[go: up one dir, main page]

WO2019167485A1 - Particle detecting sensor - Google Patents

Particle detecting sensor Download PDF

Info

Publication number
WO2019167485A1
WO2019167485A1 PCT/JP2019/002077 JP2019002077W WO2019167485A1 WO 2019167485 A1 WO2019167485 A1 WO 2019167485A1 JP 2019002077 W JP2019002077 W JP 2019002077W WO 2019167485 A1 WO2019167485 A1 WO 2019167485A1
Authority
WO
WIPO (PCT)
Prior art keywords
particles
particle
mass concentration
light
detection sensor
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Ceased
Application number
PCT/JP2019/002077
Other languages
French (fr)
Japanese (ja)
Inventor
吉祥 永谷
貴司 中川
則之 安池
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Panasonic Intellectual Property Management Co Ltd
Original Assignee
Panasonic Intellectual Property Management Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Panasonic Intellectual Property Management Co Ltd filed Critical Panasonic Intellectual Property Management Co Ltd
Priority to CN201980009433.4A priority Critical patent/CN111630365B/en
Priority to KR1020207021262A priority patent/KR102321560B1/en
Priority to JP2020502864A priority patent/JP6883770B2/en
Publication of WO2019167485A1 publication Critical patent/WO2019167485A1/en
Anticipated expiration legal-status Critical
Ceased legal-status Critical Current

Links

Images

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N15/00Investigating characteristics of particles; Investigating permeability, pore-volume or surface-area of porous materials
    • G01N15/02Investigating particle size or size distribution
    • G01N15/0205Investigating particle size or size distribution by optical means
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N15/00Investigating characteristics of particles; Investigating permeability, pore-volume or surface-area of porous materials
    • G01N15/02Investigating particle size or size distribution
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N15/00Investigating characteristics of particles; Investigating permeability, pore-volume or surface-area of porous materials
    • G01N15/06Investigating concentration of particle suspensions
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N21/00Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
    • G01N21/17Systems in which incident light is modified in accordance with the properties of the material investigated
    • G01N21/47Scattering, i.e. diffuse reflection
    • G01N21/49Scattering, i.e. diffuse reflection within a body or fluid
    • G01N21/51Scattering, i.e. diffuse reflection within a body or fluid inside a container, e.g. in an ampoule
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N21/00Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
    • G01N21/17Systems in which incident light is modified in accordance with the properties of the material investigated
    • G01N21/47Scattering, i.e. diffuse reflection
    • G01N21/49Scattering, i.e. diffuse reflection within a body or fluid
    • G01N21/53Scattering, i.e. diffuse reflection within a body or fluid within a flowing fluid, e.g. smoke

Definitions

  • the present invention relates to a particle detection sensor.
  • a photoelectric particle detection sensor that includes a light projecting element and a light receiving element, detects particles floating in the air, and calculates the particle size of the detected particles is known (see, for example, Patent Document 1). ).
  • the mass concentration for each particle size classification can be calculated from the particle size and the number of particles. At this time, in order to calculate the mass concentration with sufficient accuracy, a certain number of particles or more must be acquired. However, in general, as the particle size increases, the number of particles floating in the atmosphere decreases. For this reason, there exists a problem that the measurement precision of the mass concentration of a large particle size division deteriorates.
  • an object of the present invention is to provide a particle detection sensor that can accurately measure the mass concentration of a plurality of particle size categories.
  • a particle detection sensor is a particle detection sensor that detects particles contained in a target fluid, and a light projecting unit that emits light toward a detection region; A light receiving unit that has light receiving sensitivity with respect to light emitted from the light projecting unit, and generates and outputs an electric signal by photoelectrically converting the scattered light of the light from the particles passing through the detection region; and the electric signal The first mass concentration of the first particle size segment containing the first particles, and the second mass concentration of the second particle size segment containing the first particles and second particles larger than the first particles, And a correction circuit that estimates the number of the second particles based on the number of the first particles and corrects the second mass concentration based on the estimated number of particles. .
  • the particle detection sensor according to the present invention can accurately measure the mass concentration of a plurality of particle size categories.
  • FIG. 1 is a perspective view of a particle detection sensor according to an embodiment.
  • FIG. 2 is a cross-sectional view of the particle detection sensor according to the embodiment.
  • FIG. 3 is an enlarged cross-sectional view for explaining the operation of the particle detection sensor according to the embodiment.
  • FIG. 4 is a diagram illustrating an example of a signal processing circuit of the particle detection sensor according to the embodiment.
  • FIG. 5 is a diagram illustrating an electric signal output from the light receiving element of the particle detection sensor according to the embodiment, and a signal during a period in which the number of fine particles is measured.
  • FIG. 6 is a diagram illustrating an electric signal output from the light receiving element of the particle detection sensor according to the embodiment and a signal during a period in which the number of coarse particles is measured.
  • FIG. 1 is a perspective view of a particle detection sensor according to an embodiment.
  • FIG. 2 is a cross-sectional view of the particle detection sensor according to the embodiment.
  • FIG. 3 is an enlarged cross-sectional view for explaining
  • FIG. 7 is a histogram of particles detected by the particle detection sensor according to the embodiment.
  • FIG. 8 is a diagram showing the concentration distribution of each particle size of PM2.5 and PM10.
  • FIG. 9 is a diagram illustrating an example of adjusting the measurement period of the number of coarse particles as a first example of the operation of the particle detection sensor according to the embodiment.
  • FIG. 10 is a diagram illustrating an example of adjusting the number of cycles for averaging in the calculation of the mass concentration as a second example of the operation of the particle detection sensor according to the embodiment.
  • FIG. 11 is a diagram illustrating an adjustment example of the guidance amount of the target fluid as a third example of the operation of the particle detection sensor according to the embodiment.
  • FIG. 1 is a perspective view of a particle detection sensor 1 according to the present embodiment.
  • FIG. 2 is a cross-sectional view of the particle detection sensor 1 according to the present embodiment. Specifically, FIG. 2 shows a cross section parallel to the XY plane at the approximate center in the Z-axis direction of the housing 10 of the particle detection sensor 1.
  • FIG. 3 is an enlarged cross-sectional view for explaining the operation of the particle detection sensor 1 according to the present embodiment. Specifically, FIG. 3 shows an enlarged portion including the detection area DA in the cross section shown in FIG.
  • the X axis, the Y axis, and the Z axis indicate the three axes of the three-dimensional orthogonal coordinate system.
  • the X-axis direction and the Y-axis direction are directions along two sides of the casing 10 having a substantially flat rectangular parallelepiped shape.
  • the Z-axis direction corresponds to the thickness direction of the housing 10.
  • the particle detection sensor 1 is a photoelectric particle detection sensor that detects a plurality of particles P contained in a target fluid.
  • the target fluid is a gas such as air (atmosphere).
  • the particles P are micrometer-order fine particles floating in a gas, that is, particulate matter (aerosol).
  • the particles P are PM2.5, suspended particulate matter (SPM: Suspended ⁇ ⁇ Particulate Matter), PM10, and the like.
  • the particle detection sensor 1 includes a housing 10. As shown in FIG. 2, the particle detection sensor 1 includes a light projecting unit 20, a light receiving unit 30, a guidance device 40, a signal processing circuit 50, and a correction circuit 60.
  • the signal processing circuit 50 and the correction circuit 60 do not appear in the cross section shown in FIG. 2, the signal processing circuit 50 and the correction circuit 60 are schematically shown in FIG.
  • the signal processing circuit 50 and the correction circuit 60 are attached to, for example, the outer surface of the housing 10 and the surface opposite to the surface on which the inflow port 11 and the outflow port 12 are provided.
  • the housing 10 accommodates the light projecting unit 20 and the light receiving unit 30 and has a detection area DA therein.
  • the housing 10 forms a gas flow path including a plurality of particles P.
  • the detection area DA is located on the gas flow path.
  • the housing 10 has an inflow port 11 through which a gas flows in and an outflow port 12 through which the gas that flows in flows out.
  • the path from the inlet 11 to the outlet 12 inside the housing 10 corresponds to a gas flow path.
  • FIG. 2 shows an example in which the gas flow path is formed in an L shape, the gas flow path may be formed in a straight line connecting the inlet 11 and the outlet 12. .
  • the housing 10 has, for example, light shielding properties, and suppresses external light that causes noise from entering the light receiving unit 30 and the detection area DA.
  • the housing 10 is formed by injection molding using, for example, a black resin material.
  • the housing 10 is configured by combining a plurality of parts formed by injection molding.
  • the light projecting unit 20 and the light receiving unit 30 are sandwiched between the plurality of components and fixed at predetermined positions in the housing 10.
  • An optical trap structure that attenuates stray light by multiple reflection may be provided inside the housing 10.
  • the stray light is light other than the light L1 emitted from the light projecting unit 20 (see FIG. 3) that is not scattered by the particles P passing through the detection area DA, that is, the scattered light L2 (see FIG. 3). Light.
  • the light trap structure can also attenuate external light incident on the inside from the inlet 11 or the outlet 12.
  • the light projecting unit 20 emits light L1 toward the detection area DA. As shown in FIGS. 2 and 3, the light projecting unit 20 includes a light projecting element 21 and a lens 22.
  • the light projecting element 21 is, for example, a solid light emitting element, and specifically a laser element such as a semiconductor laser.
  • the light projecting element 21 may be a light emitting diode (LED: Light Emitting Diode) or an organic EL (Electroluminescence) element.
  • the light L1 emitted from the light projecting element 21 is light having a peak at a predetermined wavelength such as infrared light, ultraviolet light, blue light, green light, or red light.
  • the half width at the peak of the light L1 may be a narrow band such as 50 nm or less.
  • the light L1 is continuous light or pulsed light by DC driving, but is not limited thereto.
  • the lens 22 is disposed between the light projecting element 21 and the detection area DA.
  • the lens 22 is, for example, a condensing lens, and efficiently condenses the light L1 emitted from the light projecting element 21 in the detection area DA.
  • the light receiving unit 30 has light receiving sensitivity with respect to the light emitted from the light projecting unit 20, and generates and outputs an electrical signal by photoelectrically converting the scattered light L2 of the light L1 from the particles P passing through the detection area DA. To do. As shown in FIGS. 2 and 3, the light receiving unit 30 includes a light receiving element 31 and a lens 32.
  • the light receiving element 31 is a photoelectric conversion element that converts received light into an electrical signal, such as a photodiode, a phototransistor, or a photomultiplier tube.
  • the light receiving element 31 outputs an electrical signal corresponding to the received light intensity of the received light.
  • the light receiving element 31 has sensitivity in the wavelength band of the light L1 emitted from the light projecting element 21.
  • the light receiving element 31 is disposed at a position where the direct light of the light L1 emitted from the light projecting element 21 does not enter. Specifically, the light receiving element 31 is disposed at a position that does not overlap the optical axis of the light projecting element 21.
  • the optical axis of the light projecting element 21 corresponds to the path of light having the highest intensity among the light L1 emitted from the light projecting element 21. Specifically, the optical axis of the light projecting element 21 corresponds to a straight line connecting the light projecting element 21 and the detection area DA.
  • the light receiving element 31 is arranged so that the optical axis of the light receiving element 31 intersects the optical axis of the light projecting element 21 in the detection area DA.
  • the lens 32 is disposed between the light receiving element 31 and the detection area DA.
  • the lens 32 efficiently collects the scattered light L2 scattered by the particles P in the detection area DA on the light receiving element 31.
  • the guiding device 40 is a device that guides the target fluid toward the detection area DA.
  • the guidance device 40 is a blower mechanism that generates an airflow that passes through the detection area DA.
  • the induction device 40 is, for example, a heating element such as a heater, and generates an upward airflow due to heat generation.
  • the particle detection sensor 1 is arranged so that the positive direction of the Y axis shown in FIGS. 1 and 2 is vertically upward and the negative direction of the Y axis is vertically downward. Is used.
  • the guiding device 40 may be a small fan or the like.
  • the guide device 40 is disposed inside the housing 10, but may be disposed outside the housing 10.
  • the signal processing circuit 50 calculates the mass concentration for each particle size category based on the electrical signal output from the light receiving unit 30. Specifically, the signal processing circuit 50 includes, based on the electrical signal, the first mass concentration of the first particle size section including the first particles, the first particles, and the second particles larger than the first particles. And the second mass concentration of the second particle size classification.
  • the first particles are specifically fine particles, and are particles having a particle size of, for example, 2.5 ⁇ m or less.
  • the first particle size division is a small particle size division such as PM2.5, for example, and the first mass concentration is the mass concentration of PM2.5.
  • the second particles are coarse particles having a particle size larger than that of the fine particles, and the particle size is, for example, 10 ⁇ m or less.
  • the second particle size classification is a large particle size classification such as PM10, and the second mass concentration is the mass concentration of PM10.
  • the second particle size classification may be SPM, and the second mass concentration may be the mass concentration of SPM.
  • the signal processing circuit 50 measures the number of particles and the particle size based on the magnitude of the peak value of the electrical signal output from the light receiving unit 30, and calculates the mass concentration for each particle size category based on the measurement result. Specifically, the signal processing circuit 50 estimates the particle size of the detected particle by comparing the peak value of the electrical signal with one or more threshold values that are predetermined to correspond to the particle size. .
  • the signal processing circuit 50 calculates the mass concentration of PM2.5 based on the first signal for the first period of the electrical signal, and the second signal for the second period of the electrical signal. Based on the above, the mass concentration of PM10 is calculated.
  • the first period is, for example, a measurement period of the number of fine particles included in PM2.5 (hereinafter referred to as PM2.5 particle number).
  • the second period is a period different from the first period, for example, a measurement period of the number of coarse particles contained in PM10 (hereinafter referred to as PM10 particle number).
  • the particle detection sensor 1 in the particle detection sensor 1 according to the present embodiment, measurement of the number of PM2.5 particles and measurement of the number of PM10 particles are performed in a time division manner. Specifically, the signal processing circuit 50 measures the number of particles for each particle size category by dividing and calculating the electric signal output from the light receiving unit 30 at predetermined intervals.
  • the signal processing circuit 50 varies the amplification factor (gain) of the electric signal output from the light receiving element 31 according to the particle size classification of the measurement target.
  • the signal processing circuit 50 includes two amplifiers 51 and 52 and a switch 53.
  • FIG. 4 is a diagram showing a configuration of the signal processing circuit 50 according to the present embodiment. As shown in FIG. 4, the signal processing circuit 50 further includes three resistors 54 to 56 and an arithmetic circuit 57. The signal processing circuit 50 has a multistage configuration of two amplifiers 51.
  • Each of the amplifiers 51 and 52 is, for example, an operational amplifier.
  • the light receiving element 31 is connected between the positive input terminal and the negative input terminal of the amplifier 51.
  • the output terminal of the amplifier 51 is connected to the negative input terminal via the resistor 54.
  • the output terminal of the amplifier 51 is further connected to the positive input terminal of the amplifier 52.
  • the negative input terminal of the amplifier 52 is grounded via a resistor 55.
  • the output terminal of the amplifier 52 is connected to the negative input terminal via the resistor 56.
  • the output terminal of the amplifier 52 is connected to the arithmetic circuit 57.
  • the switch 53 is provided in parallel with the resistor 56, that is, between the output terminal and the negative input terminal of the amplifier 52. By making the switch 53 conductive (ON), the output terminal and the negative input terminal of the amplifier 52 are short-circuited, so that amplification by the amplifier 52 is not performed. When the switch 53 is turned on, amplification by only the amplifier 51 is performed. In this way, the amplification factor of the electric signal can be varied by turning on / off the switch 53.
  • the signal processing circuit 50 increases the amplification factor by turning off the switch 53 in the first period in which the number of PM2.5 particles is measured.
  • Vout when the switch 53 is turned off is expressed by the following equation (1).
  • Vout Z 1 ⁇ (1 + Z 3 / Z 2 ) ⁇ I
  • Z 1 to Z 3 are resistance values of the resistors 54 to 56, respectively.
  • the amplification factor is represented by Z 1 ⁇ (1 + Z 3 / Z 2 ).
  • the scattered light L2 due to the particles becomes weak. For this reason, the photocurrent output from the light receiving element 31 is reduced. Therefore, the voltage of the output signal can be increased by turning off the switch 53 and increasing the amplification factor. Thereby, the comparison between the peak value and the threshold value is facilitated, and the particle diameter can be estimated with high accuracy.
  • the signal processing circuit 50 reduces the amplification factor by turning on the switch 53 in the second period in which the number of PM10 particles is measured. Vout when the switch 53 is turned on is expressed by the following equation (2).
  • the switch 53 may be turned on to reduce the amplification factor.
  • the range that Vout can take can be made equal regardless of the size of the particle to be measured. Thereby, it is possible to easily compare the peak value and the threshold value in the arithmetic circuit 57 in the subsequent stage.
  • the arithmetic circuit 57 calculates the particle size of the particles based on the peak maximum value (hereinafter referred to as the peak value) appearing in the electric signal for the first period for measuring the number of PM2.5 particles. Estimate and classify into one of multiple sub-categories.
  • the sub-section of PM2.5 is a plurality of sub-sections in which the particle size section corresponding to PM2.5 is divided by one or more threshold values.
  • FIG. 5 is a diagram showing a first signal in the first period in which the number of PM2.5 particles is measured, which is an electrical signal output from the light receiving element 31 of the particle detection sensor 1 according to the present embodiment.
  • the horizontal axis represents time
  • the vertical axis represents the signal strength of the electric signal.
  • the vertical axis corresponds to the voltage value.
  • PM2.5 is divided into four sub-sections by four threshold values 1 to 4.
  • PM2.5 is, for example, a first subsection of 1.0 ⁇ m or more, a second subsection of less than 1.0 ⁇ m and 0.5 ⁇ m or more, and a third subsection of less than 0.5 ⁇ m and 0.3 ⁇ m or more.
  • a section and a fourth sub-section smaller than 0.3 ⁇ m are included.
  • the threshold value 4 is a threshold value for removing a noise component.
  • FIG. 5 shows an example in which five peaks S1 to S5 appear.
  • Each of the peaks S1 to S5 corresponds to a change in an electric signal that appears when the light receiving element 31 receives scattered light L2 due to particles that have passed through the detection area DA.
  • the arithmetic circuit 57 classifies the particles into any one of the first subsection to the fourth subsection of PM2.5 by comparing each peak value of the peaks S1 to S5 with the threshold value.
  • the particles corresponding to peak S1 are classified into the third sub-section.
  • the particles corresponding to the peak S2 are classified into the fourth subsection.
  • the peak value of the peak S3 is smaller than the threshold value 1 and greater than or equal to the threshold value 2
  • the particles corresponding to the peak S3 are classified into the second sub-section.
  • the peak value of each of the peaks S4 and S5 is greater than or equal to the threshold value 1, particles corresponding to each of the peaks S4 and S5 are classified into the first sub-section.
  • the arithmetic circuit 57 estimates the particle size of the particle based on the peak maximum value (peak value) appearing in the electric signal for the second period in which the number of PM10 particles is measured, Classify either.
  • the sub-section of PM10 is a plurality of sub-sections in which the particle size section corresponding to PM10 is divided by one or more threshold values.
  • FIG. 6 is a diagram illustrating a second signal in the second period in which the number of PM10 particles is measured, which is an electric signal output from the light receiving element 31 of the particle detection sensor 1 according to the present embodiment.
  • the horizontal axis represents time
  • the vertical axis represents the signal strength of the electric signal.
  • the vertical axis corresponds to the voltage value.
  • the PM 10 is divided into four sub-sections by four threshold values A to D.
  • the PM 10 includes, for example, a first subsection smaller than 10 ⁇ m and 5 ⁇ m or more, a second subsection smaller than 5 ⁇ m and 2.5 ⁇ m or more, a third subsection smaller than 2.5 ⁇ m and 1.0 ⁇ m or more, and A fourth subsection smaller than 1.0 ⁇ m is included.
  • FIG. 6 shows an example in which five peaks Sa to Se appear.
  • Each of the peaks Sa to Se corresponds to a change in an electrical signal that appears when the light receiving element 31 receives scattered light L2 due to particles that have passed through the detection area DA.
  • the arithmetic circuit 57 classifies the particles into any one of the first sub-section to the fourth sub-section of the PM 10 by comparing each peak value of the peaks Sa to Se with a threshold value.
  • the specific process is the same as in PM2.5.
  • the number of at least one sub-section of PM2.5 and PM10 is not limited to four, and may be two or three, or five. Alternatively, the number of subsections may be one. That is, at least one of PM2.5 and PM10 may not be divided into a plurality of sub-sections.
  • the particle detection sensor 1 actually includes many particles that pass through a portion other than the center of the detection area DA. For example, when a large particle passes through the end of the detection area DA, the light receiving intensity of the scattered light from the particle by the light receiving element 31 decreases. For this reason, although it is a large particle, the size of the particle may be erroneously determined as “small”.
  • the arithmetic circuit 57 for example, as shown in FIG. 7, a histogram in which signal intensity (voltage value) is associated with the frequency of particles for each particle size. Is stored in memory.
  • FIG. 7 is a histogram of particles detected by the particle detection sensor 1 according to the present embodiment. In FIG. 7, the horizontal axis represents signal intensity, and the vertical axis represents the frequency of particles for each particle size.
  • the arithmetic circuit 57 estimates the size of the particle P corresponding to the peak by referring to the histogram shown in FIG. 7 based on the peak intensity of the electric signal.
  • the arithmetic circuit 57 counts the number of particles P detected during a certain operation period for each sub-section.
  • the arithmetic circuit 57 calculates a product of a predetermined average mass and the counted number for each sub-section, and adds the calculated product for each sub-section, thereby obtaining a mass concentration of PM2.5 and PM10. Each mass concentration is calculated.
  • the arithmetic circuit 57 is realized by one or more electronic components including a comparator, for example.
  • the arithmetic circuit 57 may be realized by an MPU (Micro Processing Unit) or the like.
  • the processing performed by the arithmetic circuit 57 may be realized by hardware or may be realized by software executed by a processor.
  • the correction circuit 60 estimates the number of particles of the second particle included in the second particle size category based on the number of particles of the first particle included in the first particle size category, and the second particle based on the estimated number of particles. Correct the mass concentration of the diameter category. Specifically, the correction circuit 60 estimates the number of coarse particles contained in PM10 based on the number of fine particles contained in PM2.5. The correction circuit 60 corrects the mass concentration of PM10 based on the estimated number of coarse particles.
  • the number of fine particles is the number of particles included in the sub-section having the maximum particle size among the plurality of sub-sections into which PM2.5 is divided.
  • the number of fine particles in the example shown in FIG. 5 is the number of particles included in the fourth subsection having a particle size of 1.0 ⁇ m or more.
  • the correction circuit 60 estimates the number of coarse particles based on the content ratio of the number of particles included in the fourth subsection.
  • the content rate corresponds to the ratio of the number of particles included in the fourth subsection to the total number of particles corresponding to PM2.5.
  • the correction circuit 60 roughly performs two corrections.
  • the two corrections are a first correction for correcting the mass concentration of PM10 calculated by the signal processing circuit 50 and a second correction for adjusting the method for measuring the number of PM10 particles. Details of each correction process will be described later.
  • the correction circuit 60 is realized by one or more electronic components, for example.
  • the correction circuit 60 may be realized by an MPU or the like.
  • the operation performed by the correction circuit 60 may be realized by hardware or may be realized by software executed by a processor.
  • FIG. 8 is a diagram showing the concentration distribution of each particle size of PM2.5 and PM10.
  • the horizontal axis represents the particle size [ ⁇ m]
  • the vertical axis represents the mass concentration.
  • An overlapping part is a part corresponded to the 4th subsection of PM2.5, for example.
  • the correction circuit 60 includes a memory that stores correspondence information indicating a correspondence relationship between the content rate and the number of coarse particles. The correction circuit 60 reads the correspondence information from the memory and refers to the read correspondence information to estimate coarse particles based on the content ratio of the number of fine particles.
  • the correction circuit 60 corrects the mass concentration of PM10 calculated by the arithmetic circuit 57 based on the estimated number of coarse particles. For example, the correction circuit 60 corrects when a difference of a predetermined value or more occurs between the mass concentration based on the estimated number of particles and the mass concentration calculated based on the measurement result of the number of PM10 particles (that is, the actually measured number).
  • the circuit 60 averages the estimation result and the actual measurement result, and outputs the result as a correction value of the mass concentration of PM10.
  • the correction value may not be an average of the estimation result and the actual measurement result, and may be a weighted addition value obtained by strongly weighting the estimation result, for example.
  • correspondence information that associates the estimated number of coarse particles with the correction value of the mass concentration may be stored in the memory.
  • the correction circuit 60 may read out the correspondence information from the memory and refer to the read correspondence information to determine and output a correction value for the mass concentration from the estimated number of particles.
  • the correspondence information can be generated in advance by, for example, obtaining an estimated value based on the number of PM2.5 particles in an environment where the mass concentration of PM10 is known.
  • FIG. 9 is a diagram illustrating an example of adjustment of the measurement period of the number of coarse particles as a first example of correction of the particle detection sensor 1 according to the present embodiment.
  • the correction circuit 60 changes the length of the second period, which is the measurement period of the number of PM10 particles, based on the estimated number of coarse particles.
  • the measurement of the number of fine particles, the measurement of the number of coarse particles, the calculation of the mass concentration of PM2.5, and the PM10 The calculation of the mass concentration is performed in this order.
  • Measurement of the number of fine particles corresponds to the first period for calculating the mass concentration of PM2.5.
  • Measurement of the number of coarse particles corresponds to a second period for calculating the mass concentration of PM10.
  • the correction circuit 60 makes the second period longer when the estimated number of particles is smaller than when the estimated number of particles is large. This makes it easy to secure a certain number or more of coarse particles to be detected (detection number), so that the number of coarse particles can be measured with high accuracy, and the mass concentration of PM10 can be calculated with high accuracy. .
  • the estimated number of particles when the estimated number of particles is large, it is possible to ensure a detection number of coarse particles of a certain number or more without lengthening the second period. Therefore, the number of coarse particles can be measured with high accuracy, and the mass concentration of PM10 can be calculated with high accuracy. Moreover, the time required from the measurement of the number of particles to the calculation of the mass concentration can be shortened.
  • FIG. 10 is a diagram showing an example of adjusting the number of cycles for averaging in the calculation of mass concentration as a second example of correction of the particle detection sensor 1 according to the present embodiment.
  • the correction circuit 60 changes the number of averaging cycles when calculating the mass concentration of PM10 based on the estimated number of coarse particles.
  • the measurement of the number of fine particles, the measurement of the number of coarse particles, the calculation of the mass concentration of PM2.5, and the PM10 is one cycle, and this cycle is repeated a plurality of times.
  • the mass concentration is calculated by averaging the mass concentration calculated for each cycle for a plurality of times.
  • the arithmetic circuit 57 repeats the process of calculating the mass concentration of PM10 a predetermined number of times based on the electrical signal (second signal) obtained during the measurement period of the coarse particles, and the obtained mass for the predetermined number of times. By averaging the concentration, the mass concentration of PM10 is calculated.
  • the correction circuit 60 changes the number of cycles that is the number of times of averaging.
  • the correction circuit 60 increases the number of cycles when the estimated number of particles is small than when the estimated number of particles is large.
  • FIG. 10 shows an example in which the number of cycles is 3 when the estimated number of particles is large, whereas the number of cycles is 6 when the estimated number of particles is small. Yes. Note that specific numerical examples of the number of cycles are not limited to these.
  • the calculation circuit 57 is the same for the mass concentration of PM2.5.
  • the number of cycles for averaging may be the same or different between PM2.5 and PM10.
  • the number of cycles in the case of PM2.5 may always be constant regardless of the estimated number of particles.
  • FIG. 11 is a diagram illustrating an adjustment example of the guidance amount of the target fluid as a third example of the correction of the particle detection sensor 1 according to the present embodiment.
  • the correction circuit 60 changes the guidance amount of the target fluid that is guided by the guidance device 40 within the second period, which is the coarse particle measurement period.
  • the guidance device 40 is a blower mechanism for taking gas into the housing 10.
  • the correction circuit 60 changes the intake air amount as the induction amount.
  • the correction circuit 60 adjusts the amount of heat generated by adjusting the current flowing through the resistance element.
  • the correction circuit 60 can increase the amount of intake air by increasing the amount of heat generated by increasing the amount of heat generated by flowing a large amount of current.
  • the correction circuit 60 increases the intake amount when the estimated number of particles is small than when the estimated number of particles is large. Thereby, since the quantity of the gas taken in by one measurement increases, the number of particles contained in gas can also be increased. Therefore, it is possible to secure a detection number of coarse particles of a certain number or more. Therefore, the number of coarse particles can be measured with high accuracy, and the mass concentration of PM10 can be calculated with high accuracy.
  • the particle detection sensor 1 is a particle detection sensor that detects particles contained in a target fluid, and includes a light projecting unit 20 that emits light toward the detection area DA, and a light projecting unit.
  • a light receiving unit 30 that has light receiving sensitivity with respect to the light L1 emitted from the light unit 20, and that generates and outputs an electrical signal by photoelectrically converting the scattered light L2 of the light passing through the detection area DA.
  • the particle detection sensor 1 further includes a first mass concentration (for example, a mass concentration of PM2.5) of the first particle size classification in which the fine particles are included based on the electrical signal, the fine particles and the coarser than the fine particles.
  • the signal processing circuit 50 that calculates the second mass concentration (for example, the mass concentration of PM10) of the second particle size classification in which the particles are included, and the number of coarse particles are estimated based on the number of fine particles, and estimated And a correction circuit 60 for correcting the second mass concentration based on the number of particles obtained.
  • the second mass concentration for example, the mass concentration of PM10
  • the number of fine particles is the number of particles included in the sub-section having the maximum particle size among the plurality of sub-sections obtained by dividing the first particle size section.
  • the correction circuit 60 estimates the number of coarse particles based on the content of the number of fine particles.
  • the particles of coarse particles are based on the correlation.
  • the number can be estimated with high accuracy. Since the estimation accuracy of the number of coarse particles is increased, the measurement accuracy of the mass concentration of PM10 is also increased. Therefore, not only PM2.5 but also the mass concentration of PM10 can be accurately measured.
  • the signal processing circuit 50 calculates the mass concentration of PM2.5 based on the first signal for the first period of the electric signal, and for the second period different from the first period of the electric signal. Based on the second signal, the mass concentration of PM10 is calculated.
  • the mass concentration of PM2.5 and the mass concentration of PM10 can be calculated in time series. Since the actual measurement value of the mass concentration of PM10 is obtained, the accuracy of correction is improved. Therefore, not only PM2.5 but also the mass concentration of PM10 can be accurately measured.
  • the correction circuit 60 corrects the mass concentration of PM10 calculated based on the second signal based on the estimated number of particles as correction.
  • the correction circuit 60 changes the length of the coarse particle measurement period based on the estimated number of particles as a correction.
  • the signal processing circuit 50 repeats the process of calculating the mass concentration of PM10 based on the second signal a predetermined number of times, and averages the obtained mass concentration for the predetermined number of times, thereby obtaining the mass concentration of PM10. calculate.
  • the correction circuit 60 changes the number of repetitions (that is, the number of cycles) as correction.
  • the particle detection sensor 1 further includes a guidance device 40 that guides the target fluid toward the detection area DA.
  • the correction circuit 60 changes the induction amount of the target fluid induced by the induction device 40 within the second period as correction.
  • the target fluid may be a liquid such as water.
  • the particle detection sensor 1 detects particles contained in a liquid such as water and calculates a mass concentration.
  • the particle detection sensor 1 has a waterproof mechanism that prevents the signal processing circuit 50 attached to the outer surface of the housing 10 from coming into contact with the liquid.
  • the waterproof mechanism is, for example, a metal shield member provided so as to cover the signal processing circuit 50.
  • the shield member is fixed to the housing 10 without a gap by, for example, welding.
  • the particle detection sensor 1 does not need to measure the number of PM10 particles.
  • the signal processing circuit 50 may perform measurement of fine particles, calculation of the mass concentration of PM2.5, and calculation of the mass concentration of PM10 in this order.
  • the mass concentration of PM10 may be calculated using the number of coarse particles estimated based on the content rate of the number of fine particles contained in PM2.5.
  • the correction circuit 60 may estimate the number of coarse particles based on the total number of fine particles contained in PM2.5 instead of the subclass of the maximum particle size of PM2.5.
  • the particle detection sensor 1 may not include the guidance device 40.
  • the particle detection sensor 1 may be arranged in a place where the airflow is flowing in a certain direction so that the inlet 11 is located upstream of the airflow and the outlet 12 is located downstream.
  • each of the light projecting unit 20 and the light receiving unit 30 includes a lens
  • the present invention is not limited thereto.
  • at least one of the light projecting unit 20 and the light receiving unit 30 may include a mirror (reflector) instead of the lens.
  • grain detection sensor 1 is mounted in various household appliances, such as an air conditioner, an air cleaner, and a ventilation fan, for example.
  • Various home appliances may control the operation according to the mass concentration of the particles detected by the particle detection sensor 1.
  • the air cleaner may increase the operating strength (specifically, the air purifying power) when the mass concentration of the particles is larger than a predetermined threshold.
  • the embodiment can be realized by arbitrarily combining the components and functions in each embodiment without departing from the scope of the present invention, or a form obtained by subjecting each embodiment to various modifications conceived by those skilled in the art. Forms are also included in the present invention.

Landscapes

  • Chemical & Material Sciences (AREA)
  • Physics & Mathematics (AREA)
  • Health & Medical Sciences (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Analytical Chemistry (AREA)
  • Biochemistry (AREA)
  • General Health & Medical Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • Immunology (AREA)
  • Pathology (AREA)
  • Dispersion Chemistry (AREA)
  • Investigating Or Analysing Materials By Optical Means (AREA)

Abstract

This particle detecting sensor (1) detects particles contained in a fluid of interest, and is provided with: a light projecting unit (20) which emits light (L1) toward a detection area (DA); a light receiving unit (30) which has light-receiving sensitivity with respect to the light emitted by the light projecting unit (20), and which generates and outputs an electrical signal by performing photoelectric conversion of scattered light (L2) originating from the light (L1), caused by a particle passing through the detection area (DA); a signal processing circuit (50) which, on the basis of the electrical signal, calculates a first mass concentration of a first particle category including a first particle, and a second mass concentration of a second particle category including the first particle and a second particle larger than the first particle; and a correcting circuit (60) which estimates the number of second particles on the basis of the number of first particles, and corrects the second mass concentration on the basis of the estimated number of particles.

Description

粒子検出センサParticle detection sensor

 本発明は、粒子検出センサに関する。 The present invention relates to a particle detection sensor.

 従来、投光素子と受光素子とを備え、空気中に浮遊する粒子を検出し、検出した粒子の粒径を算出する光電式の粒子検出センサが知られている(例えば、特許文献1を参照)。 Conventionally, a photoelectric particle detection sensor that includes a light projecting element and a light receiving element, detects particles floating in the air, and calculates the particle size of the detected particles is known (see, for example, Patent Document 1). ).

特開2015-210183号公報Japanese Patent Laid-Open No. 2015-210183

 光電式の粒子検出センサでは、粒径と粒子の個数とから粒径区分毎の質量濃度を算出することができる。このとき、質量濃度を十分な精度で算出するためには、一定数以上の粒子数を取得しなければならない。しかしながら、一般的には、粒子径が大きくなるにつれて、大気中に浮遊する粒子の数が少なくなる。このため、大きい粒径区分の質量濃度の計測精度が悪化するという問題がある。 In the photoelectric particle detection sensor, the mass concentration for each particle size classification can be calculated from the particle size and the number of particles. At this time, in order to calculate the mass concentration with sufficient accuracy, a certain number of particles or more must be acquired. However, in general, as the particle size increases, the number of particles floating in the atmosphere decreases. For this reason, there exists a problem that the measurement precision of the mass concentration of a large particle size division deteriorates.

 そこで、本発明は、複数の粒径区分の質量濃度を精度良く計測することができる粒子検出センサを提供することを目的とする。 Therefore, an object of the present invention is to provide a particle detection sensor that can accurately measure the mass concentration of a plurality of particle size categories.

 上記目的を達成するため、本発明の一態様に係る粒子検出センサは、対象流体に含まれる粒子を検出する粒子検出センサであって、検出領域に向けて光を出射する投光部と、前記投光部が出射する光に対して受光感度を有し、前記検出領域を通過する粒子による前記光の散乱光を光電変換することで電気信号を生成して出力する受光部と、前記電気信号に基づいて、第1粒子が含まれる第1粒径区分の第1質量濃度と、前記第1粒子及び当該第1粒子より大きい第2粒子が含まれる第2粒径区分の第2質量濃度とを算出する信号処理回路と、前記第1粒子の粒子数に基づいて前記第2粒子の粒子数を推定し、推定した粒子数に基づいて前記第2質量濃度の補正を行う補正回路とを備える。 In order to achieve the above object, a particle detection sensor according to an aspect of the present invention is a particle detection sensor that detects particles contained in a target fluid, and a light projecting unit that emits light toward a detection region; A light receiving unit that has light receiving sensitivity with respect to light emitted from the light projecting unit, and generates and outputs an electric signal by photoelectrically converting the scattered light of the light from the particles passing through the detection region; and the electric signal The first mass concentration of the first particle size segment containing the first particles, and the second mass concentration of the second particle size segment containing the first particles and second particles larger than the first particles, And a correction circuit that estimates the number of the second particles based on the number of the first particles and corrects the second mass concentration based on the estimated number of particles. .

 本発明に係る粒子検出センサによれば、複数の粒径区分の質量濃度を精度良く計測することができる。 The particle detection sensor according to the present invention can accurately measure the mass concentration of a plurality of particle size categories.

図1は、実施の形態に係る粒子検出センサの斜視図である。FIG. 1 is a perspective view of a particle detection sensor according to an embodiment. 図2は、実施の形態に係る粒子検出センサの断面図である。FIG. 2 is a cross-sectional view of the particle detection sensor according to the embodiment. 図3は、実施の形態に係る粒子検出センサの動作を説明するための拡大断面図である。FIG. 3 is an enlarged cross-sectional view for explaining the operation of the particle detection sensor according to the embodiment. 図4は、実施の形態に係る粒子検出センサの信号処理回路の一例を示す図である。FIG. 4 is a diagram illustrating an example of a signal processing circuit of the particle detection sensor according to the embodiment. 図5は、実施の形態に係る粒子検出センサの受光素子から出力される電気信号であって、微小粒子の粒子数を計測する期間の信号を示す図である。FIG. 5 is a diagram illustrating an electric signal output from the light receiving element of the particle detection sensor according to the embodiment, and a signal during a period in which the number of fine particles is measured. 図6は、実施の形態に係る粒子検出センサの受光素子から出力される電気信号であって、粗大粒子の粒子数を計測する期間の信号を示す図である。FIG. 6 is a diagram illustrating an electric signal output from the light receiving element of the particle detection sensor according to the embodiment and a signal during a period in which the number of coarse particles is measured. 図7は、実施の形態に係る粒子検出センサによって検出された粒子のヒストグラムである。FIG. 7 is a histogram of particles detected by the particle detection sensor according to the embodiment. 図8は、PM2.5及びPM10の各々の粒径に対する濃度分布を示す図である。FIG. 8 is a diagram showing the concentration distribution of each particle size of PM2.5 and PM10. 図9は、実施の形態に係る粒子検出センサの動作の第1例として、粗大粒子の粒子数の計測期間の調整例を示す図である。FIG. 9 is a diagram illustrating an example of adjusting the measurement period of the number of coarse particles as a first example of the operation of the particle detection sensor according to the embodiment. 図10は、実施の形態に係る粒子検出センサの動作の第2例として、質量濃度の演算の際の平均化のサイクル数の調整例を示す図である。FIG. 10 is a diagram illustrating an example of adjusting the number of cycles for averaging in the calculation of the mass concentration as a second example of the operation of the particle detection sensor according to the embodiment. 図11は、実施の形態に係る粒子検出センサの動作の第3例として、対象流体の誘導量の調整例を示す図である。FIG. 11 is a diagram illustrating an adjustment example of the guidance amount of the target fluid as a third example of the operation of the particle detection sensor according to the embodiment.

 以下では、本発明の実施の形態に係る粒子検出センサについて、図面を用いて詳細に説明する。なお、以下に説明する実施の形態は、いずれも本発明の一具体例を示すものである。したがって、以下の実施の形態で示される数値、形状、材料、構成要素、構成要素の配置及び接続形態、ステップ、ステップの順序などは、一例であり、本発明を限定する趣旨ではない。よって、以下の実施の形態における構成要素のうち、独立請求項に記載されていない構成要素については、任意の構成要素として説明される。 Hereinafter, the particle detection sensor according to the embodiment of the present invention will be described in detail with reference to the drawings. Each of the embodiments described below shows a specific example of the present invention. Therefore, numerical values, shapes, materials, components, arrangement and connection forms of components, steps, order of steps, and the like shown in the following embodiments are merely examples, and are not intended to limit the present invention. Therefore, among the constituent elements in the following embodiments, constituent elements not described in the independent claims are described as arbitrary constituent elements.

 また、各図は、模式図であり、必ずしも厳密に図示されたものではない。したがって、例えば、各図において縮尺などは必ずしも一致しない。また、各図において、実質的に同一の構成については同一の符号を付しており、重複する説明は省略又は簡略化する。 Each figure is a schematic diagram and is not necessarily shown strictly. Therefore, for example, the scales and the like do not necessarily match in each drawing. Moreover, in each figure, the same code | symbol is attached | subjected about the substantially same structure, The overlapping description is abbreviate | omitted or simplified.

 (実施の形態)
 [構成]
 まず、実施の形態に係る粒子検出センサ1について、図1~図3を用いて説明する。
(Embodiment)
[Constitution]
First, a particle detection sensor 1 according to an embodiment will be described with reference to FIGS.

 図1は、本実施の形態に係る粒子検出センサ1の斜視図である。図2は、本実施の形態に係る粒子検出センサ1の断面図である。具体的には、図2は、粒子検出センサ1の筐体10のZ軸方向における略中央におけるXY面に平行な断面を示している。図3は、本実施の形態に係る粒子検出センサ1の動作を説明するための拡大断面図である。具体的には、図3は、図2に示す断面において、検出領域DAを含む部分を拡大して示している。 FIG. 1 is a perspective view of a particle detection sensor 1 according to the present embodiment. FIG. 2 is a cross-sectional view of the particle detection sensor 1 according to the present embodiment. Specifically, FIG. 2 shows a cross section parallel to the XY plane at the approximate center in the Z-axis direction of the housing 10 of the particle detection sensor 1. FIG. 3 is an enlarged cross-sectional view for explaining the operation of the particle detection sensor 1 according to the present embodiment. Specifically, FIG. 3 shows an enlarged portion including the detection area DA in the cross section shown in FIG.

 なお、X軸、Y軸及びZ軸は、三次元直交座標系の三軸を示している。X軸方向及びY軸方向は、略扁平な直方体形状を有する筐体10の2つの辺に沿った方向である。Z軸方向は、筐体10の厚み方向に相当する。 In addition, the X axis, the Y axis, and the Z axis indicate the three axes of the three-dimensional orthogonal coordinate system. The X-axis direction and the Y-axis direction are directions along two sides of the casing 10 having a substantially flat rectangular parallelepiped shape. The Z-axis direction corresponds to the thickness direction of the housing 10.

 粒子検出センサ1は、対象流体に含まれる複数の粒子Pを検出する光電式の粒子検出センサである。本実施の形態では、対象流体は、例えば空気(大気)などの気体である。粒子Pは、気体中を浮遊するマイクロメートルオーダーの微粒子、すなわち、粒子状物質(エアロゾル)である。具体的には、粒子Pは、PM2.5、浮遊粒子状物質(SPM:Suspended Particulate Matter)、PM10などである。 The particle detection sensor 1 is a photoelectric particle detection sensor that detects a plurality of particles P contained in a target fluid. In the present embodiment, the target fluid is a gas such as air (atmosphere). The particles P are micrometer-order fine particles floating in a gas, that is, particulate matter (aerosol). Specifically, the particles P are PM2.5, suspended particulate matter (SPM: Suspended な ど Particulate Matter), PM10, and the like.

 図1に示されるように、粒子検出センサ1は、筐体10を備える。図2に示されるように、粒子検出センサ1は、投光部20と、受光部30と、誘導装置40と、信号処理回路50と、補正回路60とを備える。 As shown in FIG. 1, the particle detection sensor 1 includes a housing 10. As shown in FIG. 2, the particle detection sensor 1 includes a light projecting unit 20, a light receiving unit 30, a guidance device 40, a signal processing circuit 50, and a correction circuit 60.

 なお、図2に示す断面には、信号処理回路50及び補正回路60が現れていないので、図2では、信号処理回路50及び補正回路60を模式的に表している。信号処理回路50及び補正回路60は、例えば、筐体10の外側面であって、流入口11及び流出口12が設けられた面とは反対側の面などに取り付けられている。 Since the signal processing circuit 50 and the correction circuit 60 do not appear in the cross section shown in FIG. 2, the signal processing circuit 50 and the correction circuit 60 are schematically shown in FIG. The signal processing circuit 50 and the correction circuit 60 are attached to, for example, the outer surface of the housing 10 and the surface opposite to the surface on which the inflow port 11 and the outflow port 12 are provided.

 筐体10は、投光部20及び受光部30を収納し、内部に検出領域DAを有する。筐体10は、複数の粒子Pを含む気体の流路を形成している。検出領域DAは、気体の流路上に位置している。 The housing 10 accommodates the light projecting unit 20 and the light receiving unit 30 and has a detection area DA therein. The housing 10 forms a gas flow path including a plurality of particles P. The detection area DA is located on the gas flow path.

 具体的には、筐体10は、図1に示されるように、内部に気体を流入させる流入口11と、流入した気体を外部に流出させる流出口12とを有する。図2の太破線の矢印で示すように、筐体10の内部を、流入口11から流出口12まで至る経路が、気体の流路に相当する。図2には、気体の流路がL字状に形成されている例を示しているが、気体の流路は、流入口11と流出口12とを結ぶ直線状に形成されていてもよい。 Specifically, as shown in FIG. 1, the housing 10 has an inflow port 11 through which a gas flows in and an outflow port 12 through which the gas that flows in flows out. As indicated by the thick broken line arrows in FIG. 2, the path from the inlet 11 to the outlet 12 inside the housing 10 corresponds to a gas flow path. Although FIG. 2 shows an example in which the gas flow path is formed in an L shape, the gas flow path may be formed in a straight line connecting the inlet 11 and the outlet 12. .

 筐体10は、例えば、遮光性を有し、受光部30及び検出領域DAに、ノイズの原因となる外光が入射するのを抑制する。筐体10は、例えば黒色の樹脂材料を用いた射出成形により形成されている。具体的には、筐体10は、射出成形により形成された複数の部品が組み合わされて構成されている。当該複数の部品によって、投光部20及び受光部30が挟まれて筐体10内の所定位置に固定されている。 The housing 10 has, for example, light shielding properties, and suppresses external light that causes noise from entering the light receiving unit 30 and the detection area DA. The housing 10 is formed by injection molding using, for example, a black resin material. Specifically, the housing 10 is configured by combining a plurality of parts formed by injection molding. The light projecting unit 20 and the light receiving unit 30 are sandwiched between the plurality of components and fixed at predetermined positions in the housing 10.

 筐体10の内部には、迷光を多重反射させることにより減衰させる光トラップ構造が設けられていてもよい。迷光は、投光部20から出射された光L1(図3を参照)のうち、検出領域DAを通過中の粒子Pによって散乱されなかった光、すなわち、散乱光L2(図3を参照)以外の光である。光トラップ構造は、流入口11又は流出口12から内部に入射した外光も減衰させることができる。 An optical trap structure that attenuates stray light by multiple reflection may be provided inside the housing 10. The stray light is light other than the light L1 emitted from the light projecting unit 20 (see FIG. 3) that is not scattered by the particles P passing through the detection area DA, that is, the scattered light L2 (see FIG. 3). Light. The light trap structure can also attenuate external light incident on the inside from the inlet 11 or the outlet 12.

 投光部20は、検出領域DAに向けて光L1を出射する。図2及び図3に示されるように、投光部20は、投光素子21と、レンズ22とを備える。 The light projecting unit 20 emits light L1 toward the detection area DA. As shown in FIGS. 2 and 3, the light projecting unit 20 includes a light projecting element 21 and a lens 22.

 投光素子21は、例えば固体発光素子であり、具体的には半導体レーザなどのレーザ素子である。あるいは、投光素子21は、発光ダイオード(LED:Light Emitting Diode)又は有機EL(Electroluminescence)素子などでもよい。 The light projecting element 21 is, for example, a solid light emitting element, and specifically a laser element such as a semiconductor laser. Alternatively, the light projecting element 21 may be a light emitting diode (LED: Light Emitting Diode) or an organic EL (Electroluminescence) element.

 投光素子21が出射する光L1は、赤外光、紫外光、青色光、緑色光又は赤色光などの所定の波長にピークを有する光である。光L1のピークにおける半値幅は、例えば50nm以下などの狭帯域でもよい。また、光L1は、DC駆動による連続光又はパルス光であるが、これらに限られない。 The light L1 emitted from the light projecting element 21 is light having a peak at a predetermined wavelength such as infrared light, ultraviolet light, blue light, green light, or red light. The half width at the peak of the light L1 may be a narrow band such as 50 nm or less. The light L1 is continuous light or pulsed light by DC driving, but is not limited thereto.

 レンズ22は、投光素子21と検出領域DAとの間に配置されている。レンズ22は、例えば集光レンズであり、投光素子21から出射された光L1を効率良く検出領域DAに集光させる。 The lens 22 is disposed between the light projecting element 21 and the detection area DA. The lens 22 is, for example, a condensing lens, and efficiently condenses the light L1 emitted from the light projecting element 21 in the detection area DA.

 受光部30は、投光部20が出射する光に対して受光感度を有し、検出領域DAを通過する粒子Pによる光L1の散乱光L2を光電変換することで電気信号を生成して出力する。図2及び図3に示されるように、受光部30は、受光素子31と、レンズ32とを備える。 The light receiving unit 30 has light receiving sensitivity with respect to the light emitted from the light projecting unit 20, and generates and outputs an electrical signal by photoelectrically converting the scattered light L2 of the light L1 from the particles P passing through the detection area DA. To do. As shown in FIGS. 2 and 3, the light receiving unit 30 includes a light receiving element 31 and a lens 32.

 受光素子31は、例えばフォトダイオード、フォトトランジスタ、又は光電子増倍管などの、受光した光を電気信号に変換する光電変換素子である。受光素子31は、受光した光の受光強度に応じた電気信号を出力する。受光素子31は、投光素子21が出射する光L1の波長帯域に感度を有する。 The light receiving element 31 is a photoelectric conversion element that converts received light into an electrical signal, such as a photodiode, a phototransistor, or a photomultiplier tube. The light receiving element 31 outputs an electrical signal corresponding to the received light intensity of the received light. The light receiving element 31 has sensitivity in the wavelength band of the light L1 emitted from the light projecting element 21.

 受光素子31は、図2に示されるように、投光素子21が出射した光L1の直接光が入射しない位置に配置されている。具体的には、受光素子31は、投光素子21の光軸と重ならない位置に配置されている。なお、投光素子21の光軸は、投光素子21が出射する光L1のうち、強度が最も強い光の経路に相当する。具体的には、投光素子21の光軸は、投光素子21と検出領域DAとを結ぶ直線に相当する。本実施の形態では、受光素子31は、受光素子31の光軸が検出領域DAで投光素子21の光軸と交差するように配置されている。 As shown in FIG. 2, the light receiving element 31 is disposed at a position where the direct light of the light L1 emitted from the light projecting element 21 does not enter. Specifically, the light receiving element 31 is disposed at a position that does not overlap the optical axis of the light projecting element 21. The optical axis of the light projecting element 21 corresponds to the path of light having the highest intensity among the light L1 emitted from the light projecting element 21. Specifically, the optical axis of the light projecting element 21 corresponds to a straight line connecting the light projecting element 21 and the detection area DA. In the present embodiment, the light receiving element 31 is arranged so that the optical axis of the light receiving element 31 intersects the optical axis of the light projecting element 21 in the detection area DA.

 レンズ32は、受光素子31と検出領域DAとの間に配置されている。レンズ32は、検出領域DAにおいて粒子Pによって散乱された散乱光L2を効率良く受光素子31に集光させる。 The lens 32 is disposed between the light receiving element 31 and the detection area DA. The lens 32 efficiently collects the scattered light L2 scattered by the particles P in the detection area DA on the light receiving element 31.

 誘導装置40は、検出領域DAに向けて対象流体を誘導する装置である。具体的には、誘導装置40は、検出領域DAを通過する気流を生成する送風機構である。誘導装置40は、例えば、ヒータなどの発熱素子であり、発熱による上昇気流を生成する。なお、上昇気流を効率良く利用するため、本実施の形態では、図1及び図2に示すY軸の正方向が鉛直上方、Y軸の負方向が鉛直下方になるように、粒子検出センサ1を立てて使用される。 The guiding device 40 is a device that guides the target fluid toward the detection area DA. Specifically, the guidance device 40 is a blower mechanism that generates an airflow that passes through the detection area DA. The induction device 40 is, for example, a heating element such as a heater, and generates an upward airflow due to heat generation. In order to efficiently use the updraft, in the present embodiment, the particle detection sensor 1 is arranged so that the positive direction of the Y axis shown in FIGS. 1 and 2 is vertically upward and the negative direction of the Y axis is vertically downward. Is used.

 誘導装置40は、小型のファンなどでもよい。誘導装置40は、筐体10の内部に配置されているが、筐体10の外側に配置されていてもよい。 The guiding device 40 may be a small fan or the like. The guide device 40 is disposed inside the housing 10, but may be disposed outside the housing 10.

 信号処理回路50は、受光部30から出力される電気信号に基づいて、粒径区分毎に質量濃度を算出する。具体的には、信号処理回路50は、電気信号に基づいて、第1粒子が含まれる第1粒径区分の第1質量濃度と、第1粒子及び当該第1粒子より大きい第2粒子が含まれる第2粒径区分の第2質量濃度とを算出する。 The signal processing circuit 50 calculates the mass concentration for each particle size category based on the electrical signal output from the light receiving unit 30. Specifically, the signal processing circuit 50 includes, based on the electrical signal, the first mass concentration of the first particle size section including the first particles, the first particles, and the second particles larger than the first particles. And the second mass concentration of the second particle size classification.

 第1粒子は、具体的には微小粒子であり、粒径が例えば2.5μm以下の粒子である。本実施の形態では、第1粒径区分は、例えばPM2.5などの小粒径区分であり、第1質量濃度は、PM2.5の質量濃度である。 The first particles are specifically fine particles, and are particles having a particle size of, for example, 2.5 μm or less. In the present embodiment, the first particle size division is a small particle size division such as PM2.5, for example, and the first mass concentration is the mass concentration of PM2.5.

 第2粒子は、具体的には、微小粒子よりも粒径が大きい粗大粒子であり、粒径が例えば10μm以下の粒子である。本実施の形態では、第2粒径区分は、例えばPM10などの大粒径区分であり、第2質量濃度は、PM10の質量濃度である。なお、第2粒径区分は、SPMであってもよく、第2質量濃度は、SPMの質量濃度であってもよい。 Specifically, the second particles are coarse particles having a particle size larger than that of the fine particles, and the particle size is, for example, 10 μm or less. In the present embodiment, the second particle size classification is a large particle size classification such as PM10, and the second mass concentration is the mass concentration of PM10. The second particle size classification may be SPM, and the second mass concentration may be the mass concentration of SPM.

 信号処理回路50は、受光部30から出力される電気信号のピーク値の大きさに基づいて、粒子数及び粒径を計測し、計測結果に基づいて粒径区分毎の質量濃度を算出する。具体的には、信号処理回路50は、電気信号のピーク値と、粒径に対応するように予め定められた1以上の閾値とを比較することで、検出された粒子の粒径を推定する。 The signal processing circuit 50 measures the number of particles and the particle size based on the magnitude of the peak value of the electrical signal output from the light receiving unit 30, and calculates the mass concentration for each particle size category based on the measurement result. Specifically, the signal processing circuit 50 estimates the particle size of the detected particle by comparing the peak value of the electrical signal with one or more threshold values that are predetermined to correspond to the particle size. .

 本実施の形態では、信号処理回路50は、電気信号のうち第1期間分の第1信号に基づいて、PM2.5の質量濃度を算出し、電気信号のうち第2期間分の第2信号に基づいて、PM10の質量濃度を算出する。第1期間は、例えば、PM2.5に含まれる微小粒子の粒子数(以下、PM2.5粒子数と記載する)の計測期間である。第2期間は、第1期間とは異なる期間であり、例えばPM10に含まれる粗大粒子の粒子数(以下、PM10粒子数と記載する)の計測期間である。 In the present embodiment, the signal processing circuit 50 calculates the mass concentration of PM2.5 based on the first signal for the first period of the electrical signal, and the second signal for the second period of the electrical signal. Based on the above, the mass concentration of PM10 is calculated. The first period is, for example, a measurement period of the number of fine particles included in PM2.5 (hereinafter referred to as PM2.5 particle number). The second period is a period different from the first period, for example, a measurement period of the number of coarse particles contained in PM10 (hereinafter referred to as PM10 particle number).

 つまり、本実施の形態に係る粒子検出センサ1では、PM2.5粒子数の計測とPM10粒子数の計測とが時分割で行われる。具体的には、信号処理回路50は、受光部30から出力される電気信号を所定の期間毎に区切って演算することで、粒径区分毎の粒子数の計測を行う。 That is, in the particle detection sensor 1 according to the present embodiment, measurement of the number of PM2.5 particles and measurement of the number of PM10 particles are performed in a time division manner. Specifically, the signal processing circuit 50 measures the number of particles for each particle size category by dividing and calculating the electric signal output from the light receiving unit 30 at predetermined intervals.

 このとき、信号処理回路50は、受光素子31から出力される電気信号の増幅率(ゲイン)を、計測対象の粒径区分に応じて異ならせる。具体的には、図4に示されるように、信号処理回路50は、2つの増幅器51及び52と、スイッチ53とを備える。 At this time, the signal processing circuit 50 varies the amplification factor (gain) of the electric signal output from the light receiving element 31 according to the particle size classification of the measurement target. Specifically, as shown in FIG. 4, the signal processing circuit 50 includes two amplifiers 51 and 52 and a switch 53.

 図4は、本実施の形態に係る信号処理回路50の構成を示す図である。図4に示されるように、信号処理回路50は、さらに、3つの抵抗54~56と、演算回路57とを備える。信号処理回路50は、2つの増幅器51の多段構成を有する。 FIG. 4 is a diagram showing a configuration of the signal processing circuit 50 according to the present embodiment. As shown in FIG. 4, the signal processing circuit 50 further includes three resistors 54 to 56 and an arithmetic circuit 57. The signal processing circuit 50 has a multistage configuration of two amplifiers 51.

 増幅器51及び52はそれぞれ、例えばオペアンプである。増幅器51の正入力端子と負入力端子との間に受光素子31が接続されている。増幅器51の出力端子は、抵抗54を介して負入力端子に接続されている。増幅器51の出力端子は、さらに、増幅器52の正入力端子に接続されている。 Each of the amplifiers 51 and 52 is, for example, an operational amplifier. The light receiving element 31 is connected between the positive input terminal and the negative input terminal of the amplifier 51. The output terminal of the amplifier 51 is connected to the negative input terminal via the resistor 54. The output terminal of the amplifier 51 is further connected to the positive input terminal of the amplifier 52.

 増幅器52の負入力端子は、抵抗55を介して接地されている。増幅器52の出力端子は、抵抗56を介して負入力端子に接続されている。増幅器52の出力端子は、演算回路57に接続されている。 The negative input terminal of the amplifier 52 is grounded via a resistor 55. The output terminal of the amplifier 52 is connected to the negative input terminal via the resistor 56. The output terminal of the amplifier 52 is connected to the arithmetic circuit 57.

 スイッチ53は、抵抗56に対して並列に、すなわち、増幅器52の出力端子と負入力端子との間に設けられている。スイッチ53を導通(オン)させることにより、増幅器52の出力端子と負入力端子とが短絡されるので、増幅器52による増幅が行われない。スイッチ53がオンされた場合には、増幅器51のみによる増幅が行われる。このように、スイッチ53のオン/オフによって、電気信号の増幅率を異ならせることができる。 The switch 53 is provided in parallel with the resistor 56, that is, between the output terminal and the negative input terminal of the amplifier 52. By making the switch 53 conductive (ON), the output terminal and the negative input terminal of the amplifier 52 are short-circuited, so that amplification by the amplifier 52 is not performed. When the switch 53 is turned on, amplification by only the amplifier 51 is performed. In this way, the amplification factor of the electric signal can be varied by turning on / off the switch 53.

 具体的には、信号処理回路50は、PM2.5粒子数を計測する第1期間では、スイッチ53をオフにすることで、増幅率を大きくする。例えば、受光素子31から出力される光電流の大きさをI、増幅器52の出力信号の電圧をVoutとした場合、スイッチ53がオフされたときのVoutは、以下の式(1)で表される。 Specifically, the signal processing circuit 50 increases the amplification factor by turning off the switch 53 in the first period in which the number of PM2.5 particles is measured. For example, when the magnitude of the photocurrent output from the light receiving element 31 is I and the voltage of the output signal of the amplifier 52 is Vout, Vout when the switch 53 is turned off is expressed by the following equation (1). The

 (1) Vout=Z×(1+Z/Z)×I (1) Vout = Z 1 × (1 + Z 3 / Z 2 ) × I

 なお、Z~Zはそれぞれ、抵抗54~56の抵抗値である。増幅率は、Z×(1+Z/Z)で表される。 Z 1 to Z 3 are resistance values of the resistors 54 to 56, respectively. The amplification factor is represented by Z 1 × (1 + Z 3 / Z 2 ).

 PM2.5粒子数を計測する場合、投光素子21からの光を反射する粒子が微小粒子であるため、当該粒子による散乱光L2が弱くなる。このため、受光素子31から出力される光電流が小さくなる。したがって、スイッチ53をオフし、増幅率を大きくすることで、出力信号の電圧を大きくすることができる。これにより、ピーク値と閾値との比較を容易にし、粒径の推定を精度良く行うことができる。 When measuring the number of PM2.5 particles, since the particles that reflect the light from the light projecting element 21 are microparticles, the scattered light L2 due to the particles becomes weak. For this reason, the photocurrent output from the light receiving element 31 is reduced. Therefore, the voltage of the output signal can be increased by turning off the switch 53 and increasing the amplification factor. Thereby, the comparison between the peak value and the threshold value is facilitated, and the particle diameter can be estimated with high accuracy.

 また、信号処理回路50は、PM10粒子数を計測する第2期間では、スイッチ53をオンすることで、増幅率を小さくする。スイッチ53がオンされたときのVoutは、以下の式(2)で表される。 In addition, the signal processing circuit 50 reduces the amplification factor by turning on the switch 53 in the second period in which the number of PM10 particles is measured. Vout when the switch 53 is turned on is expressed by the following equation (2).

 (2) Vout=Z×I (2) Vout = Z 1 × I

 PM10粒子数を計測する場合、投光素子21からの光を反射する粒子が粗大粒子であるため、微小粒子に比べて散乱光L2が強くなる。このため、受光素子31から出力される光電流も大きくなる。したがって、スイッチ53をオンし、増幅率を小さくしてもよい。 When measuring the number of PM10 particles, since the particles that reflect the light from the light projecting element 21 are coarse particles, the scattered light L2 becomes stronger than the fine particles. For this reason, the photocurrent output from the light receiving element 31 also increases. Therefore, the switch 53 may be turned on to reduce the amplification factor.

 このように、計測対象の粒子の大きさに応じて増幅率を異ならせることで、計測対象の粒子の大きさによらず、Voutが取りうる範囲を同等にすることができる。これにより、後段の演算回路57でのピーク値と閾値との比較を容易に行わせることができる。 Thus, by varying the amplification factor according to the size of the particle to be measured, the range that Vout can take can be made equal regardless of the size of the particle to be measured. Thereby, it is possible to easily compare the peak value and the threshold value in the arithmetic circuit 57 in the subsequent stage.

 本実施の形態では、演算回路57は、PM2.5粒子数の計測を行う第1期間分の電気信号に表れるピークの極大値(以下、ピーク値と記載する)に基づいて粒子の粒径を推定し、複数のサブ区分のいずれかに分類する。PM2.5のサブ区分は、PM2.5に相当する粒径区分が1以上の閾値によって分割された複数のサブ区分である。 In the present embodiment, the arithmetic circuit 57 calculates the particle size of the particles based on the peak maximum value (hereinafter referred to as the peak value) appearing in the electric signal for the first period for measuring the number of PM2.5 particles. Estimate and classify into one of multiple sub-categories. The sub-section of PM2.5 is a plurality of sub-sections in which the particle size section corresponding to PM2.5 is divided by one or more threshold values.

 図5は、本実施の形態に係る粒子検出センサ1の受光素子31から出力される電気信号であって、PM2.5粒子数を計測する第1期間の第1信号を示す図である。図5において、横軸は時間を表しており、縦軸は電気信号の信号強度を表している。本実施の形態では、受光素子31から出力される電気信号が電圧Voutに変換されているので、縦軸は、電圧値に相当する。 FIG. 5 is a diagram showing a first signal in the first period in which the number of PM2.5 particles is measured, which is an electrical signal output from the light receiving element 31 of the particle detection sensor 1 according to the present embodiment. In FIG. 5, the horizontal axis represents time, and the vertical axis represents the signal strength of the electric signal. In the present embodiment, since the electric signal output from the light receiving element 31 is converted into the voltage Vout, the vertical axis corresponds to the voltage value.

 例えば、図5に示されるように、PM2.5は、4つの閾値1~4によって4つのサブ区分に分割されている。具体的には、PM2.5は、例えば、1.0μm以上の第1サブ区分、1.0μmより小さく0.5μm以上の第2サブ区分、0.5μmより小さく0.3μm以上の第3サブ区分、及び、0.3μmより小さい第4サブ区分が含まれる。なお、閾値4は、ノイズ成分を除去するための閾値である。 For example, as shown in FIG. 5, PM2.5 is divided into four sub-sections by four threshold values 1 to 4. Specifically, PM2.5 is, for example, a first subsection of 1.0 μm or more, a second subsection of less than 1.0 μm and 0.5 μm or more, and a third subsection of less than 0.5 μm and 0.3 μm or more. A section and a fourth sub-section smaller than 0.3 μm are included. The threshold value 4 is a threshold value for removing a noise component.

 図5には、5つのピークS1~S5が現れた例を示している。ピークS1~S5はそれぞれ、検出領域DAを通過した粒子による散乱光L2を受光素子31が受光することで現れた電気信号の変化に相当する。演算回路57は、ピークS1~S5の各々のピーク値と閾値とを比較することにより、粒子をPM2.5の第1サブ区分~第4サブ区分のいずれかに分類する。 FIG. 5 shows an example in which five peaks S1 to S5 appear. Each of the peaks S1 to S5 corresponds to a change in an electric signal that appears when the light receiving element 31 receives scattered light L2 due to particles that have passed through the detection area DA. The arithmetic circuit 57 classifies the particles into any one of the first subsection to the fourth subsection of PM2.5 by comparing each peak value of the peaks S1 to S5 with the threshold value.

 例えば、ピークS1のピーク値は、閾値2より小さく閾値3以上であるので、ピークS1に相当する粒子は、第3サブ区分に分類される。同様に、ピークS2のピーク値は、閾値3より小さく閾値4以上であるので、ピークS2に相当する粒子は、第4サブ区分に分類される。ピークS3のピーク値は、閾値1より小さく閾値2以上であるので、ピークS3に相当する粒子は、第2サブ区分に分類される。ピークS4及びS5の各々のピーク値は、閾値1以上であるので、ピークS4及びS5の各々に相当する粒子は、第1サブ区分に分類される。 For example, since the peak value of peak S1 is smaller than threshold value 2 and greater than or equal to threshold value 3, the particles corresponding to peak S1 are classified into the third sub-section. Similarly, since the peak value of the peak S2 is smaller than the threshold 3 and greater than or equal to the threshold 4, the particles corresponding to the peak S2 are classified into the fourth subsection. Since the peak value of the peak S3 is smaller than the threshold value 1 and greater than or equal to the threshold value 2, the particles corresponding to the peak S3 are classified into the second sub-section. Since the peak value of each of the peaks S4 and S5 is greater than or equal to the threshold value 1, particles corresponding to each of the peaks S4 and S5 are classified into the first sub-section.

 PM10についても同様である。具体的には、演算回路57は、PM10粒子数の計測を行う第2期間分の電気信号に現れるピークの極大値(ピーク値)に基づいて粒子の粒径を推定し、複数のサブ区分のいずれかに分類する。PM10のサブ区分は、PM10に相当する粒径区分が1以上の閾値によって分割された複数のサブ区分である。 The same applies to PM10. Specifically, the arithmetic circuit 57 estimates the particle size of the particle based on the peak maximum value (peak value) appearing in the electric signal for the second period in which the number of PM10 particles is measured, Classify either. The sub-section of PM10 is a plurality of sub-sections in which the particle size section corresponding to PM10 is divided by one or more threshold values.

 図6は、本実施の形態に係る粒子検出センサ1の受光素子31から出力される電気信号であって、PM10粒子数を計測する第2期間の第2信号を示す図である。図6において、横軸は時間を表しており、縦軸は電気信号の信号強度を表している。本実施の形態では、受光素子31から出力される電気信号が電圧Voutに変換されているので、縦軸は、電圧値に相当する。 FIG. 6 is a diagram illustrating a second signal in the second period in which the number of PM10 particles is measured, which is an electric signal output from the light receiving element 31 of the particle detection sensor 1 according to the present embodiment. In FIG. 6, the horizontal axis represents time, and the vertical axis represents the signal strength of the electric signal. In the present embodiment, since the electric signal output from the light receiving element 31 is converted into the voltage Vout, the vertical axis corresponds to the voltage value.

 例えば、図6に示されるように、PM10は、4つの閾値A~Dによって4つのサブ区分に分割されている。具体的には、PM10は、例えば、10μmより小さく5μm以上の第1サブ区分、5μmより小さく2.5μm以上の第2サブ区分、2.5μmより小さく1.0μm以上の第3サブ区分、及び、1.0μmより小さい第4サブ区分が含まれる。 For example, as shown in FIG. 6, the PM 10 is divided into four sub-sections by four threshold values A to D. Specifically, the PM 10 includes, for example, a first subsection smaller than 10 μm and 5 μm or more, a second subsection smaller than 5 μm and 2.5 μm or more, a third subsection smaller than 2.5 μm and 1.0 μm or more, and A fourth subsection smaller than 1.0 μm is included.

 図6には、5つのピークSa~Seが現れた例を示している。ピークSa~Seはそれぞれ、検出領域DAを通過した粒子による散乱光L2を受光素子31が受光することで現れた電気信号の変化に相当する。演算回路57は、ピークSa~Seの各々のピーク値と閾値とを比較することにより、粒子をPM10の第1サブ区分~第4サブ区分のいずれかに分類する。具体的な処理は、PM2.5の場合と同様である。 FIG. 6 shows an example in which five peaks Sa to Se appear. Each of the peaks Sa to Se corresponds to a change in an electrical signal that appears when the light receiving element 31 receives scattered light L2 due to particles that have passed through the detection area DA. The arithmetic circuit 57 classifies the particles into any one of the first sub-section to the fourth sub-section of the PM 10 by comparing each peak value of the peaks Sa to Se with a threshold value. The specific process is the same as in PM2.5.

 なお、PM2.5及びPM10の少なくとも一方のサブ区分の個数は、4個に限らず、2個又は3個でもよく、5個でもよい。あるいは、サブ区分の個数は1個でもよい。すなわち、PM2.5及びPM10の少なくとも一方は、複数のサブ区分に分割されなくてもよい。 Note that the number of at least one sub-section of PM2.5 and PM10 is not limited to four, and may be two or three, or five. Alternatively, the number of subsections may be one. That is, at least one of PM2.5 and PM10 may not be divided into a plurality of sub-sections.

 なお、本実施の形態に係る粒子検出センサ1では、実際には、検出領域DAの中心以外の部分を通過する粒子も多数含まれる。例えば、検出領域DAの端を大きな粒子が通過した場合、当該粒子による散乱光の受光素子31による受光強度が小さくなる。このため、大きな粒子であるにも関わらず、当該粒子のサイズが「小さい」と誤判定される可能性がある。 Note that the particle detection sensor 1 according to the present embodiment actually includes many particles that pass through a portion other than the center of the detection area DA. For example, when a large particle passes through the end of the detection area DA, the light receiving intensity of the scattered light from the particle by the light receiving element 31 decreases. For this reason, although it is a large particle, the size of the particle may be erroneously determined as “small”.

 本実施の形態に係る演算回路57は、当該誤判定を抑制するため、例えば、図7に示すような、信号強度(電圧値)と、粒子のサイズ毎の粒子の頻度とを対応付けたヒストグラムをメモリに保持している。図7は、本実施の形態に係る粒子検出センサ1によって検出された粒子のヒストグラムである。図7において、横軸は信号強度、縦軸は粒子のサイズ毎の粒子の頻度である。 In order to suppress the erroneous determination, the arithmetic circuit 57 according to the present embodiment, for example, as shown in FIG. 7, a histogram in which signal intensity (voltage value) is associated with the frequency of particles for each particle size. Is stored in memory. FIG. 7 is a histogram of particles detected by the particle detection sensor 1 according to the present embodiment. In FIG. 7, the horizontal axis represents signal intensity, and the vertical axis represents the frequency of particles for each particle size.

 図7に示されるように、信号強度が大きい場合には、そのほとんどは、粒径が大きい粒子である。一方で、信号強度が小さい場合には、粒径が小さい粒子だけでなく、検出領域DAの中心以外の部分を通過する粒径が大きい粒子及び中くらいの粒子も含まれる。演算回路57は、電気信号のピーク強度に基づいて、図7に示すヒストグラムを参照することで、当該ピークに対応する粒子Pのサイズを推定する。 As shown in FIG. 7, when the signal intensity is large, most of them are particles having a large particle size. On the other hand, when the signal intensity is small, not only particles having a small particle size but also particles having a large particle size and medium particles passing through a portion other than the center of the detection area DA are included. The arithmetic circuit 57 estimates the size of the particle P corresponding to the peak by referring to the histogram shown in FIG. 7 based on the peak intensity of the electric signal.

 演算回路57は、一定の動作期間中に検出された粒子Pの個数をサブ区分毎にカウントする。演算回路57は、サブ区分毎に、予め定められた平均質量と、カウントした個数との積を算出し、算出したサブ区分毎の積を加算することで、PM2.5の質量濃度及びPM10の質量濃度をそれぞれ算出する。 The arithmetic circuit 57 counts the number of particles P detected during a certain operation period for each sub-section. The arithmetic circuit 57 calculates a product of a predetermined average mass and the counted number for each sub-section, and adds the calculated product for each sub-section, thereby obtaining a mass concentration of PM2.5 and PM10. Each mass concentration is calculated.

 演算回路57は、例えば比較器などを含む1以上の電子部品で実現される。例えば、演算回路57は、MPU(Micro Processing Unit)などで実現されてもよい。演算回路57が行う処理は、ハードウェアで実現されてもよく、プロセッサによって実行されるソフトウェアで実現されてもよい。 The arithmetic circuit 57 is realized by one or more electronic components including a comparator, for example. For example, the arithmetic circuit 57 may be realized by an MPU (Micro Processing Unit) or the like. The processing performed by the arithmetic circuit 57 may be realized by hardware or may be realized by software executed by a processor.

 補正回路60は、第1粒径区分に含まれる第1粒子の粒子数に基づいて第2粒径区分に含まれる第2粒子の粒子数を推定し、推定した粒子数に基づいて第2粒径区分の質量濃度の補正を行う。具体的には、補正回路60は、PM2.5に含まれる微小粒子の粒子数に基づいて、PM10に含まれる粗大粒子の粒子数を推定する。補正回路60は、推定した粗大粒子の粒子数に基づいてPM10の質量濃度の補正を行う。 The correction circuit 60 estimates the number of particles of the second particle included in the second particle size category based on the number of particles of the first particle included in the first particle size category, and the second particle based on the estimated number of particles. Correct the mass concentration of the diameter category. Specifically, the correction circuit 60 estimates the number of coarse particles contained in PM10 based on the number of fine particles contained in PM2.5. The correction circuit 60 corrects the mass concentration of PM10 based on the estimated number of coarse particles.

 本実施の形態では、微小粒子の粒子数は、PM2.5が分割された複数のサブ区分のうち、最大粒径のサブ区分に含まれる粒子数である。例えば、図5に示される例における微小粒子の粒子数は、粒径が1.0μm以上である第4サブ区分に含まれる粒子の粒子数である。 In the present embodiment, the number of fine particles is the number of particles included in the sub-section having the maximum particle size among the plurality of sub-sections into which PM2.5 is divided. For example, the number of fine particles in the example shown in FIG. 5 is the number of particles included in the fourth subsection having a particle size of 1.0 μm or more.

 補正回路60は、第4サブ区分に含まれる粒子の粒子数の含有率に基づいて、粗大粒子の粒子数を推定する。含有率は、PM2.5に相当する全粒子数に対する、第4サブ区分に含まれる粒子の粒子数の割合に相当する。 The correction circuit 60 estimates the number of coarse particles based on the content ratio of the number of particles included in the fourth subsection. The content rate corresponds to the ratio of the number of particles included in the fourth subsection to the total number of particles corresponding to PM2.5.

 本実施の形態では、補正回路60は、大きく分けて2つの補正を行う。2つの補正は、信号処理回路50によって算出されたPM10の質量濃度を補正する第1の補正と、PM10粒子数の計測方法を調整する第2の補正とである。各補正処理の詳細については、後で説明する。 In this embodiment, the correction circuit 60 roughly performs two corrections. The two corrections are a first correction for correcting the mass concentration of PM10 calculated by the signal processing circuit 50 and a second correction for adjusting the method for measuring the number of PM10 particles. Details of each correction process will be described later.

 補正回路60は、例えば1以上の電子部品で実現される。例えば、補正回路60は、MPUなどで実現されてもよい。補正回路60が行う動作は、ハードウェアで実現されてもよく、プロセッサによって実行されるソフトウェアで実現されてもよい。 The correction circuit 60 is realized by one or more electronic components, for example. For example, the correction circuit 60 may be realized by an MPU or the like. The operation performed by the correction circuit 60 may be realized by hardware or may be realized by software executed by a processor.

 [補正処理]
 以下では、補正回路60が行う補正処理について説明する。
[Correction process]
Below, the correction process which the correction circuit 60 performs is demonstrated.

 まず、PM10の質量濃度を補正する第1の補正について、図8を用いて説明する。図8は、PM2.5及びPM10の各々の粒径に対する濃度分布を示す図である。図8において、横軸は粒径[μm]を表しており、縦軸は質量濃度を示している。 First, the first correction for correcting the mass concentration of PM10 will be described with reference to FIG. FIG. 8 is a diagram showing the concentration distribution of each particle size of PM2.5 and PM10. In FIG. 8, the horizontal axis represents the particle size [μm], and the vertical axis represents the mass concentration.

 図8で示されるように、PM2.5の濃度分布とPM10の濃度分布とには、重複する部分(網掛け部分)が存在している。重複部分は、例えば、PM2.5の第4サブ区分に相当する部分である。 As shown in FIG. 8, there are overlapping portions (shaded portions) in the concentration distribution of PM2.5 and the concentration distribution of PM10. An overlapping part is a part corresponded to the 4th subsection of PM2.5, for example.

 PM2.5の濃度分布とPM10の濃度分布とには、相関関係がある。このため、重複部分に相当する第4サブ区分に含まれる微小粒子の粒子数の含有率に基づいて、PM10に含まれる粗大粒子の粒子数の推定が可能になる。例えば、補正回路60は、含有率と粗大粒子の粒子数との対応関係を示す対応情報を記憶するメモリを有する。補正回路60は、当該メモリから対応情報を読み出し、読み出した対応情報を参照することで、微小粒子の粒子数の含有率に基づいて粗大粒子の推定を行う。 There is a correlation between the concentration distribution of PM2.5 and the concentration distribution of PM10. Therefore, the number of coarse particles contained in PM10 can be estimated based on the content ratio of the number of fine particles contained in the fourth sub-section corresponding to the overlapping portion. For example, the correction circuit 60 includes a memory that stores correspondence information indicating a correspondence relationship between the content rate and the number of coarse particles. The correction circuit 60 reads the correspondence information from the memory and refers to the read correspondence information to estimate coarse particles based on the content ratio of the number of fine particles.

 補正回路60は、推定した粗大粒子の粒子数に基づいて、演算回路57によって算出されたPM10の質量濃度を補正する。例えば、補正回路60は、推定した粒子数に基づく質量濃度と、PM10粒子数の計測結果(すなわち、実測数)に基づいて算出された質量濃度とに所定値以上の差分が生じた場合、補正回路60は、推定結果と実測結果とを平均化することで、PM10の質量濃度の補正値として出力する。なお、補正値は、推定結果と実測結果との平均でなくてもよく、例えば推定結果を強く重み付けした重み付け加算値であってもよい。 The correction circuit 60 corrects the mass concentration of PM10 calculated by the arithmetic circuit 57 based on the estimated number of coarse particles. For example, the correction circuit 60 corrects when a difference of a predetermined value or more occurs between the mass concentration based on the estimated number of particles and the mass concentration calculated based on the measurement result of the number of PM10 particles (that is, the actually measured number). The circuit 60 averages the estimation result and the actual measurement result, and outputs the result as a correction value of the mass concentration of PM10. The correction value may not be an average of the estimation result and the actual measurement result, and may be a weighted addition value obtained by strongly weighting the estimation result, for example.

 また、推定した粗大粒子の粒子数と質量濃度の補正値とを対応付けた対応情報がメモリに記憶されていてもよい。補正回路60は、当該対応情報をメモリから読み出し、読み出した対応情報を参照することで、推定した粒子数から質量濃度の補正値を決定して出力してもよい。なお、対応情報は、例えば、PM10の質量濃度が判明している環境下でPM2.5粒子数に基づく推定値を得ることで、予め生成しておくことができる。 Further, correspondence information that associates the estimated number of coarse particles with the correction value of the mass concentration may be stored in the memory. The correction circuit 60 may read out the correspondence information from the memory and refer to the read correspondence information to determine and output a correction value for the mass concentration from the estimated number of particles. The correspondence information can be generated in advance by, for example, obtaining an estimated value based on the number of PM2.5 particles in an environment where the mass concentration of PM10 is known.

 次に、粒子数の計測方法に対する第2の補正の詳細について説明する。 Next, details of the second correction for the particle count measurement method will be described.

 <計測期間の補正(第1例)>
 まず、粒子数の計測処理に対する補正の第1例について、図9を用いて説明する。
<Correction of measurement period (first example)>
First, a first example of correction for the particle count measurement process will be described with reference to FIG.

 図9は、本実施の形態に係る粒子検出センサ1の補正の第1例として、粗大粒子の粒子数の計測期間の調整例を示す図である。補正回路60は、推定した粗大粒子の粒子数に基づいて、PM10粒子数の計測期間である第2期間の長さを変更する。 FIG. 9 is a diagram illustrating an example of adjustment of the measurement period of the number of coarse particles as a first example of correction of the particle detection sensor 1 according to the present embodiment. The correction circuit 60 changes the length of the second period, which is the measurement period of the number of PM10 particles, based on the estimated number of coarse particles.

 本実施の形態に係る粒子検出センサ1では、図9に示されるように、微小粒子の粒子数の計測と、粗大粒子の粒子数の計測と、PM2.5の質量濃度の算出と、PM10の質量濃度の算出とがこの順で行われる。微小粒子の粒子数の計測が、PM2.5の質量濃度の算出のための第1期間に相当する。粗大粒子の粒子数の計測が、PM10の質量濃度の算出のための第2期間に相当する。 In the particle detection sensor 1 according to the present embodiment, as shown in FIG. 9, the measurement of the number of fine particles, the measurement of the number of coarse particles, the calculation of the mass concentration of PM2.5, and the PM10 The calculation of the mass concentration is performed in this order. Measurement of the number of fine particles corresponds to the first period for calculating the mass concentration of PM2.5. Measurement of the number of coarse particles corresponds to a second period for calculating the mass concentration of PM10.

 本実施の形態では、図9に示されるように、補正回路60は、推定された粒子数が少ない場合、推定された粒子数が多い場合よりも、第2期間を長くする。これにより、検出される粗大粒子の数(検出数)を一定数以上確保しやすくなるので、粗大粒子の粒子数を精度良く計測することができ、PM10の質量濃度を精度良く算出することができる。 In this embodiment, as shown in FIG. 9, the correction circuit 60 makes the second period longer when the estimated number of particles is smaller than when the estimated number of particles is large. This makes it easy to secure a certain number or more of coarse particles to be detected (detection number), so that the number of coarse particles can be measured with high accuracy, and the mass concentration of PM10 can be calculated with high accuracy. .

 なお、推定された粒子数が多い場合は、第2期間を長くしなくても、一定数以上の粗大粒子の検出数を確保することができる。したがって、粗大粒子の粒子数を精度良く計測することができ、PM10の質量濃度を精度良く算出することができる。また、粒子数の計測から質量濃度の算出までに要する時間を短くすることができる。 In addition, when the estimated number of particles is large, it is possible to ensure a detection number of coarse particles of a certain number or more without lengthening the second period. Therefore, the number of coarse particles can be measured with high accuracy, and the mass concentration of PM10 can be calculated with high accuracy. Moreover, the time required from the measurement of the number of particles to the calculation of the mass concentration can be shortened.

 <平均化のサイクル数の補正(第2例)>
 次に、粒子数の計測処理に対する補正の第2例について、図10を用いて説明する。
<Correction of number of averaging cycles (second example)>
Next, a second example of correction for the particle count measurement process will be described with reference to FIG.

 図10は、本実施の形態に係る粒子検出センサ1の補正の第2例として、質量濃度の演算の際の平均化のサイクル数の調整例を示す図である。補正回路60は、推定した粗大粒子の粒子数に基づいて、PM10の質量濃度の演算の際の平均化のサイクル数を変更する。 FIG. 10 is a diagram showing an example of adjusting the number of cycles for averaging in the calculation of mass concentration as a second example of correction of the particle detection sensor 1 according to the present embodiment. The correction circuit 60 changes the number of averaging cycles when calculating the mass concentration of PM10 based on the estimated number of coarse particles.

 本実施の形態に係る粒子検出センサ1では、図10に示されるように、微小粒子の粒子数の計測と、粗大粒子の粒子数の計測と、PM2.5の質量濃度の算出と、PM10の質量濃度の算出とを1サイクルとして、当該サイクルが複数回繰り返される。1サイクル毎に算出される質量濃度を、複数回分で平均化することで、質量濃度が算出される。 In the particle detection sensor 1 according to the present embodiment, as shown in FIG. 10, the measurement of the number of fine particles, the measurement of the number of coarse particles, the calculation of the mass concentration of PM2.5, and the PM10 The calculation of mass concentration is one cycle, and this cycle is repeated a plurality of times. The mass concentration is calculated by averaging the mass concentration calculated for each cycle for a plurality of times.

 具体的には、演算回路57は、粗大粒子の計測期間に得られた電気信号(第2信号)に基づいてPM10の質量濃度を算出する処理を所定回数繰り返し、得られた所定回数分の質量濃度を平均化することで、PM10の質量濃度を算出する。補正回路60は、平均化の回数であるサイクル数を変更する。 Specifically, the arithmetic circuit 57 repeats the process of calculating the mass concentration of PM10 a predetermined number of times based on the electrical signal (second signal) obtained during the measurement period of the coarse particles, and the obtained mass for the predetermined number of times. By averaging the concentration, the mass concentration of PM10 is calculated. The correction circuit 60 changes the number of cycles that is the number of times of averaging.

 本実施の形態では、図10に示されるように、補正回路60は、推定された粒子数が少ない場合、推定された粒子数が多い場合よりも、サイクル数を多くする。例えば、図10には、推定された粒子数が多い場合は、サイクル数が3回であるのに対して、推定された粒子数が少ない場合は、サイクル数が6回である例を示している。なお、サイクル数の具体的な数値例は、これらに限らない。 In the present embodiment, as shown in FIG. 10, the correction circuit 60 increases the number of cycles when the estimated number of particles is small than when the estimated number of particles is large. For example, FIG. 10 shows an example in which the number of cycles is 3 when the estimated number of particles is large, whereas the number of cycles is 6 when the estimated number of particles is small. Yes. Note that specific numerical examples of the number of cycles are not limited to these.

 これにより、平均化の仮定で、検出される粗大粒子の数(検出数)を一定数以上確保しやすくなるので、粗大粒子の粒子数を精度良く計測することができ、PM10の質量濃度を精度良く算出することができる。 This makes it easy to ensure the number of detected coarse particles (number of detections) above a certain number under the assumption of averaging, so that the number of coarse particles can be accurately measured, and the mass concentration of PM10 can be accurately measured. It can be calculated well.

 なお、演算回路57は、PM2.5の質量濃度の場合も同様である。このとき、平均化のサイクル数は、PM2.5の場合とPM10の場合とで同じであってもよく、異なっていてもよい。例えば、PM2.5の場合のサイクル数は、推定された粒子数によらず、常に一定であってもよい。 Note that the calculation circuit 57 is the same for the mass concentration of PM2.5. At this time, the number of cycles for averaging may be the same or different between PM2.5 and PM10. For example, the number of cycles in the case of PM2.5 may always be constant regardless of the estimated number of particles.

 <誘導量の補正(第3例)>
 次に、粒子数の計測処理に対する補正の第3例について、図11を用いて説明する。
<Induction amount correction (third example)>
Next, a third example of correction for the particle count measurement process will be described with reference to FIG.

 図11は、本実施の形態に係る粒子検出センサ1の補正の第3例として、対象流体の誘導量の調整例を示す図である。補正回路60は、粗大粒子の計測期間である第2期間内に誘導装置40によって誘導される対象流体の誘導量を変更する。 FIG. 11 is a diagram illustrating an adjustment example of the guidance amount of the target fluid as a third example of the correction of the particle detection sensor 1 according to the present embodiment. The correction circuit 60 changes the guidance amount of the target fluid that is guided by the guidance device 40 within the second period, which is the coarse particle measurement period.

 本実施の形態では、誘導装置40は、気体を筐体10の内部に取り入れるための送風機構である。このため、補正回路60は、誘導量として吸気量を変更する。例えば、誘導装置40が抵抗素子であり、発熱による上昇気流を利用する場合、補正回路60は、抵抗素子に流す電流を調整することで、発熱量を調整する。例えば、補正回路60は、電流を多く流し、発熱量を増やすことで、上昇気流が強くなり、吸気量を多くすることができる。 In the present embodiment, the guidance device 40 is a blower mechanism for taking gas into the housing 10. For this reason, the correction circuit 60 changes the intake air amount as the induction amount. For example, when the induction device 40 is a resistance element and uses an upward air flow due to heat generation, the correction circuit 60 adjusts the amount of heat generated by adjusting the current flowing through the resistance element. For example, the correction circuit 60 can increase the amount of intake air by increasing the amount of heat generated by increasing the amount of heat generated by flowing a large amount of current.

 図11に示されるように、補正回路60は、推定された粒子数が少ない場合、推定された粒子数が多い場合よりも、吸気量を増加させる。これにより、1回の計測で取り入れられる気体の量が増加するので、気体に含まれる粒子数も増加させることができる。したがって、一定数以上の粗大粒子の検出数を確保することができる。よって、粗大粒子の粒子数を精度良く計測することができ、PM10の質量濃度を精度良く算出することができる。 As shown in FIG. 11, the correction circuit 60 increases the intake amount when the estimated number of particles is small than when the estimated number of particles is large. Thereby, since the quantity of the gas taken in by one measurement increases, the number of particles contained in gas can also be increased. Therefore, it is possible to secure a detection number of coarse particles of a certain number or more. Therefore, the number of coarse particles can be measured with high accuracy, and the mass concentration of PM10 can be calculated with high accuracy.

 PM10粒子数の計測方法の第2の補正では、上述した第1例~第3例の全てが行われてもよく、1つのみが行われてもよい。また、PM10粒子数の計測方法の第2の補正と、PM10の質量濃度の第1の補正との両方が行われてもよく、いずれか一方のみが行われてもよい。 In the second correction of the PM10 particle count measurement method, all of the first to third examples described above may be performed, or only one may be performed. In addition, both the second correction of the PM10 particle number measurement method and the first correction of the mass concentration of PM10 may be performed, or only one of them may be performed.

 [効果など]
 以上のように、本実施の形態に係る粒子検出センサ1は、対象流体に含まれる粒子を検出する粒子検出センサであって、検出領域DAに向けて光を出射する投光部20と、投光部20が出射する光L1に対して受光感度を有し、検出領域DAを通過する粒子による光の散乱光L2を光電変換することで電気信号を生成して出力する受光部30とを備える。粒子検出センサ1は、さらに、電気信号に基づいて、微小粒子が含まれる第1粒径区分の第1質量濃度(例えば、PM2.5の質量濃度)と、微小粒子及び当該微小粒子より大きい粗大粒子が含まれる第2粒径区分の第2質量濃度(例えば、PM10の質量濃度)とを算出する信号処理回路50と、微小粒子の粒子数に基づいて粗大粒子の粒子数を推定し、推定した粒子数に基づいて第2質量濃度の補正を行う補正回路60とを備える。
[Effects, etc.]
As described above, the particle detection sensor 1 according to the present embodiment is a particle detection sensor that detects particles contained in a target fluid, and includes a light projecting unit 20 that emits light toward the detection area DA, and a light projecting unit. A light receiving unit 30 that has light receiving sensitivity with respect to the light L1 emitted from the light unit 20, and that generates and outputs an electrical signal by photoelectrically converting the scattered light L2 of the light passing through the detection area DA. . The particle detection sensor 1 further includes a first mass concentration (for example, a mass concentration of PM2.5) of the first particle size classification in which the fine particles are included based on the electrical signal, the fine particles and the coarser than the fine particles. The signal processing circuit 50 that calculates the second mass concentration (for example, the mass concentration of PM10) of the second particle size classification in which the particles are included, and the number of coarse particles are estimated based on the number of fine particles, and estimated And a correction circuit 60 for correcting the second mass concentration based on the number of particles obtained.

 これにより、一定数以上の粒子数が容易に計測でき、精度良く計測された微小粒子の粒子数に基づいて粗大粒子の粒子数を推定するので、粗大粒子の粒子数の推定精度も高くなる。本実施の形態によれば、推定結果に基づいてPM10の質量濃度を補正するので、PM10の質量濃度の計測精度も高められる。したがって、PM2.5だけでなく、PM10の質量濃度も精度良く計測することができる。このように、本実施の形態に係る粒子検出センサ1によれば、複数の粒径区分の質量濃度を精度良く計測することができる。 This makes it possible to easily measure the number of particles of a certain number or more and estimate the number of coarse particles based on the number of fine particles measured with high accuracy, thus increasing the accuracy of estimating the number of coarse particles. According to the present embodiment, since the mass concentration of PM10 is corrected based on the estimation result, the measurement accuracy of the mass concentration of PM10 is also improved. Therefore, not only PM2.5 but also the mass concentration of PM10 can be accurately measured. Thus, according to particle detection sensor 1 concerning this embodiment, the mass concentration of a plurality of particle size divisions can be measured with high accuracy.

 また、例えば、微小粒子の粒子数は、第1粒径区分が分割された複数のサブ区分のうち、最大粒径のサブ区分に含まれる粒子数である。補正回路60は、微小粒子の粒子数の含有率に基づいて粗大粒子の粒子数を推定する。 Further, for example, the number of fine particles is the number of particles included in the sub-section having the maximum particle size among the plurality of sub-sections obtained by dividing the first particle size section. The correction circuit 60 estimates the number of coarse particles based on the content of the number of fine particles.

 これにより、PM2.5の最大粒径のサブ区分の粒子数の含有率と、PM10に含まれる粗大粒子の粒子数とには相関関係があるので、当該相関関係に基づいて、粗大粒子の粒子数を精度良く推定することができる。粗大粒子の粒子数の推定精度が高くなるので、PM10の質量濃度の計測精度も高められる。したがって、PM2.5だけでなく、PM10の質量濃度も精度良く計測することができる。 Thereby, since there is a correlation between the content ratio of the number of particles in the sub-section of the maximum particle size of PM2.5 and the number of coarse particles contained in PM10, the particles of coarse particles are based on the correlation. The number can be estimated with high accuracy. Since the estimation accuracy of the number of coarse particles is increased, the measurement accuracy of the mass concentration of PM10 is also increased. Therefore, not only PM2.5 but also the mass concentration of PM10 can be accurately measured.

 また、例えば、信号処理回路50は、電気信号のうち第1期間分の第1信号に基づいてPM2.5の質量濃度を算出し、電気信号のうち第1期間とは異なる第2期間分の第2信号に基づいてPM10の質量濃度を算出する。 Further, for example, the signal processing circuit 50 calculates the mass concentration of PM2.5 based on the first signal for the first period of the electric signal, and for the second period different from the first period of the electric signal. Based on the second signal, the mass concentration of PM10 is calculated.

 これにより、PM2.5の質量濃度とPM10の質量濃度とを時系列で算出することができる。PM10の質量濃度の実測値が得られるので、補正の精度が高められる。したがって、PM2.5だけでなく、PM10の質量濃度も精度良く計測することができる。 Thereby, the mass concentration of PM2.5 and the mass concentration of PM10 can be calculated in time series. Since the actual measurement value of the mass concentration of PM10 is obtained, the accuracy of correction is improved. Therefore, not only PM2.5 but also the mass concentration of PM10 can be accurately measured.

 また、例えば、補正回路60は、補正として、推定した粒子数に基づいて、第2信号に基づいて算出したPM10の質量濃度を補正する。 For example, the correction circuit 60 corrects the mass concentration of PM10 calculated based on the second signal based on the estimated number of particles as correction.

 これにより、PM10の質量濃度の演算結果を補正するので、PM10の質量濃度を精度良く計測することができる。 Thereby, since the calculation result of the mass concentration of PM10 is corrected, the mass concentration of PM10 can be accurately measured.

 また、例えば、補正回路60は、補正として、推定した粒子数に基づいて粗大粒子の計測期間の長さを変更する。 Also, for example, the correction circuit 60 changes the length of the coarse particle measurement period based on the estimated number of particles as a correction.

 これにより、粗大粒子の計測に要する時間を長くすることができるので、粗大粒子の粒子数を一定数以上確保しやすくなる。したがって、PM2.5だけでなく、PM10の質量濃度も精度良く計測することができる。 This makes it possible to lengthen the time required for measuring coarse particles, so that it is easy to secure a certain number of coarse particles or more. Therefore, not only PM2.5 but also the mass concentration of PM10 can be accurately measured.

 また、例えば、信号処理回路50は、第2信号に基づいてPM10の質量濃度を算出する処理を所定回数繰り返し、得られた所定回数分の質量濃度を平均化することで、PM10の質量濃度を算出する。補正回路60は、補正として、上記繰り返しの回数(すなわち、サイクル数)を変更する。 Further, for example, the signal processing circuit 50 repeats the process of calculating the mass concentration of PM10 based on the second signal a predetermined number of times, and averages the obtained mass concentration for the predetermined number of times, thereby obtaining the mass concentration of PM10. calculate. The correction circuit 60 changes the number of repetitions (that is, the number of cycles) as correction.

 これにより、PM10の質量濃度の算出の際の平均化サイクルを長くすることができるので、粗大粒子の粒子数を一定数以上確保しやすくなる。したがって、PM2.5だけでなく、PM10の質量濃度も精度良く計測することができる。 This makes it possible to lengthen the averaging cycle when calculating the mass concentration of PM10, so that it is easy to secure a certain number of coarse particles. Therefore, not only PM2.5 but also the mass concentration of PM10 can be accurately measured.

 また、例えば、粒子検出センサ1は、さらに、検出領域DAに向けて対象流体を誘導する誘導装置40を備える。補正回路60は、補正として、第2期間内に誘導装置40によって誘導される対象流体の誘導量を変更する。 For example, the particle detection sensor 1 further includes a guidance device 40 that guides the target fluid toward the detection area DA. The correction circuit 60 changes the induction amount of the target fluid induced by the induction device 40 within the second period as correction.

 これにより、粗大粒子の粒子数の計測時に誘導される気体の量が多くなるので、粗大粒子の粒子数を一定数以上確保しやすくなる。したがって、PM2.5だけでなく、PM10の質量濃度も精度良く計測することができる。 This increases the amount of gas induced when measuring the number of coarse particles, so that it is easy to secure a certain number of coarse particles or more. Therefore, not only PM2.5 but also the mass concentration of PM10 can be accurately measured.

 (その他)
 以上、本発明に係る粒子検出センサについて、上記の実施の形態に基づいて説明したが、本発明は、上記の実施の形態に限定されるものではない。
(Other)
As mentioned above, although the particle | grain detection sensor which concerns on this invention was demonstrated based on said embodiment, this invention is not limited to said embodiment.

 例えば、上記の実施の形態では、対象流体が気体である場合を説明したが、これに限らない。対象流体は、水などの液体でもよい。粒子検出センサ1は、水などの液体中に含まれる粒子を検出し、質量濃度を算出する。このとき、粒子検出センサ1は、筐体10の外側面に取り付けられた信号処理回路50が液体に接触するのを防ぐ防水機構を有する。防水機構は、例えば、信号処理回路50を覆うように設けられた金属製のシールド部材である。当該シールド部材は、例えば溶接などにより筐体10に隙間なく固定される。 For example, in the above embodiment, the case where the target fluid is a gas has been described. However, the present invention is not limited to this. The target fluid may be a liquid such as water. The particle detection sensor 1 detects particles contained in a liquid such as water and calculates a mass concentration. At this time, the particle detection sensor 1 has a waterproof mechanism that prevents the signal processing circuit 50 attached to the outer surface of the housing 10 from coming into contact with the liquid. The waterproof mechanism is, for example, a metal shield member provided so as to cover the signal processing circuit 50. The shield member is fixed to the housing 10 without a gap by, for example, welding.

 また、例えば、粒子検出センサ1では、PM10粒子数の計測が行われなくてもよい。具体的には、信号処理回路50は、微小粒子の計測と、PM2.5の質量濃度の演算と、PM10の質量濃度の演算とをこの順に行ってもよい。PM10の質量濃度の演算では、PM2.5に含まれる微小粒子の粒子数の含有率に基づいて推定された粗大粒子の粒子数を用いて、PM10の質量濃度を算出してもよい。 Further, for example, the particle detection sensor 1 does not need to measure the number of PM10 particles. Specifically, the signal processing circuit 50 may perform measurement of fine particles, calculation of the mass concentration of PM2.5, and calculation of the mass concentration of PM10 in this order. In the calculation of the mass concentration of PM10, the mass concentration of PM10 may be calculated using the number of coarse particles estimated based on the content rate of the number of fine particles contained in PM2.5.

 また、例えば、補正回路60は、PM2.5の最大粒径のサブ区分ではなく、PM2.5に含まれる微小粒子の全粒子数に基づいて、粗大粒子の粒子数を推定してもよい。 Further, for example, the correction circuit 60 may estimate the number of coarse particles based on the total number of fine particles contained in PM2.5 instead of the subclass of the maximum particle size of PM2.5.

 また、例えば、粒子検出センサ1は、誘導装置40を備えなくてもよい。例えば、粒子検出センサ1は、一定方向に気流が流れている場所に、流入口11が気流の上流側、流出口12が下流側に位置するように配置されてもよい。 For example, the particle detection sensor 1 may not include the guidance device 40. For example, the particle detection sensor 1 may be arranged in a place where the airflow is flowing in a certain direction so that the inlet 11 is located upstream of the airflow and the outlet 12 is located downstream.

 また、例えば、上記の実施の形態では、投光部20及び受光部30の各々がレンズを備える例について示したが、これに限らない。例えば、投光部20及び受光部30の少なくとも一方は、レンズの代わりに、ミラー(反射体)を備えてもよい。 Further, for example, in the above-described embodiment, the example in which each of the light projecting unit 20 and the light receiving unit 30 includes a lens is shown, but the present invention is not limited thereto. For example, at least one of the light projecting unit 20 and the light receiving unit 30 may include a mirror (reflector) instead of the lens.

 なお、粒子検出センサ1は、例えば、エアコン、空気清浄機、換気扇などの各種家電機器などに搭載される。各種家電機器は、粒子検出センサ1によって検出された粒子の質量濃度に応じて、その動作を制御してもよい。例えば、空気清浄機は、粒子の質量濃度が所定の閾値より大きい場合に、運転強度(具体的には、空気の浄化力)を強くしてもよい。 In addition, the particle | grain detection sensor 1 is mounted in various household appliances, such as an air conditioner, an air cleaner, and a ventilation fan, for example. Various home appliances may control the operation according to the mass concentration of the particles detected by the particle detection sensor 1. For example, the air cleaner may increase the operating strength (specifically, the air purifying power) when the mass concentration of the particles is larger than a predetermined threshold.

 その他、各実施の形態に対して当業者が思いつく各種変形を施して得られる形態や、本発明の趣旨を逸脱しない範囲で各実施の形態における構成要素及び機能を任意に組み合わせることで実現される形態も本発明に含まれる。 In addition, the embodiment can be realized by arbitrarily combining the components and functions in each embodiment without departing from the scope of the present invention, or a form obtained by subjecting each embodiment to various modifications conceived by those skilled in the art. Forms are also included in the present invention.

1 粒子検出センサ
20 投光部
30 受光部
40 誘導装置
50 信号処理回路
60 補正回路
DA 検出領域
L1 光
L2 散乱光
DESCRIPTION OF SYMBOLS 1 Particle detection sensor 20 Light projection part 30 Light reception part 40 Guidance device 50 Signal processing circuit 60 Correction circuit DA Detection area | region L1 Light L2 Scattered light

Claims (7)

 対象流体に含まれる粒子を検出する粒子検出センサであって、
 検出領域に向けて光を出射する投光部と、
 前記投光部が出射する光に対して受光感度を有し、前記検出領域を通過する粒子による前記光の散乱光を光電変換することで電気信号を生成して出力する受光部と、
 前記電気信号に基づいて、第1粒子が含まれる第1粒径区分の第1質量濃度と、前記第1粒子及び当該第1粒子より大きい第2粒子が含まれる第2粒径区分の第2質量濃度とを算出する信号処理回路と、
 前記第1粒子の粒子数に基づいて前記第2粒子の粒子数を推定し、推定した粒子数に基づいて前記第2質量濃度の補正を行う補正回路とを備える
 粒子検出センサ。
A particle detection sensor for detecting particles contained in a target fluid,
A light projecting unit that emits light toward the detection region;
A light receiving unit that has light receiving sensitivity with respect to the light emitted from the light projecting unit, and generates and outputs an electrical signal by photoelectrically converting the scattered light of the light from the particles passing through the detection region;
Based on the electrical signal, the first mass concentration of the first particle size segment including the first particles and the second mass of the second particle size segment including the first particles and second particles larger than the first particles. A signal processing circuit for calculating the mass concentration;
A particle detection sensor comprising: a correction circuit that estimates the number of particles of the second particle based on the number of particles of the first particle and corrects the second mass concentration based on the estimated number of particles.
 前記第1粒子の粒子数は、前記第1粒径区分が分割された複数のサブ区分のうち、最大粒径のサブ区分に含まれる粒子数であり、
 前記補正回路は、前記第1粒子の粒子数の含有率に基づいて前記第2粒子の粒子数を推定する
 請求項1に記載の粒子検出センサ。
The number of particles of the first particle is the number of particles included in the sub-section of the maximum particle size among the plurality of sub-sections into which the first particle size section is divided
The particle detection sensor according to claim 1, wherein the correction circuit estimates the number of particles of the second particle based on a content ratio of the number of particles of the first particle.
 前記信号処理回路は、
 前記電気信号のうち第1期間分の第1信号に基づいて、前記第1質量濃度を算出し、
 前記電気信号のうち前記第1期間とは異なる第2期間分の第2信号に基づいて、前記第2質量濃度を算出する
 請求項1又は2に記載の粒子検出センサ。
The signal processing circuit includes:
Based on the first signal for the first period of the electrical signal, the first mass concentration is calculated,
The particle detection sensor according to claim 1, wherein the second mass concentration is calculated based on a second signal for a second period different from the first period in the electrical signal.
 前記補正回路は、前記補正として、推定した粒子数に基づいて、前記第2信号に基づいて算出した第2質量濃度を補正する
 請求項3に記載の粒子検出センサ。
The particle detection sensor according to claim 3, wherein the correction circuit corrects the second mass concentration calculated based on the second signal based on the estimated number of particles as the correction.
 前記補正回路は、前記補正として、推定した粒子数に基づいて前記第2期間の長さを変更する
 請求項3に記載の粒子検出センサ。
The particle detection sensor according to claim 3, wherein the correction circuit changes the length of the second period based on the estimated number of particles as the correction.
 前記信号処理回路は、前記第2信号に基づいて前記第2質量濃度を算出する処理を所定回数繰り返し、得られた所定回数分の質量濃度を平均化することで、前記第2質量濃度を算出し、
 前記補正回路は、前記補正として、前記所定回数を変更する
 請求項3に記載の粒子検出センサ。
The signal processing circuit calculates the second mass concentration by repeating the process of calculating the second mass concentration based on the second signal a predetermined number of times and averaging the obtained mass concentrations for the predetermined number of times. And
The particle detection sensor according to claim 3, wherein the correction circuit changes the predetermined number of times as the correction.
 さらに、前記検出領域に向けて前記対象流体を誘導する誘導装置を備え、
 前記補正回路は、前記補正として、前記第2期間内に前記誘導装置によって誘導される前記対象流体の誘導量を変更する
 請求項3に記載の粒子検出センサ。
And a guidance device for guiding the target fluid toward the detection region,
The particle detection sensor according to claim 3, wherein the correction circuit changes, as the correction, an induced amount of the target fluid that is induced by the guidance device within the second period.
PCT/JP2019/002077 2018-02-27 2019-01-23 Particle detecting sensor Ceased WO2019167485A1 (en)

Priority Applications (3)

Application Number Priority Date Filing Date Title
CN201980009433.4A CN111630365B (en) 2018-02-27 2019-01-23 Particle Detection Sensor
KR1020207021262A KR102321560B1 (en) 2018-02-27 2019-01-23 particle detection sensor
JP2020502864A JP6883770B2 (en) 2018-02-27 2019-01-23 Particle detection sensor

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
JP2018-033439 2018-02-27
JP2018033439 2018-02-27

Publications (1)

Publication Number Publication Date
WO2019167485A1 true WO2019167485A1 (en) 2019-09-06

Family

ID=67808827

Family Applications (1)

Application Number Title Priority Date Filing Date
PCT/JP2019/002077 Ceased WO2019167485A1 (en) 2018-02-27 2019-01-23 Particle detecting sensor

Country Status (5)

Country Link
JP (1) JP6883770B2 (en)
KR (1) KR102321560B1 (en)
CN (1) CN111630365B (en)
TW (1) TW201939009A (en)
WO (1) WO2019167485A1 (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US10935480B1 (en) 2018-09-26 2021-03-02 Airviz Inc. Optical-particle sensor head
WO2021129919A1 (en) * 2019-12-23 2021-07-01 Robert Bosch Gmbh Gaseous fluid monitor and method for monitoring properties of gaseous fluid
US12248103B2 (en) 2020-03-27 2025-03-11 National Yang Ming Chiao Tung University System and method for lidar defogging

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
TWI739528B (en) * 2020-07-24 2021-09-11 熱映光電股份有限公司 Gas detecting device
KR102681896B1 (en) * 2022-03-21 2024-07-05 (주)인프라칩 Method and apparatus for detecting density of fine dust

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2001337028A (en) * 2000-05-30 2001-12-07 Nikkiso Co Ltd Particle size distribution measuring method and apparatus
US8854621B1 (en) * 2012-08-29 2014-10-07 University Of South Florida Systems and methods for determining nanoparticle dimensions
WO2017051149A1 (en) * 2015-09-23 2017-03-30 Malvern Instruments Limited Particle characterisation
JP2017187381A (en) * 2016-04-06 2017-10-12 パナソニックIpマネジメント株式会社 Fine particle detection device

Family Cites Families (19)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3609043A (en) * 1968-11-19 1971-09-28 Parker Hannifin Corp Spray droplet analyzer
US3936666A (en) * 1974-09-16 1976-02-03 Coulter Electronics, Inc. Apparatus for measuring a particle size dividing one of the mass or particle number of a particulate system into predetermined fractions
JPH0718788B2 (en) * 1988-11-08 1995-03-06 富士電機株式会社 Optical particle measuring device
JPH0785052B2 (en) * 1990-11-17 1995-09-13 株式会社堀場製作所 Particle size distribution analysis method
JP3672158B2 (en) * 1997-03-10 2005-07-13 富士電機システムズ株式会社 Turbidity measuring method and apparatus
DE69938992D1 (en) * 1998-09-29 2008-08-14 Horiba Ltd Apparatus and method for measuring the particle size distribution
JP3645760B2 (en) * 1998-10-30 2005-05-11 株式会社堀場製作所 Particle size distribution analysis method
JP3302991B2 (en) * 1999-11-16 2002-07-15 独立行政法人 航空宇宙技術研究所 Particle size distribution measuring device
JP5104643B2 (en) * 2008-08-19 2012-12-19 株式会社島津製作所 Particle size measuring apparatus and particle size measuring method
JP5212224B2 (en) * 2009-03-31 2013-06-19 トヨタ自動車株式会社 Particle size distribution model preparation method, fuel cell catalyst deterioration prediction method using the particle size distribution model preparation method, and fuel cell control method using the fuel cell catalyst deterioration prediction method
KR100962541B1 (en) * 2010-02-11 2010-06-14 한은정 Method of calibration of particle counter
JP5950319B2 (en) * 2010-06-15 2016-07-13 新日本空調株式会社 Particle concentration measuring device
JP2015072135A (en) * 2013-10-01 2015-04-16 東邦チタニウム株式会社 Particle size distribution measurement method
EP3130909B1 (en) * 2014-04-08 2021-07-14 Mitsubishi Electric Corporation Floating particle detection device
CN203929579U (en) * 2014-04-11 2014-11-05 苏州宏瑞净化科技有限公司 A kind of binary channels high-flux dust particle sensor
JP2015210188A (en) * 2014-04-25 2015-11-24 パナソニックIpマネジメント株式会社 Particle measuring apparatus
JP6233711B2 (en) 2014-04-25 2017-11-22 パナソニックIpマネジメント株式会社 Particle measuring device
EP3214429B1 (en) * 2014-10-31 2021-03-03 Panasonic Intellectual Property Management Co., Ltd. Particle detection sensor
CN106018223A (en) * 2016-05-24 2016-10-12 深圳市蜂联科技有限公司 Method for improving measurement precision of air quality detection equipment by segmentation optimal calibration

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2001337028A (en) * 2000-05-30 2001-12-07 Nikkiso Co Ltd Particle size distribution measuring method and apparatus
US8854621B1 (en) * 2012-08-29 2014-10-07 University Of South Florida Systems and methods for determining nanoparticle dimensions
WO2017051149A1 (en) * 2015-09-23 2017-03-30 Malvern Instruments Limited Particle characterisation
JP2017187381A (en) * 2016-04-06 2017-10-12 パナソニックIpマネジメント株式会社 Fine particle detection device

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US10935480B1 (en) 2018-09-26 2021-03-02 Airviz Inc. Optical-particle sensor head
WO2021129919A1 (en) * 2019-12-23 2021-07-01 Robert Bosch Gmbh Gaseous fluid monitor and method for monitoring properties of gaseous fluid
US12248103B2 (en) 2020-03-27 2025-03-11 National Yang Ming Chiao Tung University System and method for lidar defogging

Also Published As

Publication number Publication date
CN111630365A (en) 2020-09-04
KR102321560B1 (en) 2021-11-03
KR20200099588A (en) 2020-08-24
JPWO2019167485A1 (en) 2020-12-03
CN111630365B (en) 2023-02-24
JP6883770B2 (en) 2021-06-09
TW201939009A (en) 2019-10-01

Similar Documents

Publication Publication Date Title
KR102321560B1 (en) particle detection sensor
US20200011779A1 (en) Highly integrated optical particle counter (opc)
KR101913973B1 (en) Particle detection sensor
US9995667B2 (en) Portable device for detecting and measuring particles entrained in the air
US8009290B2 (en) Compact, low cost particle sensor
CN1898551B (en) Method for measuring scattered light signal and scattered light detector for realizing the method
CN210051741U (en) Vehicle air quality detection device with calibration function and vehicle
CN110987745A (en) Particulate matter detection device and detection method
KR20200009707A (en) Fine dust detection device and method
CN111051851B (en) Particle detection sensor
KR102017257B1 (en) Small-sized optical fine dust sensor capable of counting by particle size
JP6233711B2 (en) Particle measuring device
JP7110852B2 (en) Particle sensors and electronics
CN111051853B (en) Particle detection system and particle detection method
KR101844941B1 (en) Particle counter with particle counting device which removes electrical noise
JP2016212024A (en) Fine particle detection device
JP5907498B1 (en) Particle detection sensor
JP3783991B2 (en) Smoke detector
KR20180113341A (en) Apparatus for sensing particle
CN208607120U (en) A kind of particle sensor with zero reference calibration module
WO2022210258A1 (en) Smoke detector
JP2003106982A (en) Dust amount detector

Legal Events

Date Code Title Description
121 Ep: the epo has been informed by wipo that ep was designated in this application

Ref document number: 19760787

Country of ref document: EP

Kind code of ref document: A1

ENP Entry into the national phase

Ref document number: 2020502864

Country of ref document: JP

Kind code of ref document: A

ENP Entry into the national phase

Ref document number: 20207021262

Country of ref document: KR

Kind code of ref document: A

NENP Non-entry into the national phase

Ref country code: DE

122 Ep: pct application non-entry in european phase

Ref document number: 19760787

Country of ref document: EP

Kind code of ref document: A1