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<br />e
<br />
<br />.
<br />
<br />.
<br />
<br />;
<br />
<br />e~
<br />
<br />where
<br />
<br />MEASUREMENT OF PEAK DISCHARGE AT CULVERTS BY INDIRECT METHODg
<br />
<br />fi
<br />
<br />O=the discharge coefficient,
<br />A,=the flow area at the control section,
<br />V, = the mean velocity in the approach
<br />section,
<br />a,=the velocity-head coefficient at the
<br />approach section, and
<br />h/,_.=thehead loss due to friction between
<br />the approach section and the inlet
<br />=L~(Q'fK1K,), and
<br />K= conveyance = (1.486fn) R'!3A , (6)
<br />
<br />Other notation is evident from figure 1 or it
<br />has been previously explained. The discharge
<br />coefficient, 0, is discussed in detail in the ~ection
<br />entitled "Coefficients of Discharge."
<br />
<br />Type 2 "ow
<br />
<br />Type 2 flow, as shown on figure 2, passes
<br />through critical depth at the culvert outlet,
<br />The headwater-diameter ratio does not exceed
<br />1.5, and the barrel flows partly full. The slope
<br />of the culvert is less than critical, and the tail-
<br />water elevation does not exceed the elevation of
<br />the water surface at the control section, h,.
<br />The discharge equation is
<br />
<br />Q=CA,~2g (hl+ a~" -d,-h"_.-h,,.,} (7)
<br />where
<br />
<br />h/,.3=the head loss due to friction in the
<br />culvert barrel=L(Q'fK,J(,),
<br />
<br />Flow with backwater
<br />
<br />When backwater is the controlling factor in
<br />culvert flow, critical depth cannot occur and the
<br />upstream water-surface elevation for a given
<br />discharge is a function of the surface elevation
<br />of the tailwater. If the culvert flows partly full,
<br />the headwater-diameter ratio is less than 1.5; or
<br />if it flows full, both ends of the culvert are
<br />completely submerged and the headwater-
<br />diameter ratio may be any value greater than
<br />1.0. The two types of flow in this classification
<br />are 3 and 4.
<br />Type 3 flow
<br />
<br />Type 3 flow is tranquil throughout the length
<br />of the culvert, as indicated on figure 2. The
<br />headwater-diameter ratio is less than 1.5, and
<br />
<br />the culvert barrel flows partly full. The tail-
<br />water elevation does not submerge the cuh-ert
<br />outlet, but it does exceed the elevation of crit.;cal
<br />depth at the terminal section.
<br />The lower limit of tailwater must be such that
<br />(1) if the culvert slope is steep enough that
<br />under free-fall conditions critical depth at the
<br />inlet would result from a given elevation of
<br />headwater, the tailwater must be at an elevation
<br />higher than the elevation of critical depth at tbe
<br />inlet; and (2) if the culvert slope is mild enough
<br />that under free-fall conditions critical depth at,
<br />the outlet would result from a given elevation of
<br />headwater, then the tailwater must be at an
<br />elevation higher than the elevation of critical
<br />depth at the outlet.
<br />The discharge equation for this type of flow is
<br />
<br />Q=CA3~2g (h,+ a'~"-h,-h/l-2-h,,_,} (8)
<br />
<br />Type 4 flow
<br />
<br />In this classification the culvert is submerged
<br />by both headwater and tailwater, as is shown
<br />in figure 2. The headwater-diameter ratio can
<br />be anything greater than 1.0. No differentiation
<br />is made between low-head and high-head flow
<br />on this basis for type 4 flow. The culvert flows
<br />full and the discharge may be computed directly
<br />from the energy equation between sections 1
<br />and 4. Thus,
<br />
<br />[h,+h.,=h,+h.,+h'l-2+h,
<br />+h"., +h/3-4 +(h., -h..)],
<br />
<br />where
<br />
<br />h.=head loss due to entrance contraction.
<br />
<br />In the derivation of the discharge formula
<br />shown below, the velocity head at section 1
<br />and the friction loss between sections 1 and 2
<br />and between sections 3 and 4 have been ne-
<br />glected, Between sections 3 and 4 the energy
<br />loss due to sudden expansion is assumed to be
<br />(h.,-h..). Thus,
<br />
<br />h,=h.+h.+h,..,+h."
<br />
<br />or
<br />
<br />Q= OA ~ 2g(h,-h.) , (9)
<br />o 290'n'L
<br />1+ Ro'!3
<br />
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