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Specific energy from alternate depths

Short answer

Equate the specific energy expressions for alternate depths y1 and y2, cancel (y2−y1), and substitute the resulting q²/(2g) into E. This gives E = (y1^2 + y1 y2 + y2^2) / (y1 + y2).

If y1y_1 and y2y_2 are alternate depths in rectangular channel show that specific energy E=y12+y1y2+y22(y1+y2)E = \frac{y_1^2 + y_1 y_2 + y_2^2}{(y_1 + y_2)}.

Set-up

For a rectangular channel with discharge qq per unit width, two alternate depths y1y_1 and y2y_2 have the same specific energy EE:

E=y1+q22gy12=y2+q22gy22(1)E=y_1+\frac{q^2}{2gy_1^2}=y_2+\frac{q^2}{2gy_2^2}\qquad(1)

Eliminate qq

From the equality in (1):

y2−y1=q22g(1y12−1y22)=q22g (y2−y1)(y2+y1)y12y22y_2-y_1=\frac{q^2}{2g}\left(\frac{1}{y_1^2}-\frac{1}{y_2^2}\right)=\frac{q^2}{2g}\,\frac{(y_2-y_1)(y_2+y_1)}{y_1^2y_2^2}

Cancelling (y2−y1)≠0(y_2-y_1)\neq0:

q22g=y12y22y1+y2(2)\frac{q^2}{2g}=\frac{y_1^2y_2^2}{y_1+y_2}\qquad(2)

Specific energy

Substitute (2) into E=y1+q22gy12E=y_1+\dfrac{q^2}{2gy_1^2}:

E=y1+y12y22(y1+y2)y12=y1+y22y1+y2E=y_1+\frac{y_1^2y_2^2}{(y_1+y_2)y_1^2}=y_1+\frac{y_2^2}{y_1+y_2} E=y1(y1+y2)+y22y1+y2E=\frac{y_1(y_1+y_2)+y_2^2}{y_1+y_2} E=y12+y1y2+y22y1+y2\boxed{E=\frac{y_1^2+y_1y_2+y_2^2}{y_1+y_2}}

Hence proved.

✓ Answer checked by Claude Opus 5.5 (high effort)

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