Fluid Mechanics Lectures 2nd year/2nd semister/ /Al-Mustansiriyah unv

Slides:



Advertisements
Similar presentations
Fluid Mechanics.
Advertisements

Fluid Mechanics 07.
Energy Conservation (Bernoulli’s Equation)
Pipeline Hydraulics.
CE 230-Engineering Fluid Mechanics
Reynolds Experiment Laminar Turbulent Reynolds Number
Pertemuan CLOSED CONDUIT FLOW 1
Fluid Mechanics 06. Energy, Work and Power Work:- Work is force acting through a distance when the force is parallel to the direction of motion. Energy:-
Test 1A Same material Voluntary Outside regular class.
Fluid Mechanics 08.
CE 230-Engineering Fluid Mechanics
CBE 150A – Transport Spring Semester 2014 Friction Losses Flow through Conduits Incompressible Flow.
CE Fluid Mechanics Diogo Bolster
KNTU CIVIL ENGINEERIG FACULTY ` FLOW IN PIPES With special thanks to Mr.VAKILZADE.
Energy Conservation (Bernoulli’s Equation)
FE Hydraulics/Fluid Mechanics Review
Core Ag Engineering Principles – Session 1
Assignment No. 1 [Grup 8] Figure below shows a portion of a hydraulic circuit. The pressure point B must be 200 psig when the volume flow rate is 60 gal/min.
MER Design of Thermal Fluid Systems Pumps and Fans Professor Anderson Spring Term
PHAROS UNIVERSITY ME 259 FLUID MECHANICS FOR ELECTRICAL STUDENTS Basic Equations for a Control Volume.
Pumps and Lift Stations. Background Fluid Moving Equipment Fluids are moved through flow systems using pumps, fans, blowers, and compressors. Such devices.
Boundary layer concept
Things to grab for this session (in priority order)  Pencil  Henderson, Perry, and Young text (Principles of Process Engineering)  Calculator  Eraser.
Unit: V-Flow Through Pipes. Flow Through Pipes  Major Energy Losses - Darcy-Weisbach Formula - Chezy’s Formula  Minor Energy Losses -Sudden expansion.
CTC 450 Energy Equation.
Viscous Flow.
Things to grab for this session (in priority order)  Pencil  Henderson, Perry, and Young text (Principles of Process Engineering)  Calculator  Eraser.
 V 1 2 / 2 + p 1 /  + gz 1 =  V 2 2 /2 + p 2 /  + gz 2 + h lT h lT = h l + h m HEADLOSSHEADLOSS.
Lesson 23 HEAD LOSS DEFINE the terms head loss, frictional loss, and minor losses. DETERMINE friction factors for various flow situations using the Moody.
CBE 150A – Transport Spring Semester 2014 Other Friction Losses Valves and Fittings.
Hydraulics & Hydrology Review 1 Lecture3 Dr. Jawad Al-rifai.
Elementary Mechanics of Fluids CE 319 F Daene McKinney Momentum Equation.
Things to grab for this session (in priority order)  Pencil  Henderson, Perry, and Young text (Principles of Process Engineering)  Calculator  Eraser.
Pharos University ME 259 Fluid Mechanics for Electrical Students Revision for Final Exam Dr. A. Shibl.
Viscous Flow in Pipes: Overview
FLUID FOW FOR CHEMICAL ENGINEERING
SUGGESTED MINIMUM KNOWLEDGE OF FLUID MECHANICS AND FOR FE EXAM
Major loss in Ducts, Tubes and Pipes
8.2 OBJECTIVES  Describe the appearance of laminar flow and turbulent flow  State the relationship used to compute the Reynolds number  Identify the.
Power – Energy Relationships
EXERCISES Two water reservoirs are connected by a pipe 610m of 0.3m diameter, f’=0.038 and the flow produced by the difference in water surface elevations.
Energy Conservation (Bernoulli’s Equation)
Design of Cold Water Networks
and the like in the pipe or duct system.
Subject Name: FLUID MECHANICS
C.k.pithawalla college of enginnering & technology
Environmental Engineering CIV2257
FRICTION FACTOR A common parameter used in LAMINAR and especially in TURBULENT flow is the Fanning friction factor, f ‘f ’is as the ratio defined of wall.
CTC 450 Energy Equation.
Chapter 4. Analysis of Flows in Pipes
Exergy analysis of geothermal Energy
Losses due to Fluid Friction
Pumps and Lift Stations
Chapter 6 THE MECHANICAL ENERGY BALANCE.
CTC 450 Review Energy Equation Pressure head Velocity head
Head Loss in storm water systems Check valves
Fluid Mechanics Lectures 2nd year/1st semister/ /Al-Mustansiriyah unv
Line Sizing By Shardul Kulkarni.
50 m EML3015C Thermal-Fluid I Fall 2000 Homework 4
Mohammed Al-Nasheri Madi Al-Hajri Fahad Al-Jubreen Omar Hassan
Fluid Mechanics Lectures 2nd year/1st semister/ /Al-Mustansiriyah unv
Lecture Objectives: Learn about Pumps and System Curves.
Pumps and pumping station
Fluid Mechanics Lectures 2nd year/2nd semister/ /Al-Mustansiriyah unv
Fluid Mechanics Lectures 2nd year/2nd semister/ /Al-Mustansiriyah unv
Fluid Mechanics Lectures 2nd year/2nd semister/ /Al-Mustansiriyah unv
Fluid Mechanics Lectures 2nd year/2nd semister/ /Al-Mustansiriyah unv
Fluid Mechanics Lectures 2nd year/2nd semister/ /Al-Mustansiriyah unv
Energy Conservation (Bernoulli’s Equation)
9. FLUID FLOW: Working Problems
Presentation transcript:

Fluid Mechanics Lectures 2nd year/2nd semister/2018-2019/Al-Mustansiriyah unv./College of engineering/Highway &Transportation Dep.Lec.1

. Ex1:Oil with µ= 0.38 N.s/m2, Ƿ= 912 kg/m3, flows through a horizontal 100 mm dia. and 500 m length, pipe at flow rate = 0.01 m3/s. Determine the pressure drop in the pipe? ΔPf= 128 𝜇 𝑄 𝐿 𝜋 𝐷 2 = 128∗0.38∗500∗0.01 𝜋( 0.1) 4 = 774000 pa =772 kpa. To find Re: V=v avg.=Q/A= 0.01 𝜋 4 ∗ (0.1) 2 = 1.27 m/s Re = 𝜌𝑣 𝐷 𝜇 = 912∗1.27∗0.1 0.38 = 306 ˂ 2000 laminar flow and the analysis is valid.

Ex2'; Oil (µ=4*10-3)lb.s/ft2, Ƿ=1.8 slugs/ft3,flows through an inclined pipe (fig. 6) dia.=3 in, find the slope of the pipe that will cause the pressure to be constant along the pipe? (𝜀=0.00026) . Z1+ 𝑣 1 2 2𝑔 + 𝑃 1 𝛾 - 32 𝜇 𝑣 𝐿 𝛾 𝐷 2 = Z2 + 𝑣 2 2 2𝑔 + 𝑃 2 𝛾 P1= p2 and v1=v2 𝑍1−𝑍2 𝐿 = 32 𝜇 𝑣 𝐿 𝛾 𝐷 2 = 32 𝜇𝑣 𝜌𝑔𝐷 2 v=vavg.=Q/A= 0.3 𝜋 4 ( 3 12 ) 2 =6.11 ft/s sin𝜃= 𝑍1−𝑍2 𝐿 sin𝜃= 32 𝜇𝑣 𝜌𝑔𝐷 2 = (32)(4∗10 −3 )(6.11) 1.8∗32.2∗( 3 12 ) =0.216 𝑓𝑡/𝑓𝑡 𝜃=12.5° Re= 6.11∗ 3 12 ∗1.8 4∗10 −3 = 687 ˂ 2000 laminar flow

Ex3: The pump (fig. 7) delivers 0 Ex3: The pump (fig.7) delivers 0.03 m3/s water from lake to the top of a hill. The cast iron pipe has a diameter of 80 mm and a length of 200 m , find the required power the pump must be deliver to the water?

Z1+ 𝑣 1 2 2𝑔 + 𝑃 1 𝛾 + Hp - 𝑓 𝐿 𝐷 𝑣 2 2𝑔 = Z2 + 𝑣 2 2 2𝑔 + 𝑃 2 𝛾 P1=p2 𝑣 1 2 2𝑔 =0 Hp = 𝑣 2 2 2𝑔 (Z2-Z1) + 𝑓 𝐿 𝐷 𝑣 2 2𝑔 V2=Q/A= 0.03 𝜋/4(0.08) 2 =5.97 m/s Solve for Re v=1.12 *10-6 m2/s Re= 𝑉𝐷 𝑣 = 5.97∗0.08 1.12 =4.26 *105 𝜀 𝐷 = 0.00026 0.08 =0.00325 from Moody diagram f=0.026 Hp= 5.97 2∗9.81 +50+0.026∗ 200 0.08 ∗ (5.97) 2 2∗9.81 =169.8 m Pump power =γ Hp Q =9800* 169.8*0.03 =49900 watt= 49.9 kwatt Note:Pump efficiency = 𝑝𝑜𝑤𝑒𝑟 𝑜𝑢𝑡 𝑝𝑜𝑤𝑒𝑟 𝑖𝑛 ∗100%

For example: A pump have an efficiency 60% lift water to height 50 m at flow rate 0.1 m3/s, what is the required pump power in KW? Pump power =γ Hp Q Power out= 9.8 * 50* 0.1 =49 KW Efficiency = 𝑝𝑜𝑤𝑒𝑟 𝑜𝑢𝑡 𝑝𝑜𝑤𝑒𝑟 𝑖𝑛 ∗100% Pin = ( Pout/ eff.)*100% =82 KW -

Ex4: The pump (fig.) add a 15 ft head to water being pumped when the flow rate is 1.5 ft3/s. Determine the friction factor for the pipe?

∑KL= Kent +K elbow +Kexit =0.6+ 2(0.3) + 1=2.2 Z1+ 𝑣 1 2 2𝑔 + 𝑃 1 𝛾 + Hp - 𝑓 𝐿 𝐷 𝑣 2 2𝑔 +𝐾 𝐿 𝑣 2 2𝑔 = Z2 + 𝑣 2 2 2𝑔 + 𝑃 2 𝛾 P1=0 V1=0 Z1=0 Hp=15 Z2=195m V2=0 ∑KL= Kent +K elbow +Kexit =0.6+ 2(0.3) + 1=2.2 200 +15= 3∗144 62.4 +195 + 𝑓 200 0.5 +2.2∗ 𝑣 2 2∗32.2 V=Q/A= 1.5 𝜋 4 ∗0.5 2 = 7.64 ft/s f=0.0306

. Ex5: When water flows from the tank shown if fig.9, find the water velocity if the water depth in tank is h= 1.5 ft , the total length of 0.6 in dia. pipe is 20 ft, and the friction factor is 0.03. The loss coefficients are 0.5 for entrance, 1.5 for each elbow and 10 for valve? .

. P1=P2 Z1=0 Z2=3 ft+h V1=0 V2=V AND HL= 𝑓 𝐿 𝐷 𝑣 2 2𝑔 +𝐾 𝐿 𝑣 2 2𝑔 Z1+ 𝑣 1 2 2𝑔 + 𝑃 1 𝛾 + HL = Z2 + 𝑣 2 2 2𝑔 + 𝑃 2 𝛾 P1=P2 Z1=0 Z2=3 ft+h V1=0 V2=V AND HL= 𝑓 𝐿 𝐷 𝑣 2 2𝑔 +𝐾 𝐿 𝑣 2 2𝑔 Z1=4.5 ft 4.5 = (0.3 20 0.6/12 +18+1) 𝑣 2 2∗32.2 V=3.06 ft/s Q=AV= 𝜋 4 ( 0.6 12 ) 2 (3.06) = 0.00601 ft 3/s

Thanks