HYDRAULIC JUMP AND WEIR FLOW

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HYDRAULIC JUMP AND WEIR FLOW 1

Condition for formation of hydraulic jump When depth of flow is forced to change from a supercritical depth to a subcritical depth Or Froude number decreases from greater than 1.0 to less than 1.0. Jump will not occur when Froude number is less than 1.0 Jump does not occur from subcritical to supercritical flow only vice versa. Figure 14.3 2

y1 supercritical flow y2 subcritical flow 2 y 2 = ( y1 / 2)( 1+ 8N F1 1) Where N F1 is the Froude number at section 1. Note subcritical depth y 2 only depends on y 1 and the Froude number. 3

Figure 14.4 Specific Energy conditions in the Hydraulic jump Loss of energy E 3 1 E2 = y2 y1) / 4 ( y y Theoretical depth after jump alternate depth Actual depth after jump sequent depth Length of jump varies but about 7 times the subcritical depth. 1 2 4

Problem 14.6 Q = 18m 3 /s Rectangular channel = 3m wide Channel unfinished form concrete Hydraulic jump occurs where the depth is 1m = y1. Determine Velocity before jump Depth after jump Velocity after jump Energy dissipated in the jump 5

Solution y 1 = 1m A 1 = 3* 1 = 3m 2 V 1 = 18/3 = 6m/s N = F v gy h y h = A/T For rectangular channel, y h = y Therefore Nf = 1.92 > 1.0 (supercritical flow) Find y2 using the equation y 2 = 2.26 m 2 y 2 = ( y1 / 2)( 1+ 8N F1 1) v 2 = Q/A 2 = 18/(3*2.26) = 2.65 m/s loss of energy is computed using 6

E 3 1 E2 = y2 y1) / 4 ( y y E1 E2 = 0.22 m 1 2 7

Practical applications of hydraulic jumps: Dissipation of energy of water flowing over dams and weirs to prevent possible erosion and scouring due to high velocities Raising water levels in canals to enhance irrigation practices and reduce pumping heads Reducing uplift pressure under the foundations of hydraulic structures Creating special flow conditions to meet certain special needs at control sections gaging stations, flow measurement, flow regulation 8

You could also use it for thrills!!! (not recommended) 9

Types of hydraulic jumps Classified based on flow form, approach Froude number, and energy loss. N = F v gy h (a) Undular jump (1 < Fn1<1.7) Slight undulation Two conjugate depths are close Transition is not abrupt slightly ruffled water surface 10

(b) Weak jump (1.7<Fn1<2.5) Eddies and rollers are formed on the surface Energy loss is small The ratio of final depth to initial depth ~ between 2.0 and 3.1. 11

(c) Oscillating jump (2.5 <Fn1<4.5) Jet oscillates from top to bottom generates surface waves that persist beyond the end of the jump Ratio final depth to initial depth ~ between 3.1 to 5.0 To prevent destructive effects this type of jump should be avoided 12

(d)_stable jump (4.5<Fn1<9) Many advantages Position of jump fixed regardless of downstream conditions Good dissipation of energy Considerable rise in downstream water level Ratio of final to initial depth ~ between 5.9 and 12.0 13

(e) Strong or rough jump (Fn1 > 9) Jump becomes increasingly rough Fn1 should not be allowed to exceed 12 otherwise required stilling basins will be large and massive Ability of jump to dissipate energy is massive Ratio of final to initial depth ~ over 12 and may exceed 20. 14

Uncontrolled Hydraulic jump erosion! http://www.rollanet.org/~conorw/cwome/article6&7.htm Taum Sauk reservoir on Proffit Mountain, Missouri. 80 feet dike 1.5 billion gallons (4,600 acre-feet) of water Water overtopped the dike 15

In 12 minutes after failure, 1.5 billion gallons of water roared down an un-named tributary of the East Fork and straight towards the upstream portion of Johnson's Shut-ins State Park. Although the peak flow of the flood isn't known and may or may not be uncovered by the official investigation, the average flow was 280,000 cubic feet per second, larger than the average flow of the Mississippi River just upstream from its confluence with the Ohio River! The peak flow was likely larger. 16

The flow released during the failure stripped the upper slopes of Proffit Mountain down to bare bedrock. This picture shows the ~600 foot wide break, stripped area of Proffit Mountain, and the upper portions of the lower scour zone. 17

A large scour hole was formed by the hydraulic jump marking the transition between the upper steep portion and the lower, more gradual slopes of Proffit Mountain. The hole is at least 20 feet deep and was likely much larger before the diminishing flows near the end of the flood filled much of it with debris. 18

Weirs & Flumes Devices that can be used to measure open channel flow V notch weir in streamflow Geometry of the section is used to measure the flow 19

Weirs Sharp crested edge Water should flow over as a free jet (nappe) aeration below the nappe Water depth above the edge (H) should be measured at 4H from edge Various types of weirs 20

Rectangular weir Also called suppressed weir Crest length L Crest height above the bottom of channel H c 3H max Minimum head above crest > 0.2 ft Max head above crest < L/3 Q = 3.33 LH 3 / 2 Where Q ft 3 /s and H is in ft. 21

Contracted weir Similar to rectangular but with sides extended inwards by at least 2H max Fluid contracts as it flows over the weir Crest height above the bottom of channel Hc 2H max Minimum head above crest > 0.2 ft Max head above crest < L/3 Q = 3.33( L 0.2H ) H 3/ 2 English units (ft). 22

Cipolletti weir Similar to contracted rectangular weir but with sides sloped outwards. Q = 3.367 LH 3/ 2 23

Triangular weir 24

Especially used for low flow rates since a higher head can be generated compared to rectangular weirs Angle of the weir affects the discharge equations Angles 35 to 120 degrees Typical angles used 60 and 90 degrees Generic equation for an angle Q = 4.28C tan( θ / 2) H 5/ 2 C ~ 0.58. Specific equation for 60 degree notch Q = Equation for 90 degree notch 1.43H 5/ 2 Q = 2.48H 5/ 2 25

Flumes Designed so that flow achieves critical depth within the structure Definite relationship between depth and discharge at critical flow Various types of flumes have been created with specific equations for each Parshall flume - 26

You size the flume based on throat width (6 inches in this case) 27

28

One of the suppliers of flumes http://www.globalw.com/products/flumes.html 29

Table of Dimensions Part # W A 2/3A B C D E F G J K N Price 01-006 1 14-9/32 9-17/32 14 3-21/32 6-19/32 9 3 8 9-1/4 3/4 1-1/8 $568 01-007 2 16-5/16 10-7/8 16 5-5/16 8-13/32 12 4-1/2 10 12-7/8 7/8 1-11/16 $746 01-008 3 18-3/8 12-1/4 18 7 10-3/16 24 6 12 25 1 2-1/4 $921 01-009 6 24-7/16 16-5/16 24 15-1/2 15-5/8 24 12 24 27 3 4-1/2 $1,550 01-010 9 34-5/8 23-1/8 34 15 22-5/8 30 24 18 33 3 4-1/2 $1,978 01-011 12 54 36 52-7/8 24 33-1/4 36 24 36 39 3 9 $3,561 Prices listed are for United States and Canada only. Call or e-mail us for pricing in other countries. Terms and Conditions Table of Flow Data Size 1" 2" 3" 6" 9" 12" Min CFS 0.001 0.001 0.001 0.001 0.005 0.006 Min MGD 0.001 0.001 0.001 0.001 0.003 0.004 Max CFS 0.22 0.68 2.91 6.16 12.51 21.68 30

Max MGD 0.14 0.44 1.88 3.98 8.09 14.01 Complete Flow Table NOTE: Flow tables are only valid to the E (height) measurement of the Parshall Flume. 1" Table 2" Table 3" Table 6" Table 9" Table 12" Table Tracom Flume types Trapezoidal 31

H-type flume Cutthroat flume Montana Flume 32