Concept:
Flexibility of a module/ canal outlet: Flexibility is defined as the ratio of the rate of change of discharge of the outlet to the rate of change of discharge of the distributary channel. Thus \({\rm{F}} = \frac{{{\rm{dq}}/{\rm{q}}}}{{{\rm{dQ}}/{\rm{Q}}}}\)
where F = Flexibility of the outlet; q = Discharge passing through the outlet; Q = Discharge in the distributary channel.
If H is the head acting on the outlet, the discharge through the outlet may be expressed as \({\rm{q}} = {\rm{C}}{{\rm{H}}^{\rm{m}}}\)
where, C and m are constants depend upon the type of outlet.
Similarly, the discharge passing down the distributary channel may be expressed as \({\rm{Q}} = {\rm{K}}{{\rm{y}}^{\rm{n}}}\) where K and n are constants and y is the depth of water in the distributary.
By differentiating it can be obtained that, \(\frac{{{\rm{dq}}}}{{\rm{q}}} = {\rm{m}}\frac{{{\rm{dH}}}}{{\rm{H}}}{\rm{\;\;\;and\;\;}}\frac{{{\rm{dQ}}}}{{\rm{Q}}} = {\rm{n}}\frac{{{\rm{dy}}}}{{\rm{y}}}{\rm{\;\;\;\;\;}}\therefore {\rm{F}} = \frac{{\rm{m}}}{{\rm{n}}}\frac{{\rm{y}}}{{\rm{H}}}\frac{{{\rm{dH}}}}{{{\rm{dy}}}}\)
But since a change in the head working on the outlet (dH) would result in an equal change in the water depth of the distributary (dy), hence dy = dH.
\(\therefore {\bf{F}} = \frac{{\bf{m}}}{{\bf{n}}}\frac{{\bf{y}}}{{\bf{H}}}\)
Calculation:
Given, flow is proportional to \({{\rm{y}}^{5/3}}\) in the channel. Hence n = 5/3.
Also, for a weir type outlet flow is proportional to \({{\rm{H}}^{3/2}}\). Hence m = 3/2.
Flexibility of the module, F = 1.15; water depth in the channel, y = 3.5 m.
\(\therefore {\rm{F}} = \frac{{\rm{m}}}{{\rm{n}}}\frac{{\rm{y}}}{{\rm{H}}}{\rm{\;}} \Rightarrow 1.15 = \frac{{\frac{3}{2}}}{{\frac{5}{3}}} \times \frac{{3.5}}{{\rm{H}}}{\rm{\;\;\;}}\therefore {\rm{H}} = 2.74{\rm{\;m}}\)
Important point:
For a weir type outlet flow is proportional to \({{\bf{H}}^{3/2}}\).
For an orifice type outlet flow is proportional to \({{\bf{H}}^{1/2}}\).