Abstr:Boundary layer flow and dispersion over isolated hills and valleys

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Application Area 5: Environmental Flows

Application Challenge AC5-05

Abstract

Flow fields around isolated, nominally two-dimensional hills and valleys were investigated in the low speed meteorological wind tunnel at the US Environmental Protection Agency laboratories. An example of the hill case is shown in figure 1; three hills and a corresponding set of three valleys (not covered in this AC document) were studied. A neutrally stable atmospheric boundary layer of height about 1m was simulated and the hills (or valleys) were located some 7-8m downstream, where the flow was reasonably well developed. For the velocity and turbulence measurements carefully calibrated hot wire and hot film probes were used, with particular attention given to the probes’ yaw responses at low velocities. For the steeper hills, where separation occurred in the lee, use was made of a double-ended pitot probe to assess the size of the separation region; thermal anemometry is inaccurate in such regions.

The experiment was originally designed in the context of pollutant dispersion in the atmosphere. Theoretical models for estimating downwind concentration from sources in the vicinity of isolated topographical features were at that time (and still are) not very reliable so the intention was to obtain data suitable for improving understanding, comparing against theoretical (or computational ) models and, hopefully, thus improving such models. In addition to mean flow and turbulence data, therefore, concentration data was obtained both at ground level and at elevation for cases in which a (scalar) pollutant source was located at x=-a, 0 or a (where a is the hill half-length) and, in each case, at various heights. This allowed determination of ‘terrain amplification factors’ – i.e. the ratio of the maximum surface concentration in the presence of the hill to that in its absence – which is a useful practical measure of the influence of the hill, although not the only one.

These flows were not computed using CFD for a number of years subsequent to the experiments but there have more recently been a number of such attempts (see references). It is suggested here that those performed by Apsley as part of his PhD work and subsequently published in the open literature (see references, particularly Castro & Apsley, 1997, hereafter designated as CA) be used for review, largely because this is the only work which includes computation of the scalar concentration field as well as the flow itself. These computations used a finite-volume, incompressible Navier-Stokes solver employing a cartesian velocity decomposition on a staggered grid. Terrain-fitting, curvilinear meshes were used, along with a variety of turbulence models. These were largely the standard k-e model along with varients of it, designed to take better account of the effects of streamline curvature and streamwise strains, both of which are known to degrade the adequacy of the standard k-e model – the latter seriously so. A 2nd order, upwind-biased, flux limiting harmonic advection scheme was used for the convective terms in all equations. This is significantly more accurate than standard upwinding.

This application challenge is a good one for a number of reasons. First, the experimental data is reckoned to be of good quality. Significant care was taken to ensure measurement accuracy both of the velocity and turbulence data and of the concentration data; the smoothed data generated by Trombetti et al (1991) from the original results are particularly convenient.. Secondly, the upstream flow was properly characterised, so that appropriate upstream conditions can be applied in computations. Thirdly, the flow contains difficult features, e.g: rough walls (not easy to model properly); strong adverse pressure gradients (upstream of the steep hills); separation from a curved surface (along with the adverse pressure gradients, a serious test of turbulence models); scalar dispersion (practically important).

Figure 1. Side view of a hill mounted in the simulated atmospheric boundary layer.

Atmospheric boundary layer flow over hills and valleys is an important problem in the atmospheric sciences, not least because the surface drag, which has a major effect on the atmosphere, is significantly altered by surface topography. Despite considerable study, both in the laboratory and in the field, it remains difficult to compute such flows, particularly for cases of steep-sloped topography. Such surface features significantly affect the mean and turbulence fields and thus have an important influence on pollutant dispersion. Theoretical models for the latter are not well developed for cases in which there is topographical influence and CFD is increasingly being used as an alternative, but with little evidence yet of general adequacy.

There are various design or assessment parameters (DOAPs) which could be used. The major interest may, for example, be essentially in the flow itself. One might then choose parameters appropriate to velocity variations generated by the hill, or the presence of separation, for example. These could be the maximum velocity speed-up at x=0 and the location and size of the lee-side separation region, respectively. On the other hand, if the interest is in the downwind pollutant concentration field, one might choose the terrain amplification factor as a measure of the computational accuracy. However, particularly in this latter case, one should be cautious: it is possible to obtain good prediction of the latter for quite the wrong reasons, as a result of the influence of opposing errors. One would not expect to obtain adequate concentration results if the flow field (including turbulence levels, which influence diffusion characteristics) is inadequately predicted.

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Contributors: Ian Castro - University of Southampton

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