API MPMS 11 3 2 1-2013 Manual of Petroleum Measurement Standards Chapter 11 3 2 1 Ethylene Density (Second Edition)《石油计量标准手册 第11 3 2 1章 乙烯密度》.pdf

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1、Manual of PetroleumMeasurement StandardsChapter 11.3.2.1Ethylene DensitySECOND EDITION, MAY 2013Special NotesAPI publications necessarily address problems of a general nature. With respect to particular circumstances, local, state, and federal laws and regulations should be reviewed.Neither API nor

2、any of APIs employees, subcontractors, consultants, committees, or other assignees make any warranty or representation, either express or implied, with respect to the accuracy, completeness, or usefulness of the information contained herein, or assume any liability or responsibility for any use, or

3、the results of such use, of any information or process disclosed in this publication. Neither API nor any of APIs employees, subcontractors, consultants, or other assignees represent that use of this publication would not infringe upon privately owned rights.API publications may be used by anyone de

4、siring to do so. Every effort has been made by the Institute to assure the accuracy and reliability of the data contained in them; however, the Institute makes no representation, warranty, or guarantee in connection with this publication and hereby expressly disclaims any liability or responsibility

5、 for loss or damage resulting from its use or for the violation of any authorities having jurisdiction with which this publication may conflict.API publications are published to facilitate the broad availability of proven, sound engineering and operating practices. These publications are not intende

6、d to obviate the need for applying sound engineering judgment regarding when and where these publications should be utilized. The formulation and publication of API publications is not intended in any way to inhibit anyone from using any other practices.Any manufacturer marking equipment or material

7、s in conformance with the marking requirements of an API standard is solely responsible for complying with all the applicable requirements of that standard. API does not represent, warrant, or guarantee that such products do in fact conform to the applicable API standard.Users of this standard shoul

8、d not rely exclusively on the information contained in this document. Sound business, scientific, engineering, and safety judgment should be used in employing the information contained herein.All rights reserved. No part of this work may be reproduced, translated, stored in a retrieval system, or tr

9、ansmitted by any means, electronic, mechanical, photocopying, recording, or otherwise, without prior written permission from the publisher. Contact the Publisher, API Publishing Services, 1220 L Street, NW, Washington, DC 20005.Copyright 2013 American Petroleum InstituteForewordNothing contained in

10、any API publication is to be construed as granting any right, by implication or otherwise, for the manufacture, sale, or use of any method, apparatus, or product covered by letters patent. Neither should anything contained in the publication be construed as insuring anyone against liability for infr

11、ingement of letters patent.Shall: As used in a standard, “shall” denotes a minimum requirement in order to conform to the specification.Should: As used in a standard, “should” denotes a recommendation or that which is advised but not required in order to conform to the specification.This document wa

12、s produced under API standardization procedures that ensure appropriate notification and participation in the developmental process and is designated as an API standard. Questions concerning the interpretation of the content of this publication or comments and questions concerning the procedures und

13、er which this publication was developed should be directed in writing to the Director of Standards, American Petroleum Institute, 1220 L Street, NW, Washington, DC 20005. Requests for permission to reproduce or translate all or any part of the material published herein should also be addressed to th

14、e director.Generally, API standards are reviewed and revised, reaffirmed, or withdrawn at least every five years. A one-time extension of up to two years may be added to this review cycle. Status of the publication can be ascertained from the API Standards Department, telephone (202) 682-8000. A cat

15、alog of API publications and materials is published annually by API, 1220 L Street, NW, Washington, DC 20005.Suggested revisions are invited and should be submitted to the Standards Department, API, 1220 L Street, NW, Washington, DC 20005, standardsapi.org.iiiContentsPage1 Scope . . . . . . . . . .

16、. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 12 Normative References. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .

17、 . . 13 Terms and Definitions. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 14 Ethylene Equations of State. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .

18、 . . . . . . . . . . . . 14.1 General . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 14.2 IUPAC-88 Equation of State . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .

19、. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 25 Implementation Procedures . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 3Bibliography . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .

20、 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 4vIntroductionThe purpose of this standard is to provide an equation of state that can be used to obtain an accurate determination of ethylene density. Other thermodynamic properties can be calculated using

21、the equation of state, but this standard is primarily concerned with the determination of ethylene density. Temperature and pressure can have significant effects on the accurate determination of ethylene density, and as a result, the means for temperature and pressure determination have to be assess

22、ed appropriately for these applications. The previous edition of this standard, published in 1974, was in the form of a measurement manual and was not confined to calculating the physical properties of ethylene. The previous edition included orifice and turbine metering calculations, as well as data

23、 that were not in agreement with the current API Manual of Petroleum Measurement Standards (MPMS) that cover these metering devices. The original density lookup tables were based on FORTRAN code originally published in the mid-1960s as API 2565 Subroutine Ethyl. This Second Edition of API MPMS Chapt

24、er 11.3.2.1 is intended to replace the 30+ year old equations with references to more modern equations of state, limited to the physical properties of ethylene.Typically, ethylene equations of state are used in custody transfer metering applications. Such is the case with modern flow computers, whic

25、h have various options for selecting which equation of state is utilized in determining flowing ethylene density. vi1Ethylene Density1 ScopeThis standard identifies an equation of state (EOS) suitable for use in custody transfer measurement of pure ethylene (99 %) in the gaseous, liquid, and super c

26、ritical phases. Given flowing temperature and pressure, an EOS is capable of calculating density and other thermodynamic properties used to calculate mass and volumetric flow of ethylene to custody transfer accuracy. All accuracy and uncertainty statements in this standard are limited to the EOS res

27、ults and do not include the uncertainty added by the primary and secondary measuring equipment. 2 Normative ReferencesThe following referenced documents are indispensable for the application of this document. For dated references, only the edition cited applies. For undated references, the latest ed

28、ition of the referenced document (including any amendments) applies.IUPAC-88 1, Ethylene (Ethene), International Thermodynamic Tables of the Fluid State, Volume 10 (1988)3 Terms and DefinitionsFor the purposes of this document, the following definitions apply.3.1critical regionThermodynamic state of

29、 a fluid in which phase boundaries cease to exist. NOTE In the case of ethylene, a vapour-liquid critical region exists. Density determination is extremely sensitive in the critical region, as minor changes in flowing pressure can bring about significant changes in density for a given temperature.3.

30、2equation of stateEOSThermodynamic equation describing the state of matter under a given set of physical conditions.NOTE An EOS provides a mathematical relationship between two or more state functions associated with the material, such as its temperature or pressure. 4 Ethylene Equations of State4.1

31、 GeneralThis standard provides a reference for an ethylene EOS: IUPAC-88, part of the Ethylene, International Thermodynamic Tables of the Fluid State, Volume 10 (1988) publication.IUPAC-88 is a publication that incorporates the work carried out by Jahangiri et al. 1 on ethylene. The paper “Thermodyn

32、amic Properties of Ethylene from the Freezing Line to 450 K at Pressures to 260 MPa” was published a year or so before IUPAC published lookup tables in 1988. 1International Union of Pure and Applied Chemistry, 104 T.W. Alexander Drive, Building 19, Research Triangle Park, North Carolina 27709, www.i

33、upac.org.2 API MPMS CHAPTER 11.3.2.1The IPUAC EOS is acceptable for use in custody transfer applications. However, the user should be aware that a critical region for ethylene exists across pressures ranging approximately from 5171.1 kPa to 5860.5 kPa (750 psig to 850 psig) and temperatures ranging

34、approximately from 10 C to 21.1 C (50 F to 70 F). Density predictions using the IUPAC EOS are not recommended in this region. For the IUPAC-88 density prediction, the estimated uncertainty of the EOS is less than 0.08 % for pressures up to 260 MPa (65,266.9 psig) and temperatures up to 176.85 C (350

35、.3 F), with the exception of the critical region. 4.2 IUPAC-88 Equation of StateThe paper by Jahangiri et al. 1 is the basis for the IUPAC-88 EOS. According to the paper, the Helmholtz energy for ethylene is given below by the fundamental equation:(1)where is the ideal gas contribution to the Helmho

36、ltz energy of any state. The term is the contribution represented by the compressibility of the real gas. After additional manipulation, the functional form used for the fundamental equation for ethylene is a nondimensional Helmholtz energy potential function below: (2)where(3)wherecis the critical

37、density;Tcis the critical temperature;T0is the reference temperature 298.15 K;P0is the reference pressure 0.101525 MPa;0is the ideal gas density at T0and P0;is the reference enthalpy at T0;is the reference entropy at T0and P0;R is the gas constant 0.00831434 (MPa dm3)/(mol K). Given the equations ab

38、ove, it is possible to derive functions for calculating properties of ethylene such as density. The equations and procedures described in Section 5.4 of Jahangiri et al.s paper illustrate how density can be calculated from the methods above. A T,()AT,()A T,()+=AT,()A T,() ,()A T,()R T ,(),()+=H0RTc-

39、S0R- 100-R-Cp2-0d1R-Cp-0d+ln+= TcT 0, TcT0, c0, 0c=H0S0ETHYLENE DENSITY 35 Implementation ProceduresTo properly implement an ethylene EOS, the user should follow the implementation procedures in the IUPAC-88 publication. Through mathematical manipulation it is possible to derive a form in terms of d

40、ensity, pressure and temperature. However, it is recognized that tolerances for solutions and validation procedures are not provided in the publication itself. To maintain industry consistency, a technical report will be issued separate of this standard providing guidance on how to perform the calcu

41、lations. Ultimately though, the end use for an ethylene EOS will determine the procedures of implementation. In some custody transfer applications, programming support could be required to implement the proper code for each EOS. In other custody transfer applications, the EOS could already be in a c

42、ompiled form and available for use. An example of this would be the use of an ethylene EOS in flow computing applications to determine mass flow rate. Example and auxiliary calculations are presented in the individual publication IUPAC-88.4Bibliography1 Majid Jahangiri, Richard T. Jacobsen, and Rich

43、ard B. Stewart, “Thermodynamic Properties of Ethylene from the Freezing Line to 450 K at Pressures to 260 MPa,” Journal of Physical and Chemical Reference Data(1986), Vol. 15, No. 2, 1986API MonogramLicensing ProgramSales: 877-562-5187(Toll-free U.S. and Canada)(+1) 202-682-8041(Local and Internatio

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