SlideShare uma empresa Scribd logo
1 de 7
Fluid Mechanics and Thermodynamics<br />Weekly Assessed Tutorial Sheets <br />Tutor Sheets: WATS 6.<br />The WATS form a collection of weekly homework type problems in the form of out-of-class tutorial sheets. <br />Each WATS typically comprises of a couple of main questions of which each has around four/five linked supplementary questions. They were developed as part of an LTSN Engineering Mini-Project, funded at the University of Hertfordshire which aimed to develop a set of 'student unique' tutorial sheets to actively encourage and improve student participation within a first year first ‘fluid mechanics and thermodynamics’ module. Please see the accompanying Mini-Project Report “Improving student success and retention through greater participation and tackling student-unique tutorial sheets” for more information.<br />The WATS cover core Fluid Mechanics and Thermodynamics topics at first year undergraduate level. 11 tutorial sheets and their worked solutions are provided here for you to utilise in your teaching. The variables within each question can be altered so that each student answers the same question but will need to produce a unique solution.<br />FURTHER INFORMATION<br />Please see http://tinyurl.com/2wf2lfh to access the WATS Random Factor Generating Wizard. <br />There are also explanatory videos on how to use the Wizard and how to implement WATS available at http://www.youtube.com/user/MBRBLU#p/u/7/0wgC4wy1cV0 and http://www.youtube.com/user/MBRBLU#p/u/6/MGpueiPHpqk.<br />For more information on WATS, its use and impact on students please contact Mark Russell, School of Aerospace, Automotive and Design Engineering at University of Hertfordshire.<br /> <br />Fluid Mechanics and Thermodynamics<br />Weekly Assessed Tutorial Sheet 6 (WATS 6)<br />TUTOR SHEET – Data used in the Worked Solution<br />Q1. Consider the pipe and tank layout shown in figure 1. Assuming a fluid with a relative density of 1.06 flows through a 68 mm diameter pipe from the large tank to the small tank - calculate - <br />i)the velocity of the fluid flowing through the pipe (m/s) (3 marks)<br />ii)the Reynolds Number of the flow (1 mark).<br />iii)the likely nature of the flow regime i.e. laminar, transitional or turbulent(1 mark).<br />iv)the mass flow rate of fluid flowing through the pipe system (kg/s) (1 mark)<br />v)the volume flow rate of fluid flowing through the pipe system (m3/s) (1 mark).<br />Assume now that the velocity for part i) has been calculated to be 2.960 m/s calculate <br />vi)the head loss associated with the pipe line only (m) (1 mark)<br />vii)the pressure loss associated with the pipe line only (Pa) (1 mark)<br />viii)the head loss due to all the minor losses (m) (2 mark)<br />ix)the pressure loss due to all the minor losses (Pa) (1 mark)<br />x)the loss coefficient of the valve and (2 mark)<br />xi)the ratio, as a percentage, of the minor to the pipe losses.(%) (1 mark)<br />You may assume the following :<br />The friction factor associated with the interaction of the fluid and the pipe surface is 0.00600.<br />The fluids kinematic viscosity is 1.13 x 10-6 m2/s<br />The loss coefficients associated with the fluid as it leaves and enters the tanks are 0.78 and 1.02 respectively. <br />Figure 1. Drawing for Q1.<br />14.20 mPipe length 229 m1.70 mValve.Pressure loss = 33 Pa <br /> WATS 6 <br />Worked solution<br />This sheet is solved using the TUTOR data set. <br />Q1 i)the velocity of the fluid flowing through the pipe <br />The actual total head loss must equal the available head. For this case the available head is 14.2 – 1.7m = 12.5m. It is assumed that the flow of water somehow does not drain the large tank nor does it change the height of the fluid of the low tank. <br />For the system shown the actual total head loss is the sum of the head losses due to –<br />a)The exit from the large tank in-to the pipe line.<br />b)The pipe itself.<br />c)The valve and <br />d)The inlet from the pipeline into the small tank.<br />For fittings, the head loss is usually calculated via <br /> (m) <br />Where-as for straight pipe the head loss is usually calculated via<br /> (m)  <br />Collecting all the terms together allows us to write<br />Since the pressure loss of the valve is given we need to re-write this as a head loss. i.e. <br />     Writing this for the valve and collecting the student specific data gives.<br /> which is <br />  Hence <br /> = 1.72 m/s<br />ii)the Reynolds Number of the flow.<br />    In this case you are given kinematic viscosity () and not dynamic viscosity () hence <br />  because  <br />Application of student specific data gives. <br />   = 103504<br />iii)the likely nature of the flow regime i.e. laminar, transitional or turbulent.<br />For flow in pipes turbulence is likely when Re > 4000. In this case, therefore, the flow is likely to be turbulent. Note we do not say the fluid is turbulent but the flow is turbulent.<br />iv)the mass flow rate of fluid flowing through the pipe system<br />  and   therefore    i.e.  for this case <br /> = 6.62 kg/s<br />v)the volume flow rate of fluid flowing through the pipe system<br />Volume flow rate   therefore for this case<br /> = 0.00625 m3/s<br />vi)the head loss associated with the pipe line only<br /> <br /> = 36.09 m<br />vii) Pressure loss associated with the pipe only <br /> = 374931 Pa<br />viii) Head losses due to all the minor losses.<br />In this case the minor losses are derived from the exit from the tank into the pipe, the valve and the exit from the pipe into the small tank. Remembering <br />For tank to pipe and pipe to tank losses.<br /> = 0.804m<br />For the valve<br />=  0.0032m<br />Therefore total minor losses = 0.804 + 0.003 = 0.807 m<br />ix) Pressure losses due to all the minor losses.<br /> therefore <br /> = 8344 Pa<br />x)the loss coefficient of the valve.<br />Recall the minor head losses, (i.e. fittings etc), are found via - <br /> or in terms of pressure loss is <br /> writing for the loss coefficient () gives <br />   Which, using the data, gives, <br />  = 0.0071<br />xi)The ratio, as a percentage, of the minor to the pipe losses.<br />The minor losses = 8344 Pa<br />The pipe losses = 374931Pa<br />Hence the minor losses to the pipe losses =  = 0.0225 which is 2.25 %<br />Hope this helps.<br />If you see any errors or can offer any suggestions for improvements then please <br />e-mail me at                 m.b.russell@herts.ac.uk<br />Credits<br />This resource was created by the University of Hertfordshire and released as an open educational resource through the Open Engineering Resources project of the HE Academy Engineering Subject Centre. The Open Engineering Resources project was funded by HEFCE and part of the JISC/HE Academy UKOER programme.<br />© University of Hertfordshire 2009<br />This work is licensed under a Creative Commons Attribution 2.0 License. <br />The name of the University of Hertfordshire, UH and the UH logo are the name and registered marks of the University of Hertfordshire. To the fullest extent permitted by law the University of Hertfordshire reserves all its rights in its name and marks which may not be used except with its written permission.<br />The JISC logo is licensed under the terms of the Creative Commons Attribution-Non-Commercial-No Derivative Works 2.0 UK: England & Wales Licence.  All reproductions must comply with the terms of that licence.<br />The HEA logo is owned by the Higher Education Academy Limited may be freely distributed and copied for educational purposes only, provided that appropriate acknowledgement is given to the Higher Education Academy as the copyright holder and original publisher.<br />
WATS 6 Fluid Mechanics and Thermodynamics- Master And Solution
WATS 6 Fluid Mechanics and Thermodynamics- Master And Solution
WATS 6 Fluid Mechanics and Thermodynamics- Master And Solution
WATS 6 Fluid Mechanics and Thermodynamics- Master And Solution
WATS 6 Fluid Mechanics and Thermodynamics- Master And Solution
WATS 6 Fluid Mechanics and Thermodynamics- Master And Solution

Mais conteúdo relacionado

Destaque

Uu no 43_th_2007 perpustakaan
Uu no 43_th_2007 perpustakaanUu no 43_th_2007 perpustakaan
Uu no 43_th_2007 perpustakaan
Agus Sukyanto
 
Mary Kate And Ashley Olsen Powerpoint
Mary Kate And Ashley Olsen PowerpointMary Kate And Ashley Olsen Powerpoint
Mary Kate And Ashley Olsen Powerpoint
belene333
 
Presentation1
Presentation1Presentation1
Presentation1
jhommes5
 

Destaque (18)

Risultati sapienza
Risultati sapienzaRisultati sapienza
Risultati sapienza
 
Professional Development: Distance Learning Opportunities (Museums, Science C...
Professional Development: Distance Learning Opportunities (Museums, Science C...Professional Development: Distance Learning Opportunities (Museums, Science C...
Professional Development: Distance Learning Opportunities (Museums, Science C...
 
Portfolio Pp
Portfolio PpPortfolio Pp
Portfolio Pp
 
WATS 8 (1-50) Fluid Mechanics and Thermodynamics
WATS 8 (1-50) Fluid Mechanics and ThermodynamicsWATS 8 (1-50) Fluid Mechanics and Thermodynamics
WATS 8 (1-50) Fluid Mechanics and Thermodynamics
 
fotos
fotosfotos
fotos
 
Uu no 43_th_2007 perpustakaan
Uu no 43_th_2007 perpustakaanUu no 43_th_2007 perpustakaan
Uu no 43_th_2007 perpustakaan
 
SUperMe forum pa
SUperMe forum paSUperMe forum pa
SUperMe forum pa
 
Nino
NinoNino
Nino
 
Scholarship Links
Scholarship LinksScholarship Links
Scholarship Links
 
Sosyal Oyun Eğitimi-Social Media Academy
Sosyal Oyun Eğitimi-Social Media AcademySosyal Oyun Eğitimi-Social Media Academy
Sosyal Oyun Eğitimi-Social Media Academy
 
Natal
NatalNatal
Natal
 
Nino
NinoNino
Nino
 
WATS 4 (1-50) Fluid Mechanics and Thermodynamics
WATS 4 (1-50) Fluid Mechanics and ThermodynamicsWATS 4 (1-50) Fluid Mechanics and Thermodynamics
WATS 4 (1-50) Fluid Mechanics and Thermodynamics
 
Mary Kate And Ashley Olsen Powerpoint
Mary Kate And Ashley Olsen PowerpointMary Kate And Ashley Olsen Powerpoint
Mary Kate And Ashley Olsen Powerpoint
 
Presentation1
Presentation1Presentation1
Presentation1
 
Culture Of Contact
Culture Of ContactCulture Of Contact
Culture Of Contact
 
FF3300 issue #3
FF3300 issue #3FF3300 issue #3
FF3300 issue #3
 
Code: The Hidden Language of Computer Hardware and Software
Code: The Hidden Language of Computer Hardware and SoftwareCode: The Hidden Language of Computer Hardware and Software
Code: The Hidden Language of Computer Hardware and Software
 

Mais de Mark Russell

Iblc10 making an existing assessment more efficient
Iblc10   making an existing assessment more efficientIblc10   making an existing assessment more efficient
Iblc10 making an existing assessment more efficient
Mark Russell
 

Mais de Mark Russell (10)

Iblc10 making an existing assessment more efficient
Iblc10   making an existing assessment more efficientIblc10   making an existing assessment more efficient
Iblc10 making an existing assessment more efficient
 
Two-Dimension Steady-State Conduction
Two-Dimension Steady-State ConductionTwo-Dimension Steady-State Conduction
Two-Dimension Steady-State Conduction
 
WATS 9 (1-50) Fluid Mechanics and Thermodynamics
WATS 9 (1-50) Fluid Mechanics and ThermodynamicsWATS 9 (1-50) Fluid Mechanics and Thermodynamics
WATS 9 (1-50) Fluid Mechanics and Thermodynamics
 
WATS 10 (1-50) Fluid Mechanics and Thermodynamics
WATS 10 (1-50) Fluid Mechanics and ThermodynamicsWATS 10 (1-50) Fluid Mechanics and Thermodynamics
WATS 10 (1-50) Fluid Mechanics and Thermodynamics
 
WATS 7 (1-50) Fluid Mechanics and Thermodynamics
WATS 7 (1-50) Fluid Mechanics and ThermodynamicsWATS 7 (1-50) Fluid Mechanics and Thermodynamics
WATS 7 (1-50) Fluid Mechanics and Thermodynamics
 
WATS 6 (1-50) Fluid Mechanics and Thermodynamics
WATS 6 (1-50) Fluid Mechanics and ThermodynamicsWATS 6 (1-50) Fluid Mechanics and Thermodynamics
WATS 6 (1-50) Fluid Mechanics and Thermodynamics
 
WATS 5 (1-50) Fluid Mechanics and Thermodynamics
WATS 5 (1-50) Fluid Mechanics and ThermodynamicsWATS 5 (1-50) Fluid Mechanics and Thermodynamics
WATS 5 (1-50) Fluid Mechanics and Thermodynamics
 
WATS 1 (1-50) Fluid Mechanics and Thermodynamics
WATS 1 (1-50) Fluid Mechanics and ThermodynamicsWATS 1 (1-50) Fluid Mechanics and Thermodynamics
WATS 1 (1-50) Fluid Mechanics and Thermodynamics
 
WATS 3 (1-50) Fluid Mechanics and Thermodynamics
WATS 3 (1-50) Fluid Mechanics and ThermodynamicsWATS 3 (1-50) Fluid Mechanics and Thermodynamics
WATS 3 (1-50) Fluid Mechanics and Thermodynamics
 
WATS 11 (1-50) Fluid Mechanics and Thermodynamics
WATS 11 (1-50)  Fluid Mechanics and ThermodynamicsWATS 11 (1-50)  Fluid Mechanics and Thermodynamics
WATS 11 (1-50) Fluid Mechanics and Thermodynamics
 

Último

Ecosystem Interactions Class Discussion Presentation in Blue Green Lined Styl...
Ecosystem Interactions Class Discussion Presentation in Blue Green Lined Styl...Ecosystem Interactions Class Discussion Presentation in Blue Green Lined Styl...
Ecosystem Interactions Class Discussion Presentation in Blue Green Lined Styl...
fonyou31
 
Russian Escort Service in Delhi 11k Hotel Foreigner Russian Call Girls in Delhi
Russian Escort Service in Delhi 11k Hotel Foreigner Russian Call Girls in DelhiRussian Escort Service in Delhi 11k Hotel Foreigner Russian Call Girls in Delhi
Russian Escort Service in Delhi 11k Hotel Foreigner Russian Call Girls in Delhi
kauryashika82
 
The basics of sentences session 2pptx copy.pptx
The basics of sentences session 2pptx copy.pptxThe basics of sentences session 2pptx copy.pptx
The basics of sentences session 2pptx copy.pptx
heathfieldcps1
 
1029 - Danh muc Sach Giao Khoa 10 . pdf
1029 -  Danh muc Sach Giao Khoa 10 . pdf1029 -  Danh muc Sach Giao Khoa 10 . pdf
1029 - Danh muc Sach Giao Khoa 10 . pdf
QucHHunhnh
 

Último (20)

Introduction to Nonprofit Accounting: The Basics
Introduction to Nonprofit Accounting: The BasicsIntroduction to Nonprofit Accounting: The Basics
Introduction to Nonprofit Accounting: The Basics
 
Código Creativo y Arte de Software | Unidad 1
Código Creativo y Arte de Software | Unidad 1Código Creativo y Arte de Software | Unidad 1
Código Creativo y Arte de Software | Unidad 1
 
Presentation by Andreas Schleicher Tackling the School Absenteeism Crisis 30 ...
Presentation by Andreas Schleicher Tackling the School Absenteeism Crisis 30 ...Presentation by Andreas Schleicher Tackling the School Absenteeism Crisis 30 ...
Presentation by Andreas Schleicher Tackling the School Absenteeism Crisis 30 ...
 
Advanced Views - Calendar View in Odoo 17
Advanced Views - Calendar View in Odoo 17Advanced Views - Calendar View in Odoo 17
Advanced Views - Calendar View in Odoo 17
 
Disha NEET Physics Guide for classes 11 and 12.pdf
Disha NEET Physics Guide for classes 11 and 12.pdfDisha NEET Physics Guide for classes 11 and 12.pdf
Disha NEET Physics Guide for classes 11 and 12.pdf
 
Ecosystem Interactions Class Discussion Presentation in Blue Green Lined Styl...
Ecosystem Interactions Class Discussion Presentation in Blue Green Lined Styl...Ecosystem Interactions Class Discussion Presentation in Blue Green Lined Styl...
Ecosystem Interactions Class Discussion Presentation in Blue Green Lined Styl...
 
BAG TECHNIQUE Bag technique-a tool making use of public health bag through wh...
BAG TECHNIQUE Bag technique-a tool making use of public health bag through wh...BAG TECHNIQUE Bag technique-a tool making use of public health bag through wh...
BAG TECHNIQUE Bag technique-a tool making use of public health bag through wh...
 
A Critique of the Proposed National Education Policy Reform
A Critique of the Proposed National Education Policy ReformA Critique of the Proposed National Education Policy Reform
A Critique of the Proposed National Education Policy Reform
 
Call Girls in Dwarka Mor Delhi Contact Us 9654467111
Call Girls in Dwarka Mor Delhi Contact Us 9654467111Call Girls in Dwarka Mor Delhi Contact Us 9654467111
Call Girls in Dwarka Mor Delhi Contact Us 9654467111
 
Russian Escort Service in Delhi 11k Hotel Foreigner Russian Call Girls in Delhi
Russian Escort Service in Delhi 11k Hotel Foreigner Russian Call Girls in DelhiRussian Escort Service in Delhi 11k Hotel Foreigner Russian Call Girls in Delhi
Russian Escort Service in Delhi 11k Hotel Foreigner Russian Call Girls in Delhi
 
Key note speaker Neum_Admir Softic_ENG.pdf
Key note speaker Neum_Admir Softic_ENG.pdfKey note speaker Neum_Admir Softic_ENG.pdf
Key note speaker Neum_Admir Softic_ENG.pdf
 
The basics of sentences session 2pptx copy.pptx
The basics of sentences session 2pptx copy.pptxThe basics of sentences session 2pptx copy.pptx
The basics of sentences session 2pptx copy.pptx
 
INDIA QUIZ 2024 RLAC DELHI UNIVERSITY.pptx
INDIA QUIZ 2024 RLAC DELHI UNIVERSITY.pptxINDIA QUIZ 2024 RLAC DELHI UNIVERSITY.pptx
INDIA QUIZ 2024 RLAC DELHI UNIVERSITY.pptx
 
Measures of Dispersion and Variability: Range, QD, AD and SD
Measures of Dispersion and Variability: Range, QD, AD and SDMeasures of Dispersion and Variability: Range, QD, AD and SD
Measures of Dispersion and Variability: Range, QD, AD and SD
 
Q4-W6-Restating Informational Text Grade 3
Q4-W6-Restating Informational Text Grade 3Q4-W6-Restating Informational Text Grade 3
Q4-W6-Restating Informational Text Grade 3
 
Z Score,T Score, Percential Rank and Box Plot Graph
Z Score,T Score, Percential Rank and Box Plot GraphZ Score,T Score, Percential Rank and Box Plot Graph
Z Score,T Score, Percential Rank and Box Plot Graph
 
1029 - Danh muc Sach Giao Khoa 10 . pdf
1029 -  Danh muc Sach Giao Khoa 10 . pdf1029 -  Danh muc Sach Giao Khoa 10 . pdf
1029 - Danh muc Sach Giao Khoa 10 . pdf
 
IGNOU MSCCFT and PGDCFT Exam Question Pattern: MCFT003 Counselling and Family...
IGNOU MSCCFT and PGDCFT Exam Question Pattern: MCFT003 Counselling and Family...IGNOU MSCCFT and PGDCFT Exam Question Pattern: MCFT003 Counselling and Family...
IGNOU MSCCFT and PGDCFT Exam Question Pattern: MCFT003 Counselling and Family...
 
Grant Readiness 101 TechSoup and Remy Consulting
Grant Readiness 101 TechSoup and Remy ConsultingGrant Readiness 101 TechSoup and Remy Consulting
Grant Readiness 101 TechSoup and Remy Consulting
 
microwave assisted reaction. General introduction
microwave assisted reaction. General introductionmicrowave assisted reaction. General introduction
microwave assisted reaction. General introduction
 

WATS 6 Fluid Mechanics and Thermodynamics- Master And Solution

  • 1. Fluid Mechanics and Thermodynamics<br />Weekly Assessed Tutorial Sheets <br />Tutor Sheets: WATS 6.<br />The WATS form a collection of weekly homework type problems in the form of out-of-class tutorial sheets. <br />Each WATS typically comprises of a couple of main questions of which each has around four/five linked supplementary questions. They were developed as part of an LTSN Engineering Mini-Project, funded at the University of Hertfordshire which aimed to develop a set of 'student unique' tutorial sheets to actively encourage and improve student participation within a first year first ‘fluid mechanics and thermodynamics’ module. Please see the accompanying Mini-Project Report “Improving student success and retention through greater participation and tackling student-unique tutorial sheets” for more information.<br />The WATS cover core Fluid Mechanics and Thermodynamics topics at first year undergraduate level. 11 tutorial sheets and their worked solutions are provided here for you to utilise in your teaching. The variables within each question can be altered so that each student answers the same question but will need to produce a unique solution.<br />FURTHER INFORMATION<br />Please see http://tinyurl.com/2wf2lfh to access the WATS Random Factor Generating Wizard. <br />There are also explanatory videos on how to use the Wizard and how to implement WATS available at http://www.youtube.com/user/MBRBLU#p/u/7/0wgC4wy1cV0 and http://www.youtube.com/user/MBRBLU#p/u/6/MGpueiPHpqk.<br />For more information on WATS, its use and impact on students please contact Mark Russell, School of Aerospace, Automotive and Design Engineering at University of Hertfordshire.<br /> <br />Fluid Mechanics and Thermodynamics<br />Weekly Assessed Tutorial Sheet 6 (WATS 6)<br />TUTOR SHEET – Data used in the Worked Solution<br />Q1. Consider the pipe and tank layout shown in figure 1. Assuming a fluid with a relative density of 1.06 flows through a 68 mm diameter pipe from the large tank to the small tank - calculate - <br />i)the velocity of the fluid flowing through the pipe (m/s) (3 marks)<br />ii)the Reynolds Number of the flow (1 mark).<br />iii)the likely nature of the flow regime i.e. laminar, transitional or turbulent(1 mark).<br />iv)the mass flow rate of fluid flowing through the pipe system (kg/s) (1 mark)<br />v)the volume flow rate of fluid flowing through the pipe system (m3/s) (1 mark).<br />Assume now that the velocity for part i) has been calculated to be 2.960 m/s calculate <br />vi)the head loss associated with the pipe line only (m) (1 mark)<br />vii)the pressure loss associated with the pipe line only (Pa) (1 mark)<br />viii)the head loss due to all the minor losses (m) (2 mark)<br />ix)the pressure loss due to all the minor losses (Pa) (1 mark)<br />x)the loss coefficient of the valve and (2 mark)<br />xi)the ratio, as a percentage, of the minor to the pipe losses.(%) (1 mark)<br />You may assume the following :<br />The friction factor associated with the interaction of the fluid and the pipe surface is 0.00600.<br />The fluids kinematic viscosity is 1.13 x 10-6 m2/s<br />The loss coefficients associated with the fluid as it leaves and enters the tanks are 0.78 and 1.02 respectively. <br />Figure 1. Drawing for Q1.<br />14.20 mPipe length 229 m1.70 mValve.Pressure loss = 33 Pa <br /> WATS 6 <br />Worked solution<br />This sheet is solved using the TUTOR data set. <br />Q1 i)the velocity of the fluid flowing through the pipe <br />The actual total head loss must equal the available head. For this case the available head is 14.2 – 1.7m = 12.5m. It is assumed that the flow of water somehow does not drain the large tank nor does it change the height of the fluid of the low tank. <br />For the system shown the actual total head loss is the sum of the head losses due to –<br />a)The exit from the large tank in-to the pipe line.<br />b)The pipe itself.<br />c)The valve and <br />d)The inlet from the pipeline into the small tank.<br />For fittings, the head loss is usually calculated via <br /> (m) <br />Where-as for straight pipe the head loss is usually calculated via<br /> (m) <br />Collecting all the terms together allows us to write<br />Since the pressure loss of the valve is given we need to re-write this as a head loss. i.e. <br /> Writing this for the valve and collecting the student specific data gives.<br /> which is <br /> Hence <br /> = 1.72 m/s<br />ii)the Reynolds Number of the flow.<br /> In this case you are given kinematic viscosity () and not dynamic viscosity () hence <br /> because <br />Application of student specific data gives. <br /> = 103504<br />iii)the likely nature of the flow regime i.e. laminar, transitional or turbulent.<br />For flow in pipes turbulence is likely when Re > 4000. In this case, therefore, the flow is likely to be turbulent. Note we do not say the fluid is turbulent but the flow is turbulent.<br />iv)the mass flow rate of fluid flowing through the pipe system<br /> and therefore i.e. for this case <br /> = 6.62 kg/s<br />v)the volume flow rate of fluid flowing through the pipe system<br />Volume flow rate therefore for this case<br /> = 0.00625 m3/s<br />vi)the head loss associated with the pipe line only<br /> <br /> = 36.09 m<br />vii) Pressure loss associated with the pipe only <br /> = 374931 Pa<br />viii) Head losses due to all the minor losses.<br />In this case the minor losses are derived from the exit from the tank into the pipe, the valve and the exit from the pipe into the small tank. Remembering <br />For tank to pipe and pipe to tank losses.<br /> = 0.804m<br />For the valve<br />= 0.0032m<br />Therefore total minor losses = 0.804 + 0.003 = 0.807 m<br />ix) Pressure losses due to all the minor losses.<br /> therefore <br /> = 8344 Pa<br />x)the loss coefficient of the valve.<br />Recall the minor head losses, (i.e. fittings etc), are found via - <br /> or in terms of pressure loss is <br /> writing for the loss coefficient () gives <br /> Which, using the data, gives, <br /> = 0.0071<br />xi)The ratio, as a percentage, of the minor to the pipe losses.<br />The minor losses = 8344 Pa<br />The pipe losses = 374931Pa<br />Hence the minor losses to the pipe losses = = 0.0225 which is 2.25 %<br />Hope this helps.<br />If you see any errors or can offer any suggestions for improvements then please <br />e-mail me at m.b.russell@herts.ac.uk<br />Credits<br />This resource was created by the University of Hertfordshire and released as an open educational resource through the Open Engineering Resources project of the HE Academy Engineering Subject Centre. The Open Engineering Resources project was funded by HEFCE and part of the JISC/HE Academy UKOER programme.<br />© University of Hertfordshire 2009<br />This work is licensed under a Creative Commons Attribution 2.0 License. <br />The name of the University of Hertfordshire, UH and the UH logo are the name and registered marks of the University of Hertfordshire. To the fullest extent permitted by law the University of Hertfordshire reserves all its rights in its name and marks which may not be used except with its written permission.<br />The JISC logo is licensed under the terms of the Creative Commons Attribution-Non-Commercial-No Derivative Works 2.0 UK: England & Wales Licence.  All reproductions must comply with the terms of that licence.<br />The HEA logo is owned by the Higher Education Academy Limited may be freely distributed and copied for educational purposes only, provided that appropriate acknowledgement is given to the Higher Education Academy as the copyright holder and original publisher.<br />