赤松 ラジカル自発光と › mpe06009 › HomePage › Che…2 S 1 S 2 For Example,, Then f...
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ラジカル自発光とラジカル自発光とラジカル自発光とラジカル自発光と
その計測その計測その計測その計測
ラジカル自発光とラジカル自発光とラジカル自発光とラジカル自発光と
その計測その計測その計測その計測
燃焼工学講座燃焼工学講座燃焼工学講座燃焼工学講座 赤松赤松赤松赤松 史光史光史光史光
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Spectrum of flame luminosity
Non-luminous Flame
11.4 mm
Direct photograph of the Bunsen flamewith the measurement point of MICROand electro-static probe
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Spectrum of flame luminosity
Luminous Flame
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OH and CH chemiluminescences are emitted in thedeactivation course (2) of OH* and (4) of CH*produced from the reaction (1) and (3), respectively.
CH + O2 ---> CO + OH* (1) OH* ---> OH + h νννν (2)
C2 + OH ---> CO + CH* (3) CH* ---> CH + h νννν (4)
where the superscript * denotes an excited state, h isthe Plank’s constant, and νννν is the frequency of thechemiluminescence.
OH and CH radical chemiluminescences
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Direct photograph of Bunsen flame withmeasurement point
11.4 mm
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Single-lens optics for point measurement
Paraxial Approximation, Gaussian Lens Equation
S1 S2
S1 S2
In Typical Case,S1 S2
S1S2For Example, , Then
f0: Focal Length
Control Volume
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可視域可視域可視域可視域 紫外域紫外域紫外域紫外域赤外域赤外域赤外域赤外域
OH* 306.4 nm
CH* 431.5 nm
C2*516.5 nm
Convex Lens
Concave + convex mirrors
Conventional method
Newly proposed method
Chromatic aberration of optics
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1f0
= (n−1) 1r1
− 1r2
�
� �
�
� �
Refractive index and focal lengthas functions of wavelength
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Typical aberration of point measurement optics
DL=50mm, f0=150mm
S2opt = 285.1 mm
近軸公式では
at Wave Length for Lens Design, λ λ λ λ = 546.1 nmSpherical Aberration
Chromatic Aberration
Rays passing through outer portion of lens are focused closer to the lens.
The shorter the rays' wave length, The shorter the focal length
Paraxial App. GLE
S2opt = 257.4 mmat OH-radical Wave Length, λ λ λ λ = 310 nm
S2 = 300 mmRay-Tracing Method
T i l Ab i f P i
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Dpopt
Control volume
285.1
Pinhole
S2opt
’300260
Ray-Tracing Method
Y
mm
Y mm
(light wave length for the lens design: 546.1nm)Circle of Least Confusion
Optimum pinhole location and diameterusing ray-tracing method (DL=50mm)
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Optimum pinhole location and diameteras functions of lens diameter
546.1nm
310nm
opt
S2op
t
Wave Length for Lens Design
OH-radical Wave Length
285.1
257.4
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300
Optimum pinhole location and diameteras functions of wavelength
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Single-lens optics and Cassegrain optics
Single-Lens Optics
Cassegrain Optics
Control Volume
Control Volume
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MICRO probe
Front viewFront viewFront viewFront view Side viewSide viewSide viewSide view
Bird eyeBird eyeBird eyeBird eye’s views views views view
Multi-color Integrated CassegrainReceiving Optics (MICRO)
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Cassegrain optics
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Sperical aberration of single-lensand Cassegrain optics
Single-Lens Optics Cassegrain Optics
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Estimation method of point measurementoptics and distribution of collection rate
Collection Rate G = Solid Angle of OpticsTotal Solid Angle (4π)π)π)π)
G
Direction to Optics
Pinhole
Control volume
Estimation Method of Point Measurement
= Total Rays Rays collected onto Pinhole
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Collection rate distributions ofsingle-lens and Cassegrain optics
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Measured collection rate distributions
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Light detection system of Cassegrain optics
紫外光透過コア径200
for UV, Core Diam. 200 µµµµm
Control volume
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OH C2(0,0)
488 nmCH
C2(0,1)
New Light detection system of Cassegrain
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・・・・No Chromatic Aberration Consisting of only mirrors
・・・・Minimum Spherical Aberration Optimization of two mirrors’ curvature combination
・・・・Very High Light Collection Rate Large diameter optics can be available due to elimination of spherical aberration.
・・・・Short Control Volume Length Along Optical Path Minimum spherical aberration and masking effect of the center of convex mirror
・・・・Easy Alignment of Optics Control volume can be visualized
Advantage of the MICRO system
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Direct photograph of Bunsen flame withmeasurement point
11.4 mm
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Ion current is produced from the followingreactions.
CH + O ---> CHO+ + e- (1) CH + C2H2 ---> C3H3
+ + e- (2)
OH chemiluminescence is emitted in the deactivationcourse (3) of OH* produced from the reaction (4).
CH + O2 ---> CO + OH* (3) OH* ---> OH + h νννν (4)
where the superscript * denotes an excited state, h isthe Plank’s constant, and νννν is the frequency of thechemiluminescence.
Ion current and OH chemiluminescence
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Time-series signals of ion current obtained by electro-static probe, and OH chemiluminescence obtained byMICRO and single-lens optics
100
200
300
400
Ion
n
A
0
50
100
150
200
0
10
2030
40
0 10 20 30 40 50 60 70 80 90
Time ms
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400
600
800
1000
0
100
200
300
0 50 100Time ms
Time-series signals of OH radical chemiluminescence bythe MICRO and ion current by the electro-static probe
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CLx
x
PMMSPMCH
PMOH
FMSP
FOH
FCH P
PDM1
DM2
DM: Dicroic mirror PM: Photomultiplier F : Optical filter CL : Collection lens P : Pinhole
Light guide
CL
x-x
4mm
2mm
Previous point measurement system
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Example of MICRO Application
MICRO
Mirror
Interference filter
Burner port
Cylindrical lens
Optical fiber cable
Pulse delay generator
Lens
Extension tube
Image intensifier
CCD camera
V/V amp.
Low pass filter A/D
PC
Detection unit
Argon-ion laser
PC
I/V OH I/V CH I/V MS
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0
10
20
30
0
100
200
0
50
50 55 60Time ms
t=55.2 ms t=56.1 ms t=57.0 ms t=57.9 ms t=58.8 ms
15
85
Simultaneous measurement with images
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Rayleigh scattering measurement
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Photograph of experiment
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Measurement of spectrum
Fiber (φφφφ=0.1mm)
50mm
Fiber
(φφφφ=0.1mm,N.A.=0.2)
r
z
Cassegrain Optics
Nozzle burner(φφφφ10mm)
Grating
CCDI.I.
Mirror
Processor PC
Fiber
MonochromatorMonochromator
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Spectrum of flame luminosity
Wavelength (nm)
Emis
sion
inte
nsity
(rela
tive)
300 350 400 450 5000
1 CassegrainFiber
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Change of spectrum with location
Wavelength (nm)
Emis
sion
inte
nsity
(a.u
.)
300 350 400 450 500
0.730.760.78
r/R=CH4-air
premixed
OH*(0,0)
CH*(0,0)
C2*(0,0)
C2*(1,0)
1E4
0
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Wavelength (nm)
Emis
sion
inte
nsity
(a.u
.)
300 350 400 450 500
0.810.840.9
r/R=1E3
Change of spectrum with location
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0.7 0.8
0.8
1
r/R
Emis
sion
inte
nsity
(rela
tive)
0.5 1 1.50
0.5
1
OH*(0,0)CH*(0,0)C2*(0,0)
Unburned
Burned
Locations of chemiluminescence intensity peak
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Wavelength (nm)
Emis
sion
inte
nsity
(a.u
.)
300 350 400 450 500
0.91.11.21.3
OH*(0,0)
0
1E4CH*(0,0)
C2*(1,0)
C2*(0,0)
CH4-air premixed
φ=
Change of spectrum with equivalence ratio
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Emis
sion
inte
nsity
(rela
tive)
0
1
(4,3)(3,2)(2,1)(1,0)(1,0)Band
Equivalence ratio
Em
issi
onin
tens
ity(re
lativ
e)
0.9 1 1.1 1.2 1.3 1.4
(0,0)Q(0,0)Q(1,1)R(1,1)QBand
OH
Em
issi
onin
tens
ity(re
lativ
e)
(0,0)Band
CH*
C2*(1,0)
(a)
(b)
(c)
Equivalence ratio
Emis
sion
inte
nsity
(rela
tive)
0.9 1 1.1 1.2 1.3 1.4 1.50
1
(1,1)(0,0)(0,0)Band
C2*(0,0) (d)
Change of peak intensity with equivalence ratio
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Equivalence ratio
Emis
sion
inte
nsity
(rela
tive)
0.9 1 1.1 1.2 1.3 1.4 1.510-1
100
101
C2*/CH*C2*/OH*OH*/CH*
CH4/Air Premixed
Single-lens optics for point measurement
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425 430 435
0.91.11.21.3
CH*(0,0)Q
(2,2)R
Emis
sion
inte
nsity
(a.u
.)
305 310 3150
1E4OH*
(0,0)R
(0,0)Q
(1,1)R
(1,1)Q
Wavelength (nm)
Emis
sion
inte
nsity
(a.u
.)
465 470 475
(5,4) (4,3)
C2*(1,0)1E4
0
(2,1)(3,2)
(1,0)
CH4-air premixed
Wavelength (nm)505 510 515 520
(1,1)
C2*(0,0)
(2,2)
(0,0)
φ=
Change of spectrum with equivalence ratio
![Page 41: 赤松 ラジカル自発光と › mpe06009 › HomePage › Che…2 S 1 S 2 For Example,, Then f 0: Focal Length Control Volume 可視域 紫外域 赤外域 OH* 306.4 nm CH* 43](https://reader034.fdocument.pub/reader034/viewer/2022042315/5f03a5827e708231d40a13f5/html5/thumbnails/41.jpg)
Measurement of time-series spectrum
![Page 42: 赤松 ラジカル自発光と › mpe06009 › HomePage › Che…2 S 1 S 2 For Example,, Then f 0: Focal Length Control Volume 可視域 紫外域 赤外域 OH* 306.4 nm CH* 43](https://reader034.fdocument.pub/reader034/viewer/2022042315/5f03a5827e708231d40a13f5/html5/thumbnails/42.jpg)
Multi-point measurement