ASTM D4222-2003(2008) Standard Test Method for Determination of Nitrogen Adsorption and Desorption Isotherms of Catalysts and Catalyst Carriers by Static Volumetric Measurements《静态.pdf
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1、Designation: D 4222 03 (Reapproved 2008)Standard Test Method forDetermination of Nitrogen Adsorption and DesorptionIsotherms of Catalysts and Catalyst Carriers by StaticVolumetric Measurements1This standard is issued under the fixed designation D 4222; the number immediately following the designatio
2、n 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 (e) indicates an editorial change since the last revision or reapproval.1. Scope1.1 This test method covers the determi
3、nation 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 each branch of the isotherm toadequately define the adsorption and desorpt
4、ion 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 thestandard. The values given in parentheses are for informationonly.1.3 This sta
5、ndard 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-bility of regulatory limitations prior to use.2. Referenced Documents2.1
6、ASTM Standards:3D 3663 Test Method for Surface Area of Catalysts andCatalyst CarriersD 3766 Terminology Relating to Catalysts and CatalysisE 177 Practice for Use of the Terms Precision and Bias inASTM Test MethodsE 456 Terminology Relating to Quality and StatisticsE 691 Practice for Conducting an In
7、terlaboratory Study toDetermine the Precision of a Test Method3. Terminology3.1 DefinitionsSee Terminology D 3766.3.2 Symbols:PH1= initial helium pressure, torr.PH2= helium pressure after equilibration, torr.TH1= temperature of manifold at initial helium pressure,C.TH2= temperature of manifold after
8、 equilibration, C.P1= initial N2pressure, torr.T1= manifold temperature at initial N2pressure, K.T81= manifold temperature at initial N2pressure, C.P2= pressure after equilibration, torr.T2= manifold temperature after equilibrrium, K.T82= manifold temperature after equilibrium, C.P3= initial N2press
9、ure during desorption, torr.T3= manifold temperature at initial N2pressure, K.T83= manifold temperature at initial N2pressure, C.P4= pressure after equilibration during desorption, torr.T4= manifold temperature after equilibration, K.T84= manifold temperature after equilibration, C.P0= liquid nitrog
10、en 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.W82= sample mass + tare of tube after degassing, g.W2= sample mass + tare of tube af
11、ter 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 12.5.4. Summary of Test Method4.1 The sample is heated and evacuated to remove adsorbedvapors from the surface. The nitrogen adsorption branch of theisotherm is
12、 determined by evacuating the sample, cooling the1This test is under the jurisdiction ofASTM Committee D32 on Catalysts and isthe direct responsibility of Subcommittee D32.01 on Physical-Chemical Properties.Current edition approved April 1, 2008. Published April 2008. Originallyapproved in 1983. Las
13、t previous edition approved in 2003 as D 422203.2Adamson, A. W., Physical Chemistry of Surfaces, 3rd ed., John 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 p
14、ressure ofnitrogen is reached. Each additional dose of nitrogen isintroduced to the sample only after the foregoing 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. Thedes
15、orption isotherm is determined by desorbing nitrogen fromthe saturated sample in a stepwise mode with the sameprecautions 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 as
16、to correctly identify and define the isotherm. If the additions orwithdrawals of nitrogen are too large, the temporarily 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-deso
17、rptionbranches of the isotherm. The occurrence of scanning mayresult in too-high equilibrium values for the adsorption 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
18、 size distribution ofcatalyst materials, which in turn may influence their perfor-mance; and second, it serves 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 ap
19、paratusrequirement is shown in Fig. 1. A commercial instrument maybe used and may be constructed of glass or of 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 thecalculat
20、ions and equations used. It should have the followingfeatures as a minimum:6.1.1 Distribution Manifold, having a (Vd), known to thenearest 0.05 cm3. This volume is defined as the volumebetween the stopcocks or valves and includes the pressuregage.6.1.2 Vacuum System, capable of attaining pressures b
21、elow10-4torr (1 torr = 133.3 Pa). This will include a vacuum gage(not shown in Fig. 1). Access to the distribution 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
22、 torr = 133.3 Pa).6.1.4 Value (H), from the helium supply to the distributionmanifold.6.1.5 Valve (N), from the 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.
23、6.2 Sample Tubes, with volumes from 5 cm3to 100 cm3depending on the application.6.3 Heating Mantles or Small 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 T81(i)orT82(i) i
24、n C.6.6.1 The manifold may be thermostated at a particulartemperature, a few degrees above ambient, to obviate 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 ther-mometer will be
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