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Cited by 85 publications
(55 citation statements)
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“…5a, a sharp peak appears in each of the power spectra of fluctuating velocities at Y=B 1:31-2:6 when no element is applied. The frequency at the peak is fB=V 1 0:13, close to the Strouhal number measured by other authors [9,10]. On the other hand, when vortex shedding is suppressed, the velocity fluctuations at all points are weakened and no sharp peaks appear in the power spectra (Fig.…”
Section: Resultssupporting
confidence: 84%
“…5a, a sharp peak appears in each of the power spectra of fluctuating velocities at Y=B 1:31-2:6 when no element is applied. The frequency at the peak is fB=V 1 0:13, close to the Strouhal number measured by other authors [9,10]. On the other hand, when vortex shedding is suppressed, the velocity fluctuations at all points are weakened and no sharp peaks appear in the power spectra (Fig.…”
Section: Resultssupporting
confidence: 84%
“…Also, a series of time-and spanwise-averaged resolved velocity and turbulent stresses are provided for comparison with experiments. Okajima (1982) [18], Igarashi (1984) [11] and Norberg (1993) [17] the Strouhal number is…”
Section: Resultsmentioning
confidence: 99%
“…This trend is being currently developed. Thus, a certain progress is achieved in the field of the experimental and numerical calculations for relatively simple blunt bodies, such as a cube in a boundary layer, a long square prism, and some others [1][2][3][4][5][6][7][8][9][10][11]. Still, little is known at present about the interaction between few buildings and their arrangement effect on the airflow interference.…”
Section: Introductionmentioning
confidence: 99%