Chapter 5-22The friction factor chart 天大化工原理上册英文版课件

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(流体力学与传热英文课件)Pressure drop and loss due to friction

(流体力学与传热英文课件)Pressure drop and loss due to friction

The equation(1.4-10) is the equation usually used to calculate skin friction loss in straight pipe.
For laminar flow only, combining Eqs. (1.4-20 ) and (1.4-10) .gives
f 16 Re
64
Re
(1.4-22 )
It is not possible to predict theoretically the Fanning friction factor f for turbulent flow as was done for laminar flow.
1.4.3 Turbulent Flow in Pipes and Channels
Although the problem has not been completely solved, useful relationships are available.
• For turbulent flow the friction factor must be determined empirically, and it not only depends upon the Reynolds number but also on surface roughness of the pipe.
L R
Rearranging equation (1.4-2 ) gives
w
Rp 2L
Substituting from equation above into equation (1.4-7) gives
fV 2 w /2R V p 2//2 2 L4D L pf V 2 2

1.4流体在管内的流动阻力

1.4流体在管内的流动阻力
Re ≤ 2000 2000 < Re <4000 Re ≥ 4000
稳定的层流区 由层流向湍流过渡区 湍流区
du
1.4 流体在管内的流动阻力 雷诺数Re的物理意义:
u2 u( uA) u 质 量 流 速 Re u / d . u . A 粘性力 d 单位时间单位截面积流 动量 惯性力 体 粘性力 粘性力 du
1.4 流体在管内的流动阻力 ⒉摩擦系数:
32 lu Pf d2
——哈根—泊谡叶公式
32 2 l u 2 64 l u 2 64 l u 2 Pf . . . . . . du d 2 ud d 2 Re d 2
64 Re
1.4 流体在管内的流动阻力 (三)湍流时的速度分布与摩擦系数
1.4 流体在管内的流动阻力
幂函数形式:
Pf K d a Lbu c e h g
将式中各物理量的因次用基本因次表达,根据因次 分析法的原则,等号两端的因次相同。
M
2
L
1
L L L ML ML
a b 1 c 3 h
1

1 e
L
1000kgm10103pas设吸入和排出管内流速为14流体在管内的流动阻力14流体在管内的流动阻力取管壁绝对粗糙度03mm则查图得摩擦系数水泵吸水底阀90的标准弯头闸阀全开取水池液面11截面为基准面泵吸入点处a为22截面在该两截jkg5710022106010002614流体在管内的流动阻力14流体在管内的流动阻力取水池液面11截面为基准面储罐b液面为33截面在该两截jkg792000211002214流体在管内的流动阻力将柏努利方程整理并代入数据得
g
物理量 英文名称 压力降 Pressure Drop Diameter 管径 Length 管长 平均速度 Average velocity Density 密度 Viscosity 粘度 粗糙度 Roughness parameter

Hagen-Poiseuille

Hagen-Poiseuille

General T eaching Outline forPrinciples of Chemical EngineeringCourse Number:Suitable for:Majors of chemical engineering and technology, biochemical engineering, food engineering, environment engineering, applied chemistry, industry equipment and control engineering, pulp and paper, polymer and inorganic material engineering.Course character: Basic course for technologyAcademic Credits: 7Academic Hours: 114Written by Hao Shixiong Writing Date: 2006.03.06 Proofread by Proofreading Date: 2006.03.06Section ⅠBasic requirements1. The Course objectiveThe ‘principles of chemical engineering’is a requirement course for general chemical engineering speciality. It is suitable for undergraduate students in the senior years who have the usual training in mathematics, physics, chemistry, and mechanics. It includes the principles of a fluid flow, heat transfer, principles of mass transfer and separation processes, the construction and operating principle of typical equipment, the experimental and researching methods of unit operation, and the calculation and selection of typical equipment. The course aims are to train and educate students to know or understand basic unit operations of chemical engineering. The course emphasizes the combination between the theory and practices, and ability of analysis and solution to practical process.2. Previous coursesAdvanced mathematics, physics, physical chemistry, mechanics, mechani cal drawi ng3. The basic requirements and contents for each chapterChapter 1 Definitions and principlesBasic law; Material balance; Law of motion; Energy balance; Equilibrium; Units and dimensions; Physical quantities; Primary and secondary quantities; Dimensions and dimensional formulas; Conversion of units; Dimensionless equations and consistent units; Dimensi onal equati ons.Chapter 2 Fluid statics and its applicationsNature of fluids; Hydrostatic equilibrium; Applications of fluid statics; Manometers continuous gravity decanter.Chapter 3 Fluid flow phenomenaThe velocity field; Laminar flow; Shear rate, and shear stress; Newtonian and non-Newtonian fluids; Viscosity; Kinematic viscosity.Turbulence; Laminar and turbulent flow; Reynolds number and transition from laminar to turbulence flow; Nature of turbulence; Deviating velocities in turbulence flow; Eddy viscosity; Flow in boundary layers; Laminar and turbulent flow in boundary layers; Boundary-layer formation in straight tubes; Boundary-layer separation and wake formation.Chapter 4 Basic equations of fluid flowOne-dimensional flow; Mass balance; Macroscopic momentum balance; Layer flow with free surface; Momentum balance in potential flow; Discussion of Bernoulli equation; Bernoulli equation: correction for effects of solid boundaries; Kinetic-energy correction factor; Correction of Bernoulli equation for fluid friction; Pump work in Bernoulli equation.Chapter 5 Incompressible flow in pipes and channelsShear stress and skin friction in pipes; Relation between skin friction and wall shear; Relations between skin-friction factor; Laminar flow of Newtonian fluids; V elocity distribution in a pipe;A verage velocity for laminar flow in a pipe; Hagen-Poiseuille equation; Relations between maximum velocity and average velocity; Laminar flow in an annulus; Friction factor in flow through channel of noncircular cross section; Turbulent flow in pipes and channels; Effect of roughness; Hydraulically smooth; The friction factor and friction coefficient chart; Friction from changes in velocity or direction; Friction loss from sudden expansion of cross section; Friction loss from sudden contraction of cross section; Effect of fittings and valves; Form-friction losses in the Bernoulli equation.Chapter 6 Flow past immersed bodiesDrag, Drag coefficients; Drag coefficients of typical shapes; Mechanics of particle motion, Equation for one-dimensional motion of particle through fluid; Terminal velocity, drag coefficient, movement of spherical particles; The terminal velocities at the different Reynolds number; Criterion for settling regime.Chapter 7 Separation equipmentsGravity settling processes; Centrifugal settling processes; Separation of solids from gases; cyclones, filtration; Clarifying filters; Gas cleaning; Liquid clarification, discontinuous pressure filters; Filter press; Shell-and-leaf filters; Continuous pressure filters; Principles of cake filtration; Pressure drop through filter cake; Filter medium resistance; Constant-pressure filtration; Continuous filtration; Washing filter cakes.Chapter 8 T ransportation and metering of fluidsPipe and tubing; Selection of pipe sizes; Fluid-moving machinery; Developed head; Power requirement; Suction lift and cavitation; Suction lift; Positive-displacement pumps; V olumetric efficiency; Rotary pumps; Centrifugal pumps; Centrifugal pump theory; Head-flow relations for an ideal pump; The relation between head and volumetric flow; Effects of speed and impeller sizechange; Characteristic curves; Head-capacity relation; Efficiency; Centrifugal-pump characteristics; System head curve; Operating point; Operating point change; Operation in parallel and in series of centrifugal pump; Multistage centrifugal pumps; Pump priming; Fans; Blowers.Measurement of flowing fluids; Full-bore meters; V enturi meter; The basic equation for venturi meter; V enturi coefficient; Flow rate; Pressure recovery; Orifice meter; Pressure recovery; Area meters: rot meters; Theory and calibration of rotameters; Inserti on meters; Pi cot tube.Chapter 10 Heat T ransferNature of heat flow; Heat transfer by conduction; Basic law of conduction; Unsteady-state conduction; Steady-state conduction; Thermal conductivity; Steady-state conduction; Compound resistance in series; Heat flow through a cylinder.Chapter 11 Principles of heat flow in fluidsTypical heat-exchange equipment; Countercurrent and parallel-current flows; Single-pass shell-and-tube condenser; Energy balances, heat flux and heat transfer coefficient; Heat flux, A verage temperature of fluid stream; Overall heat-transfer coefficient; Mean temperature difference; Individual heat-transfer coefficients; Special cases of the overal l coeffi ci ent.Chapter 12 Heat transfer to fluids without phase changeRegimes of heat transfer in fluids; Heat transfer by forced convection in turbulent flow; Empirical equation; Effect of tube length; Estimation of wall temperature t w; Cross sections other than circular; Heat transfer in transition region between laminar and turbulent flow; Heating and cooling of fluids in forced convection outside tubes, fluids flowing normal to a single tube; Natural convection; Natural convection to air from vertical shapes and hori zontal pl ates.Chapter 13 Heat transfer to fluids with phase changeHeat transfer from condensing vapors; Dropwise and film-type condensation; Coefficients for film-type condensation; V ertical tubes, Horizontal tubes; Effect of noncondensables; Heat transfer to boiling liquids; Pool boiling of saturated liquid.Chapter 14 Radiation heat transferFundamental facts concerning radiation; Emission of radiation; Wavelength of radiation; Emissive power; Blackbody radiation; Emissivities of solids; Practical source of blackbody radiation; Laws of blackbody radiation; Absorption of radiation by opaque solids; Radiation between surfaces.Chapter 17 Principles of Diffusion and Mass T ransfer Between PhasesTheory of diffusion; Comparison of diffusion and heat transfer; Diffusion quantities; V eloc ities in diffusion; Molal flow rate, velocity, and flux; Relations between diffusivities; Interpretation of diffusion equations; Equimolal diffusion; One-component mass transfer (one-way di ffusi on).Prediction of Diffusivities; Diffusion in gases; Diffusion in liquids; Turbul ent di ffusi on.Mass transfer theories; Mass transfer coefficient; Film theory; Two-fi l m theory.Chapter18. Gas AbsorptionDefinition of absorption; Principles of absorption; Material balances; Limiting gas-liquid ratio; Rate of absorption; Calculation of tower height; Number of transfer units; Alternate forms of transfer coefficients; Effect of pressure; Temperature variations in packed towers; Stripping factor method for calculating the number of transfer units; Absorption efficiency A.Empirical correlations for mass transfer coefficients in absorption.Chapter 19 Introduction to Mass T ransfer and Separation ProcessesDefinition of separation processes; Importance and variety of separations; Economic significance of separation processes; Categorizations of separation processes; General separation process; Technological maturity of processes; Terminology and symbols.Supplementary:Phase equilibria: Phase rule; Equilibrium and equilibrium stage; Thermodynamic relationships: Equilibrium ratio ( or equilibrium constant or K value); Relative volatility----key separation factor in distillation; Ideal system and Dalton’s law, Raoult’s law; Phase equilibrium diagrams for ideal systems(t-x-y diagram; x-y diagram); Henry’s law; Azeotropes; Effect of total pressure on vapor/liquid equilibrium.Chapter 20 Equilibrium-Stage OperationsCascades. Ideal stage/equilibrium stage/theoretical stage; Equipment for stage contacts; Principles of stage processes; Terminology for stage-contact plants; Material balances; Enthalpy balances; Graphical methods for two-component system; Operating line diagram; Ideal contact stages; Determining the number of ideal stages; Absorption factor method for calculating the number of ideal stages.Supplementary:Introduction to distillation: Process description; Equilibrium/flash distillation; Principles and flow diagram of distillation.Chapter 21 DistillationContinuous distillation with Reflux. Material balances in plate columns: Overall material balances for two-component systems; Net flow rates; Operating linesNumber of ideal plates; McCabe-Thiele Method. Constant molal overflow; Reflux ratio; Condenser and top plate; Bottom plate and reboiler; Feed plate; Feed line; Construction of operating lines; Optimum feed plate location; Heating and cooling requirements; Minimum number of plates/total reflux; Minimum reflux/infinite number of plates; Invariant zone; Optimum reflux; Nearly pure products; Some special cases of distillation (Multiple feeds and side-stream drawoffs; Direct steam heating); Use of Murphree efficiency/determining the number of actual plates.Batch distillation. Simple distillation; Batch distillation with reflux. Calculation and analysisfor the operation of a distillation column.Chapter 24 Drying of SolidsIntroduction to methods for removing liquid from solid materials; Purposes and applications of drying; Classification of drying processes; Drying conditions for convecti ve dryers.Properties of moist air and humidity chart. Moist air properties: Humidity; Relative humidity; Humid volume; Humid heat; Total enthalpy of moist air; Dry-bulb temperature and wet-bulb temperature; Adiabatic saturation temperature; Dew point. Humidity chart of Air-Water system. Applications of H-I diagram.Material and energy balances; Expressions of water (moisture) content of solids; Material balances; Heat balances; Thermal efficiency of drying process; Air states when passing through the drying system.Phase equilibria and drying rates. Phase equilibria: Equilibrium water(moisture) and free water(moisture); Equilibrium-moisture curves; Bound and unbound water; Drying curves and drying rate curves under constant drying conditions; Drying mechanism of wet solids and the influencing factors: Constant-rate period (Period of controls of surface water vaporization); Drying in the falling-rate period (period of controls of water diffusing from interior to solid surface); Critical water(moisture) content and its influencing factors. Methods for increasing rate of drying.Calculation of drying time under constant drying conditions.4. T extbook and reference booksT extbook:Unit operation of chemical engineering(Sixth edition) Author: Warren L. McCabe, Julian C. Smith and Peter HarriottReference books:[1]. 姚玉英主编. 化工原理(上、下册)(新版)[M] . 天津: 天津大学出版社, 1998[2]. 赵汝溥, 管国锋. 化工原理[M] . 北京: 化学工业出版社, 1995.[3]. 大连理工大学化工原理教研室编. 化工原理(上、下册)[M]. 大连:大连理工大学出版社, 1992[4]. 陈敏恒,丛德滋,方图南,齐鸣斋编. 化工原理(上、下册)[M].(第二版).北京: 化学工业出版社, 1999[5]. 朱家骅,叶世超等编. 化工原理(上、下册)[M]. 北京:科学技术出版社, 2002[6]. 姚玉英. 化工原理例题与习题[M](第三版). 北京: 化学工业出版社, 2003[7]. 柴成敬,王军,陈常贵,郭翠梨编.化工原理课程学习指导[M]. 天津: 天津大学出版社, 2003[8]. 匡国柱. 化工原理学习指导[M]. 大连: 大连理工大学出版社, 20025. Periods for Every Unitl. Fluid flow 20 hours2. Fluid transportation 10 hours3. Separation of heterogeneous mixture 10 hours4. Heat transfer 20 hours5 Gas Absorption 24 hours6 Distillation 18 hours7 Drying of Solids 12 hours6. Evaluation Methods of the CourseThe assess method: quiz, homework and course report et al. which are determined by the teacher, and the unified final examination。

国际经济学Chapter 5

国际经济学Chapter 5

CHAPTER 5The Standard Trade Model* The differences and common features of the three models developed in previous chapter.·Differences·Common features(1)different PPF(2)different PPF different RS(3)different RS different P C/P F trade* A more general trade model: the models we have studied may be viewed as special cases.·Different PPF?(1)Home’s relative labor productivity of cloth is higher thanForeign’sor(2)Q C=Q C(K,L C), Q F=Q F(T,L F). Home has more capital while Foreign has more land.or(3)Home is labor-abundant and cloth is labor-intensive, while …Model Merit DefectThe Ricardian modelTechnology(trade pattern)Income distribution The Specific factormodelIncome distribution Trade patternThe H-O modelResources(trade pattern)Technology·Different Pc/P F?At any given Pc/P F, (Q C/Q F)>(Q C*/Q F*), RS lies to the right of RS*, that is (P C/P F)H<(P C/P F)F。

克鲁格曼国际经济学第五章

克鲁格曼国际经济学第五章

•© Pearson Education Limited 2015. All rights reserved.
1-13
Fig. 5-1: The Production Possibility Frontier without Factor Substitution
•© Pearson Education Limited 2015. All rights reserved.
Total calories of food production
aLCQC + aLFQF ≤ L
Labor used for each yard of cloth production
•© Pearson Education Limited 2015. All rights reserved.
Total amount of labor resources
•© Pearson Education Limited 2015. All rights reserved.
1-3
CONCEPTS
(Country-specific) relative abundance of factors
proportion of factors available in the country( 国家要素丰裕度): 一国拥有的生产要素的相对比例。 存量概念、相对概念 在只考虑劳动和资本两种生产要素时,A国拥有资本-劳动存量比称为该国 的资本丰裕度 K / L 国家的要素禀赋类型(relative abundance of factor) 若两国有K / L ,K / L 则就A、B两国而言,称B国为资本丰裕(或劳动稀 缺)型国家,A国为劳动丰裕(资本稀缺)型国家。(in terms of physical

曼昆微观经济学第五版第五章课文

曼昆微观经济学第五版第五章课文
Price
1. A 22% $5 increase in price... 4
Demand
90 100
Quantity
2. ...leads to a 11% decrease in quantity.
Harcourt, Inc. items and derived items copyright © 2001 by Harcourt, Inc.
Price elasticity of demand is greater than one.
Harcourt, Inc. items and derived items copyright © 2001 by Harcourt, Inc.
Computing the Price Elasticity
Elastic Demand
- Elasticity is greater than 1
Price
1. A 22% $5 increase in price... 4
Demand
50
100
Quantity
2. ...leads to a 67% decrease in quantity.
Example: If the price of an ice cream cone increases from $2.00 to $2.20 and the amount you buy falls from 10 to 8 cones then your elasticity of demand would be calculated as:
The price elasticity of demand is computed as the percentage change in the quantity demanded divided by the percentage change in price.

化工原理讲稿(上册)-应化第1章流体流动3

化工原理讲稿(上册)-应化第1章流体流动3

⒋湍流摩擦系数-因次分析法的应用 :
实验证明:d、u、ρ 、μ 一定时,ΔPf∝l/d
Pf du l K 2 u d d
e g
e g
l u 2 Pf 2KRe d d 2
而:
Pf
1 u umax 2
(二)层流时的速度分布和摩擦系数
32 lu Pf 2 d
——哈根—泊谡叶公式
32 2 l u 2 64 l u 2 64 l u 2 Pf . . . . . . du d 2 ud d 2 Re d 2

64 Re
(三)湍流时的速度分布与摩擦系数 ⒈湍流速度分布: 湍流流动加剧了管内流体的混合 与传递,使截面上的速度分布更 趋平坦。 速度分布符合1/n 次方规律:
四、直管阻力损失
(一) 计算通式
因摩擦阻力而引起的能量损失:
l u2 hf d 2
J/k g
--范宁公式
λ是无因次的系数,称为摩擦阻力系数。
(一) 计算通式
流体的压力损失:
l u 2 p f d 2
J/m3(pa)
流体的压头损失:
l u2 Hf d 2g
u↑, μ ↓ → 惯性力主导 → 湍流 u↓, μ ↑ → 粘性力主导 → 层流
二、 边界层概念
1.平壁边界层的形成及发展
u0
u0
边界层界限
u0
y
x
定义:通常把从流速为0的壁面处至流速等于主体流 速的99%处之间的区域称为边界层。
1.平壁边界层的形成及发展
判据:
流型由Rex= xu0ρ /μ 值来决定,对于光滑的平板壁面:
Pf K d l u

06.摩擦与阻力mm

06.摩擦与阻力mm

层流摩擦系数
Friction Coefficient in Laminar Flow
4L 32 Lu P s 2 d d L u 2 L u 2 P 4 f λ


d
2
d
2
层流时的摩擦系数
64 4f 64 Re du
上式为流体在圆管内作滞流流动时λ与Re 的关系式。若将此式在对数坐标上进行标绘, 可得一直线。
L L P = 2 s 4 s R d
f
u 2 / 2
s
L u 2 L u 2 P 4 f λ d 2 d 2

L u2 hf λ d 2
P
λ 4 f
上两式就是普遍使用的直管阻力计算式。
直管阻力计算式
Formula for Straight Pipe Resistance


du dy

du l dy
2
2
流体流动阻力机理
Mechanics of Resistance in Fluid Flow

形体阻力:边界层分离时,由于逆压差的 作用,流体将发生倒流形成尾涡,消耗能 量,这称之为形体阻力。
流体流动阻力分类
Classification of Resistance in Fluid Flow

白金汉π定理指出:任何因次一致的物理方 程式都可以表示成为由若干个无因次数群 构成的函数,若物理量的数目为n ,用来表 示这些物理量的基本因次数目为m ,则特 征数的数目N=n-m。
因次分析法的基本步骤
Steps of Dimensional Analysis Method
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V a : average velocity in pipe leading to fitting
K f : loss factor for fitting (管件), which is found by experiment and differs for
each type of connection. A short list of
hfc
Kc
Vb2 2
(5.69)
K c is called the contraction loss coefficient
V b is the average velocity in the smaller, or downstream, section
19
• By experiment,
• For laminar flow, Kc 0.1
7
8
10. Nonisothermal flow
• Liquid is being cooled • f is increased. • Liquid is being heated • f is decreased.
9
Байду номын сангаас
• f = f ’/ Ψ
•For Re>2,100:
w w00..1117
Note that flow rate, velocity and cross section area can’t be calculated by Deq .
12
5.4 FRICTION FROM CHANGES IN VELOCITY OR DIRECTION
• 1. Friction loss from sudden expansion of cross section
28
6. Separation from velocity decrease
• Boundary layer separation in no sudden change
cross section
sA :line of zero
tangential velocity
separation point
• 2. Friction loss from sudden contraction of cross section
13
• 3. Effect of fittings and valves • 4. Form friction losses in the Bernoulli equation • 5. Velocity heads • 6. Separation from velocity decrease • 7. Minimizing expansion and contraction losses
Re.
1
Laminar flow
f 16 16 DV Re
Turbulent flow: for hydraulically smooth pipe
Coburn equation Blasius equation
f 0.04R 6 e0.2
f 0.07R 9e0.25
This applies over Re from about 50,000 to 1 x 106.
11
11. Turbulent flow in noncircular channels
• Relationships for turbulent flow in pipes may be applied to noncircular channels by substituting the equivalent diameter Deq (or 4 times the hydraulic radius rH) for the diameter D in the relevant equations.
31
5.5 Design of piping system
• 1. Compound pipes in series • Pipeline has the same diameter or consist of
sections of different diameters. 2. Compound pipes in parallel Pipeline branches off at a common point or has a bypass.
6
9. Drag reduction in turbulent flow
• Dilute solutions of polymers in water or other solvents sometimes give the peculiar effect of a reduction in drag in turbulent flow.
For Re<2,100:
w w00..2338
fohr eating focrooling
fohr eating focr ooling
(5.60a) (5.60b)
(5.61a) (5.61b)
10
Viscous dissipation
• Frictional or viscous dissipation of mechanical energy can result in heating a fluid, especially highly viscous liquids in small channels.
Zb)4f
D LKcKeKf V22
27
5. Velocity heads
• velocity heads
2
V /2
the friction loss in a complicated flow system can be expressed as a number of velocity heads(速度 头).
The skin friction loss in the straight tube is
4fL /D V 2/2
The contraction loss at the entrance to the tube is
2
KcV /2 2
The expansion loss at the exit of the tube is KeV /2
14
1. Friction loss from sudden expansion of cross section
15
• The friction loss from a sudden expansion of cross section
hfe
Ke
Va2 2
(5.63)
K e is a proportionality factor called the
expansion loss coefficient
V a is the average velocity in the smaller, or
upstream, conduit.
16
• According to the steady-flow momentum-balance
equation (4.42), and the Bernoulli equation (4.62),
30
7. Minimizing expansion and contraction losses
• Changing the cross section gradually rather than suddenly can minimize the friction loss.
• Such as using Conical reducer(trumpet-shape ) Conical expander
f 0.00140.125 Re0.3 2
Applicable over Re from 3,000 to 3 x 106
4
Turbulent flow: for rough pipe
f Re,k D
Complete turbulent flow:
f k D
5
☆ 8. Reynolds numbers and friction factor for non-newtonian fluids
•the contraction loss is negligible
For turbulent flow,
Kc
0.41
Sb Sa
(5.70)
where Sa and Sb are the cross-sectional areas of the upstream and downstream conduits, respectively.
2
The friction loss in the globe valve is Kf V /2
26
The total friction is
hf 4fD LKcKeKfV22
(5.72)
To write the Bernoulli equation for this assembly
pa
pb
g(Za
VQcTpS
T pS
c
(5.62)
• For the flow of polymers the temperature rise is about 4°C for a pressure drop of 10 MPa; for hydrocarbons it is about 6°C per 10 MPa.
• (a) Calculate the pressure drop in lbf/in.2 per 100 ft of pipe.
• (b) If the pressure drop must be limited to 2 lbf/in.2 per 100 ft of pipe, what is the maximum allowable velocity of the water?
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