CN113218816B - Method for testing density of unknown gas at different temperatures by using thermogravimetric method - Google Patents

Method for testing density of unknown gas at different temperatures by using thermogravimetric method Download PDF

Info

Publication number
CN113218816B
CN113218816B CN202110511821.1A CN202110511821A CN113218816B CN 113218816 B CN113218816 B CN 113218816B CN 202110511821 A CN202110511821 A CN 202110511821A CN 113218816 B CN113218816 B CN 113218816B
Authority
CN
China
Prior art keywords
gas
density
value
temperature
volume
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.)
Active
Application number
CN202110511821.1A
Other languages
Chinese (zh)
Other versions
CN113218816A (en
Inventor
余亮
王哲
蒋文波
陈富航
谷少鹏
董婧蒙
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.)
Chongqing University
Original Assignee
Chongqing University
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 Chongqing University filed Critical Chongqing University
Priority to CN202110511821.1A priority Critical patent/CN113218816B/en
Publication of CN113218816A publication Critical patent/CN113218816A/en
Application granted granted Critical
Publication of CN113218816B publication Critical patent/CN113218816B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N9/00Investigating density or specific gravity of materials; Analysing materials by determining density or specific gravity
    • G01N9/08Investigating density or specific gravity of materials; Analysing materials by determining density or specific gravity by measuring buoyant force of solid materials by weighing both in air and in a liquid
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N9/00Investigating density or specific gravity of materials; Analysing materials by determining density or specific gravity
    • G01N9/36Analysing materials by measuring the density or specific gravity, e.g. determining quantity of moisture

Landscapes

  • 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)
  • Pathology (AREA)
  • Investigating Or Analyzing Materials Using Thermal Means (AREA)

Abstract

The invention discloses a method for testing density of unknown gas at different temperatures by using a thermogravimetric method, which comprises the following steps of; step one, as the buoyancy effect is caused by the change of the gas density, the density of different gases can be distinguished by utilizing the phenomenon, the gas flow is ensured to be consistent when the thermal analysis test is carried out, the gas flow is controlled by using a mass flowmeter, the T value can be described as T-G-F (1) from the analysis of the T value of the thermal analysis, and the T value is cleared to zero in order to facilitate the calculation when the test is started; the invention can test the density of the known gas at different temperatures, the density of the unknown gas at different temperatures and the volume of the small object with different properties by utilizing the buoyancy effect of the thermal analysis TG curve.

Description

Method for testing density of unknown gas at different temperatures by using thermogravimetric method
Technical Field
The invention relates to the technical field of gas density testing, in particular to a method for testing densities of unknown gas at different temperatures by using a thermogravimetric method.
Background
In industrial applications, the petrochemical industry, the electronics industry, and all industries involving the use of gases have a need to test the density of the gas. Current methods of measuring gas density are by scales; a measuring cylinder; and bottles with plugs and good sealing performance can not be tested by simple and crude instruments, automatic measurement cannot be realized, and the change of gas density under different temperature changes cannot be accurately measured.
Disclosure of Invention
The invention aims to overcome the defects that the prior method for testing the gas density passes through a balance; a measuring cylinder; the method for testing the density of the unknown gas at different temperatures by using the thermogravimetric method has the effects of testing the density of the known gas at different temperatures, the density of the unknown gas at different temperatures and the small object volume of the different types by using the buoyancy effect of a thermal analysis TG curve.
In order to achieve the purpose, the invention provides the following technical scheme: a method for testing the density of unknown gas at different temperatures by using a thermogravimetric method comprises the following steps;
step one, as the buoyancy effect is caused by the change of gas density, the phenomenon can be used for distinguishing the densities of different gases, the gas flow is ensured to be consistent when a thermal analysis test is carried out, a mass flowmeter is used for controlling the gas flow, the T value can be described as T (G-F (1)) from the analysis of the thermal analysis T value, in the formula (1), T is a thermogravimetric balance numerical value, G is the gravity of a support, F is the buoyancy of the support, and when the test is started, the T value is required to be cleared to zero in order to facilitate calculation;
step two, the buoyancy of the object in the gas can be expressed as F ═ ρ gV (2), and it can be obtained in formula (2) that F is the buoyancy to which the support is subjected, ρ is the gas density, g is the gravity acceleration, V is the support volume, and the gas density is mainly affected by three factors, i.e. 1 gas type, 2 temperature, and 3 atmosphere pressure standard conditions (0 ℃, 100 kPa);
step three, when the temperature in the thermal analysis furnace body rises, the density of the gas is reduced along with the rise of the temperature, the atmospheric pressure at the same place is unchanged, the gravity acceleration is also unchanged, the volume of the bracket is slightly increased, the change of V can be obtained through calculation, and the volume expansion of the gas is far greater than that of the bracket, so that the T value of the thermal analysis TG curve is gradually increased along with the temperature, and the increase of the T value is mainly influenced by the reduction of the density of the gas;
fourthly, calculating the density of the gas at the known temperature at different temperature points by utilizing the buoyancy effect; knowing that the change of the T value at any two points in the curve is the increase of the T value due to the change of the gas buoyancy, Tb-Ta-rho agV-rho bgV (3) can be obtained, the T value at any temperature can be read by a thermobalance, gV-Ta)/(rho a-rho b (4) can be obtained, and the density value of the gas at any other temperature point can be calculated from rho-rho b- (T-Tb)/gV (5);
step five, calculating the density of the unknown gas according to the density of the known gas; at the same temperature, g is gravity acceleration, V is the same volume of the stent, and then the change of the T value is mainly related to the gas density, so that Te/ρ e ═ k ═ ρ a (Ta/ρ a) (6) can be obtained for different gases at the same temperature, Te and Ta in the formula (6) are respectively the T values of the known gas tests, k is a correction coefficient, ρ a and ρ e are gas a, and the density of the gas e is obtained, then k ═ Ta ═ ρ e/Te ═ ρ a (7) can be obtained, and in the case of the known T value, any unknown gas density ρ ═ k ═ T ═ ρ a/Ta (7) can be obtained;
calculating the volume change of the small special-shaped object according to the known gas; in the same gas, although the gas density is the same, the buoyancy is different due to different volumes of objects such as different crucibles, so that the difference with the temperature change can be displayed on the thermal analysis thermogravimetric curve, the volume of an unknown object including the volume of an object with opposite sex can be obtained by utilizing the difference, the k value can be obtained by calculation by using the volume of a known object, and the arbitrary small object volume formula can be obtained as V VaT/kTa (10).
Preferably, any desired gas molar volume is 22.4L/mol.
Compared with the prior art, the invention provides a method for testing the density of unknown gas at different temperatures by using a thermogravimetric method, which has the following beneficial effects:
the invention can utilize buoyancy effect of thermal analysis TG curve to test density of known gas at different temperatures, density of unknown gas at different temperatures and volume of small object with different characteristics, the thermogravimetric analyzer is used for testing weight change of a sample along with temperature change process, because the resolution of the thermal analysis balance is milligram precision, the thermogravimetric data precision of the sample test is very high, atmosphere with constant mass, generally argon, helium, nitrogen, air, carbon dioxide and the like, is introduced into a furnace body in order to protect or react the sample in the thermal analysis test process, and baseline test is carried out on the instrument before the sample is tested to deduct background, the degree of the balance is generated by the sample in the gas under the combined action of gravity and buoyancy in the gas, because the buoyancy in the gas is too small relative to the gravity, the buoyancy in the gas is often ignored, and the minute change can be sensed under high precision, the buoyancy effect is shown as that the TG value is gradually increased along with the temperature increase, the gas density is reduced due to the temperature increase in the temperature rise process, the buoyancy of a sample support surrounded by gas is reduced, and the gravity is unchanged, so that the TG value of the balance reaction is increased, the baseline background of the TG value is different in the heating process when different gases are introduced into a furnace body experiment, although the buoyancy effect is not beneficial to the baseline deduction of the thermogravimetric analysis of the sample, the buoyancy effect is caused by the change of the gas density, so that the density of different gases can be distinguished by using the phenomenon, the gas flow is ensured to be consistent when the thermogravimetric analysis test is carried out, and the mass flow meter is used for controlling the gas flow.
Drawings
FIG. 1 is a graph showing the variation of a blank TG curve under different gases according to the present invention;
FIG. 2 is a graph showing the variation of blank TG curves of crucibles of different sizes in the same gas.
Detailed Description
The following detailed description of embodiments of the invention refers to the accompanying drawings. It should be understood that the detailed description and specific examples, while indicating the present invention, are given by way of illustration and explanation only, not limitation.
Referring to fig. 1-2, the present invention provides a technical solution: a method for testing the density of unknown gas at different temperatures by using a thermogravimetric method comprises the following steps;
step one, as the buoyancy effect is caused by the change of gas density, the phenomenon can be used for distinguishing the densities of different gases, the gas flow is ensured to be consistent when a thermal analysis test is carried out, a mass flowmeter is used for controlling the gas flow, the T value can be described as T (G-F (1)) from the analysis of the thermal analysis T value, in the formula (1), T is a thermogravimetric balance numerical value, G is the gravity of a support, F is the buoyancy of the support, and when the test is started, the T value is required to be cleared to zero in order to facilitate calculation;
step two, the buoyancy of the object in the gas can be expressed as F ═ ρ gV (2), it can be obtained in formula (2) that F is the buoyancy to which the support is subjected, ρ is the gas density, g is the gravitational acceleration, and V is the support volume, and the gas density is mainly affected by three factors, i.e. 1 gas type, 2 temperatures, and 3 atmospheric pressure standard conditions (0 ℃, 100 kPa);
step three, when the temperature in the thermal analysis furnace body rises, the density of the gas is reduced along with the rise of the temperature, the atmospheric pressure at the same place is unchanged, the gravity acceleration is also unchanged, the volume of the bracket is slightly increased, the change of V can be obtained through calculation, and the volume expansion of the gas is far greater than the expansion of the bracket, so that the T value of a thermal analysis TG curve is gradually increased along with the temperature, and the increase of the T value is mainly influenced by the reduction of the density of the gas;
fourthly, calculating the density of the gas at the known temperature at different temperature points by utilizing the buoyancy effect; knowing that the change of the T value at any two points in the curve is the increase of the T value due to the change of the gas buoyancy, Tb-Ta can be obtained as ρ agV- ρ bgV (3), the T value at any temperature can be read by a thermobalance, gV can be obtained as (Tb-Ta)/(ρ a- ρ b) (4), and the density value of the gas to obtain other any temperature points can be calculated as ρ b- (T-Tb)/gV (5);
step five, calculating the density of the unknown gas according to the density of the known gas; at the same temperature, g is gravity acceleration, V is the same volume of the stent, and then the change of the T value is mainly related to the gas density, so that Te/ρ e ═ k ═ ρ a (Ta/ρ a) (6) can be obtained for different gases at the same temperature, Te and Ta in the formula (6) are respectively the T values of the known gas tests, k is a correction coefficient, ρ a and ρ e are gas a, and the density of the gas e is obtained, then k ═ Ta ═ ρ e/Te ═ ρ a (7) can be obtained, and in the case of the known T value, any unknown gas density ρ ═ k ═ T ═ ρ a/Ta (7) can be obtained;
step six, calculating the volume change of the small irregular object according to the known gas; in the same gas, although the gas density is the same, the buoyancy is different due to different volumes of objects such as different crucibles, so that the difference with the temperature change can be displayed on the thermal analysis thermogravimetric curve, the volume of an unknown object including the object with the opposite sex can be obtained by utilizing the volume of the known object, the k value can be obtained by calculation through Ta/rho gVa (kTe/rho gVe (8), and the k value can be obtained through TeVa/Tave (9), so that the arbitrary small object volume formula can be obtained, wherein V is VaT/kTa (10).
In the present invention, it is preferred that any desired gas molar volume be 22.4L/mol.
Example 1
A method for testing the density of unknown gas at different temperatures by using a thermogravimetric method comprises the following steps;
firstly, because the buoyancy effect is caused by the change of gas density, the phenomenon can be used for distinguishing the densities of different gases, the gas flow is ensured to be consistent when a thermal analysis test is carried out, a mass flowmeter is used for controlling the gas flow, a T value can be described as T (G-F (1) from the analysis of a thermal analysis T value, and the T value is required to be cleared to zero in order to facilitate calculation when the test is started;
step two, the buoyancy of the object in the gas can be expressed as F ═ ρ gV (2), and the density of the gas is mainly influenced by three factors, namely 1 gas type, 2 temperature and 3 atmospheric pressure standard conditions (0 ℃, 100 kPa);
step three, when the temperature in the thermal analysis furnace body rises, the density of the gas is reduced along with the rise of the temperature, the atmospheric pressure at the same place is unchanged, the gravity acceleration is also unchanged, the volume of the bracket is slightly increased, the change of V can be obtained through calculation, and the volume expansion of the gas is far greater than that of the bracket, so that the T value of the thermal analysis TG curve is gradually increased along with the temperature, and the increase of the T value is mainly influenced by the reduction of the density of the gas;
fourthly, calculating the density of the gas at the known temperature at different temperature points by utilizing the buoyancy effect; knowing that the change of the T value at any two points in the curve is the increase of the T value due to the change of the gas buoyancy, Tb-Ta-rho agV-rho bgV (3) can be obtained, the T value at any temperature can be read by a thermobalance, gV-Ta)/(rho a-rho b (4) can be obtained, and the density value of the gas at any other temperature point can be calculated from rho-rho b- (T-Tb)/gV (5);
step five, calculating the density of the unknown gas according to the density of the known gas; at the same temperature, g is the gravity acceleration, V is the same volume of the bracket, and the change of the T value is mainly related to the gas density, so that Te/rho (k) is obtained by different gases at the same temperature (Ta/rho a) (6);
calculating the volume change of the small special-shaped object according to the known gas; in the same gas, although the gas density is the same, the buoyancy is different due to different volumes of objects such as different crucibles, and therefore, the difference with the temperature change can be displayed on the thermal analysis thermogravimetric curve, and by utilizing the difference, the volume of an unknown object including the object volume with the opposite sex can be obtained by utilizing the volume of a known object, the k value can be obtained by calculation at Ta/rho gVa ═ kTe/rho gVe (8), and the k value can be obtained at TeVa/Tave (9), so that the arbitrary small object volume formula can be obtained as V ═ VaT/kTa (10).
Example 2
In the formula (1), T is a thermogravimetric balance value, G is a support gravity, F is a buoyancy force applied to the support, in the formula (2), F can be obtained as the buoyancy force applied to the support, ρ is a gas density, G is a gravity acceleration, V is a support volume, any ideal gas molar volume is 22.4L/mol, in the formula (6), Te and Ta are respectively a T value of a known gas test, k is a correction coefficient, ρ a and ρ e are a gas a and a gas e density, so that k is Ta ρ e/Te ρ a (7) can be obtained, and in the case of the known T value, any unknown gas density ρ is k ρ T ρ a/Ta (7) can be obtained.
The invention can utilize buoyancy effect of thermal analysis TG curve to test density of known gas at different temperatures, density of unknown gas at different temperatures and volume of small object with different characteristics, the thermogravimetric analyzer is used for testing weight change of a sample along with temperature change process, because the resolution of the thermal analysis balance is milligram precision, the thermogravimetric data precision of the sample test is very high, atmosphere with constant mass, generally argon, helium, nitrogen, air, carbon dioxide and the like, is introduced into a furnace body in order to protect or react the sample in the thermal analysis test process, and baseline test is carried out on the instrument before the sample is tested to deduct background, the degree of the balance is generated by the sample in the gas under the combined action of gravity and buoyancy in the gas, because the buoyancy in the gas is too small relative to the gravity, the buoyancy in the gas is often ignored, and the minute change can be sensed under high precision, the buoyancy effect appears in TG analysis, the buoyancy effect shows that TG value is gradually increased along with temperature increase, gas density is reduced due to temperature increase in the temperature rise process, buoyancy of a sample support surrounded by gas is reduced, and gravity is unchanged, so that TG value of balance reaction is increased, the phenomenon shows that base line background of TG value is different in the heating process when different gases are introduced into a furnace body experiment, although the buoyancy effect is not beneficial to base line deduction of thermogravimetric analysis of the sample, the buoyancy effect is caused by gas density change, so that the density of different gases can be distinguished by the phenomenon, gas flow is ensured to be consistent when the thermogravimetric analysis test is carried out, and the mass flow meter is used for controlling gas flow.
The preferred embodiments of the present invention have been described above in detail, but the present invention is not limited thereto. Within the scope of the technical idea of the invention, many simple modifications can be made to the technical solution of the invention, including various technical features being combined in any other suitable way, and these simple modifications and combinations should also be regarded as the disclosure of the invention, and all fall within the scope of the invention.

Claims (2)

1. A method for testing the density of unknown gas at different temperatures by using a thermogravimetric method is characterized by comprising the following steps;
step one, as the buoyancy effect is caused by the change of the gas density, the density of different gases can be distinguished by utilizing the phenomenon, the gas flow is ensured to be consistent when a thermal analysis test is carried out, the gas flow is controlled by using a mass flow meter, the T value can be described as T-G-F (1) from the analysis of the T value of the thermal analysis, in the formula (1), T is the value of a thermal gravimetric balance, G is the gravity of a support, F is the buoyancy force borne by the support, and the T value needs to be reset in order to facilitate calculation when the test is started;
step two, the buoyancy of the object in the gas can be expressed as F ═ ρ gV (2), and it can be obtained in formula (2) that F is the buoyancy to which the support is subjected, ρ is the gas density, g is the gravitational acceleration, and V is the support volume;
step three, when the temperature in the thermal analysis furnace body rises, the density of the gas is reduced along with the rise of the temperature, the atmospheric pressure at the same place is unchanged, the gravity acceleration is also unchanged, the volume of the bracket is slightly increased, the change of V can be obtained through calculation, and the volume expansion of the gas is far greater than that of the bracket, so that the T value of the thermal analysis TG curve is gradually increased along with the temperature, and the increase of the T value is mainly influenced by the reduction of the density of the gas;
fourthly, calculating the density of the gas at the known temperature at different temperature points by utilizing the buoyancy effect; knowing that the change of the T value at any two points in the curve is the increase of the T value due to the change of the gas buoyancy, Tb-Ta-rho agV-rho bgV (3) can be obtained, the T value at any temperature can be read by a thermobalance, gV-Ta)/(rho a-rho b (4) can be obtained, and the density value of the gas at any other temperature point can be calculated from rho-rho b- (T-Tb)/gV (5);
step five, calculating the density of the unknown gas according to the density of the known gas; at the same temperature, g is gravity acceleration, V is the same volume of the stent, and then the change of the T value is mainly related to the gas density, so that Te/ρ e ═ k ═ ρ a (Ta/ρ a) (6) can be obtained for different gases at the same temperature, Te and Ta in the formula (6) are respectively the T values of the known gas tests, k is a correction coefficient, ρ a and ρ e are gas a, and the density of the gas e is obtained, then k ═ Ta ═ ρ e/Te ═ ρ a (7) can be obtained, and in the case of the known T value, any unknown gas density ρ ═ k ═ T ═ ρ a/Ta (7) can be obtained;
step six, calculating the volume change of the small irregular object according to the known gas; in the same gas, although the gas density is the same, the buoyancy is different due to different volumes of different crucibles, so that the difference with the temperature change can be displayed on the thermogravimetric curve of thermal analysis, the volume of an unknown object including the object with the opposite property can be obtained by utilizing the volume of the known object by utilizing the difference, the k value can be obtained by calculation through Ta/rho gVa (kTe/rho gVe (8), and the k value can be obtained by calculation through TeVa/Tave (9), so that the arbitrary small object volume formula can be obtained as V (VaT/kTa) (10).
2. The method of claim 1, wherein the desired gas molar volume is 22.4L/mol for any desired gas.
CN202110511821.1A 2021-05-11 2021-05-11 Method for testing density of unknown gas at different temperatures by using thermogravimetric method Active CN113218816B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN202110511821.1A CN113218816B (en) 2021-05-11 2021-05-11 Method for testing density of unknown gas at different temperatures by using thermogravimetric method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN202110511821.1A CN113218816B (en) 2021-05-11 2021-05-11 Method for testing density of unknown gas at different temperatures by using thermogravimetric method

Publications (2)

Publication Number Publication Date
CN113218816A CN113218816A (en) 2021-08-06
CN113218816B true CN113218816B (en) 2022-07-15

Family

ID=77094670

Family Applications (1)

Application Number Title Priority Date Filing Date
CN202110511821.1A Active CN113218816B (en) 2021-05-11 2021-05-11 Method for testing density of unknown gas at different temperatures by using thermogravimetric method

Country Status (1)

Country Link
CN (1) CN113218816B (en)

Citations (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB254232A (en) * 1926-03-08 1926-07-01 Alfred Stock A magnetic balance for weighing small masses, ascertaining the density of gases, and for other purposes
CN101405600A (en) * 2006-03-17 2009-04-08 株式会社理光 Gas analyzer
CN205538550U (en) * 2015-10-12 2016-08-31 鞍山安然燃气设备有限公司 Gaseous dynamic close measuring device
CN107257918A (en) * 2015-01-05 2017-10-17 沙特阿拉伯石油公司 Crude oil and its fraction are characterized by thermogravimetric analysis
CN107884115A (en) * 2016-09-30 2018-04-06 中国石油天然气股份有限公司 Method and device for measuring air buoyancy change
CN108225528A (en) * 2017-10-18 2018-06-29 赛多利斯科学仪器(北京)有限公司 Folding electronic balance density measure kit device
CN109060595A (en) * 2018-07-05 2018-12-21 天津力神电池股份有限公司 A method of detection lithium ion battery separator ceramic coating surface density
CN111351733A (en) * 2020-03-12 2020-06-30 中国科学院上海微系统与信息技术研究所 High-precision thermo-gravimetric analyzer

Patent Citations (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB254232A (en) * 1926-03-08 1926-07-01 Alfred Stock A magnetic balance for weighing small masses, ascertaining the density of gases, and for other purposes
CN101405600A (en) * 2006-03-17 2009-04-08 株式会社理光 Gas analyzer
CN107257918A (en) * 2015-01-05 2017-10-17 沙特阿拉伯石油公司 Crude oil and its fraction are characterized by thermogravimetric analysis
CN205538550U (en) * 2015-10-12 2016-08-31 鞍山安然燃气设备有限公司 Gaseous dynamic close measuring device
CN107884115A (en) * 2016-09-30 2018-04-06 中国石油天然气股份有限公司 Method and device for measuring air buoyancy change
CN108225528A (en) * 2017-10-18 2018-06-29 赛多利斯科学仪器(北京)有限公司 Folding electronic balance density measure kit device
CN109060595A (en) * 2018-07-05 2018-12-21 天津力神电池股份有限公司 A method of detection lithium ion battery separator ceramic coating surface density
CN111351733A (en) * 2020-03-12 2020-06-30 中国科学院上海微系统与信息技术研究所 High-precision thermo-gravimetric analyzer

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
KNO3-NaNO2系熔盐的物理化学性质研究;章凯羽;《中国优秀博硕士学位论文全文数据库(硕士) 工程科技Ⅰ辑》;20120315(第03期);第1-65页 *
静风环境热重气体行为模式分析;张兴凯 等;《中国安全生产科学技术》;20051031;第1卷(第5期);第8-11页 *

Also Published As

Publication number Publication date
CN113218816A (en) 2021-08-06

Similar Documents

Publication Publication Date Title
Poulter et al. Thermal transpiration correction in capacitance manometers
CN102589809A (en) Portable leak detector calibration system and method
CN113218816B (en) Method for testing density of unknown gas at different temperatures by using thermogravimetric method
CN111044560A (en) Method for rapidly evaluating service life of atomic gas chamber
CN107515379B (en) Method for testing quality of high-low temperature low-pressure test chamber
Mizushima et al. Mass measurement of 1 kg silicon spheres to establish a density standard
CN117537954A (en) Geological cold and hot table correction method
Kuchkarov et al. Investigation of particular parameters of a semiconductor ammonia gas analyzer
Watanabe Thermal dilatation of water between 0° C and 44° C
Ooiwa et al. New mercury interferometric baromanometer as the primary pressure standard of Japan
Kovacich et al. Highly accurate measurement of oxygen using a paramagnetic gas sensor
Wortman et al. Gas transport in vitreous silica fibers
Keyes High-Pressure Technic1
CN105043928A (en) Foundry moulding sand gas-forming property testing device and gas-forming property obtaining method based on same
Rodebush et al. A NEW ABSOLUTE MANOMETER FOR LOW PRESSURES
CN117647300B (en) CVD online in-situ weighing system and method
CN110310711B (en) Uncertainty assessment method for impurity content analysis result of diamond micropowder
CN117849111A (en) Method for measuring hydrogen concentration in metal material
JP4247493B2 (en) Humidity measuring method and humidity measuring device
CN107356624B (en) Method for judging melting speed of crystallizer covering slag
Sauer Experimental Automatic Recording Dilatometer for Thermal Expansion and Shrinkage Studies over the Temperature Range− 150 to+ 1500° C
Berry Oxygen–Activated Thermal Cycling Effects in Pt Resistance Thermometers
Madley et al. An apparatus for the micro-analysis of gas samples
Zhao et al. Thermal stability evaluation of sheathed platinum resistance sensor based on nitride nano-coating
CN116106362A (en) Method for measuring high-temperature specific heat capacity of titanium alloy and titanium-based composite material

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant