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    ISO 11358-1-2014.pdf

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    ISO 11358-1-2014.pdf

    1、 ISO 2014Plastics Thermogravimetry(TG)of polymers Part 1:General principlesPlastiques Thermogravimtrie(TG)des polymres Partie 1:Principes gnrauxINTERNATIONAL STANDARDISO11358-1First edition2014-07-15Reference numberISO 11358-1:2014(E)Copyright International Organization for Standardization Provided

    2、by IHS under license with ISO Licensee=University of Alberta/5966844001,User=ahmadi,rozitaNot for Resale,01/26/2015 09:54:28 MSTNo reproduction or networking permitted without license from IHS-,-,-ISO 11358-1:2014(E)ii ISO 2014 All rights reservedCOPYRIGHT PROTECTED DOCUMENT ISO 2014All rights reser

    3、ved.Unless otherwise specified,no part of this publication may be reproduced or utilized otherwise in any form or by any means,electronic or mechanical,including photocopying,or posting on the internet or an intranet,without prior written permission.Permission can be requested from either ISO at the

    4、 address below or ISOs member body in the country of the requester.ISO copyright officeCase postale 56 CH-1211 Geneva 20Tel.+41 22 749 01 11Fax+41 22 749 09 47E-mail copyrightiso.orgWeb www.iso.orgPublished in SwitzerlandCopyright International Organization for Standardization Provided by IHS under

    5、license with ISO Licensee=University of Alberta/5966844001,User=ahmadi,rozitaNot for Resale,01/26/2015 09:54:28 MSTNo reproduction or networking permitted without license from IHS-,-,-ISO 11358-1:2014(E)ISO 2014 All rights reserved iiiContents PageForeword.iv1 Scope.12 Normative references.13Termsan

    6、ddefinitions.14 Principle.25 Apparatus.26 Test specimen preparation.26.1 General.26.2 Test specimens from finished products.36.3 Test specimen conditioning.36.4 Test specimen mass.37 Calibration.37.1 Mass calibration.37.2 Temperature calibration.38 Procedure.48.1 General.48.2 Temperature scanning mo

    7、de.48.3 Isothermal mode.59 Expression of results.59.1 Graphical representation.59.2 Determination of increase in mass.59.3 Determination of loss in mass.610 Test report.8Copyright International Organization for Standardization Provided by IHS under license with ISO Licensee=University of Alberta/596

    8、6844001,User=ahmadi,rozitaNot for Resale,01/26/2015 09:54:28 MSTNo reproduction or networking permitted without license from IHS-,-,-ISO 11358-1:2014(E)ForewordISO(the International Organization for Standardization)is a worldwide federation of national standards bodies(ISO member bodies).The work of

    9、 preparing International Standards is normally carried out through ISO technical committees.Each member body interested in a subject for which a technical committee has been established has the right to be represented on that committee.International organizations,governmental and non-governmental,in

    10、 liaison with ISO,also take part in the work.ISO collaborates closely with the International Electrotechnical Commission(IEC)on all matters of electrotechnical standardization.The procedures used to develop this document and those intended for its further maintenance are described in the ISO/IEC Dir

    11、ectives,Part 1.In particular the different approval criteria needed for the different types of ISO documents should be noted.This document was drafted in accordance with the editorial rules of the ISO/IEC Directives,Part 2(see www.iso.org/directives).Attention is drawn to the possibility that some o

    12、f the elements of this document may be the subject of patent rights.ISO shall not be held responsible for identifying any or all such patent rights.Details of any patent rights identified during the development of the document will be in the Introduction and/or on the ISO list of patent declarations

    13、 received(see www.iso.org/patents).Any trade name used in this document is information given for the convenience of users and does not constitute an endorsement.For an explanation on the meaning of ISO specific terms and expressions related to conformity assessment,as well as information about ISOs

    14、adherence to the WTO principles in the Technical Barriers to Trade(TBT)see the following URL:Foreword-Supplementary informationThe committee responsible for this document is ISO/TC 61,Plastics,Subcommittee SC 5,Physical chemical properties.This first edition of ISO 11358-1 cancels and replaces ISO 1

    15、1358:1997,which has been technically revised.The main changes are:a)addition of ISO 472 to the Normative references clause and removal of definitions specified therein;b)revision of apparatus specifications.ISO 11358 consists of the following parts,under the general title Plastics Thermogravimetry(T

    16、G)of polymers:Part 1:General principles Part 2:Determination of activation energy Part 3:Determination of the activation energy using the Ozawa-Friedman plot and analysis of the reaction kinetics iv ISO 2014 All rights reservedCopyright International Organization for Standardization Provided by IHS

    17、under license with ISO Licensee=University of Alberta/5966844001,User=ahmadi,rozitaNot for Resale,01/26/2015 09:54:28 MSTNo reproduction or networking permitted without license from IHS-,-,-INTERNATIONAL STANDARD ISO 11358-1:2014(E)Plastics Thermogravimetry(TG)of polymers Part 1:General principles1

    18、ScopeThis part of ISO 11358 specifies general conditions for the analysis of polymers using thermogravimetric techniques.It is applicable to liquids or solids.Solid materials may be in the form of pellets,granules or powders.Fabricated shapes reduced to appropriate specimen size may also be analysed

    19、 by this method.Thermogravimetry can be used to determine the temperature(s)and rate(s)of decomposition of polymers,and to measure at the same time the amounts of volatile matter,additives and/or fillers they contain.The thermogravimetric measurements may be carried out in dynamic mode(mass change v

    20、ersus temperature or time under programmed conditions)or isothermal mode(mass change versus time at constant temperature).Thermogravimetric measurements may also be carried out using different testing atmospheres,e.g.to separate decomposition in an inert atmosphere from oxidative degradation.2 Norma

    21、tive referencesThe following documents,in whole or in part,are normatively referenced in this document and are indispensable for its application.For dated references,only the edition cited applies.For undated references,the latest edition of the referenced document(including any amendments)applies.I

    22、SO 291,Plastics Standard atmospheres for conditioning and testingISO 472,Plastics VocabularyISO 11357-1,Plastics Differential scanning calorimetry(DSC)Part 1:General principles3 TermsanddefinitionsFor the purposes of this document,the terms and definitions given in ISO 472 and the following apply.3.

    23、1dynamic mass-change determinationtechnique for recording the variation of the mass of a test specimen with temperature T which is changing at a programmed rate3.2isothermal mass-change determinationtechnique for recording the variation of the mass of a test specimen with time t at constant temperat

    24、ure T3.3Curie temperaturetemperature at which a ferromagnetic material passes from the ferromagnetic state to the paramagnetic state or vice versa ISO 2014 All rights reserved 1Copyright International Organization for Standardization Provided by IHS under license with ISO Licensee=University of Albe

    25、rta/5966844001,User=ahmadi,rozitaNot for Resale,01/26/2015 09:54:28 MSTNo reproduction or networking permitted without license from IHS-,-,-ISO 11358-1:2014(E)4 PrincipleA test specimen is heated at specified rates with a controlled temperature programme,and the change in mass is measured as a funct

    26、ion of temperature.Alternatively,the specimen is kept at a given constant temperature and the change in mass is measured as a function of time over a given period.During measurement the test specimen is held in a controlled inert or oxidising atmosphere.In general,the reactions which cause the mass

    27、of a test specimen to change are decomposition or oxidation reactions or the volatilisation of a component.The change in mass is recorded as a thermogravimetric(TG)curve.The change in mass of a material as a function of temperature and the extent of this change are indicators of the thermal stabilit

    28、y of the material.TG data can therefore be used to evaluate the relative thermal stability of polymers of the same generic family and polymer-polymer or polymer-additive interactions,using measurements made under the same test conditions.NOTE TG data may be used for process control,process developme

    29、nt and material evaluation.Long-term thermal stability is a complex function of service and environmental conditions.TG data alone may not be able to describe the long-term thermal stability of a polymer.5 ApparatusA number of commercial instruments suitable for thermogravimetric measurements are av

    30、ailable.The basic apparatus consists of the following.5.1 Thermobalance,meeting the following requirements:capability to generate constant heating and cooling rates suitable for intended measurements;capability to maintain the test temperature constant(to within 0,3 K or less for the duration of mea

    31、surement);capability to maintain a constant purge gas flow rate controllable to within 10%over a range of flow rates(e.g.10 ml/min to 150 ml/min);temperature and mass range in line with experimental requirements;recording device capable of automatically recording the measured curve of mass versus te

    32、mperature and time;measurement of temperature signals with an accuracy of 2 K or better;measurement of time with an accuracy of 1 s or better;measurement of mass with an accuracy of 20 g or better.5.2 Purge gas,dry air or oxygen(oxidizing conditions)or a suitable inert gas with an oxygen content of

    33、0,001%by volume or less(non-oxidizing conditions).In either case,the water content of the purge gas shall be less than 0,001%by mass.6 Test specimen preparation6.1 GeneralTest specimens may be liquids or solids.Solids may be in the form of powders,pellets,granules or cut pieces.For finished products

    34、,the test specimen shall be in the form normally found in use.2 ISO 2014 All rights reservedCopyright International Organization for Standardization Provided by IHS under license with ISO Licensee=University of Alberta/5966844001,User=ahmadi,rozitaNot for Resale,01/26/2015 09:54:28 MSTNo reproductio

    35、n or networking permitted without license from IHS-,-,-ISO 11358-1:2014(E)6.2 TestspecimensfromfinishedproductsCut the test specimen to appropriate size for the specimen holder.Microtomes or razor blades are suitable for this purpose.NOTE Test specimen size and shape are generally dependent on the s

    36、ample holder.Surface area affects the overall results.For instance,in comparing a test specimen of large surface area with a test specimen of smaller surface area,both having the same mass,the smaller surface area test specimen normally changes at a slower rate.6.3 Test specimen conditioningUnless o

    37、therwise specified in a material specification or product standard,test specimens shall be conditioned,prior to measurement,at one of the standard atmospheres specified in ISO 291,or by any other method specified by agreement between the interested parties.6.4 Test specimen massPreferably,the mass o

    38、f the test specimen shall be in the range of 10 mg to 100 mg.7 Calibration7.1 Mass calibrationWithout any gas flow through the thermobalance(to prevent any disturbance through buoyancy and/or convection effects),calibrate the thermobalance as follows,using calibrated masses in the range of 10 mg to

    39、100 mg:Record the temperature at which the mass calibration was carried out.Zero the thermobalance.Place the calibration weight on the thermobalance and measure the corresponding mass change.If necessary,adjust the thermobalance so that the measured mass is equal to the calibration mass.If mass cali

    40、bration is done by procedures included in the instrument control software or by external service providers a valid calibration certificate may be acceptable to demonstrate adequate mass calibration.7.2 Temperature calibrationCarry out the temperature calibration using the same atmosphere,rate of gas

    41、 flow and heating rate as shall be used in the procedure specified in Clause 8.If the thermobalance is not coupled with another thermoanalytical method,use the following procedure.a)Choose two or more calibration materials with a Curie temperature near the temperature range to be examined.If possibl

    42、e,choose the calibration materials in such a way that the temperature range to be examined lies between the Curie temperatures of two of them.b)Start heating at the same heating rate as will be used in the procedure specified in Clause 8 and carry out a calibration based on the start temperature TA,

    43、mid-point temperature TC and end temperature TB for the Curie temperature transition.NOTE 1 The Curie point is the temperature at which a ferromagnetic material becomes paramagnetic on heating.The effect is reversible.Applying a magnetic field(e.g.by placing a strong magnet below the furnace)exerts

    44、a downward force on the ferromagnetic sample.This creates an apparent increase of weight which is lost upon heating the sample above its Curie temperature.NOTE 2 Certified calibration materials traceable to metrology laboratories should be preferably used.Suitable calibration materials may be availa

    45、ble via instrument manufacturers or National Metrology Institutes.ISO 2014 All rights reserved 3Copyright International Organization for Standardization Provided by IHS under license with ISO Licensee=University of Alberta/5966844001,User=ahmadi,rozitaNot for Resale,01/26/2015 09:54:28 MSTNo reprodu

    46、ction or networking permitted without license from IHS-,-,-ISO 11358-1:2014(E)If the thermobalance is combined with a DSC(differential scanning calorimetry)detector,it is recommended that the thermobalance is temperature-calibrated using procedures specified in corresponding standards,e.g.ISO 11357-

    47、1 for DSC.NOTE 3 The melting point of a calibration material is defined as the intercept of the extrapolated baseline and the tangent to the slope of the endotherm at the point of inflection of the curve(the so-called onset temperature).NOTE 4 Calibration is the most critical stage in obtaining reli

    48、able thermogravimetry data;the relationship between the temperature sensor,specimen geometry and type of atmosphere,including the rate of gas flow,will affect the calibration of the measurement system.NOTE 5 The rate of mass loss is dependent upon the rate of oxidation of the test specimen,and there

    49、fore dependent in part upon the atmosphere and rate of gas flow to which it is exposed.It is therefore important to use the same atmosphere and rate of gas flow in the calibration as in the procedure specified in Clause 8.8 Procedure8.1 GeneralDepending on the measurement requirements a suitable ins

    50、trument setup has to be chosen.Two modes can be used:temperature scanning(see 8.2)and isothermal(see 8.3).NOTE 1 A change in buoyancy and convection occurs in the thermobalance when the gas flow is operating.Even if there is no actual change in mass,an apparent change in mass is observed and the acc


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