UNIT 1 OPEN CHANNEL FLOW 2 MARK QUESTIONS AND ANSWERS

Size: px
Start display at page:

Download "UNIT 1 OPEN CHANNEL FLOW 2 MARK QUESTIONS AND ANSWERS"

Transcription

1 DEPARTMENT: CIVIL ENGINEERING SEMESTER: IV- SEMESTER SUBJECT CODE / Name: CE53 / Applied Hydrauli Engineering 1. Define open hannel flow with examples. Examples: UNIT 1 OPEN CHANNEL FLOW MARK QUESTIONS AND ANSWERS Flow of liquid with a free surfae (i.e., surfae exposed to atmosphere) through any passage is known as open hannel flow. The liquid flowing through any losed passage without touhing the top an also treated as open hannels. 1. Flow in natural waterfalls, river and streams. Flow in artifiial or man-made hannels suh as irrigation hannels and flumes. 3. Closed onduit or pipe arries liquid partially (sewers that arry domesti or industrial waste water). Generally, liquid flowing in open hannel in water.. Explain laminar and turbulent flow. (a) Laminar flow: If Reynolds number of flow is less than 500, it is alled as Laminar flow. The value of Reynolds number is between 500 and 000, the flow is transitional. (b) Turbulent flow: For values of Reynolds number greater than 000, the flow is turbulent. 3. What are the various types of flow in open hannels? The flow in open hannel is lassified into the following types: (a) Steady and unsteady flow (b) Uniform and non- uniform flow () Laminar and turbulent flow (d) Subritial, ritial and superritial flow. 4. Define the term uniform flow. If the depth of flow, slope of the bed of hannel and ross setion remain onstant with respet to distane is alled uniform flow. y V 0, 0 s s IV Semester CE53 / Applied Hydrauli Engineering by P.Dhanabal AP / Civil Page 1

2 5. Define non uniform flow. Flow properties, suh as depth of flow, veloity of flow are not onstant with respet to distane is alled non uniform flow. y V 0, 0 s s 6. Distinguish between steady and unsteady flow. In steady flow, various harateristis of flowing fluids suh as veloity, pressure, density, temperature et. at a point do not hange with time. In other words, a steady flow may be defined as that in whih the various harateristis are independent of time. Mathematially it an be expressed as u v w 0, 0 ; 0 t t t p 0, 0 t t In unsteady flow, various harateristis of flowing fluids suh as veloity, pressure, density, et. at a point hange with respet to time. Mathematially, v p 0 and ( or) 0... t t et Unsteadiness refers to the hange of flow pattern with the passage of time at a position in the flow. 7. Explain the terms: (i) Gradually varied flow and (ii) Rapidly varied flow. [Anna Univ.Nov 07&Nov 08] 1. Gradually varied flow If the depth of flow hanges gradually over a long length of the hannel, the flow is said to gradually varied flow (GVF) IV Semester CE53 / Applied Hydrauli Engineering by P.Dhanabal AP / Civil Page

3 . Rapidly varied flow. If the depth of flow hanges rapidly over a small length of the hannel, the flow is said to be rapidly varied flow. 8. Write down the formula for Froude number Froute Number F V gd 1.0 Where V = Average veloity of flow in m/s g = Aeleration due to gravity =9.81 m / s D = Hydrauli depth in meter Cross Setion Area of flow Top Width 9. Define hydrauli mean depth. A T D = Hydrauli depth in meter Cross Setion Area of flow Top Width A T 10.Define speifi energy. [Anna Univ.Nov 06&Nov 08] Speifi energy of a flowing liquid is defined as energy per unit weight of a liquid with respet to the bottom of the hannel. By a symbol E. Where V E y g E = Speifi Energy V = Veloity of flow y = Depth of flow IV Semester CE53 / Applied Hydrauli Engineering by P.Dhanabal AP / Civil Page 3

4 11. Define ritial flow. Depth of flow of water at whih the speifi energy. E is minimum is alled as ritial depth (y) For retangular hannel, ritial depth, 1.Define ritial veloity. h q g 1 3 Veloity of flow at the ritial depth is alled ritial veloity V V g* y Where y = Critial Depth g = Aeleration due to gravity 13.Distinguish between ritial, sub ritial and subritial flows. Critial flow: Depth of flow of water at whih the speifi energy is minimum is alled as ritial flow. Otherwise, flow orresponding to ritial depth is alled as ritial flow. For Critial Depth Froute Number F V gd 1.0 Where D Hydrauli Mean Depth Area of flow Top Width A T Sub ritial flow: When the depth of flow in a hannel is greater than the ritial depth y, the flow is alled as sub ritial flow. It is otherwise, alled as streaming flow or tranquil flow. For sub ritial flow, Froude number, F<1 IV Semester CE53 / Applied Hydrauli Engineering by P.Dhanabal AP / Civil Page 4

5 Sub ritial flow: When the depth of flow in a hannel is less than the ritial flow, y, the flow is alled as sub ritial flow or torrential flow. For superritial flow, Froude number, F>1 14. Differentiate prismati and non-prismati hannels. Prismati hannel Geometri dimensions of the hannel, suh as ross setion and bottom slope are onstant throughout the length of the hannel is alled as a prismati hannel. Eg. Most of the artifiial hannels of irular, retangular, trapezoidal and triangular ross setion are alled prismati hannels. Non- prismati hannel Geometri dimensions of the hannel, suh as ross setion and bottom slope are onstant for length of the hannel is alled as a non-prismati hannel. Eg. All natural hannels suh as river, are non-prismati hannels. 15. Explain speifi fore (F) [Anna Univ. Nov 08] Speifi fore is the sum of the pressure fore (F) and momentum fore due to flow (M) per unit weight of the liquid at a setion. Speifi Fore F Where s F M weight density of Liquid 16.What is speifi energy and what is ondition for obtaining only one depth for a given speifi energy? [Anna Univ. May 07] Total Energy on open hannel flow V E Z y g Considering the hannel bed as datum line, z 0 IV Semester CE53 / Applied Hydrauli Engineering by P.Dhanabal AP / Civil Page 5

6 Speifi Energy E V y g From Speifi Energy urve, Corresponding to the Minimum speifi energy E, there is only one depth of floe that is alled Critial depth (min) 17. Differentiate losed flow losed onduit flow and open hannel flow. [Anna Univ. May 07] S.No Closed onduit flow Open hannel flow 1. Water does not have with free surfae. Water flows with a free surfae.. Water does not ontat with atmosphere pressure but it has only hydrauli Water ontents with atmospheri pressure. pressure. 3. Flow may be due to either by pump pressure or by gravity flow Flow is obtained only by gravity. 18.Define sub ritial flow: If the Froude number is less than one then the flow is said to be sub ritial flow 19.Define ritial flow: If the Froude number is less equal to one it is alled as ritial flow. 0.Define superritial flow: If the Froude number is greater than one it is alled as super ritial flow 1. What are the possible types of flow in open hannel with respet to spae and time? A. steady and unsteady flow B. uniform and non-uniform flow IV Semester CE53 / Applied Hydrauli Engineering by P.Dhanabal AP / Civil Page 6

7 .what do you know about uniform and non uniform flow? Uniform flow: If the given length of the hannel,depth,veloity,the rate of flow, ross setion are onstant. Non Uniform flow: If the given length of the hannel,depth,veloity,the rate of flow, ross setion are not onstant. 3.Define speifi energy: It is defined as energy per unit weight of the liquid with respet to the bottom of the hannel. 4.Define ritial depth: It is defined as the depth of flow of water at whih the speifi energy is minimum. 5.Define ritial veloity: The veloity of flow at the ritial depth is known as ritial veloity. 6.Define gradually varying flow If the hange in depth in a varying flow is gradual so that the urvature of the streaming line is not exessive suh flow is alled gradually varying flow. 7.Define Rapidly varying flow If the urvature in a varied flow is large and depth hanges appreiably over short length it is alled rapidly varying flow. 8.What are the onditions of retangular hannel of best setion? The two onditions are breadth is equal to two times the depth (b=d) and hydrauli mean depth is equal to half the depth (m=d/) 9.What do you mean by open hannel flow? 1.Open hannel flow has a free surfae whih is subjeted to atmospheri pressure..in open hannel flow the ross setion is irregular. 30.List the instrument used to measure open hannel flow 1.pitot tube.ultrasoni flow instrument. 3.Dropper instrument 4.Gurley instrument. IV Semester CE53 / Applied Hydrauli Engineering by P.Dhanabal AP / Civil Page 7

8 31.What are the assumptions of gradually varying flow profile? 1.Pressure distribution at any setion is assumed to be hydrostati..the veloity distribution at the hannel setion is fixed 3.The hannel is prismati 4.The roughness oeffiient is independent of the depth of flow 3.What do you mean by speifi energy urve? It is defined as the urve whih shows the variation of speifi energy with respet to depth of flow. 33.Define open hannel flow? The term open hannel flow denotes the gravity-driven flow of a liquid with a free surfae. 34.What do you mean by stream lining? Streamlining is adding a faired tail setion to redue the extent of separated flow on the downstream portion of an objet. 35. What do you meant by Open hannel flow? Give few Examples. Open Channel Flow is defined as fluid flow with a free surfae open to the atmosphere. Examples inlude streams, rivers and ulverts not flowing full. Open hannel flow assumes that the pressure at the surfae is onstant and the hydrauli grade line is at the surfae of the fluid. 36. Define the term Critial depth Depth of flow at whih speifi energy is a minimum; depth in a onduit at whih maximum flow will our if the onduit is at ritial slope, the water is flowing at ritial veloity, and an adequate supply of water exists. 37. What is meant by Critial Slope The slope at whih maximum flow will our at minimum veloity; the slope equal to loss of head per foot resulting from flow at a depth giving uniform flow at ritial depth. 38. Define the term Hydrauli Gradient Pressure gradient, or a line representing pressure or piezometrihead in a pipe flowing full, or the water surfae in open hannel flow. IV Semester CE53 / Applied Hydrauli Engineering by P.Dhanabal AP / Civil Page 8

9 39. What is meant by Hydrauli jump A hydrauli jump is a phenomenon in the siene of hydraulis whih is frequently observed in open hannel flow suh as rivers and spillways. When liquid at high veloity disharges into a zone of lower veloity, a rather abrupt rise ours in the liquid surfae. The rapidly flowing liquid is abruptly slowed and inreases in height, onverting some of the flow's initial kineti energy into an inrease in potential energy, with some energy irreversibly lost through turbulene to heat. In an open hannel flow, this manifests as the fast flow rapidly slowing and piling up on top of itself similar to how a shokwave forms IV Semester CE53 / Applied Hydrauli Engineering by P.Dhanabal AP / Civil Page 9

10 16 MARK QUESTIONS AND ANSWERS 1.Calulate the Speifi energy,critial depth and the veloity of the flow of 10 m 3 in a ement lined retangular hannel.5m wide with m depth of water. Is the given flow is sub ritial or super ritial Given Data SOLUTION: To find Q = 10 m 3 /s b =.5 m y = m 1. Speifi Energy. Critial Depth 3. Veloity for the flow STEP 1: To find the Speifi Energy: V Q 10 E y V m / s g A.5* E *9.81 E 0.0 m E.0 m STEP : To find Critial Depth: y 1 3 q g Q b.5 q 4 m / s 1.18 m IV Semester CE53 / Applied Hydrauli Engineering by P.Dhanabal AP / Civil Page 10

11 STEP 3: Veloity of flow: V g * y 9.81* m/ s STEP 3: To find weather the flow is Sub ritial of Super ritial: F V g* D 9.81* Hene the flow is Sub-ritial. A Trapezoidal hannel has a bottom width of 6.1 m and side Slopes of H : 1 V.When the depth of the flow is 1.07 m. The flow is m 3 /s. What is the Speifi energy of flow? Is the Flow is sub ritial or super ritial Given Data SOLUTION: b = 6.1 m m = m Q = 1.07 m 3 /s To find 1. Speifi Energy. 3. Flow is tranquil or Rapid STEP 1: To find the Speifi Energy: A b my y 6.1* m IV Semester CE53 / Applied Hydrauli Engineering by P.Dhanabal AP / Civil Page 11

12 V Q A m/ s V E y g 1.19 E 1.07 * 9.81 E 1.14 m STEP 3: To find weather the flow is Sub ritial of Super ritial: V F g* D A D T A b my y 6.1 * m T b my 6.1 * * m D D 0.85 m Finally we an get F * F Hene the flow is Tranquil flow or Sub-Critial Flow IV Semester CE53 / Applied Hydrauli Engineering by P.Dhanabal AP / Civil Page 1

13 3. Calulate the Speifi Energy of 1 m 3 /s of water flowing with a veloity of 1.5 m 3 /s in a Retangular hannel 8 m wide. Find the depth of water in the hannel when the Speifi energy would be minimum. What would be the value of Critial as well minimum Speifi Energy Given Data SOLUTION: To find V = 1.5 m / s m = m b = 8 m 1. Speifi Energy. Critial veloity 3. minimum Speifi Energy STEP 1: To find the Speifi Energy: Q Q Q V * A A b* d V V note Q d V * b A b * d 1 b 1 m y 1.5 * 8 We Know that b y, Finally we Will Get V E y g * m Critial Depth (h ) is given by ( y ) IV Semester CE53 / Applied Hydrauli Engineering by P.Dhanabal AP / Civil Page 13

14 y or h q g 1 3 note Q b 1 8 q 1.5 m / s m 1 3 STEP : To find the Critial veloity V : V g * y 9.81* m/ s STEP 3: To find the minimum Speifi Energy: 3 E min y E min 3 * m 4. A 8 m wide Channel onveys 15 umes of water at a depth of 1. m. Determine the (1) Speifi energy of the flowing water () Critial depth, Critial veloity and minimum Speifi Energy (3) Froude number and the weather flow is sub-ritial or Super-ritial Given Data V = 1.5 m / s m = m b = 8 m IV Semester CE53 / Applied Hydrauli Engineering by P.Dhanabal AP / Civil Page 14

15 SOLUTION: To find (1) Speifi energy of the flowing water () Critial depth, Critial veloity and minimum Speifi Energy (3) Froude number and the weather flow is sub-ritial or Super-ritial STEP 1: To find the Speifi Energy: V Q A 15 8* m / s V E y g * m Step : To find Critial Depth Q b 15 8 q m / s y q g 1 3 y m IV Semester CE53 / Applied Hydrauli Engineering by P.Dhanabal AP / Civil Page 15

16 Step 3 :To find Critial Veloity V g * y 9.81* m/ s Step 4 :To Minimum Speifi Energy: 3 E min y E min 3 * m Step 5 :To find the Froude Number: F V gd V gy note D A b* y T b y * Hene the Flow is Sub-Critial IV Semester CE53 / Applied Hydrauli Engineering by P.Dhanabal AP / Civil Page 16

17 5. Find the ritial depth for a speifi energy of 1.5 m in: (1) Retangular hannel of bottom width m () Triangular hannel of side slope 1:1.5 Given Data E = 1.5 m SOLUTION: To find ritial depth for Retangular Trapezoidal and Triangular Channel Step 1 :Retangular Channel: E 3 y E * 3 y 1.5* 3 y y 1.0 m Step :Triangular Channel: E 5 y 4 E 4 * 5 y 1.5*4 5 y y 1.0 m IV Semester CE53 / Applied Hydrauli Engineering by P.Dhanabal AP / Civil Page 17

18 6. A Trapezoidal hannel with side slope of H:3V Has to arry 0 m 3 /s. Find the slope of the hannel when the bottom width of the hannel is 4 m and the depth of the water is 3 m.take manning s n=0.03 Given Data SOLUTION: b = 4 m y = 3 m m = m Q = 0 m 3 /s n = 0.03 To find Slope of the trapezoidal Channel A b my y 4 * 3 30 m P b my 4 * * 3 16 m A R P m Use manning s onstant Formulae C 1 N R 1 6 IV Semester CE53 / Applied Hydrauli Engineering by P.Dhanabal AP / Civil Page 18

19 1 1 (1.875) To find the Slope of the Channel Q AC RS 18* * S Take Square root onboth Sides * 1369 * * S * S S S This is the required Slope range for the given Trapezoidal Channel. IV Semester CE53 / Applied Hydrauli Engineering by P.Dhanabal AP / Civil Page 19

20 IV Semester CE53 / Applied Hydrauli Engineering by P.Dhanabal AP / Civil Page 0

21 IV Semester CE53 / Applied Hydrauli Engineering by P.Dhanabal AP / Civil Page 1

22 9. How do you lassify open hannels? Explain in detail. Also explain the veloity distribution in open hannel. (AUC Nov/De 010) IV Semester CE53 / Applied Hydrauli Engineering by P.Dhanabal AP / Civil Page

23 IV Semester CE53 / Applied Hydrauli Engineering by P.Dhanabal AP / Civil Page 3

24 IV Semester CE53 / Applied Hydrauli Engineering by P.Dhanabal AP / Civil Page 4

25 10.Write short notes on the following: (i) Critial flow and its omputations (ii) Channel Transition (AUC Nov/De 010) 1. Critial flow and its omputations i) Critial flow: Depth of flow of water at whih the speifi energy is minimum is alled as ritial flow. Otherwise, flow orresponding to ritial depth is alled as ritial flow. For Critial Depth Froute Number F V gd 1.0 Where D Hydrauli Mean Depth IV Semester CE53 / Applied Hydrauli Engineering by P.Dhanabal AP / Civil Page 5

26 ii)sub ritial flow: When the depth of flow in a hannel is greater than the ritial depth y, the flow is alled as sub ritial flow. It is otherwise, alled as streaming flow or tranquil flow. For sub ritial flow, Froude number, F<1 iii)sub ritial flow: When the depth of flow in a hannel is less than the ritial flow, y, the flow is alled as sub ritial flow or torrential flow. For superritial flow, Froude number, F>1.Channel Transition: IV Semester CE53 / Applied Hydrauli Engineering by P.Dhanabal AP / Civil Page 6

27 IV Semester CE53 / Applied Hydrauli Engineering by P.Dhanabal AP / Civil Page 7

28 IV Semester CE53 / Applied Hydrauli Engineering by P.Dhanabal AP / Civil Page 8

29 IV Semester CE53 / Applied Hydrauli Engineering by P.Dhanabal AP / Civil Page 9

30 11. Define speifi energy. How would you express the speifi energy for a wide retangular hannel with depth of flow D and veloity of flow V? Draw the typial speifi energy diagram and explain its features. It is defined as energy per unit weight of the liquid with respet to the bottom of the hannel. The extra information needed to solve the above problem an be provided by the speifi energy equation. Speifi energy, Es, is defined as the energy of the flow with referene to the hannel bed as the datum: Total Energy on open hannel flow V E Z y g Considering the hannel bed as datum line, z 0 Speifi Energy E V y g From Speifi Energy urve, Corresponding to the Minimum speifi energy E, there is only one depth of floe that is alled Critial depth (min) IV Semester CE53 / Applied Hydrauli Engineering by P.Dhanabal AP / Civil Page 30

31 IV Semester CE53 / Applied Hydrauli Engineering by P.Dhanabal AP / Civil Page 31

32 For steady flow this an be written in terms of disharge Q For a retangular hannel of width b, Q/A = q/y This is a ubi in y. It has three solutions but only two will be positive (so disard the other). IV Semester CE53 / Applied Hydrauli Engineering by P.Dhanabal AP / Civil Page 3

33 1. Define Froude number F R. Desribe the flow for F R =, F R < and F R >1. Represent a disharge versus depth urve for a onstant speifi energy and explain its features. Froude Number Froude number in onnetion with open surfae flow is defined as V/ gl. In the ase of open hannel flow, the harateristi length, l, is the depth y and V is the flow veloity. Hene Froude number an be represented by the ratio, Flow veloity/wave veloity. As already indiated, there are three possible flow situations namely (V/) < 1, (V/) = 1 and (V/) > 1 or the Froude number for the flow is less than or equal to or greater than 1. IV Semester CE53 / Applied Hydrauli Engineering by P.Dhanabal AP / Civil Page 33

34 Case (i) If Fr < 1, then V < and any disturbane an travel upstream. The downstream onditions an hange the flow onditions upstream. Suh a flow is alled subritial or tranquil flow. Only gradual hanges our in suh a situation. Case (ii) Fr = 1. The flow is alled ritial flow. Disturbanes annot travel upstream. A standing wave may generally result. Case (iii) Fr > 1, suh flows are alled superritial or rapid or shooting flows. Disturbanes annot travel upstream. Downstream onditions annot be felt upstream. Changes our only in the downstream flow. These are similar to subsoni, soni and supersoni flows in the ase of flow of ompressible fluids where Math number is the governing fator also defined as V/, where is the soni speed or veloity of propagation of small disturbane in the fluid. 13.How are the flows lassified under speifi energy onepts? It is defined as energy per unit weight of the liquid with respet to the bottom of the hannel. The extra information needed to solve the above problem an be provided by the speifi energy equation. Speifi energy, Es, is defined as the energy of the flow with referene to the hannel bed as the datum: Total Energy on open hannel flow V E Z y g Considering the hannel bed as datum line, z 0 Speifi Energy E V y g From Speifi Energy urve, Corresponding to the Minimum speifi energy E, there is only one depth of floe that is alled Critial depth (min) IV Semester CE53 / Applied Hydrauli Engineering by P.Dhanabal AP / Civil Page 34

35 ***ALL THE BEST*** IV Semester CE53 / Applied Hydrauli Engineering by P.Dhanabal AP / Civil Page 35

36 1.0. QUESTION BANK PART A 1. Differentiate open hannel flow from pipe flow.. What is speifi energy and is the ondition for getting only one depth for a given speifi energy? 3. How will do you distinguish between ritial, sub- ritial, super- ritial flow. 4. Sketh the veloity distribution in a trapezoidal hannel. 5. What is the use of a pitot tube? 6. Briefly write a note on anemometers 7. Find the relationship between Chezy's C and Manning's n. 8. Sketh the veloity distribution in retangular and triangular hannels. 9. What are the possible types of flow in open hannel with respet to spae and time? 10. What are the equations for ritial depth for retangular hannel? 11. Distinguish between steady uniform flow and unsteady non uniform flow. 1. Define speifi energy. IV Semester CE53 / Applied Hydrauli Engineering by P.Dhanabal AP / Civil Page 36

37 PART B 1. Explain any two formulae for estimation of veloity in open hannels?. A trapezoidal hannel has side slopes of 1 horizontal to vertial and the slope of the bed is 1 in 000. The area of the setion is 4 m. Find the dimensions of the setion if it is to be most eonomial. Determine the disharge of the most eonomial setion of C = Desribe various types of flow in an open hannel. 4. A retangular hannel with a base width of 0.60 m arries a disharge of 100 lps. The Chezy's C is 60. If the depth of flow is 0.5 m, determine the bed slope of the hannel 5. In a flow through a retangular hannel for a ertain disharge froude number orresponding the two alternate depths are y1 and y. show that (F /F 1 ) (3/) =(+F )/(+F1 ) 6. A retangular hannel 1.5m wide and depth.5m, disharge is 10m3/se. alulate the speifi energy and depth alternate to the given depth. 7. A trapezoidal hannel has a bottom width 6m, and side slope of h to 1v if a depth of flow is 1.m at a disharge of 10m3/se. ompute the speifi energy and ritial depth. 8. Define wide open hannel and also what are the important assumptions in hydrauli parameters? 9. The retangular hannel arries a disharge of 30m3/se. The bottom width of the hannel is 6.0m and flow veloity is 1.75m/se. Determine two alternate depths possible in the hannel. 10. If y 1 and y are alternate depths in a retangular hannel show thaty C 3 = (y 1 y ) / (y1 + y ) And hene the speifi energy E = (y 1 + y1 y + y ) / (y1 + y ) 11. For a onstant speifi energy of 3.0m, what maximum flow may our in a retangular hannel of 4.5m bed width? 1. The speifi energy for a 3m wide hannel is 8N.m/N. What is the maximum possible disharge in the hannel? IV Semester CE53 / Applied Hydrauli Engineering by P.Dhanabal AP / Civil Page 37

38 13. Show that in a retangular hannel maximum disharges ours when the flow is ritial for a given value of speifi energy. 14. The speifi energy for a 5m wide retangular hannel is 4m, the disharge of water through the hannel is 19umes. Determine the alternate depths of flow. 15. Show that the minimum speifi energy in a retangular hannel is 1.5 times the ritial depth. 16. Show that the relation between alternate depths y1 and y in a retangular hannel an be 3 expressed by y 1 y /(y1 +y )=y where y is the ritial depth of flow. 17. For a onstant energy of.4n.m/n. Calulate the maximum disharge that may our in a retangular hannel 4m wide. 18. For a purpose of disharge measurement the width of a retangular hannel is redued gradually from 3m tom and floor is raised by 0.3m at a given setion when the approahing depth of flow is m, what rate flow will be indiated by a drop of 0.15m in the water surfae elevation at the ontrated setion? 19. How to estimate the hydrauli jump and draw sketh of the jump? IV Semester CE53 / Applied Hydrauli Engineering by P.Dhanabal AP / Civil Page 38

2. The Energy Principle in Open Channel Flows

2. The Energy Principle in Open Channel Flows . The Energy Priniple in Open Channel Flows. Basi Energy Equation In the one-dimensional analysis of steady open-hannel flow, the energy equation in the form of Bernoulli equation is used. Aording to this

More information

10.2 The Occurrence of Critical Flow; Controls

10.2 The Occurrence of Critical Flow; Controls 10. The Ourrene of Critial Flow; Controls In addition to the type of problem in whih both q and E are initially presribed; there is a problem whih is of pratial interest: Given a value of q, what fators

More information

Energy Concept g. y 1

Energy Concept g. y 1 nerg Conept Components of the energ euation z is the elevation head is the pressure head-potential head V /g is the dnami head-kineti head H z + + V g V g S f x V g GL HGL S o x x SPCIFIC NRGY CONCPT Speifi

More information

What are the locations of excess energy in open channels?

What are the locations of excess energy in open channels? Leture 26 Energy Dissipation Strutures I. Introdution Exess energy should usually be dissipated in suh a way as to avoid erosion in unlined open hannels In this ontext, exess energy means exess water veloity

More information

CHAPTER 10 Flow in Open Channels

CHAPTER 10 Flow in Open Channels CHAPTER 10 Flow in Open Channels Chapter 10 / Flow in Open Channels Introdution 1 α os (1 0.) 1.159 rad or 66.4 10. QB Qdsinα ga g d /4( α sinα os α) 4 sin(1.159) 1 5 9.81 ( d / 64) 1.159 sin1.159os1.159)

More information

Minimum Specific Energy and Critical Flow Conditions in Open Channels

Minimum Specific Energy and Critical Flow Conditions in Open Channels Minimum Speifi Energy and Critial Flow Conditions in Open Channels H. Chanson Abstrat: In open hannels, the relationship between the speifi energy and the flow depth exhibits a minimum, and the orresponding

More information

Determination the Invert Level of a Stilling Basin to Control Hydraulic Jump

Determination the Invert Level of a Stilling Basin to Control Hydraulic Jump Global Avane Researh Journal of Agriultural Siene Vol. (4) pp. 074-079, June, 0 Available online http://garj.org/garjas/inex.htm Copyright 0 Global Avane Researh Journals Full Length Researh Paper Determination

More information

Uniform Flow in Open Channels

Uniform Flow in Open Channels 1 UNIT 2 Uniform Flow in Open Channels Lecture-01 Introduction & Definition Open-channel flow, a branch of hydraulics, is a type of liquid flow within a conduit with a free surface, known as a channel.

More information

Closed duct flows are full of fluid, have no free surface within, and are driven by a pressure gradient along the duct axis.

Closed duct flows are full of fluid, have no free surface within, and are driven by a pressure gradient along the duct axis. OPEN CHANNEL FLOW Open channel flow is a flow of liquid, basically water in a conduit with a free surface. The open channel flows are driven by gravity alone, and the pressure gradient at the atmospheric

More information

1 Branch: CIVIL ENGINEERING Sub: HYDRAULICS AND HYDRAULIC MACHINERY Date: 11/03/2017

1 Branch: CIVIL ENGINEERING Sub: HYDRAULICS AND HYDRAULIC MACHINERY Date: 11/03/2017 G.PULLAIAH COLLEGE OF ENGINEERING & TECHNOLOGY (AT) II B.Tech Objective Paper I MID EXAM 1 Branch: CIVIL ENGINEERING Sub: HYDRAULICS AND HYDRAULIC MACHINERY Date: 11/03/2017 Time: 20 min Max.Marks:10 Roll

More information

Part G-4: Sample Exams

Part G-4: Sample Exams Part G-4: Sample Exams 1 Cairo University M.S.: Eletronis Cooling Faulty of Engineering Final Exam (Sample 1) Mehanial Power Engineering Dept. Time allowed 2 Hours Solve as muh as you an. 1. A heat sink

More information

SOME FUNDAMENTAL ASPECTS OF COMPRESSIBLE FLOW

SOME FUNDAMENTAL ASPECTS OF COMPRESSIBLE FLOW SOE FUNDAENAL ASECS OF CORESSIBLE FLOW ah number gas veloity mah number, speed of sound a a R < : subsoni : transoni > : supersoni >> : hypersoni art three : ah Number 7 Isentropi flow in a streamtube

More information

Closed duct flows are full of fluid, have no free surface within, and are driven by a pressure gradient along the duct axis.

Closed duct flows are full of fluid, have no free surface within, and are driven by a pressure gradient along the duct axis. OPEN CHANNEL FLOW Open channel flow is a flow of liquid, basically water in a conduit with a free surface. The open channel flows are driven by gravity alone, and the pressure gradient at the atmospheric

More information

Presented by: Civil Engineering Academy

Presented by: Civil Engineering Academy Presented by: Civil Engineering Academy Open-Channel Flow Uniform Flow (See CERM Ch. 19) Characterized by constant depth volume, and cross section. It can be steady or unsteady Non-uniform Flow *Not on

More information

NPTEL Quiz Hydraulics

NPTEL Quiz Hydraulics Introduction NPTEL Quiz Hydraulics 1. An ideal fluid is a. One which obeys Newton s law of viscosity b. Frictionless and incompressible c. Very viscous d. Frictionless and compressible 2. The unit of kinematic

More information

STEADY UNIFORM FLOW IN OPEN CHANNEL

STEADY UNIFORM FLOW IN OPEN CHANNEL 11/4/018 School of Environmental Engineering STEY UNIFORM FLOW IN OEN CHNNEL ZULKRNIN BIN HSSN COURSE OUTCOMES CO1: ble to analyze and design the steady flow in pipeline (O1) CO: ble to analyze and design

More information

Heat exchangers: Heat exchanger types:

Heat exchangers: Heat exchanger types: Heat exhangers: he proess of heat exhange between two fluids that are at different temperatures and separated by a solid wall ours in many engineering appliations. he devie used to implement this exhange

More information

Lecture Note for Open Channel Hydraulics

Lecture Note for Open Channel Hydraulics Chapter -one Introduction to Open Channel Hydraulics 1.1 Definitions Simply stated, Open channel flow is a flow of liquid in a conduit with free space. Open channel flow is particularly applied to understand

More information

13.Prandtl-Meyer Expansion Flow

13.Prandtl-Meyer Expansion Flow 3.Prandtl-eyer Expansion Flow This hapter will treat flow over a expansive orner, i.e., one that turns the flow outward. But before we onsider expansion flow, we will return to onsider the details of the

More information

Experiment 7 Energy Loss in a Hydraulic Jump

Experiment 7 Energy Loss in a Hydraulic Jump Experiment 7 Energ Loss in a Hdraulic Jump n Purpose: The purpose of this experiment is to examine the transition from supercritical (rapid) flow to subcritical (slow) flow in an open channel and to analze

More information

Architecture and facies distribution of organic-clastic lake fills in the fluvio-deltaic Rhine-Meuse system, The Netherlands Ingwer J.

Architecture and facies distribution of organic-clastic lake fills in the fluvio-deltaic Rhine-Meuse system, The Netherlands Ingwer J. Arhiteture and faies distribution of organi-lasti lake fills in the fluvio-deltai Rhine-Meuse system, The Netherlands Ingwer J.Bos Supplement 1. Duration and harateristis of fluvial regime disharge and

More information

Chapter 4: Non uniform flow in open channels

Chapter 4: Non uniform flow in open channels Chapter 4: Non uniform flow in open channels Learning outcomes By the end of this lesson, students should be able to: Relate the concept of specific energy and momentum equations in the effect of change

More information

EXPERIMENTAL STUDY ON BOTTOM BOUNDARY LAYER BENEATH SOLITARY WAVE

EXPERIMENTAL STUDY ON BOTTOM BOUNDARY LAYER BENEATH SOLITARY WAVE VOL. 11, NO. 8, APRIL 16 ISSN 1819-668 6-16 Asian Researh Publishing Network (ARPN). All rights reserved. EXPERIMENTAL STUDY ON BOTTOM BOUNDARY LAYER BENEATH SOLITARY WAVE Bambang Winarta 1, Nadiatul Adilah

More information

We will assume straight channels with simple geometries (prismatic channels) and steady state flow (in time).

We will assume straight channels with simple geometries (prismatic channels) and steady state flow (in time). 56 Review Drag & Lift Laminar vs Turbulent Boundary Layer Turbulent boundary layers stay attached to bodies longer Narrower wake! Lower pressure drag! 8. Open-Channel Flow Pipe/duct flow closed, full,

More information

Chapter 3 Lecture 7. Drag polar 2. Topics. Chapter-3

Chapter 3 Lecture 7. Drag polar 2. Topics. Chapter-3 hapter 3 eture 7 Drag polar Topis 3..3 Summary of lift oeffiient, drag oeffiient, pithing moment oeffiient, entre of pressure and aerodynami entre of an airfoil 3..4 Examples of pressure oeffiient distributions

More information

COMPUTER METHODS FOR THE DETERMINATION OF THE CRITICAL PARAMETERS OF POLLUTED INSULATORS

COMPUTER METHODS FOR THE DETERMINATION OF THE CRITICAL PARAMETERS OF POLLUTED INSULATORS COMPUTER METHODS FOR THE DETERMINATION OF THE CRITICAL PARAMETERS OF POLLUTED INSULATORS I. F. GONOS S. A. SUFLIS F. V. TOPALIS I.A. STATHOPULOS NATIONAL TECHNICAL UNIVERSITY OF ATHENS DEPARTMENT OF ELECTRICAL

More information

Where as discussed previously we interpret solutions to this partial differential equation in the weak sense: b

Where as discussed previously we interpret solutions to this partial differential equation in the weak sense: b Consider the pure initial value problem for a homogeneous system of onservation laws with no soure terms in one spae dimension: Where as disussed previously we interpret solutions to this partial differential

More information

Wood Design. = theoretical allowed buckling stress

Wood Design. = theoretical allowed buckling stress Wood Design Notation: a = name for width dimension A = name for area A req d-adj = area required at allowable stress when shear is adjusted to inlude self weight b = width of a retangle = name for height

More information

Natural Convection Experiment Measurements from a Vertical Surface

Natural Convection Experiment Measurements from a Vertical Surface OBJECTIVE Natural Convetion Experiment Measurements from a Vertial Surfae 1. To demonstrate te basi priniples of natural onvetion eat transfer inluding determination of te onvetive eat transfer oeffiient.

More information

Chapter 2 Lecture 8 Longitudinal stick fixed static stability and control 5 Topics

Chapter 2 Lecture 8 Longitudinal stick fixed static stability and control 5 Topics Flight dynamis II Stability and ontrol hapter 2 Leture 8 Longitudinal stik fied stati stability and ontrol 5 Topis 2.6 ontributions of power plant to mg and mα 2.6.1 Diret ontributions of powerplant to

More information

Open Channel Flow Part 2. Ch 10 Young, notes, handouts

Open Channel Flow Part 2. Ch 10 Young, notes, handouts Open Channel Flow Part 2 Ch 10 Young, notes, handouts Uniform Channel Flow Many situations have a good approximation d(v,y,q)/dx=0 Uniform flow Look at extended Bernoulli equation Friction slope exactly

More information

Lecture 11 Buckling of Plates and Sections

Lecture 11 Buckling of Plates and Sections Leture Bukling of lates and Setions rolem -: A simpl-supported retangular plate is sujeted to a uniaxial ompressive load N, as shown in the sketh elow. a 6 N N a) Calulate and ompare ukling oeffiients

More information

Process engineers are often faced with the task of

Process engineers are often faced with the task of Fluids and Solids Handling Eliminate Iteration from Flow Problems John D. Barry Middough, In. This artile introdues a novel approah to solving flow and pipe-sizing problems based on two new dimensionless

More information

Homework Set 4. gas B open end

Homework Set 4. gas B open end Homework Set 4 (1). A steady-state Arnold ell is used to determine the diffusivity of toluene (speies A) in air (speies B) at 298 K and 1 atm. If the diffusivity is DAB = 0.0844 m 2 /s = 8.44 x 10-6 m

More information

Wave Propagation through Random Media

Wave Propagation through Random Media Chapter 3. Wave Propagation through Random Media 3. Charateristis of Wave Behavior Sound propagation through random media is the entral part of this investigation. This hapter presents a frame of referene

More information

Hydraulics Part: Open Channel Flow

Hydraulics Part: Open Channel Flow Hydraulics Part: Open Channel Flow Tutorial solutions -by Dr. K.N. Dulal Uniform flow 1. Show that discharge through a channel with steady flow is given by where A 1 and A 2 are the sectional areas of

More information

Fluid Mechanics Prof. S.K. Som Department of Mechanical Engineering Indian Institute of Technology, Kharagpur

Fluid Mechanics Prof. S.K. Som Department of Mechanical Engineering Indian Institute of Technology, Kharagpur Fluid Mechanics Prof. S.K. Som Department of Mechanical Engineering Indian Institute of Technology, Kharagpur Lecture - 42 Flows with a Free Surface Part II Good morning. I welcome you to this session

More information

Fiber Optic Cable Transmission Losses with Perturbation Effects

Fiber Optic Cable Transmission Losses with Perturbation Effects Fiber Opti Cable Transmission Losses with Perturbation Effets Kampanat Namngam 1*, Preeha Yupapin 2 and Pakkinee Chitsakul 1 1 Department of Mathematis and Computer Siene, Faulty of Siene, King Mongkut

More information

Open Channel Flow - General. Hydromechanics VVR090

Open Channel Flow - General. Hydromechanics VVR090 Open Channel Flow - General Hydromechanics VVR090 ppt by Magnus Larson; revised by Rolf L Jan 2014, Feb 2015 SYNOPSIS 1. Introduction and Applications 2. The History of Open Channel Flow 3. Flow Classification

More information

Open Channel Flow I - The Manning Equation and Uniform Flow COURSE CONTENT

Open Channel Flow I - The Manning Equation and Uniform Flow COURSE CONTENT Open Channel Flow I - The Manning Equation and Uniform Flow Harlan H. Bengtson, PhD, P.E. COURSE CONTENT 1. Introduction Flow of a liquid may take place either as open channel flow or pressure flow. Pressure

More information

Beams on Elastic Foundation

Beams on Elastic Foundation Professor Terje Haukaas University of British Columbia, Vanouver www.inrisk.ub.a Beams on Elasti Foundation Beams on elasti foundation, suh as that in Figure 1, appear in building foundations, floating

More information

1. Open Channel Hydraulics

1. Open Channel Hydraulics Open Channel Flow. Open Channel Hydraulics.... Definition and differences between pipe flow and open channel flow.... Types of flow.... Properties of open channels...4.4 Fundamental equations... 5.4. The

More information

Duct Acoustics. Chap.4 Duct Acoustics. Plane wave

Duct Acoustics. Chap.4 Duct Acoustics. Plane wave Chap.4 Dut Aoustis Dut Aoustis Plane wave A sound propagation in pipes with different ross-setional area f the wavelength of sound is large in omparison with the diameter of the pipe the sound propagates

More information

( ) ( ) Volumetric Properties of Pure Fluids, part 4. The generic cubic equation of state:

( ) ( ) Volumetric Properties of Pure Fluids, part 4. The generic cubic equation of state: CE304, Spring 2004 Leture 6 Volumetri roperties of ure Fluids, part 4 The generi ubi equation of state: There are many possible equations of state (and many have been proposed) that have the same general

More information

Name... Class... Date...

Name... Class... Date... Energy transfers Speifiation referenes: Maths skills 1a, 1b, 2a, 2h, 3a, 3b, 3, 3d Aims In this worksheet you will learn how to alulate kineti energy, gravitational, and elasti potential energy. You will

More information

A NORMALIZED EQUATION OF AXIALLY LOADED PILES IN ELASTO-PLASTIC SOIL

A NORMALIZED EQUATION OF AXIALLY LOADED PILES IN ELASTO-PLASTIC SOIL Journal of Geongineering, Vol. Yi-Chuan 4, No. 1, Chou pp. 1-7, and April Yun-Mei 009 Hsiung: A Normalized quation of Axially Loaded Piles in lasto-plasti Soil 1 A NORMALIZD QUATION OF AXIALLY LOADD PILS

More information

presented by Umut Türker Open Channel Flow

presented by Umut Türker Open Channel Flow presented by Umut Türker Open Channel Flow What is open channel flow? Open channel flow is a flow which has a free surface and flows due to the gravitational effect What is open channel flow? Open channel

More information

LECTURE 9: Open channel flow: Uniform flow, best hydraulic sections, energy principles, Froude number

LECTURE 9: Open channel flow: Uniform flow, best hydraulic sections, energy principles, Froude number LECTURE 9: Open channel flow: Uniform flow, best hydraulic sections, energy principles, Froude number Assist. Prof. Neslihan SEMERCİ Marmara University Department of Environmental Engineering Open channel

More information

Open Channel Flow - General. Open Channel Flow

Open Channel Flow - General. Open Channel Flow Open Channel Flow - General Hydromechanics VVR090 Open Channel Flow Open channel: a conduit for flow which has a free surface Free surface: interface between two fluids of different density Characteristics

More information

OPEN CHANNEL FLOW. One-dimensional - neglect vertical and lateral variations in velocity. In other words, Q v = (1) A. Figure 1. One-dimensional Flow

OPEN CHANNEL FLOW. One-dimensional - neglect vertical and lateral variations in velocity. In other words, Q v = (1) A. Figure 1. One-dimensional Flow OPEN CHANNEL FLOW Page 1 OPEN CHANNEL FLOW Open Channel Flow (OCF) is flow with one boundary exposed to atmospheric pressure. The flow is not pressurized and occurs because of gravity. Flow Classification

More information

gradp -the fluid is inviscid -the fluid is barotropic -the mass forces form a potential field

gradp -the fluid is inviscid -the fluid is barotropic -the mass forces form a potential field J. Szantyr Leture No. 5 Bernoulli equation Bernoulli equation exresses, under ertain assumtions, the riniles of momentum onservation and energy onservation of the fluid. Assumtions: -the flow is stationary

More information

Stability Analysis of Orbital Motions around Uniformly Rotating Irregular Asteroids

Stability Analysis of Orbital Motions around Uniformly Rotating Irregular Asteroids Stability Analysis of Orbital Motions around Uniformly Rotating Irregular Asteroids By Xiyun HoU, ) Daniel J. SCHEERES, ) Xiaosheng XIN, ) Jinglang FENG, ) Jingshi TANG, ) Lin LIU, ) ) Shool of Astronomy

More information

UNIVERSAL RELATIONSHIP BETWEEN COLLECTION EFFICIENCY AND THE CORONA POWER OF THE ELECTROSTATIC PRECIPITATOR

UNIVERSAL RELATIONSHIP BETWEEN COLLECTION EFFICIENCY AND THE CORONA POWER OF THE ELECTROSTATIC PRECIPITATOR Australia 006 Paper 5B UNIVERSAL RELATIONSHIP BETWEEN COLLECTION EFFICIENCY AND THE CORONA POWER OF THE ELECTROSTATIC PRECIPITATOR YAKOV S. KHODORKOVSKY & MICHAEL R. BELTRAN Beltran, In., U.S.A. ABSTRACT

More information

Physical Laws, Absolutes, Relative Absolutes and Relativistic Time Phenomena

Physical Laws, Absolutes, Relative Absolutes and Relativistic Time Phenomena Page 1 of 10 Physial Laws, Absolutes, Relative Absolutes and Relativisti Time Phenomena Antonio Ruggeri modexp@iafria.om Sine in the field of knowledge we deal with absolutes, there are absolute laws that

More information

Stress triaxiality to evaluate the effective distance in the volumetric approach in fracture mechanics

Stress triaxiality to evaluate the effective distance in the volumetric approach in fracture mechanics IOSR Journal of ehanial and Civil Engineering (IOSR-JCE) e-issn: 78-1684,p-ISSN: 30-334X, Volume 11, Issue 6 Ver. IV (Nov- De. 014), PP 1-6 Stress triaxiality to evaluate the effetive distane in the volumetri

More information

Review for Exam #2. Specific Heat, Thermal Conductivity, and Thermal Diffusivity. Conduction

Review for Exam #2. Specific Heat, Thermal Conductivity, and Thermal Diffusivity. Conduction Review for Exam # Speifi Heat, Thermal Condutivity, and Thermal Diffusivity Speifi heat ( p ) A measure of how muh energy is required to raise the temperature of an objet Thermal ondutivity (k) A measure

More information

2. Mass transfer takes place in the two contacting phases as in extraction and absorption.

2. Mass transfer takes place in the two contacting phases as in extraction and absorption. PRT 11- CONVECTIVE MSS TRNSFER 2.1 Introdution 2.2 Convetive Mass Transfer oeffiient 2.3 Signifiant parameters in onvetive mass transfer 2.4 The appliation of dimensional analysis to Mass Transfer 2.4.1

More information

Heat propagation and stability in a small high T superconductor. coil

Heat propagation and stability in a small high T superconductor. coil Ž. Physia C 310 1998 372 376 Heat propagation and stability in a small high T superondutor oil T. Kiss a,), V.S. Vysotsky a, H. Yuge a, H. Saho a, Yu.A. Ilyin a, M. Takeo a, K. Watanabe b, F. Irie a Graduate

More information

UTC. Engineering 329. Proportional Controller Design. Speed System. John Beverly. Green Team. John Beverly Keith Skiles John Barker.

UTC. Engineering 329. Proportional Controller Design. Speed System. John Beverly. Green Team. John Beverly Keith Skiles John Barker. UTC Engineering 329 Proportional Controller Design for Speed System By John Beverly Green Team John Beverly Keith Skiles John Barker 24 Mar 2006 Introdution This experiment is intended test the variable

More information

Buckling loads of columns of regular polygon cross-section with constant volume and clamped ends

Buckling loads of columns of regular polygon cross-section with constant volume and clamped ends 76 Bukling loads of olumns of regular polygon ross-setion with onstant volume and lamped ends Byoung Koo Lee Dept. of Civil Engineering, Wonkwang University, Iksan, Junuk, 7-79, Korea Email: kleest@wonkwang.a.kr

More information

CHAPTER 26 The Special Theory of Relativity

CHAPTER 26 The Special Theory of Relativity CHAPTER 6 The Speial Theory of Relativity Units Galilean-Newtonian Relativity Postulates of the Speial Theory of Relativity Simultaneity Time Dilation and the Twin Paradox Length Contration Four-Dimensional

More information

THE REFRACTION OF LIGHT IN STATIONARY AND MOVING REFRACTIVE MEDIA

THE REFRACTION OF LIGHT IN STATIONARY AND MOVING REFRACTIVE MEDIA HDRONIC JOURNL 24, 113-129 (2001) THE REFRCTION OF LIGHT IN STTIONRY ND MOVING REFRCTIVE MEDI C. K. Thornhill 39 Crofton Road Orpington, Kent, BR6 8E United Kingdom Reeived Deember 10, 2000 Revised: Marh

More information

Four-dimensional equation of motion for viscous compressible substance with regard to the acceleration field, pressure field and dissipation field

Four-dimensional equation of motion for viscous compressible substance with regard to the acceleration field, pressure field and dissipation field Four-dimensional equation of motion for visous ompressible substane with regard to the aeleration field, pressure field and dissipation field Sergey G. Fedosin PO box 6488, Sviazeva str. -79, Perm, Russia

More information

Name Solutions to Test 1 September 23, 2016

Name Solutions to Test 1 September 23, 2016 Name Solutions to Test 1 September 3, 016 This test onsists of three parts. Please note that in parts II and III, you an skip one question of those offered. Possibly useful formulas: F qequb x xvt E Evpx

More information

THE SPANN VIBROACOUSTIC METHOD Revision A

THE SPANN VIBROACOUSTIC METHOD Revision A THE SPNN VIBROCOUSTIC METHOD Revision By Tom Irvine Deember 15, 01 Email: tom@vibrationdata.om Figure 1. vionis Installation and Testing Introdution vionis omponents in airraft and launh vehiles may be

More information

Advanced Hydraulics Prof. Dr. Suresh A. Kartha Department of Civil Engineering Indian Institute of Technology, Guwahati

Advanced Hydraulics Prof. Dr. Suresh A. Kartha Department of Civil Engineering Indian Institute of Technology, Guwahati Advanced Hydraulics Prof. Dr. Suresh A. Kartha Department of Civil Engineering Indian Institute of Technology, Guwahati Module - 5 Channel Transitions Lecture - 1 Channel Transitions Part 1 Welcome back

More information

STUDY OF INHERENT FREQUENCY OF HELMHOLTZ RESONATOR

STUDY OF INHERENT FREQUENCY OF HELMHOLTZ RESONATOR 005 WJTA Amerian Waterjet Conferene August -3, 005! Houston, Texas Paper 6B-4 STUDY OF INHERENT FREQUENCY OF HELMHOLT RESONATOR Gong Weili An Liqian Cui Longlian Xie Guixin Shool of Mehanis, Arhiteture

More information

Experiment 03: Work and Energy

Experiment 03: Work and Energy MASSACHUSETTS INSTITUTE OF TECHNOLOGY Physis Department Physis 8.01 Purpose of the Experiment: Experiment 03: Work and Energy In this experiment you allow a art to roll down an inlined ramp and run into

More information

SCHOOL OF MECHANICAL, AEROSPACE AND CIVIL ENGINEERING HYDRAULICS 2 LABORATORY EXERCISE. Forces on Two-Dimensional Bodies in a Wind Tunnel

SCHOOL OF MECHANICAL, AEROSPACE AND CIVIL ENGINEERING HYDRAULICS 2 LABORATORY EXERCISE. Forces on Two-Dimensional Bodies in a Wind Tunnel Objet SCHOOL OF MECHANICAL, AEROSPACE AND CIVIL ENGINEERING HYDRAULICS LABORATORY EXERCISE Fores on Two-Dimensional Bodies in a Wind Tnnel To ompare drag oeffiients made by diret measrement on a drag balane

More information

28.2 Classification of Jumps

28.2 Classification of Jumps 28.2 Classification of Jumps As mentioned earlier, the supercritical flow Froude number influences the characteristics of the hydraulic jump. Bradley and Peterka, after extensive experimental investigations,

More information

Topic 3 Specific Energy and Control Section

Topic 3 Specific Energy and Control Section Tpi Speifi nerg and Cntrl Setin Prepared b: Tan Lai Wai et al. laiwai@uth.edu. Learning Outes At the end f this tpi, students shuld be able t: i. Appl speifi energ nept in deterining ritial flw nditins

More information

V/ t = 0 p/ t = 0 ρ/ t = 0. V/ s = 0 p/ s = 0 ρ/ s = 0

V/ t = 0 p/ t = 0 ρ/ t = 0. V/ s = 0 p/ s = 0 ρ/ s = 0 UNIT III FLOW THROUGH PIPES 1. List the types of fluid flow. Steady and unsteady flow Uniform and non-uniform flow Laminar and Turbulent flow Compressible and incompressible flow Rotational and ir-rotational

More information

3 Tidal systems modelling: ASMITA model

3 Tidal systems modelling: ASMITA model 3 Tidal systems modelling: ASMITA model 3.1 Introdution For many pratial appliations, simulation and predition of oastal behaviour (morphologial development of shorefae, beahes and dunes) at a ertain level

More information

Millennium Relativity Acceleration Composition. The Relativistic Relationship between Acceleration and Uniform Motion

Millennium Relativity Acceleration Composition. The Relativistic Relationship between Acceleration and Uniform Motion Millennium Relativity Aeleration Composition he Relativisti Relationship between Aeleration and niform Motion Copyright 003 Joseph A. Rybzyk Abstrat he relativisti priniples developed throughout the six

More information

RESEARCH ON RANDOM FOURIER WAVE-NUMBER SPECTRUM OF FLUCTUATING WIND SPEED

RESEARCH ON RANDOM FOURIER WAVE-NUMBER SPECTRUM OF FLUCTUATING WIND SPEED The Seventh Asia-Paifi Conferene on Wind Engineering, November 8-1, 9, Taipei, Taiwan RESEARCH ON RANDOM FORIER WAVE-NMBER SPECTRM OF FLCTATING WIND SPEED Qi Yan 1, Jie Li 1 Ph D. andidate, Department

More information

Ph1c Analytic Quiz 2 Solution

Ph1c Analytic Quiz 2 Solution Ph1 Analyti Quiz 2 olution Chefung Chan, pring 2007 Problem 1 (6 points total) A small loop of width w and height h falls with veloity v, under the influene of gravity, into a uniform magneti field B between

More information

EXPERIMENTAL STUDY OF THE ENERGY DISSIPATION IN THE STEPPED CHANNELS: COMPARISON WITH THE EMPIRICAL MODEL

EXPERIMENTAL STUDY OF THE ENERGY DISSIPATION IN THE STEPPED CHANNELS: COMPARISON WITH THE EMPIRICAL MODEL EXPERIMENTAL STUDY OF TE ENERGY DISSIPATION IN TE STEPPED CANNELS: COMPARISON WIT TE EMPIRICAL MODEL Nouis Messaad a, Djaid Naima a, Gafsi Mostefa a, Boutassouna Kheira a, Gahmani Ahmed a, and Kaouahi

More information

Acoustic Waves in a Duct

Acoustic Waves in a Duct Aousti Waves in a Dut 1 One-Dimensional Waves The one-dimensional wave approximation is valid when the wavelength λ is muh larger than the diameter of the dut D, λ D. The aousti pressure disturbane p is

More information

Open Channel Hydraulics I - Uniform Flow

Open Channel Hydraulics I - Uniform Flow PDHonline Course H138 (2 PDH) Open Channel Hydraulics I - Uniform Flow Instructor: Harlan H. Bengtson, Ph.D., PE 2012 PDH Online PDH Center 5272 Meadow Estates Drive Fairfax, VA 22030-6658 Phone & Fax:

More information

VARIED FLOW IN OPEN CHANNELS

VARIED FLOW IN OPEN CHANNELS Chapter 15 Open Channels vs. Closed Conduits VARIED FLOW IN OPEN CHANNELS Fluid Mechanics, Spring Term 2011 In a closed conduit there can be a pressure gradient that drives the flow. An open channel has

More information

Collinear Equilibrium Points in the Relativistic R3BP when the Bigger Primary is a Triaxial Rigid Body Nakone Bello 1,a and Aminu Abubakar Hussain 2,b

Collinear Equilibrium Points in the Relativistic R3BP when the Bigger Primary is a Triaxial Rigid Body Nakone Bello 1,a and Aminu Abubakar Hussain 2,b International Frontier Siene Letters Submitted: 6-- ISSN: 9-8, Vol., pp -6 Aepted: -- doi:.8/www.sipress.om/ifsl.. Online: --8 SiPress Ltd., Switzerland Collinear Equilibrium Points in the Relativisti

More information

Fluvial Dynamics. M. I. Bursik ublearns.buffalo.edu October 26, Home Page. Title Page. Contents. Page 1 of 18. Go Back. Full Screen. Close.

Fluvial Dynamics. M. I. Bursik ublearns.buffalo.edu October 26, Home Page. Title Page. Contents. Page 1 of 18. Go Back. Full Screen. Close. Page 1 of 18 Fluvial Dynamics M. I. Bursik ublearns.buffalo.edu October 26, 2008 1. Fluvial Dynamics We want to understand a little of the basic physics of water flow and particle transport, as so much

More information

EFFECT OF PITCH NUMBER IN OVERALL HEAT TRANSFER RATE IN DOUBLE PIPE HELICAL HEAT EXCHANGER

EFFECT OF PITCH NUMBER IN OVERALL HEAT TRANSFER RATE IN DOUBLE PIPE HELICAL HEAT EXCHANGER Volume 116 No. 5 2017, 1-6 ISSN: 1311-8080 (printed version); ISSN: 1314-3395 (on-line version) url: http://www.ijpam.eu ijpam.eu EFFECT OF PITCH NUMBER IN OVERALL HEAT TRANSFER RATE IN DOUBLE PIPE HELICAL

More information

To investigate the relationship between the work done to accelerate a trolley and the energy stored in the moving trolley.

To investigate the relationship between the work done to accelerate a trolley and the energy stored in the moving trolley. SP2h.1 Aelerating trolleys Your teaher may wath to see if you an follow instrutions safely take areful measurements. Introdution The work done y a fore is a measure of the energy transferred when a fore

More information

INFLUENCE OF OPERATING AND CONSTRUCTION PARAMETERS ON THE BEHAVIOR OF HYDRAULIC CYLINDER SUBJECTED TO JERKY MOTION

INFLUENCE OF OPERATING AND CONSTRUCTION PARAMETERS ON THE BEHAVIOR OF HYDRAULIC CYLINDER SUBJECTED TO JERKY MOTION Proeedings of ICFDP 8: 8 th International Congress of Fluid Dynamis & Propulsion Deember 14-17, 006, Sharm El-Shiekh, Sinai, Egypt ICFDP8-EG-154 INFLUENCE OF OPERATING AND CONSTRUCTION PARAMETERS ON THE

More information

Subject: Introduction to Component Matching and Off-Design Operation % % ( (1) R T % (

Subject: Introduction to Component Matching and Off-Design Operation % % ( (1) R T % ( 16.50 Leture 0 Subjet: Introdution to Component Mathing and Off-Design Operation At this point it is well to reflet on whih of the many parameters we have introdued (like M, τ, τ t, ϑ t, f, et.) are free

More information

3.2 CRITICAL DEPTH IN NONRECTANGULAR CHANNELS AND OCCUR- RENCE OF CRITICAL DEPTH

3.2 CRITICAL DEPTH IN NONRECTANGULAR CHANNELS AND OCCUR- RENCE OF CRITICAL DEPTH 3.2 CRITICAL DEPTH IN NONRECTANGULAR CHANNELS AND OCCUR- RENCE OF CRITICAL DEPTH Critical Depth in Non-Rectangular Channels Consider an irregular channel: da w dd dd d Specific energy is defined as: E

More information

The Laws of Acceleration

The Laws of Acceleration The Laws of Aeleration The Relationships between Time, Veloity, and Rate of Aeleration Copyright 2001 Joseph A. Rybzyk Abstrat Presented is a theory in fundamental theoretial physis that establishes the

More information

Special and General Relativity

Special and General Relativity 9/16/009 Speial and General Relativity Inertial referene frame: a referene frame in whih an aeleration is the result of a fore. Examples of Inertial Referene Frames 1. This room. Experiment: Drop a ball.

More information

Hydraulics for Urban Storm Drainage

Hydraulics for Urban Storm Drainage Urban Hydraulics Hydraulics for Urban Storm Drainage Learning objectives: understanding of basic concepts of fluid flow and how to analyze conduit flows, free surface flows. to analyze, hydrostatic pressure

More information

CE 6403 APPLIED HYDRAULIC ENGINEERING UNIT - II GRADUALLY VARIED FLOW

CE 6403 APPLIED HYDRAULIC ENGINEERING UNIT - II GRADUALLY VARIED FLOW CE 6403 APPLIED HYDRAULIC ENGINEERING UNIT - II GRADUALLY VARIED FLOW Dynamic equations of gradually varied and spatially varied flows - Water surface flow profile classifications: Hydraulic Slope, Hydraulic

More information

Chapter 3.8: Energy Dissipators. By Dr. Nuray Denli Tokyay

Chapter 3.8: Energy Dissipators. By Dr. Nuray Denli Tokyay Chapter 3.8: Energy Dissipators By Dr. Nuray Denli Tokyay 3.1 Introduction A stilling basin is a short length of paved channel placed at the foot of a spillway or any other source of supercritical flow

More information

Significance of the Balance-Based Averaging Theory for Application in Energy and Process Engineering

Significance of the Balance-Based Averaging Theory for Application in Energy and Process Engineering Signifiane of the Balane-Based veraging Theory for ppliation in Energy and Proess Engineering Dissertation zur Erlangung des Grades Doktor-Ingenieur der Fakultät für Mashinenbau der Ruhr-Universität Bohum

More information

III. SURFACE PROPERTIES III.A. SURFACE TENSION SURFACE PROPERTIES

III. SURFACE PROPERTIES III.A. SURFACE TENSION SURFACE PROPERTIES III. SURFACE PROPERTIES III.A. SURFACE TENSION GOAL: To investigate the influene of the solution onentration and/or the kind of the solute on the surfae tension INTRODUCTION Liquids tend to adopt shapes

More information

CIE4491 Lecture. Hydraulic design

CIE4491 Lecture. Hydraulic design CIE4491 Lecture. Hydraulic design Marie-claire ten Veldhuis 19-9-013 Delft University of Technology Challenge the future Hydraulic design of urban stormwater systems Focus on sewer pipes Pressurized and

More information

Design of an Adaptive Neural Network Controller for Effective Position Control of Linear Pneumatic Actuators

Design of an Adaptive Neural Network Controller for Effective Position Control of Linear Pneumatic Actuators Researh Artile International Journal of Current Engineering and Tehnology E-ISSN 77 406, P-ISSN 347-56 04 INPRESSCO, All Rights Reserved Available at http://inpresso.om/ategory/ijet Design of an Adaptive

More information

Maximum Entropy and Exponential Families

Maximum Entropy and Exponential Families Maximum Entropy and Exponential Families April 9, 209 Abstrat The goal of this note is to derive the exponential form of probability distribution from more basi onsiderations, in partiular Entropy. It

More information

MODELLING THE POSTPEAK STRESS DISPLACEMENT RELATIONSHIP OF CONCRETE IN UNIAXIAL COMPRESSION

MODELLING THE POSTPEAK STRESS DISPLACEMENT RELATIONSHIP OF CONCRETE IN UNIAXIAL COMPRESSION VIII International Conferene on Frature Mehanis of Conrete and Conrete Strutures FraMCoS-8 J.G.M. Van Mier, G. Ruiz, C. Andrade, R.C. Yu and X.X. Zhang Eds) MODELLING THE POSTPEAK STRESS DISPLACEMENT RELATIONSHIP

More information

SEDIMENT TRANSPORT CALCULATION CONSIDERING COHESIVE EFFECTS AND ITS APPLICATION TO WAVE-INDUCED TOPOGRAPHIC CHANGE

SEDIMENT TRANSPORT CALCULATION CONSIDERING COHESIVE EFFECTS AND ITS APPLICATION TO WAVE-INDUCED TOPOGRAPHIC CHANGE Proeedings of the 7 th International Conferene on Asian and Paifi Coasts (APAC 03) Bali, Indonesia, September 4-6, 03 SEDIMENT TRANSPORT CALCULATION CONSIDERING COHESIVE EFFECTS AND ITS APPLICATION TO

More information

Dr G. I. Ogilvie Lent Term 2005

Dr G. I. Ogilvie Lent Term 2005 Aretion Diss Mathematial Tripos, Part III Dr G. I. Ogilvie Lent Term 2005 1.4. Visous evolution of an aretion dis 1.4.1. Introdution The evolution of an aretion dis is regulated by two onservation laws:

More information