ASTM D4222-2003(2015)e1 Standard Test Method for Determination of Nitrogen Adsorption and Desorption Isotherms of Catalysts and Catalyst Carriers by Static Volumetric Measurements《.pdf
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1、Designation: D4222 03 (Reapproved 2015)1Standard Test Method forDetermination of Nitrogen Adsorption and DesorptionIsotherms of Catalysts and Catalyst Carriers by StaticVolumetric Measurements1This standard is issued under the fixed designation D4222; the number immediately following the designation
2、 indicates the year oforiginal adoption or, in the case of revision, the year of last revision. A number in parentheses indicates the year of last reapproval. Asuperscript epsilon () indicates an editorial change since the last revision or reapproval.1NOTEEq 10 in subsection 12.4.7 was corrected edi
3、torially in August 2015.1. Scope1.1 This test method covers the determination of nitrogenadsorption and desorption isotherms of catalysts and catalystcarriers at the boiling point of liquid nitrogen.2A staticvolumetric measuring system is used to obtain sufficientequilibrium adsorption points on eac
4、h branch of the isotherm toadequately define the adsorption and desorption branches ofthe isotherm. Thirty points evenly spread over the isotherm isconsidered to be the minimum number of points that willadequately define the isotherm.1.2 The values stated in SI units are to be regarded as thestandar
5、d. The values given in parentheses are for informationonly.1.3 This standard does not purport to address all of thesafety concerns, if any, associated with its use. It is theresponsibility of the user of this standard to establish appro-priate safety and health practices and determine the applica-bi
6、lity of regulatory limitations prior to use.2. Referenced Documents2.1 ASTM Standards:3D3663 Test Method for Surface Area of Catalysts andCatalyst CarriersD3766 Terminology Relating to Catalysts and CatalysisE177 Practice for Use of the Terms Precision and Bias inASTM Test MethodsE456 Terminology Re
7、lating to Quality and StatisticsE691 Practice for Conducting an Interlaboratory Study toDetermine the Precision of a Test Method3. Terminology3.1 DefinitionsSee Terminology D3766.3.2 Symbols:PH1= initial helium pressure, torr.PH2= helium pressure after equilibration, torr.TH1= temperature of manifol
8、d at initial helium pressure,C.TH2= temperature of manifold after equilibration, C.P1= initial N2pressure, torr.T1= manifold temperature at initial N2pressure, K.T1= manifold temperature at initial N2pressure, C.P2= pressure after equilibration, torr.T2= manifold temperature after equilibrrium, K.T2
9、= manifold temperature after equilibrium, C.P3= initial N2pressure during desorption, torr.T3= manifold temperature at initial N2pressure, K.T3= manifold temperature at initial N2pressure, C.P4= pressure after equilibration during desorption, torr.T4= manifold temperature after equilibration, K.T4=
10、manifold temperature after equilibration, C.P0= liquid nitrogen vapor pressure, torr.Ts= liquid nitrogen temperature, K.X = relative pressure, P2(4)/P0.Vd= volume of manifold, cm3.Vs= the dead-space volume factor, cm3(STP)/torr.Ws= mass of sample, g.W1= tare of sample tube, g.W2= sample mass + tare
11、of tube after degassing, g.W2= sample mass + tare of tube after adsorption, g.Vds= volume of nitrogen in the dead-space, cm3(STP).V1= see 12.4.3.V2= see 12.4.4.Vt= see 12.4.5.Vad= see 12.4.7.Vde= see 12.5.1This test is under the jurisdiction ofASTM Committee D32 on Catalysts and isthe direct respons
12、ibility of Subcommittee D32.01 on Physical-Chemical Properties.Current edition approved April 1, 2015. Published August 2015. Originallyapproved in 1983. Last previous edition approved in 2008 as D4222 03 (2008).DOI: 10.1520/D4222-03R15.2Adamson, A. W., Physical Chemistry of Surfaces, 3rd ed., John
13、Wiley 77.3 K), andsubsequently adding stepwise, known amounts of nitrogen gasto the sample in such amounts that the form of the adsorptionisotherm is adequately defined and the saturation pressure ofnitrogen is reached. Each additional dose of nitrogen isintroduced to the sample only after the foreg
14、oing dose ofnitrogen has reached adsorption equilibrium with the sample.By definition, equilibrium is reached if the change in gaspressure is no greater than 0.1 torr/5 min interval. Thedesorption isotherm is determined by desorbing nitrogen fromthe saturated sample in a stepwise mode with the samep
15、recautions taken to ensure desorption equilibration as appliedunder adsorption conditions. It is essential that the experimen-tal points be distributed over the isotherm in such a manner asto correctly identify and define the isotherm. If the additions orwithdrawals of nitrogen are too large, the te
16、mporarily too-highnitrogen gas pressure during adsorption or too-low gas pressureduring desorption, may result in so-called scanning effectswithin the hysteresis loop of the adsorption-desorptionbranches of the isotherm. The occurrence of scanning mayresult in too-high equilibrium values for the ads
17、orption iso-therm and too-low values for the desorption isotherm.5. Significance and Use5.1 The test method has two main functions: first, it pro-vides data useful for establishing the pore size distribution ofcatalyst materials, which in turn may influence their perfor-mance; and second, it serves
18、as a laboratory test which may beused to study porosity changes that may occur during themanufacture and evaluation of catalysts.6. Apparatus6.1 Ageneric schematic diagram of the minimum apparatusrequirement is shown in Fig. 1. A commercial instrument maybe used and may be constructed of glass or of
19、 metal. Thespecific commercial apparatus chosen may have a differentconfiguration than that shown in Fig. 1 and may requiremodification of the sequence of valve operation and of thecalculations and equations used. It should have the followingfeatures as a minimum:6.1.1 Distribution Manifold, having
20、a (Vd), known to thenearest 0.05 cm3. This volume is defined as the volumebetween the stopcocks or valves and includes the pressuregauge.6.1.2 Vacuum System, capable of attaining pressures below10-4torr (1 torr = 133.3 Pa). This will include a vacuum gauge(not shown in Fig. 1). Access to the distrib
21、ution manifold isthrough the valve V.6.1.3 Pressure Sensing Devices or Pressure Transducers,capable of measurements with a sensitivity of at least 0.1 torr,in the range from 0 to 1000 torr (1 torr = 133.3 Pa).6.1.4 Value (H), from the helium supply to the distributionmanifold.6.1.5 Valve (N), from t
22、he nitrogen supply to the distributionmanifold.6.1.6 The connection between the sample tube and the Svalve can be a standard-taper glass joint, a glass-to-glass seal,or a compression fitting.6.2 Sample Tubes, with volumes from 5 cm3to 100 cm3depending on the application.6.3 Heating Mantles or Small
23、Furnaces.6.4 Dewar Flasks.6.5 Laboratory Balance, with 0.1-mg (107kg) sensitivity.6.6 Thermometer or Thermocouple, for measuring the tem-perature of the distribution manifold T1(i)orT2(i) in C.6.6.1 The manifold may be thermostated at a particulartemperature, a few degrees above ambient, to obviate
24、thenecessity of recording this temperature at each reading.6.7 Thermometer, for measuring the temperature of theliquid nitrogen bath (Ts(i) in Kelvin. Preferably, this thermom-eter will be a nitrogen vapor-pressure-thermometer, oftenreferred to in a commercial instrument as a pressure saturationtube
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