Mechanical Engineering - Research Publications

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    Structure Inclination Angles in the Convective Atmospheric Surface Layer
    Chauhan, K ; Hutchins, N ; Monty, J ; Marusic, I (SPRINGER, 2013-04)
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    Towards Reconciling the Large-Scale Structure of Turbulent Boundary Layers in the Atmosphere and Laboratory
    Hutchins, N ; Chauhan, K ; Marusic, I ; Monty, J ; Klewicki, J (SPRINGER, 2012-11)
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    Spatial averaging of velocity measurements in wall-bounded turbulence: single hot-wires
    Philip, J ; Hutchins, N ; Monty, JP ; Marusic, I (IOP Publishing Ltd, 2013-11)
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    Spatial averaging of streamwise and spanwise velocity measurements in wall-bounded turbulence using ν- and x-probes
    Philip, J ; Baidya, R ; Hutchins, N ; Monty, JP ; Marusic, I (IOP PUBLISHING LTD, 2013-11)
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    The quiescent core of turbulent channel flow
    Kwon, YS ; Philip, J ; de Silva, CM ; Hutchins, N ; Monty, JP (CAMBRIDGE UNIV PRESS, 2014-07)
    Abstract The identification of uniform momentum zones in wall-turbulence, introduced by Adrian, Meinhart & Tomkins (J. Fluid Mech., vol. 422, 2000, pp. 1–54) has been applied to turbulent channel flow, revealing a large ‘core’ region having high and uniform velocity magnitude. Examination of the core reveals that it is a region of relatively weak turbulence levels. For channel flow in the range $\def \xmlpi #1{}\def \mathsfbi #1{\boldsymbol {\mathsf {#1}}}\let \le =\leqslant \let \leq =\leqslant \let \ge =\geqslant \let \geq =\geqslant \def \Pr {\mathit {Pr}}\def \Fr {\mathit {Fr}}\def \Rey {\mathit {Re}}Re_{\tau } = 1000\text {--}4000$, it was found that the ‘core’ is identifiable by regions bounded by the continuous isocontour lines of the streamwise velocity at $0.95U_{CL}$ (95 % of the centreline velocity). A detailed investigation into the properties of the core has revealed it has a large-scale oscillation which is predominantly anti-symmetric with respect to the channel centreline as it moves through the channel, and there is a distinct jump in turbulence statistics as the core boundary is crossed. It is concluded that the edge of the core demarcates a shear layer of relatively intense vorticity such that the interior of the core contains weakly varying, very low-level turbulence (relative to the flow closer to the wall). Although channel flows are generally referred to as ‘fully turbulent’, these findings suggest there exists a relatively large and ‘quiescent’ core region with a boundary qualitatively similar to the turbulent/non-turbulent interface of boundary layers, jets and wakes.
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    Numerical investigation of the behaviour of wall shear stress in three-dimensional pulsatile stenotic flows
    Li, S ; Chin, C ; Barlis, P ; MARUSIC, I ; Ooi, A (Australasian Fluid Mechanics Society (AFMS), 2014)