Metal bonded cobaltferrite composites have been shown to be promising candidate materials for use in magnetoelastic stress sensors, due to their large magnetostriction and high sensitivity of magnetization to stress. However previous results have shown that below 60°C" role="presentation" style="box-sizing: borderbox; display: inline; word-wrap: normal; white-space: nowrap; float: none; direction: ltr; max-width: none; max-height: none; min-width: 0px; min-height: 0px; border: 0px; padding: 0px; margin: 0px; color: rgb(51, 51, 51); font-family: Arial, sans-serif; position: relative;">60°C60°C the cobaltferritematerial exhibits substantial magnetomechanical hysteresis. In the current study, measurements indicate that substituting Mn for some of the Fe in the cobaltferrite can lower the Curie temperature of the material while maintaining a suitable magnetostriction for stress sensing applications. These results demonstrate the possibility of optimizing the magnetomechanical hysteresis of cobalt ferrite-based composites for stress sensor applications, through control of the Curie temperature. Metal bonded cobalt ferrite composites have been shown to be promising candidate materials for use in magnetoelastic stress sensors, due to their large magnetostriction and high sensitivity of magnetization to stress. However previous results have shown that below 60°C the cobalt ferrite material exhibits substantial magnetomechanical hysteresis. In the current study, measurements indicate that substituting Mn for some of the Fe in the cobalt ferrite can lower the Curie temperature of the material while maintaining a suitable magnetostriction for stress sensing applications. These results demonstrate the possibility of optimizing the magnetomechanical hysteresis of cobalt ferrite-based composites for stress sensor applications, through control of the Curie temperature. Disciplines Materials Science and Engineering | Physics

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The temperature variation of magnetic anisotropy and coercive field of magnetoelastic manganese-substituted cobaltferrites (CoMnxFe2−xO4 with 0⩽x⩽0.6) was investigated. Major magnetic hysteresis loops were measured for each sample at temperatures over the range 10-400 K, using a superconducting quantum interference device magnetometer. The high-field regimes of the hysteresis loops were modeled using the law of approach to saturation equation, based on the assumption that at sufficiently high field only rotational processes remain, with an additional forced magnetization term that was linear with applied field. The cubic anisotropy constant K1 was calculated from the fitting of the data to the theoretical equation. It was found that anisotropy increases substantially with decreasing temperature from 400 to 150 K, and decreases with increasing Mn content. Below 150 K, it appears that even under a maximum applied field of 5 T, the anisotropy of CoFe2O4 and CoMn0.2Fe1.8O4 is so high as to prevent complete approach to saturation, thereby making the use of the law of approach questionable in these cases. The temperature variation of magnetic anisotropy and coercive field of magnetoelastic manganese-substituted cobalt ferrites ͑CoMn x Fe 2−x O 4 with 0 ഛ x ഛ 0.6͒ was investigated. Major magnetic hysteresis loops were measured for each sample at temperatures over the range 10-400 K, using a superconducting quantum interference device magnetometer. The high-field regimes of the hysteresis loops were modeled using the law of approach to saturation equation, based on the assumption that at sufficiently high field only rotational processes remain, with an additional forced magnetization term that was linear with applied field. The cubic anisotropy constant K 1 was calculated from the fitting of the data to the theoretical equation. It was found that anisotropy increases substantially with decreasing temperature from 400 to 150 K, and decreases with increasing Mn content. Below 150 K, it appears that even under a maximum applied field of 5 T, the anisotropy of CoFe 2 O 4 and CoMn 0.2 Fe 1.8 O 4 is so high as to prevent complete approach to saturation, thereby making the use of the law of approach questionable in these cases.

Controlling adhesion of living animal cells plays a key role in biosensor fabrication, drug-testing technologies, basic biological research, and tissue engineering applications. Current techniques for cell patterning have two primary limitations: (1) they require photolithography, and (2) they are limited to patterning of planar surfaces. Here we demonstrate a simple, precision spraying method for both positive and negative patterning of planar and curved surfaces to achieve cell patterns rapidly and reproducibly. In this method, which we call precision spraying (PS), a polymer solution is aerosolized, focused with sheath airflow through an orifice, and deposited on the substrate using a deposition head to create approximately 25 microm sized features. In positive patterning, adhesive molecules, such as laminin or polyethylenimine (PEI) were patterned on polydimethylsiloxane (PDMS) substrates in a single spraying operation. A variety of animal cell types were found to adhere to the adhesive regions, and avoid the non-adhesive (bare PDMS) regions. In negative patterning, hydrophobic materials, such as polytetrafluoroethylene (PTFE) and PDMS, were patterned on glass substrates. Cells then formed patterns on the exposed glass regions and avoided the hydrophobic regions. Cellular patterns were maintained for up to 2 weeks in the presence of serum, which normally fouls non-adhesive regions. Additionally, we found that precision spraying enabled micropatterning of complex-curved surfaces. Our results show that precision spraying followed by cell plating enables rapid and flexible cellular micropatterning in two simple steps.