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E-mail
ruixinjie01@163.com
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Phone
18611697209
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Address
B1-1514, Xinlong Building, No. 87 Building Materials City West Road, Changping District, Beijing
Beijing Ruixinjie Environmental Protection Technology Co., Ltd
ruixinjie01@163.com
18611697209
B1-1514, Xinlong Building, No. 87 Building Materials City West Road, Changping District, Beijing
【RG310P Type infrared gas analyzer】

RG310P The series of infrared gas analyzers are designed by our company for environmental monitoring and industrial site emissions of gases Analyze the independently developed infrared gas analyzer. This analyzer mainly measures CO、CO2、N2O、CH4 and O2 waitGas concentration, with high measurement accuracy, stability, and reliabilityCharacteristics such as high performance and fast response time.
【RG310P Infrared Gas AnalyzerApplication scenarios】
l Smoke emission detection (analysis of CO) 、CO2 、N2O 、CH4 、O2)
l Greenhouse gas detection (analysis of CO)2 、N2O 、CH4)
l Motor vehicle exhaust emission testing (analysis of CO) 、HC 、CO2)
【feature】
l Adopting single beam dual wavelength technology, compared with traditional NDIR, there is no need for a filter wheel, and the system is stable and reliablerely on
l H2O Interference deduction, real-time measurement of H2O thick度修正 H2O Interference with other measured components
l Using multiple reflection chambers, the instrument has a low detection limit
l The instrument has high internal temperature control accuracy and good environmental adaptability
l The light source adopts MEMS infrared radiation light source, and electrical modulation does not require a chopper wheel
l No optical moving parts, no cutting wheel, filtering wheel, interferometer and other optical moving parts,high reliability
l Modular design, using light sources, core circuits, gas chambers, oxygen sensors, temperature control units, etc
l Modular design, high reliability, good scalability, and easy maintenance
【Technical Specifications】
project |
Specifications |
Instructions |
CO measurement range |
(0~ 100)ppm |
Scalable range |
CO2 measurement range |
(0~25)% |
Scalable range |
N2O Measurement range |
(0~25)ppm |
Scalable range |
CH4 measurement range |
(0~500)ppm |
Scalable range |
HC measurement range |
(0~500)ppm |
Scalable range |
O2 range |
(0~25)% |
|
detection limit |
≤1% F.S. |
|
indication error |
≤±2% F.S. |
|
repetitiveness |
Not more than 2% |
|
stability |
Not more than 2% |
|
Suggested traffic |
(2~3)L/min |
|
zero drift |
±2%F.S. (24 hour) |
@100ppm |
Span Drift |
±2%F.S. (24 hour) |
|
response time |
Not exceeding 60 seconds |
@2L/min |
The impact of environmental temperature changes |
Not exceeding ± 2% F.S |
|
The impact of changes in power supply voltage |
Not exceeding ± 0.5% F.S |
|
Influence of interfering components |
CO2 For CO<± 1% F.S |
|
CO2 Regarding N2O<±1%F.S |
|
|
CO、N2O Cross interference<± 1% F.S |
|
|
H2O Regarding CO2 <0.2% |
|
|
H2O For CO not exceeding 0.5ppm |
|
|
H2O Regarding N2O is not greater than 0.2ppm |
|
|
H2O Regarding CH4 <1ppm |
|
|
Parallelism |
≤2% |
|
Working environment temperature |
15~35°C |
recommend |
analog quantity I/O |
6 Roadband isolation 4-20mA output |
|
digital quantity I/O |
6 digital inputs (5-24V) 7 Road relay output |
|
serial port |
1 RS232 1 RS485 |
|
ambient humidity |
≤98% |
|
Power Supply/Power |
220VAC±10%, 100W |
|
warm-up time |
90-120min |
|
Overall dimensions |
480mm(D)x306mm(W)133mm(H) |
|
weight |
10KG |
|
l Beer-Lambert law
image 1 Gas absorption process
I(λ) = I0(λ) * e-σ(λ)CL
Where:
I0(λ)-------The wavelength is λ The incident light intensity of the light;
I(λ)---------The wavelength is λ The emitted light of the lightstrength;
σ(λ) ---------Gas at wavelength λAbsorption cross-section;
e-------------Gas concentration to be tested;
L--------------The interaction between gas and lightUsing length (effective length of gas pool);
Beer-Lambert The law is the basis of optical quantitative analysis of substance concentration, which is shown in the tableCollecting the absorption of specific wavelengths of light by substances situation It can be seen that, with known absorption cross-section and optical path length, measuring the incident and outgoing light intensities is sufficient Calculate the concentration of the corresponding gas.
l CO2 、CO 、N2O 、CH4 Waiting for gas infraredabsorption cross-section

image 2 Infrared absorption cross-section
CO2 、CO、N2O and CH4 There are obvious characteristic absorption spectral lines in the range of (3000-5000) nm This can be measured simultaneously using infrared spectroscopy for these four gases.
l Single beam dual wavelength technology
Single beam dual wavelength technology uses a single beam to illuminate a multi-channel detector for a specific substance to be tested One of the channels is the measurement channel, and the other channel is the reference channel. The wavelength corresponding to the measurement channel is the absorption of the substance to be measured The wavelength corresponding to the reference channel in the receiving area is the substance to be tested and the backgroundThe area without gas absorption.
By comparing the measurement channel with the reference channel, it is possible to eliminate fluctuations in the energy of the light source and changes in the overall characteristics of the detector The impact of coming.
image 3 Single beam dual wavelength technology
2 Optical path structure
image Optical path structure of analyzer 4