CN107271331A - A kind of measuring method of pipe tobacco to main flume flow resistance coefficient - Google Patents

A kind of measuring method of pipe tobacco to main flume flow resistance coefficient Download PDF

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Publication number
CN107271331A
CN107271331A CN201710560756.5A CN201710560756A CN107271331A CN 107271331 A CN107271331 A CN 107271331A CN 201710560756 A CN201710560756 A CN 201710560756A CN 107271331 A CN107271331 A CN 107271331A
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pipe tobacco
main flume
cigarette
flue gas
resistance coefficient
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曾劲松
杜亮
唐大荣
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South China University of Technology SCUT
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South China University of Technology SCUT
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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N11/00Investigating flow properties of materials, e.g. viscosity, plasticity; Analysing materials by determining flow properties
    • G01N11/02Investigating flow properties of materials, e.g. viscosity, plasticity; Analysing materials by determining flow properties by measuring flow of the material
    • G01N11/04Investigating flow properties of materials, e.g. viscosity, plasticity; Analysing materials by determining flow properties by measuring flow of the material through a restricted passage, e.g. tube, aperture
    • G01N11/08Investigating flow properties of materials, e.g. viscosity, plasticity; Analysing materials by determining flow properties by measuring flow of the material through a restricted passage, e.g. tube, aperture by measuring pressure required to produce a known flow

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  • Physics & Mathematics (AREA)
  • Health & Medical Sciences (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Chemical & Material Sciences (AREA)
  • Analytical Chemistry (AREA)
  • Biochemistry (AREA)
  • General Health & Medical Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • Immunology (AREA)
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  • Measuring Volume Flow (AREA)

Abstract

The invention discloses a kind of measuring method of pipe tobacco to main flume flow resistance coefficient.Pipe tobacco is used as porous media, its resistance coefficient flowed to main flume mainly includes pipe tobacco with the coefficient of frictional resistance of mainstream smoke contacts generation and because tobacco structure changes the inertial resistance coefficient produced, is represented respectively with viscosity factor and inertial resistance coefficient.On flue gas experiment machine platform, mainstream smoke velocity by pipe tobacco is measured using PIV, using pressure gage measurement pipe tobacco inlet and outlet two ends pressure difference, the quadratic polynomial for obtaining the mainstream smoke velocity by pipe tobacco and pipe tobacco two ends pressure difference will be fitted using origin or matlab softwares by the mainstream smoke velocity of pipe tobacco and pipe tobacco two ends pressure difference, then the pressure fall equation of pipe tobacco is substituted into quadratic polynomial and obtains viscosity factor and the inertial resistance coefficient size that pipe tobacco flows to main flume.

Description

A kind of measuring method of pipe tobacco to main flume flow resistance coefficient
Technical field
The present invention relates to the technical field of measurement main flume flow resistance coefficient, a kind of pipe tobacco is referred in particular to mainstream smoke The measuring method of flow of air resistance coefficient.
Background technology
The measuring method for liquid flowing resistance coefficient mainly uses thermometer, flowmeter, fluid column differential manometer at present The straight tube resistance coefficient and coefficient of partial resistance of fluid, this method are calculated by measuring the mechanical power loss of fluid Deng instrument It is generally used for the drag losses caused when liquid flows in simply pipeline due to liquid and pipe friction and pipeline deformation;For The measuring method of gas flow resistance coefficient is mainly flowed using instruments such as blower fan, disk, dynamometer, pressure gauges by measuring Resistance, gas density, flow velocity, limited areal calculate the resistance coefficient of gas.
Although there is the measuring method of a variety of measurement fluid flow resistance coefficients both at home and abroad, PIV technologies and pressure are utilized Pipe tobacco not yet occurs to main flume flow resistance coefficient when strong meter is to measure suction cigarette.
The content of the invention
It is a primary object of the present invention to overcome the shortcoming and deficiency of prior art there is provided a kind of pipe tobacco to mainstream smoke air-flow The measuring method of dynamic resistance coefficient, pipe tobacco glues to main flume flowing when can accurately measure suction cigarette by this method Property resistance coefficient and inertial resistance coefficient.
In order to achieve the above object, the present invention uses following technical scheme:
The invention discloses a kind of measuring method of pipe tobacco to main flume flow resistance coefficient, comprise the following steps:
(1) flowing velocity of the cigarette smoke in suction sleeve when suction cigarette is shot according to PIV system experimentations, by taking out Inhale sleeve in velocity of flue gas push away cigarette outlet mainstream smoke velocity;
(2) the inlet and outlet two ends pressure difference of pipe tobacco is measured using pressure gage, in atmosphere, its is relative for the import of pipe tobacco The pressure of air is 0, and the pressure p of the outlet relative atmospheric of pipe tobacco need to be only measured with pressure1, then can calculate pipe tobacco import and Export two ends pressure difference Δ p=-p1
(3) it will be entered by the mainstream smoke velocity of pipe tobacco and pipe tobacco two ends pressure difference using origin or matlab softwares Row fitting obtains the quadratic polynomial Δ p=A ν of pipe tobacco two ends pressure difference and the mainstream smoke velocity by pipe tobaccoi+Bνi 2
(4) pressure fall equation of pipe tobacco is derived according to the equation of momentum of porous media:
I represents flow direction of the main flume in pipe tobacco in above-mentioned formula (1), and Δ p is that pipe tobacco two ends pressure difference, μ are Smoke power viscosity,Viscosity factor, the ν flowed for pipe tobacco to main flumeiTo pass through the mainstream smoke velocity of pipe tobacco, C Inertial resistance coefficient, the ρ flowed for pipe tobacco to main flume is that the density of flue gas, Δ n are cigarette length;
(5) by the pressure fall equation of pipe tobaccoThe fitting of origin softwares is substituted into obtain Quadratic polynomial Δ p=A νi+Bνi 2, obtainSo as to try to achieve pipe tobacco to mainstream smoke air-flow Dynamic viscosity factorThe inertial resistance coefficient C flowed with pipe tobacco to main flume.
As preferred technical scheme, in step (1), the main flume is the flue gas that suction side is flowed in cigarette, main It is to flow to suction side to flow flow direction of the flue gas in pipe tobacco.
As preferred technical scheme, the main flume is a kind of special aerosol, and its solid phase particles included can Using the trace particle as PIV system photographs.
As preferred technical scheme, in step (1), the suction sleeve is clear glass material, can be used in PIV systems The shooting united to flue gas.
As preferred technical scheme, in step (1), the PIV systems include laser, CCD camera, synchronizer and meter The part of calculation machine four, the computer of PIV systems controls laser to send horizontal laser light by the coordinative role of synchronizer, is irradiated to On solid particle in flue gas, computer controls the flow image of CCD camera shooting flue gas by the coordinative role of synchronizer, Image obtains the flowing velocity of flue gas after PIV systems carry software processing.
As preferred technical scheme, the velocity of flue gas in step (1) in suction sleeve push away cigarette outlet main flow Velocity of flue gas, its specific method is:
The flue gas flow that being pushed away according to the continuity equation of fluid must aspirate in sleeve is equal to the flue gas flow Q that cigarette is exported1 =Q2, i.e. VSleeveASleeve=VCigarette is exportedACigarette is exported, the velocity of flue gas aspirated in sleeve is converted into the mainstream smoke velocity of cigarette outlet, Wherein VSleeveFor the velocity of flue gas in suction sleeve, ASleeveFor suction sleeve cross-sectional area, VCigarette is exportedThe main flume exported for cigarette Speed, ACigarette is exportedFor cigarette exit cross-sectional area.
As preferred technical scheme, in step (2), pressure gage includes pressure feeler inspection syringe needle, signal transmitting device and pressure Display recorder;The pressure that the signal transmitting device of pressure gage can sound out pressure feeler inspection syringe needle carries out signal transacting, will locate Signal after reason passes to pressure display recorder, shows pressure size.
As preferred technical scheme, the pressure drop side of pipe tobacco is derived in step (4) by the equation of momentum of porous media Journey, its specific method is:
The equation of momentum of porous media is:
Push away the pressure fall equation of pipe tobacco is:
Δ p=-SiΔ n, i.e.,
I represents flow direction of the main flume in pipe tobacco, S in formulaiFor the source item of the equation of momentum, μ glues for smoke power Degree,Viscosity factor, the ν flowed for pipe tobacco to main flumeiTo be pipe tobacco to master by the mainstream smoke velocity of pipe tobacco, C Inertial resistance coefficient, the ρ of stream flow of flue gas are that the density of flue gas, Δ p are that pipe tobacco two ends pressure difference, Δ n are cigarette length.
The present invention compared with prior art, has the following advantages that and beneficial effect:
(1) present invention uses non-intrusion measurement, and pressure gage measurement pipe tobacco exports the pressure of relative atmospheric, and PIV shoots and taken out The velocity of flue gas in sleeve is inhaled, interference is not produced to flowing of the main flume in pipe tobacco;
(2) present invention can tested once to the measurement of mainstream smoke velocity and the measurement of pipe tobacco import and export pressure differential In carry out simultaneously, it is to avoid experimental error during separated measurement;
(3) measuring method of the present invention can measure the viscosity factor that pipe tobacco flows to main flume, and can survey The inertial resistance coefficient that amount pipe tobacco flows to main flume.
Brief description of the drawings
Fig. 1 passes through the mainstream smoke velocity of pipe tobacco and the experiment schematic diagram of pipe tobacco import and export two ends pressure difference for measurement;
Fig. 2 is flow chart of the pipe tobacco to main flume flow resistance coefficient measuring method.
Embodiment
With reference to embodiment and accompanying drawing, the present invention is described in further detail, but embodiments of the present invention are not limited In this.
Embodiment
As shown in figure 1, measuring the mainstream smoke velocity and pipe tobacco import and export two ends pressure difference by pipe tobacco for the present embodiment Experiment schematic diagram, including:Cigarette 1, pressure gage syringe needle socket 2, laser irradiated plane 3, CCD camera 4 and flue gas experimental machine System 5;Above-mentioned experiment realizes that the computer of the PIV systems controls to swash by the coordinative role of synchronizer based on PIV systems Light device sends horizontal laser light, is irradiated on the solid particle in flue gas, and computer controls CCD by the coordinative role of synchronizer Camera shoots the flow image of flue gas, and image obtains the flowing velocity of flue gas after PIV systems carry software processing.
Based on above-mentioned experiment schematic diagram, as shown in Fig. 2 measurement of the present embodiment pipe tobacco to main flume flow resistance coefficient Method, comprises the steps:
(1) flowing velocity of the cigarette smoke in suction sleeve, is covered by suction when suction cigarette is shot according to PIV experiment Velocity of flue gas in cylinder push away cigarette outlet mainstream smoke velocity, the main flume is to flow to the cigarette of suction side in cigarette Gas, flow direction of the main flume in pipe tobacco is to flow to suction side;Main flume is as a kind of special aerosol, and it is wrapped The trace particle that the solid phase particles contained can be shot as PIV;
Velocity of flue gas in suction sleeve push away cigarette outlet mainstream smoke velocity, its specific method is:
The flue gas flow that being pushed away according to the continuity equation of fluid must aspirate in sleeve is equal to the flue gas flow Q that cigarette is exported1 =Q2, i.e. VSleeveASleeve=VCigarette is exportedACigarette is exported, the velocity of flue gas aspirated in sleeve is converted into the mainstream smoke velocity of cigarette outlet. (V in above-mentioned formulaSleeveFor the velocity of flue gas in suction sleeve, ASleeveFor suction sleeve cross-sectional area, VCigarette is exportedExported for cigarette Mainstream smoke velocity, ACigarette is exportedFor cigarette exit cross-sectional area)
(2) the pressure gage syringe needle socket for stretching into the pressure feeler inspection syringe needle of pressure gage in flue gas experimental machine, using pressure gage The inlet and outlet two ends pressure difference of pipe tobacco is measured, in atmosphere, the pressure of its relative atmospheric is 0 for the import of pipe tobacco, only needs to use Pressure measures the pressure p of the outlet relative atmospheric of pipe tobacco1, then the inlet and outlet two ends pressure difference Δ p=- of pipe tobacco can be calculated p1
(3) it will be fitted and obtained using origin softwares by the mainstream smoke velocity of pipe tobacco and pipe tobacco two ends pressure difference The quadratic polynomial Δ p=A ν of pipe tobacco two ends pressure difference and the mainstream smoke velocity by pipe tobaccoi+Bνi 2
(4) pressure fall equation of pipe tobacco is derived according to the equation of momentum of porous media (i represents flow direction of the main flume in pipe tobacco in above-mentioned formula, Δ p be pipe tobacco two ends pressure difference, μ be smoke power viscosity,Viscosity factor, the ν flowed for pipe tobacco to main flumeiTo pass through the mainstream smoke gas velocity of pipe tobacco Degree, C are that inertial resistance coefficient, ρ that pipe tobacco flows to main flume are that the density of flue gas, Δ n are cigarette length).
The pressure fall equation of pipe tobacco is derived by the equation of momentum of porous media, its specific method is:
The equation of momentum of porous media is:Push away the pressure fall equation of pipe tobacco is: Δ p=-SiΔ n, i.e.,(i represents stream of the main flume in pipe tobacco in above-mentioned formula Dynamic direction, SiFor the source item of the equation of momentum, μ be smoke power viscosity,The viscous drag system flowed for pipe tobacco to main flume Number, νiTo be that inertial resistance coefficient, ρ that pipe tobacco flows to main flume are the close of flue gas by the mainstream smoke velocity of pipe tobacco, C Degree, Δ p are that pipe tobacco two ends pressure difference, Δ n are cigarette length);
(5) by the pressure fall equation of pipe tobaccoThe fitting of origin softwares is substituted into obtain Quadratic polynomial Δ p=A νi+Bνi 2, obtainSo as to try to achieve pipe tobacco to mainstream smoke air-flow Dynamic viscosity factorThe inertial resistance coefficient C flowed with pipe tobacco to main flume.
Above-described embodiment is preferably embodiment, but embodiments of the present invention are not by above-described embodiment of the invention Limitation, other any Spirit Essences without departing from the present invention and the change made under principle, modification, replacement, combine, simplification, Equivalent substitute mode is should be, is included within protection scope of the present invention.

Claims (8)

1. a kind of pipe tobacco is to the measuring method of main flume flow resistance coefficient, it is characterised in that comprise the following steps:
(1) flowing velocity of the cigarette smoke in suction sleeve, is covered by suction when suction cigarette is shot according to PIV system experimentations Cylinder in velocity of flue gas push away cigarette outlet mainstream smoke velocity;
(2) using pressure gage measure pipe tobacco inlet and outlet two ends pressure difference, the import of pipe tobacco in atmosphere, its relative atmospheric Pressure be 0, only need to be measured with pressure pipe tobacco outlet relative atmospheric pressure p1, then the inlet and outlet of pipe tobacco can be calculated Two ends pressure difference Δ p=-p1
(3) it will be intended by the mainstream smoke velocity of pipe tobacco and pipe tobacco two ends pressure difference using origin or matlab softwares Close the quadratic polynomial Δ p=A ν for obtaining pipe tobacco two ends pressure difference and the mainstream smoke velocity by pipe tobaccoi+Bνi 2
(4) pressure fall equation of pipe tobacco is derived according to the equation of momentum of porous media:
<mrow> <mi>&amp;Delta;</mi> <mi>p</mi> <mo>=</mo> <mrow> <mo>(</mo> <mfrac> <mi>&amp;mu;</mi> <mi>&amp;alpha;</mi> </mfrac> <msub> <mi>v</mi> <mi>i</mi> </msub> <mo>+</mo> <mi>C</mi> <mfrac> <mn>1</mn> <mn>2</mn> </mfrac> <mi>&amp;rho;</mi> <mo>|</mo> <mi>v</mi> <mo>|</mo> <msub> <mi>v</mi> <mi>i</mi> </msub> <mo>)</mo> </mrow> <mi>&amp;Delta;</mi> <mi>n</mi> <mo>;</mo> <mo>-</mo> <mo>-</mo> <mo>-</mo> <mrow> <mo>(</mo> <mn>1</mn> <mo>)</mo> </mrow> </mrow>
I represents flow direction of the main flume in pipe tobacco in above-mentioned formula (1), and Δ p is that pipe tobacco two ends pressure difference, μ are flue gas Dynamic viscosity,Viscosity factor, the ν flowed for pipe tobacco to main flumeiTo be cigarette by the mainstream smoke velocity of pipe tobacco, C Inertial resistance coefficient that silk flows to main flume, ρ are that the density of flue gas, Δ n are cigarette length;
(5) by the pressure fall equation of pipe tobaccoSubstitute into the fitting of origin softwares is obtained two Order polynomial Δ p=A νi+Bνi 2, obtainSo as to try to achieve what pipe tobacco flowed to main flume Viscosity factorThe inertial resistance coefficient C flowed with pipe tobacco to main flume.
2. measuring method of the pipe tobacco to main flume flow resistance coefficient according to claim 1, it is characterised in that step (1) in, the main flume is flows to the flue gas of suction side in cigarette, flow direction of the main flume in pipe tobacco is flow direction Suction side.
3. measuring method of the pipe tobacco to main flume flow resistance coefficient according to claim 2, it is characterised in that the master Stream flue gas is a kind of special aerosol, its solid phase particles included can as PIV system photographs trace particle.
4. measuring method of the pipe tobacco to main flume flow resistance coefficient according to claim 1, it is characterised in that step (1) in, the suction sleeve is clear glass material, can be used in shooting of the PIV systems to flue gas.
5. measuring method of the pipe tobacco to main flume flow resistance coefficient according to claim 1, it is characterised in that step (1) in, the PIV systems include laser, CCD camera, synchronizer and the part of computer four, and the computer of PIV systems passes through The coordinative role of synchronizer controls laser to send horizontal laser light, is irradiated on the solid particle in flue gas, computer passes through The coordinative role of synchronizer come control CCD camera shoot flue gas flow image, image is after PIV systems carry software processing Obtain the flowing velocity of flue gas.
6. measuring method of the pipe tobacco to main flume flow resistance coefficient according to claim 1, it is characterised in that step (1) velocity of flue gas in suction sleeve push away cigarette outlet mainstream smoke velocity, its specific method is:
The flue gas flow that being pushed away according to the continuity equation of fluid must aspirate in sleeve is equal to the flue gas flow Q that cigarette is exported1=Q2, That is VSleeveASleeve=VCigarette is exportedACigarette is exported, the velocity of flue gas aspirated in sleeve is converted into the mainstream smoke velocity of cigarette outlet, wherein VSleeveFor the velocity of flue gas in suction sleeve, ASleeveFor suction sleeve cross-sectional area, VCigarette is exportedThe mainstream smoke gas velocity exported for cigarette Degree, ACigarette is exportedFor cigarette exit cross-sectional area.
7. measuring method of the pipe tobacco to main flume flow resistance coefficient according to claim 1, it is characterised in that step (2) in, pressure gage includes pressure feeler inspection syringe needle, signal transmitting device and pressure display recorder;The signal transmitting device energy of pressure gage The enough pressure for souning out pressure feeler inspection syringe needle carries out signal transacting, and the signal after processing is passed into pressure display recorder, Show pressure size.
8. measuring method of the pipe tobacco to main flume flow resistance coefficient according to claim 1, it is characterised in that step (4) pressure fall equation of pipe tobacco is derived in by the equation of momentum of porous media, its specific method is:
The equation of momentum of porous media is:
<mrow> <msub> <mi>S</mi> <mi>i</mi> </msub> <mo>=</mo> <mo>-</mo> <mrow> <mo>(</mo> <mfrac> <mi>&amp;mu;</mi> <mi>&amp;alpha;</mi> </mfrac> <msub> <mi>v</mi> <mi>i</mi> </msub> <mo>+</mo> <mi>C</mi> <mfrac> <mn>1</mn> <mn>2</mn> </mfrac> <mi>&amp;rho;</mi> <mo>|</mo> <mi>v</mi> <mo>|</mo> <msub> <mi>v</mi> <mi>i</mi> </msub> <mo>)</mo> </mrow> <mo>,</mo> </mrow>
Push away the pressure fall equation of pipe tobacco is:
Δ p=-SiΔ n, i.e.,
I represents flow direction of the main flume in pipe tobacco, S in formulaiFor the source item of the equation of momentum, μ be smoke power viscosity, Viscosity factor, the ν flowed for pipe tobacco to main flumeiTo be pipe tobacco to mainstream smoke by the mainstream smoke velocity of pipe tobacco, C Inertial resistance coefficient, the ρ of flow of air are that the density of flue gas, Δ p are that pipe tobacco two ends pressure difference, Δ n are cigarette length.
CN201710560756.5A 2017-07-11 2017-07-11 A kind of measuring method of pipe tobacco to main flume flow resistance coefficient Pending CN107271331A (en)

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Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN108333292A (en) * 2018-02-05 2018-07-27 江苏中烟工业有限责任公司 The devices and methods therefor of internal change in pressure drop during a kind of the real time measure cigarette burning
CN109187844A (en) * 2018-08-31 2019-01-11 华南理工大学 A kind of measuring method for the nearly pipe tobacco end flue gas rate of cigarette smoking process filter tip

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN1122670A (en) * 1994-07-11 1996-05-22 大世吕化学工业株式会社 Method of estimation of an aeration resistance in a filter plug
CN104764582A (en) * 2015-03-30 2015-07-08 华南理工大学 Smoke field measurement device and method based on PIV system
CN106706268A (en) * 2017-02-28 2017-05-24 吉林大学 Method and device for measuring viscous resistance coefficient and inertial resistance coefficient of porous medium

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN1122670A (en) * 1994-07-11 1996-05-22 大世吕化学工业株式会社 Method of estimation of an aeration resistance in a filter plug
CN104764582A (en) * 2015-03-30 2015-07-08 华南理工大学 Smoke field measurement device and method based on PIV system
CN106706268A (en) * 2017-02-28 2017-05-24 吉林大学 Method and device for measuring viscous resistance coefficient and inertial resistance coefficient of porous medium

Non-Patent Citations (5)

* Cited by examiner, † Cited by third party
Title
PIV MEASUREMENT OF MAINSTREAM FLOW IN CIGARETTE SMOKE: "Jingsong Zeng et al.", 《6TH INTERNATIONAL CONFERENCE ON ENERGY, ENVIRONMENT AND SUSTAINABLE DEVELOPMENT(ICEESD 2017) ADVANCES IN ENGINEERING RESEARCH》 *
中国核学会: "《中国核科学技术进展报告(第二卷)》", 31 October 2012, 中国原子能出版社 *
余其昌 等: "基于CFD模拟卷烟烟气扩散过程的影响因素", 《烟草科技》 *
朱德祥 等: "《第21届全国水动力学研讨会暨第8届全国水动力学学术会议暨两岸船舶与海洋工程水动力学研讨会文集》", 31 August 2008 *
李栋 等: "《埋地输油管道泄漏污染物热质迁移实验技术》", 31 March 2017, 哈尔滨工业大学出版社 *

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN108333292A (en) * 2018-02-05 2018-07-27 江苏中烟工业有限责任公司 The devices and methods therefor of internal change in pressure drop during a kind of the real time measure cigarette burning
CN109187844A (en) * 2018-08-31 2019-01-11 华南理工大学 A kind of measuring method for the nearly pipe tobacco end flue gas rate of cigarette smoking process filter tip

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