transient channel
Recently Published Documents


TOTAL DOCUMENTS

23
(FIVE YEARS 3)

H-INDEX

9
(FIVE YEARS 0)

2021 ◽  
Author(s):  
Hansini Vijayaraghavan ◽  
Anna Prado ◽  
Thomas Wiese ◽  
Wolfgang Kellerer


Author(s):  
Ankit Rajkumar Singh ◽  
Andallib Tariq

Abstract Whenever, any engineering system comprising of internally heated channel/tube is exposed to the severe thermal load, the sagging or deflection measurement becomes inevitable task from its safety/design analysis perspective. As an example, in a typical horizontal type nuclear reactor safety study, it is fundamentally required to measure sagging of the channels during a postulated accidental scenario analysis. Unfortunately, measurement of the transient deflection/sagging of the channel under harsh environment at extreme temperatures is a challenging task, and cannot be performed by the means of conventional intrusive approaches. Present study proposes a non-contact digital imaging method with laser generator and bandwidth filter, which is tested to measure the continuous channel sagging in a uniquely designed test-rig. A scaled-down channel setup simulating the horizontal type nuclear reactor is used during the implementation of the present approach for sagging analysis at elevated temperatures. Digital edge detection tool with Canny method is used to extract digital edges from recorded grayscale images, wherein successive images are used to measure transient sagging. Results are compared with post-test channel deflection measurements, and difference in measurement is found to be less than ±10 percent of post-test deflection.



2021 ◽  
pp. 1-27
Author(s):  
Sai C. Mangavelli ◽  
Junlin Yuan ◽  
Giles J. Brereton


Author(s):  
Victor Coppo Leite ◽  
Elia Merzari

Abstract In this article we examine channel flow subject to spatially varying viscosity in the streamwise direction. The Reynolds number is imposed locally with three different ramps. The setup is reminiscent of transient channel flow, but with a space-dependent viscosity rather than a time dependent viscosity. It is also relevant to various applications in nuclear engineering and in particular in test reactors, where the viscosity changes significantly in the streamwise direction, and there is a severe lack of Direct Numerical Simulation (DNS) data to benchmark turbulence models in these conditions. As part of this work we set up a novel benchmark case: the channel is extended in the stream-wise direction up to 20π. The viscosity is kept constant in the first 4π region. This inlet region is used as a cyclic region to obtain a fully developed flow profile at the beginning of the ramping region. In the ramping region the Reynolds number is linearly increased along the channel. The flow is homogenous in the spanwise direction, while it is non-homogenous in the stream-wise and wall-normal direction. We perform here Direct Numerical Simulation (DNS) with Nek5000, a spectral-element computational fluid dynamics (CFD) code developed at Argonne National Laboratory. In this study, specific focus is given to the investigation of turbulence properties and structures in the near-wall region along the flow direction. Turbulent statistics are collected and investigated. Similarly to transient channel flow, the results show that a variation in the Reynolds across a channel does not cause an immediate change in the size of turbulent structures in the ramp region and a delay is in fact observed in both wall shear and friction Reynolds number. The results from the present study are compared with a correlation available in the literature for the friction velocity and as a function of the Reynolds number.



2019 ◽  
Vol 89 (8) ◽  
pp. 815-832 ◽  
Author(s):  
Vamsi Ganti ◽  
Michael P. Lamb ◽  
Austin J. Chadwick

Abstract Erosional surfaces set the architecture of fluvio-deltaic stratigraphy, and they have classically been interpreted in terms of changes in boundary conditions such as climate, tectonics, and base level (allogenic forces). Intrinsic dynamics of sedimentary systems (autogenic dynamics) can also create a rich stratigraphic architecture, and a major knowledge gap exists in parsing the relative roles of autogenic versus allogenic processes. Emerging theoretical and experimental work suggests that backwater hydrodynamics play an important role in driving transient channel incision in river deltas, even those experiencing net aggradation. Here, we identify and quantify two autogenic mechanisms that produce broad erosional surfaces in fluvio-deltaic stratigraphy, namely, floods and avulsions. Using a simple mass-balance model for single-threaded delta channel systems, we show that flood-induced scours begin near the shoreline, and avulsion-induced scours begin at the avulsion site, and both propagate upstream over a distance that scales with the backwater length, bed slope, and bed grain size. We also develop scaling relationships for the maximum scour depths arising from these mechanisms, which are functions of characteristic flow depth and formative flood variability. We test our theoretical predictions using a flume experiment of river delta evolution governed by persistent backwater hydrodynamics under constant relative sea level. Results indicate that autogenic dynamics of backwater-mediated deltas under conditions of constant base level can result in stratigraphic surfaces and shoreline trajectories similar to those often interpreted to represent multiple sea-level cycles. Our work provides a quantitative framework to decouple autogenic and allogenic controls on erosional surfaces preserved in fluvio-deltaic stratigraphy.



Entropy ◽  
2018 ◽  
Vol 20 (5) ◽  
pp. 375 ◽  
Author(s):  
Akshat Mathur ◽  
Mehdi Seddighi ◽  
Shuisheng He


2014 ◽  
Vol 89 ◽  
pp. 111-123 ◽  
Author(s):  
S. Gorji ◽  
M. Seddighi ◽  
C. Ariyaratne ◽  
A.E. Vardy ◽  
T. O’Donoghue ◽  
...  


2013 ◽  
Vol 715 ◽  
pp. 60-102 ◽  
Author(s):  
S. He ◽  
M. Seddighi

AbstractDirect numerical simulations (DNS) are performed of a transient channel flow following a rapid increase of flow rate from an initially turbulent flow. It is shown that a low-Reynolds-number turbulent flow can undergo a process of transition that resembles the laminar–turbulent transition. In response to the rapid increase of flow rate, the flow does not progressively evolve from the initial turbulent structure to a new one, but undergoes a process involving three distinct phases (pre-transition, transition and fully turbulent) that are equivalent to the three regions of the boundary layer bypass transition, namely, the buffeted laminar flow, the intermittent flow and the fully turbulent flow regions. This transient channel flow represents an alternative bypass transition scenario to the free-stream-turbulence (FST) induced transition, whereby the initial flow serving as the disturbance is a low-Reynolds-number turbulent wall shear flow with pre-existing streaky structures. The flow nevertheless undergoes a ‘receptivity’ process during which the initial structures are modulated by a time-developing boundary layer, forming streaks of apparently specific favourable spacing (of about double the new boundary layer thickness) which are elongated streamwise during the pre-transitional period. The structures are stable and the flow is laminar-like initially; but later in the transitional phase, localized turbulent spots are generated which grow spatially, merge with each other and eventually occupy the entire wall surfaces when the flow becomes fully turbulent. It appears that the presence of the initial turbulent structures does not promote early transition when compared with boundary layer transition of similar FST intensity. New turbulent structures first appear at high wavenumbers extending into a lower-wavenumber spectrum later as turbulent spots grow and join together. In line with the transient energy growth theory, the maximum turbulent kinetic energy in the pre-transitional phase grows linearly but only in terms of ${u}^{\ensuremath{\prime} } $, whilst ${v}^{\ensuremath{\prime} } $ and ${w}^{\ensuremath{\prime} } $ remain essentially unchanged. The energy production and dissipation rates are very low at this stage despite the high level of ${u}^{\ensuremath{\prime} } $. The pressure–strain term remains unchanged at that time, but increases rapidly later during transition along with the generation of turbulent spots, hence providing an unambiguous measure for the onset of transition.



Author(s):  
Syed Rameez Naqvi ◽  
Varadan Savulimedu Veeravalli ◽  
Andreas Steininger
Keyword(s):  


Sign in / Sign up

Export Citation Format

Share Document