DISCUSSIONS AND CLOSURES
Discussion of “Case Study: Numerical
Evaluation of Hydraulic Transients in a
Combined Sewer Overflow Tunnel System”
by M. Politano, A. J. Odgaard, and W.
Klecan
October 2007, Vol. 133, No. 10, pp. 1103–1110.
DOI: 10.1061/ASCE0733-94292007133:101103
Jose G. Vasconcelos, M.ASCE
1
; and Steven J. Wright
2
1
Assistant Professor, Dept. of Civil Engineering, Auburn Univ., 208 Har-
bert Engrg. Center, Auburn, AL 36849. E-mail: jvasconcelos@
auburn.edu
2
Prof., Dept. of Civil and Environmental Engineering, Univ. of Michigan,
1351 Beal Ave., Ann Arbor, MI 48109. E-mail: sjwright@engin.
umich.edu
The discussers would like to congratulate the authors for a very
interesting paper, in which the gradual flow regime transition i.e.,
in the absence of a pipe-filling bore front—an outstanding issue
in interface tracking models for flow regime transition—was ad-
dressed. The proposed model is in this regard an improvement on
the family of models presented by Song et al. 1983 and Cardle
and Song 1988, among others. Based on the discussers’ experi-
ence in modeling tunnel systems, gradual-flow regime transitions
should probably be more common than pipe-filling bores, even
though some extreme inflow conditions, which could be very im-
portant for design purposes, may require pipe-filling bore model-
ing.
The discussers would like to make a few comments and raise
some issues:
1. Geysering events are not necessarily characterized solely by
water jets, as investigated by Vasconcelos 2005. Experi-
ments and field evidence indicate that such phenomena could
also be triggered by air pocket expulsion through water-filled
vertical shafts in stormwater systems. Careful consideration
of the air pocket entrapment is required when dealing with
flow-regime transition events.
2. There is already available an alternative to model flow-
regime transition other than Preissmann slot or interface
tracking-based models, namely the TPA model of Vasconce-
los et al. 2006. The TPA model overcomes the limitations
of Preissmann-slot models of modeling subatmospheric
flows, while retaining a single set of equations to simulate
both free-surface and pressurized flows. Indeed as the au-
thors mentioned, flow-regime transition models constructed
with shock-capturing approaches may develop numerical os-
cillations in the vicinity of pipe-filling bores.
However, Vasconcelos et al. 2006 propose an approach
to attenuate such oscillations. More recently, Vasconcelos et
al. 2009 address this issue, and other techniques to attenu-
ate these numerical oscillations are proposed.
3. The discussers doubt that the proposed model would be able
to handle a depressurization scenario in which pressurized
flows are succeeded by free-surface flows. In such cases, the
flow regime interface would be characterized by air intrusion
fronts, which in turn resemble gravity currents. These flows
have been studied by Benjamin 1968, Baines 1991, and
others, and the presented model equations seem unable to
represent such flows at the depressurization interfaces.
4. The discussers would like to know how the proposed model
distinguishes a gradual from an abrupt flow regime transition
interface. Is it based on whether the flow regime transition is
coincident with the location of a bore?
5. Fig. 3 of the original paper indicates that the proposed
model is able to handle open-channel bores. How does the
proposed model test for the formation of such bores within
the computational domain?
6. Fig. 9 of the original paper indicates the formation of en-
trapped air pockets closer to the Clear Creek station at times
1.98 h, 1.99 h, and 2.00 h. Is there any special treatment for
these pockets in the modeling process?
7. How was the value for the acoustic wavespeed of 762 m / s
for the West Area CSO Tunnel System estimated? Also, was
there any calculation of continuity errors in this tunnel
modeling?
References
Baines, W. D. 1991. “Air cavity as gravity currents on slope.” J. Hy-
draul. Eng., 11712, 1600–1615.
Benjamin, T. B. 1968. “Gravity currents and related phenomena.” J.
Fluid Mech., 312, 209–248.
Cardle, J. A., and Song, C. S. S. 1988. “Mathematical modeling of
unsteady flow in storm sewers.” Int. J. Eng. Fluid Mech.,14, 495–
518.
Song, C. S. S., Cardle, J. A., and Leung, K. S. 1983. “Transient mixed-
flow models for storm sewers.” J. Hydraul. Eng., 10911, 1487–
1504.
Vasconcelos, J. G. 2005. “Dynamic approach to the description of flow
regime transition in stormwater systems.” Ph.D. dissertation, Environ-
mental Engineering, The University of Michigan, Ann Arbor, Mich.
Vasconcelos, J. G., Wright, S. J., and Roe, P. L. 2006. “Improved simu-
lation of flow regime transition in sewers: Two-component pressure
approach.” J. Hydraul. Eng., 1326, 553–562.
Vasconcelos, J. G., Wright, S. J., and Roe, P. L. 2009. “Numerical
oscillations in pipe-filing bore predictions by shock-capturing mod-
els.” J. Hydraul. Eng., 1354, 296–305.
Closure to “Case Study: Numerical
Evaluation of Hydraulic Transients in a
Combined Sewer Overflow Tunnel System”
by M. Politano, A. J. Odgaard, and W. Klecan
October 2007,Vol. 133, No. 10, pp. 1103–1110.
DOI: 10.1061/ASCE0733-94292007133:101103
M. Politano
1
; A. J. Odgaard, M.ASCE
2
; and W. Klecan
3
1
Assoc. Research Engineer, IIHR—Hydroscience & Engineering, The
Univ. of Iowa, 300 South Riverside Dr., Iowa City, IA 52242-1585.
E-mail: marcela-politano@uiowa.edu
JOURNAL OF HYDRAULIC ENGINEERING © ASCE / JUNE 2010 / 391
J. Hydraul. Eng. 2010.136:391-391.
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