Abstract

Fabricating aluminium surfaces with superhydrophobic and ice-repellent properties present nowadays a challenging task. In this work, multifunctional structures are manufactured by direct laser writing and direct laser interference patterning methods using pulsed infrared laser radiation (1064 nm). Different periodic patterns with feature sizes ranging from 7.0 to 50.0 µm are produced. In addition, hierarchical textures are produced combining both mentioned laser based methods. Water contact angle tests at room temperature showed that all produced patterns reached the superhydrophobic state after 13 to 16 days. In addition, these experiments were repeated at substrate temperatures from −30 °C to 80 °C allowing to determine three wettability behaviours as a function of the temperature. The patterned surfaces also showed ice-repellent properties characterized by a near three-fold increase in the droplets freezing times compared to the untreated samples. Using finite element simulations, it was found that the main reason behind the ice-prevention is the change in the droplet geometrical shape due to the hydrophobic nature of the treated surfaces. Finally, dynamic tests of droplets imping the treated aluminium surfaces cooled down to −20 °C revealed that only on the hierarchically patterned surface, the droplets were able to bounce off the substrate.

Highlights

  • 2 mm thick pure aluminium (Al 2024) sheets were cut into 50 mm × 50 mm pieces

  • 14 ns pulse durations were used and the repetition rate was set to 30 kHz

  • The triangular-like surface structures processed by this setup consist of 3 sequentially formed line-like structures, whose orientation was each time rotated by 60°

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Summary

Introduction

The structured samples were stored under atmospheric conditions and any additional treatment was performed[43]. The samples were processed using a laser surface texturing workstation (GF machining solutions P 600), which implements DLW technology (Fig. 9a). 14 ns pulse durations were used and the repetition rate was set to 30 kHz. The beam was focused onto the sample using a 254 mm focal length F-theta objective, obtaining a spot with a diameter of 70 μm.

Results
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