PPI TR-14-2000 WATER FLOW CHARACTERISTICS OF THERMOPLASTIC PIPE《热塑性管道的水流特征》.pdf
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1、WATER FLOW CHARACTERISTICS OF THERMOPLASTIC PIPE Foreword This software was developed and published with the technical help and fiiancial support of the members of the Plastics Pipe Institute (PPI). The members have shown their interest in quality products by assisting independent standard-making an
2、d user organizations in the development of standards, and also by developing reports on an industry-wide basis to help engineers, code officials, specifying groups, and users. The purpose of this software is to provide essential information on the water flow characteristics or properties of thermopl
3、astic pipe. The term pipe as used in this report also includes tubing. This software has been prepared by the Plastics Pipe Institute as a service to the industry. The information in this software is offered in good faith and believed to be accurate at the time of its preparation, but is offered wit
4、hout any warranty, expressed or implied. Additional information may be needed in some areas, especially with regard to unusual or special applications. Consult the manufacturer or material supplier for more detailed information. A list of member manufacturers is available from PPI. PPI does not endo
5、rse the proprietary products or processes of any manufacturer and assume no responsibility for compliance with applicable laws and regulations. The Plastics Pipe Institute intends to revise this software from time to time, in response to comments and suggestions from users of the software. Please se
6、nd suggestions or improvements to the following address: Plastics Pipe Institute 1825 Connecticut Ave., NW Suite 680 Washington, DC 20009 Phone: 202-462-9607 Fax: 202-462-9779 Web: ijsiww.plastl4.pipe. A literature list that includes all Technical Reports, Technical Notes, brochures, films, slide pr
7、esentations, and other available information, may be obtained from the Plastics Pipe Institute. This software was first issued in March, 1971, as a written Technical Report , and was revised in June, 1992. In April, 2000 , the written report was adapted to create this software program and accompanyi
8、ng online documentation. i TABLE OF CONTENTS 1 . INTRODUCTION . 1 2 . HEAD LOSS IN PRESSURE PIPES . 1 2.1 DARCY-WEISBACH FORMULA . 1 2.2 HAZEN-WILLIAMS FORMULA 2 3 . GRAVITY FLOW . 3 3.1 HAZEN-WILLIAMS FORMULA 3 3.2 MANNING EQUATION 3 4 . DESIGN VELOCITY AND TOTAL ALLOWABLE PRESSURE 4 5 . CORROSION
9、ALLOWANCE . 4 6 . FITTINGS 4 7 . REFERENCES 4 APPENDIX I. LIMITING WATER VELOCITIES IN THERMOPLASTIC PIPING SYSTEMS . 6 APPENDIX II. EQUATION TERMINOLOGY . 7 APPENDIX III. FORMS OF THE HAZEN-WILLIAMS FORMULA 8 APPENDIX IV. FORMS OF THE MANNING EQUATION 9 APPENDIX V. APPROXIMATE FRICTION LOSS IN THER
10、MOPLASTIC PIPE FITTINGS 10 APPENDIX VI. INSIDE DIAMETER DETERMINATIONS . 11 APPENDIX VII. MOODY DIAGRAM . 12 11 WATER FLOW CHARACTERISTICS OF THERMOPLASTIC PIPE 1. INTRODUCTION During the past 30 years, the use of thermoplastic piping in water and sewer systems has increased significantly. There are
11、 many reasons for this wide acceptance, but one of the primary characteristics which makes thermoplastic piping attractive to designers is the low resistance to flow that this piping offers. This report gives information on the range of pipe sizes commonly used in water and sewer systems. The tables
12、 contained in the appendices give the flow capacities of standard sizes of thermoplastic pipe in terms of velocity and head loss due to friction in pressure piping systems. Similarly, tables are presented that demonstrate the relationship of slope to flow velocity for thermoplastic pipe used in grav
13、ity flow applications. The information in this report applies to all types of thermoplastic materials used for water and sewer systems. These pipes are made by the same basic extrusion technique, which results in smooth inside surfaces. 2. HEAD LOSS IN PRESSURE PIPES A number of empirical formulae h
14、ave been developed to solve problems involving positive pressure flow in pipes. All of these depend, to some extent, on experimentally determined coefficients. The most commonly accepted approximations for pressurized flow applications are the Darcy-Weisbach Formula and the Hazen-Williams Equation.
15、2.1. Darcy-Weisbach Formula The Darcy-Weisbach Formula for head loss in a circular pipe is: Where: HL = HeadLossinfeet J = Darcy-Weisbach friction factor (approximated from Moody Diagram) L = Length of pipe in feet D = Inside diameter in feet V = Average flow velocity in feet per second g = Gravitat
16、ional constant = 32.2 feet/second/second As indicated above, the Darcy-Weisbach friction factor is a function of the Reynolds Number for the piping system under consideration. The Reynolds Number is a 1 dimensionless number relating the fluid velocity, pipe diameter, and fluid viscosity. This relati
17、onship is: D R, =VX- Where: RN = V= B= P= Reynolds Number Average flow velocity in feet per second Inside diameter of the pipe in feet Kinematic fluid viscosity in feet-feet per second Having determined the Reynolds Number, the friction factor, f, may then be obtained from the smooth pipe curve of t
18、he Moody Diagram (see Appendix VIII). This value, along with the other variables, is then substituted into the Darcy-Weisbach Formula to solve for head loss. Although the Darcy-Weisbach Formula is generally regarded as the most accurate means of relating head loss and flow, it can prove cumbersome t
19、o use due to the iterative nature of its solution. Standard practice in most situations is to then utilize a less accurate but acceptable method of calculation of flow or head loss that closely approximates the flow conditions under consideration. 2.2. Hazen-Williams Formula One of the most commonly
20、 accepted formulas for head loss approximation and the basis for the pressurized flow tables in this report is the Hazen-Williams Equation. This relationship, expressed as a function of pressure loss in feet per 100 feet of pipe, is presented below. It is the expression that serves as the basis for
21、the values presented in the appendices in Tables 1 through 30 for pressurized flow. Q“2 HL = 0.2083 x x C.852 d 4.8655 Where: HL = C= - Q= d= Head Loss in feet per 100 feet of pipe Hazen-Williams Flow Factor 150 for thermoplastic pipe Volumetric Flow Rate in gallons per minute Pipe inside diameter i
22、n inches The volumetric flow rate can be converted to flow velocity by using this equation: 0.40085 x Q d2 V= 2 Where: V = Flow velocity in feet per second Q = Volumetric Flow Rate in gallons per minute d = Pipe inside diameter in inches Other forms of the Hazen-Williams Formula are contained in App
23、endix IV. Any of these forms of the Formula can be assumed to be relatively accurate for piping systems in which the Reynolds Number is greater than 109 That is, where the flow velocity multiplied by the pipe inside diameter is greater than 15 for water flow. As noted above, a Hazen-Williams Flow Fa
24、ctor of 150 is recommended for thermoplastic pipes. This value is based upon laboratory tests and field experience. Test results have yielded higher values in the range of 155 to 165, but the use of a value of 150 is conservative in nature and, therefore, aids in providing a further factor of safety
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