Momentum equation - nptel - Indian Institute of Technology Madras
Momentum equation - nptel - Indian Institute of Technology Madras
Momentum equation - nptel - Indian Institute of Technology Madras
Create successful ePaper yourself
Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.
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 />
2 2 2<br />
Q y1 Q y1 1 ⎛y ⎞ 2 1<br />
+ − − 0<br />
3 2 2 2 3 ⎜ ⎟ =<br />
gy1b2y1 gb y1 y2 ⎝ y1 ⎠ 2<br />
2 1 2⎛ y ⎞ ⎛ 1 y ⎞ 2 1<br />
F1 + − F1 ⎜ ⎟+ ⎜ ⎟ = 0<br />
2 ⎝y2 ⎠ ⎝ y1 ⎠ 2<br />
2 2⎛ y ⎞ ⎛ 1 y ⎞ 2<br />
2F1 + 1 −2F1 ⎜ ⎟− ⎜ ⎟ = 0<br />
⎝y2 ⎠ ⎝ y1<br />
⎠<br />
( )<br />
2 ⎛y ⎞ 2 2 ⎛ y ⎞ 2<br />
2F1 + 1 ⎜ ⎟−2F1 − ⎜ ⎟ = 0<br />
⎝ y1 ⎠ ⎝ y1<br />
⎠<br />
( )<br />
3<br />
⎛y ⎞ 2 2 ⎛y ⎞ 2 2<br />
⎜ ⎟ − ( 2F1 + 1) ⎜ ⎟+<br />
2F1 = 0<br />
⎝ y1 ⎠ ⎝ y1<br />
⎠<br />
This can be rewritten<br />
as<br />
2<br />
⎡ y2 y ⎤<br />
2 2 y2<br />
⎢ 1 ⎥<br />
y1 y1 y1<br />
⎛<br />
⎜<br />
⎢⎣⎝ ⎞<br />
⎟<br />
⎠<br />
+<br />
⎡<br />
−2F ⎢<br />
⎥⎦⎣<br />
⎤<br />
− 1⎥= 0<br />
⎦<br />
y<br />
1 0 y y uniform flow.<br />
2 ∴ − = ∴ 2 = 1<br />
y1<br />
2<br />
⎛y ⎞ 2 y2<br />
2<br />
⎜ ⎟ + − 1 =<br />
y1 y1<br />
⎝ ⎠<br />
2<br />
y211 2<br />
Hence = = 1+ 8F1 −1<br />
y12 2<br />
2<br />
2<br />
3<br />
2F 0 a quadratic <strong>equation</strong>.<br />
⎛ ⎞ − 1+ 1+ 8F<br />
⎡ ⎤<br />
⎜ ⎟<br />
⎝ ⎠<br />
⎣ ⎦<br />
y2 1 ⎡ ⎤<br />
=<br />
⎢<br />
1+ 8F<br />
2<br />
−1<br />
y ⎣<br />
1 ⎥<br />
1 2<br />
⎦<br />
2<br />
(28.1)<br />
⎛ V1<br />
⎞<br />
in which y2, y1 are sequent and initial depths respectively and F= 1 ⎜ ⎟ is the initial<br />
⎜ gy ⎟<br />
⎝ 1 ⎠<br />
Froude number. Equation 28.1 has been verified by many investigators experimentally<br />
and <strong>of</strong>ten a ratio lower than the one calculated by the <strong>equation</strong> has been recorded.<br />
Belanger , did not consider the bed shear force while deriving Eq. 28.1. Rajaratnam in