All Time Past Year Past 30 Days
Abstract Views 0 0 0
Full Text Views 285 82 7
PDF Downloads 146 64 2

The Icing of an Unheated, Nonrotating Cylinder. Part II. Icing Wind Tunnel Experiments

E. P. LozowskiLow Temperature Laboratory, Division of Mechanical Engineering, National Research Council of Canada, Ottawa, Ontario, Canada KIA OR6

Search for other papers by E. P. Lozowski in
Current site
Google Scholar
PubMed
Close
,
J. R. StallabrassLow Temperature Laboratory, Division of Mechanical Engineering, National Research Council of Canada, Ottawa, Ontario, Canada KIA OR6

Search for other papers by J. R. Stallabrass in
Current site
Google Scholar
PubMed
Close
, and
P. F. HeartyLow Temperature Laboratory, Division of Mechanical Engineering, National Research Council of Canada, Ottawa, Ontario, Canada KIA OR6

Search for other papers by P. F. Hearty in
Current site
Google Scholar
PubMed
Close
Full access

Abstract

An experimental investigation of icing on non-rotating cylinders, under both wet and dry conditions was undertaken. Airspeeds of 30, 61 and 122 m s−1 appropriate to aircraft icing, liquid water contents of 0.4, 0.8 and 1.2 g m−3 and temperatures of − 15, − 8 and − 5°C, were explored. Dry accretions were lenticular or “spearhead” shapes, while wet accretions tended to develop “horns” and stagnation line depressions as the result of the runback of unfrozen water away from the stagnation line and its subsequent freezing further around the perimeter of the cylinder. Comparisons were made between the experimental accretion shapes and those predicted by the model described in Part I. The model performed best under dry growth conditions. Under wet conditions, the model behavior, while qualitatively correct, was unable to exactly duplicate the details of the accretion profiles. Nevertheless, under both dry and wet conditions, the model predictions of the accretion cross-sectional areas, were quite accurate.

Abstract

An experimental investigation of icing on non-rotating cylinders, under both wet and dry conditions was undertaken. Airspeeds of 30, 61 and 122 m s−1 appropriate to aircraft icing, liquid water contents of 0.4, 0.8 and 1.2 g m−3 and temperatures of − 15, − 8 and − 5°C, were explored. Dry accretions were lenticular or “spearhead” shapes, while wet accretions tended to develop “horns” and stagnation line depressions as the result of the runback of unfrozen water away from the stagnation line and its subsequent freezing further around the perimeter of the cylinder. Comparisons were made between the experimental accretion shapes and those predicted by the model described in Part I. The model performed best under dry growth conditions. Under wet conditions, the model behavior, while qualitatively correct, was unable to exactly duplicate the details of the accretion profiles. Nevertheless, under both dry and wet conditions, the model predictions of the accretion cross-sectional areas, were quite accurate.

Save