Open Channel Flow Gradually Varied Flow (Cont)
Example: (continued) To
remain on the specific energy diagram for q = 6 ft2/sec and
achieve critical conditions imagine inserting an artificial bump in the floor
of the channel as shown below to reach critical
flow at the highest point on the artificial bump. |
|
The
energy equation between stations 1 and c is y1 + V12/2g
+ z1 = yc + Vc2/2g
+ zc Or
(since z1 = 0) y1 + V12/2g
= yc + Vc2/2g
+ zc
and E1 = Ec
+ zc From
the specific energy diagram, Ec = Emin =
1.56 ft. |
Thus
with a bump of height zc
= E1 - Ec
= 2.59 – 1.56 =
1.03 ft the flow could then
reach supercritical flow where Fr
> 1 and thus the downstream
elevation of
the free surface, y2b, with the bump (and critical flow at the
apex of the bump) is y2b =
0.55 ft as shown on the specific energy diagram. |
Click
here to move on to a discussion of rapidly varying flow (hydraulic jump). |
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