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32.3 Baffle Stilling Basin - nptel - Indian Institute of Technology Madras

32.3 Baffle Stilling Basin - nptel - Indian Institute of Technology Madras

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Hydraulics Pr<strong>of</strong>. B.S. Thandaveswara<br />

<strong>32.3</strong> <strong>Baffle</strong> <strong>Stilling</strong> <strong>Basin</strong><br />

The baffle sill basin involves a transverse sill <strong>of</strong> height 'h' with a minimum width. For a<br />

given approach flow depth y 1 and approach Froude number F 1 , various types <strong>of</strong> flows<br />

may occur, depending on the relative sill height S = h/ y 1 and the tail water level y t .<br />

Following types <strong>of</strong> jumps are identified:<br />

<strong>Indian</strong> <strong>Institute</strong> <strong>of</strong> <strong>Technology</strong> <strong>Madras</strong><br />

• jump with end <strong>of</strong> roller above sill, (as practically no scour potential it is suitable<br />

for easily erodible beds).<br />

• B - jump with a lower tail water level, a surface boil on the sill and the roller<br />

extending in the tail water, with small erosion mainly along the side walls.<br />

• Minimum B-jump with a secondary roller, and plunging flow beyond the sill that<br />

does not reach the basin bottom, suitable for the channel with rocky beds in the<br />

downstream.<br />

• C-jump with plunging flow that causes inappropriate tailwater flow, and scour<br />

potential,<br />

• Wave type flow with supercritical flow over the sill and unacceptable energy<br />

dissipation.<br />

In case <strong>of</strong> sufficient tail water submergence type A and B-jumps are very effective for<br />

stilling basins. On the other hand, the type - c jump and the wave jump are<br />

unacceptable in view <strong>of</strong> the very poor dissipation <strong>of</strong> the energy. Figure 32.5 shows the<br />

significance <strong>of</strong> tail water submergence in the basin design. This is also an example<br />

representing the cases <strong>of</strong> a slight decrease <strong>of</strong> tailwater level below the sequent depth.<br />

The purpose <strong>of</strong> any baffle element should thus involve a length reduction. Figure shows<br />

the baffle sill basin and the hydraulic jump basin. The sill is defined with the relative<br />

height S = h/ y 1 and the relative sill location<br />

0 s<br />

X<br />

L<br />

srj<br />

s = . The sequent depth ratio required<br />

Lrj<br />

ysb = y −∆y<br />

includes the effect <strong>of</strong> normal hydraulic jump and the influence <strong>of</strong> the sill<br />

(Hager, 1992).


Hydraulics Pr<strong>of</strong>. B.S. Thandaveswara<br />

y1<br />

y1<br />

Lrj<br />

<strong>Indian</strong> <strong>Institute</strong> <strong>of</strong> <strong>Technology</strong> <strong>Madras</strong><br />

Lj<br />

h<br />

y2<br />

Classical hydraulic jump<br />

y2<br />

a) b)<br />

Adequate Tail waterproper<br />

formation <strong>of</strong> the jump<br />

and effective dissipation <strong>of</strong><br />

energy.<br />

y1<br />

y1<br />

Lsrj<br />

Ljb<br />

h<br />

xs bs<br />

c) d)<br />

h<br />

Inadequate Tail waterhence<br />

Submergence is<br />

wanting.<br />

xs = Lrj<br />

<strong>Baffle</strong> sill basin<br />

y2<br />

h<br />

y2<br />

Lsrj ____ h<br />

S = __<br />

,<br />

Figure 32.5 - Definition Sketch for <strong>Stilling</strong> basin with Sill<br />

( ) 2<br />

07 .<br />

∆ Y s = 07 . S + 3S 1−x<br />

s<br />

For any sill height h 1 , minimum approach Froude number F 1min is necessary for the<br />

formation <strong>of</strong> the hydraulic jump, and the corresponding maximum relative sill height S max<br />

for any approach flow Froude number is given by<br />

1 5/ 3<br />

S max = F1<br />

.<br />

6<br />

The relative sill height is normally limited to S max = 2 in practice. It may be noted that the<br />

sill should neither be too small nor too large.<br />

The optimum sill height S opt is<br />

1 25 .<br />

Sopt = 1+ F 1 .<br />

200<br />

y1


Hydraulics Pr<strong>of</strong>. B.S. Thandaveswara<br />

Depending mainly on the relative sill position X s three types <strong>of</strong> jump may form:<br />

I. A-jump X > 08 . ( to 1)<br />

II. B-jump 065 . < X > 08 .<br />

III. Minimum B-jump 055 . < X > 065 .<br />

<strong>Indian</strong> <strong>Institute</strong> <strong>of</strong> <strong>Technology</strong> <strong>Madras</strong><br />

s<br />

s<br />

s<br />

The length <strong>of</strong> the jump L jb from the toe to the end <strong>of</strong> the bottom roller relative to the<br />

Ljb<br />

1/ 3<br />

length <strong>of</strong> the classical jump L j is = 1−06 . S ( 1-Λ)<br />

.<br />

L<br />

j<br />

The length <strong>of</strong> the sill basin jump L jb is marginally less than the length <strong>of</strong> a classical jump<br />

L j for all three types <strong>of</strong> flows mentioned above. A sill basin improves the stabilization <strong>of</strong><br />

a hydraulic jump under variable tailwater and is somewhat shorter than a classical<br />

hydraulic jump.<br />

<strong>Baffle</strong> Block <strong>Basin</strong><br />

For optimum basin flow, the blocks must have an appropriate location and adequate<br />

height to overcome the ineffectiveness or overforcing <strong>of</strong> flow. Basco in 1971 defined the<br />

optimum height <strong>of</strong> the baffle as the ratio <strong>of</strong><br />

given by,<br />

S<br />

h<br />

=<br />

1<br />

opt<br />

opt<br />

y<br />

2<br />

( ) 16 75 F1 −<br />

L jb / h = . + .<br />

S opt<br />

opt<br />

1<br />

= 1+ F1−2 40<br />

( ) 2<br />

and the optimum basin length is<br />

Figure 32.6 shows the basin with the standard USBR blocks, where spacing <strong>of</strong> the<br />

blocks sp is equal to the block width sp= wband<br />

sp<br />

h<br />

= 075 . .


Hydraulics Pr<strong>of</strong>. B.S. Thandaveswara<br />

y<br />

<strong>Indian</strong> <strong>Institute</strong> <strong>of</strong> <strong>Technology</strong> <strong>Madras</strong><br />

1<br />

WB<br />

Xs<br />

a) Longitudinal section<br />

s<br />

p<br />

WB<br />

b) Standard baffles<br />

Figure- 32.6 Typical <strong>Baffle</strong> block basin<br />

A coefficient for representing the force on the blocks P B is given by<br />

Φ P / ⎡ρg w y / 2⎤<br />

2<br />

= B ⎣ b 2 ⎦<br />

for optimum basin performance, the coefficient Φ is<br />

F1<br />

1<br />

Φ opt = +<br />

7 100<br />

1/ 2<br />

⎛ 2 ⎞<br />

and the sequent depth ratio is Y b = ⎜ ⎟ F1−05 .<br />

⎝1+ Φ ⎠<br />

The tail water reduction is above 10% when compared to the classical jump. Type II,<br />

Type III and Type IV basins are shown below.<br />

y 2<br />

h


Hydraulics Pr<strong>of</strong>. B.S. Thandaveswara<br />

<strong>Indian</strong> <strong>Institute</strong> <strong>of</strong> <strong>Technology</strong> <strong>Madras</strong><br />

2y1 min<br />

0.8 y2<br />

Chute blocks<br />

Lb = 4.3 y2<br />

Fractional space<br />

Space = 2.5 w<br />

Lb = 6.1 y2<br />

<strong>Baffle</strong><br />

piers<br />

dentated sill<br />

(a) Type II basin F1 > 4.5<br />

v1 > 18.0 m/s Tail Water (TW) = 0.97 y2<br />

Chute<br />

blocks<br />

Fractional space<br />

h3 = y1(4+F1)/9<br />

End<br />

sill<br />

(b) Type III basin F1 > 4.5<br />

v1 < 18.0 m/s Tail Water (TW) = 0.83 y2<br />

(c) Type IV basin 2.5 F1 < 4.5<br />

Tail Water (TW) = y2<br />

Slope 2:1<br />

Sill optional<br />

h4 = y1(9+F1)/9<br />

h4 = y1(9+Fr1)/9

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