protective window and/or filter 55 .
  • the amount of radiation incident upon mirror 20 that is directed onto surface 42 is a function of the angle ⁇ .
  • surface 42 may be oriented so that a is between approximately 25° and approximately 35°.
  • a may be set at approximately 31.5°.
  • sensor component 32 primarily receives radiation that approaches mirror 20 at a angles of less than approximately five degrees above or below a line parallel to axis of symmetry 52 .
  • Such a range of angles may be referred to as a radiation range of angles.
  • sensor component 32 receives only a minimal or negligible portion of the radiation that approaches mirror 20 at a radiation range of angles greater than approximately six degrees above or below a line parallel to the axis of symmetry 52 because, given the mirror's shape and the size of surface 42 , radiation oriented at these larger angles is not reflected by the mirror along a path that intersects with or reaches surface 42 .
  • FIG. 2 depicts radiation that is directed toward mirror 20 in a direction parallel to axis of symmetry 52 . The mirror reflects most or all of this radiation, which then passes through filter component 40 to strike sensor surface 42 near to center point 44 .
  • FIG. 3 depicts radiation that is directed approximately five degrees above a line parallel to axis of symmetry 52 .
  • the mirror reflects this radiation, which then passes through filter component 40 to strike surface 42 near to the right edge of sensor component 32 .
  • FIG. 4 depicts radiation that is directed approximately five degrees below a line parallel to axis of symmetry 52 .
  • the mirror reflects this radiation, which then passes through filter component 40 to strike sensor surface 42 near to the left edge of sensor component 32 .
  • FIG. 5 depicts radiation that is directed approximately six degrees above a line parallel to axis of symmetry 52
  • FIG. 6 depicts radiation that is directed approximately six degrees below a line parallel to axis of symmetry 52 .
  • the mirror reflects the radiation, which then passes through filter component 40 ; however, the reflected radiation does not strike sensor component 32 , falling too far to the right ( FIG. 5 ) or too far to the left ( FIG. 6 ).
  • FIG. 7 depicts radiation that is directed approximately 12 degrees below a line parallel to axis of symmetry 52 , which more clearly show that the reflected radiation does not strike sensor component 32 . Accordingly, by selectively positioning the mirror in these and other embodiments, undesired radiation that does not emanate from a portion of a surface disposed in front of aperture 16 , such that this radiation is oriented outside of a desired radiation range of angles, may be diverted away from sensor component 32 .
  • sensor component 32 does not detect this undesired radiation.
  • sensor component 32 can detect desired radiation emanating from a portion of a surface disposed in front of aperture 16 because this radiation is oriented inside the desired radiation range of angles and reaches sensor component 32 . In this way, stray radiation emanating from objects other than the intended object can be prevented from reaching the sensor and being detected.
  • filter component 40 may be an infrared band-pass type filter made of silicon that allows radiation having wavelengths between approximately, e.g., 7.5 ⁇ m and 13.5 ⁇ m to reach surface 44 .
  • a filter prevents, e.g., visible light and far infrared light from reaching the sensor and affecting the sensor's output.
  • a filter may be used to reduce the intensity of the radiation in the range of desired wavelengths, e.g., IR radiation, that reaches the sensor, which may improve the accuracy and the repeatability of the sensor.
  • the intensity of the radiation passing the filter and reaching the sensor is one-seventh of the radiation that reflects from the mirror and reaches the filter.
  • a non-limiting example of a sensor that may be used in various embodiments described herein is Part No. TPiS 1T 1252, manufactured by Excelitas Technologies Corp.

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  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Spectroscopy & Molecular Physics (AREA)
  • Radiation Pyrometers (AREA)
  • Measuring And Recording Apparatus For Diagnosis (AREA)
US14/082,321 2012-11-19 2013-11-18 Medical thermometer having an improved optics system Abandoned US20140140370A1 (en)

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US14/082,321 US20140140370A1 (en) 2012-11-19 2013-11-18 Medical thermometer having an improved optics system
US15/642,438 US20170307445A1 (en) 2012-11-19 2017-07-06 Medical thermometer having an improved optics system
US15/869,259 US10054490B2 (en) 2012-11-19 2018-01-12 Medical thermometer having an improved optics system

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US201261728003P 2012-11-19 2012-11-19
US14/082,321 US20140140370A1 (en) 2012-11-19 2013-11-18 Medical thermometer having an improved optics system

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Cited By (1)

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WO2022040616A1 (en) * 2020-08-21 2022-02-24 Symptomsense, Llc Temperature sensor systems and methods for remotely measuring temperature using an optical element

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GB2532745B (en) * 2014-11-25 2017-11-22 Inova Design Solution Ltd Portable physiology monitor
FR3059824B1 (fr) * 2016-12-07 2019-06-21 Ulis Capteur d'image infrarouge

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KR101903510B1 (ko) 2018-10-04
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US20170307445A1 (en) 2017-10-26
CN105051507B (zh) 2018-02-16
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US20180136046A1 (en) 2018-05-17
TW201423067A (zh) 2014-06-16
JP6473196B2 (ja) 2019-02-20
CA2891901A1 (en) 2014-06-12
WO2014087253A3 (en) 2014-11-06
EP2920563B1 (en) 2019-12-25
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US10054490B2 (en) 2018-08-21
MX352070B (es) 2017-11-07
JP2017201328A (ja) 2017-11-09
MX2015006246A (es) 2015-12-09
CN105051507A (zh) 2015-11-11
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KR20160031995A (ko) 2016-03-23
CA2891901C (en) 2018-09-11

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Owner name: HELEN OF TROY LIMITED, BARBADOS

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Effective date: 20131101

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